MATSE 202: Introduction to Polymer Materials User account menu
MATSE 202: Introduction to Polymer Materials User account menu mjg8Welcome to MATSE 202, Introduction to Polymer Materials! This course will show you the basic principles necessary to understand structure-property relations in engineering materials. We assume you will have a basic knowledge of general physics, general chemistry, and mathematics. This course will assist you in obtaining a wide knowledge of modern challenges to the application of modern materials. Registered students should log in to the site using the link above.
Quick Facts about MATSE 202
- Instructor: Lourdes Bobbio, Assistant Teaching Professor in the Department of Materials Science and Engineering.
- Overview - Materials made from many types of natural organic materials, (cotton, wool, hemp, leather, etc.) have been with us throughout recorded history and have played crucial roles in the rise of civilizations and the economies of tribes and nations. Over the course of the last 100 years or so, the development of synthetic organic materials, particularly polymers, has transformed the way we live. Modern transportation systems, much of contemporary medicine and the entire electronics and computer industry would not be possible without these materials. In order to understand their nature and provide a basis for a more in-depth understanding of these materials provided by courses with a more specific focus, why they are ubiquitous in modern society, this course will provide students with a basic knowledge of the structure, synthesis and properties and processing of these materials, starting with a review of atomic and molecular structure and proceeding through basic elements of the chemical synthesis, structure, mechanical properties and processing of these materials. A comparison will also be made between the mechanical properties of “hard” inorganic materials such as metals and ceramics and “soft” organic materials such as polymers. The primary intended audience is undergraduates in Materials Science and Engineering. This course will provide a necessary overview of organic materials for those students who will focus on inorganic materials in the major and also provide an introduction to organic materials for those students who will specialize in polymers and other organic materials. It is also anticipated that students in other disciplines who want to obtain an overview of the science and engineering of organic materials would want to take this course.
- Learning Environment - This website provides the primary instructional materials for the course. The Resources menu links to important supporting materials, while the Lessons menu links to the course lessons. Canvas, Penn State's course management system, is used to support the delivery of this course as well, as it provides the primary communications, calendaring, and submission tools for the course.
Lesson 1: Introduction to Polymers / Polymer Size / Molar Mass
Lesson 1: Introduction to Polymers / Polymer Size / Molar Mass mjg8The links below provide an outline of the material for this lesson. Be sure to carefully read through the entire lesson before submitting your assignments.
Overview/Checklist
Overview/Checklist mrs110Overview
When you think of the word “polymer”, what do you envision — what comes to mind? My guess is that you immediately think “plastics”. Indeed, the materials we call plastics are polymers, but not all polymers are plastics, not by a long shot! Through this course, we will discover how diverse polymer materials really are, in terms of both their chemistry and structure and explore some of the unique properties that make polymers so useful in our daily lives.
Take a moment and look around you — can you identify some materials that are made of polymers? Perhaps you are wearing a shirt that has cotton (a natural polymer, cellulose) or pants that are stretchy because they have Spandex (a synthetic polymer)? Are you wearing contacts or glasses? Both are polymers — contact lenses are made of crosslinked 2-hydroxyethylmethacrylate and the lenses of most glasses are polycarbonate. Do you have hair and fingernails? (I hope so!) They are made of keratin, another polymer. You are “you” because of your DNA — yet another example of a polymer! In fact, it may be hard for you to find materials around you that aren’t made of polymers, at least in part. Polymer materials have revolutionized our world — don’t you want to know what they are and why they’re so special?

This is the root segment of the polymer shown above that is used to make contact lenses.
(Use your mouse to manipulate the interactive molecular diagram.)
Learning Outcomes
By the end of this lesson, you should be able to:
- Provide examples of polymer materials in daily life.
- Define monomer, dimer, trimer, oligomer, polymer.
- Describe the difference between monomer and repeat unit.
- Define and compare homopolymer, copolymer, and blend.
- Draw skeletal structures of linear polymers, branched polymers, network polymer.
- Compare statistical copolymer, random copolymer, alternating copolymer, block copolymer, graft copolymer, and draw schematics of each.
- Compare and contrast the properties and structure of thermoplastics, elastomers, thermosets.
- Define glass transition temperature and melting temperature, compare and contrast.
- Calculate the degree of polymerization
- Calculate the mean repeat unit molar mass
- Calculate and contrast number average molar mass, weight-average molar mass
- Define and calculate molar mass dispersity
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 1 | Continue navigating the online material. |
| To Read | Chapter 1 - Concepts and Nomenclature
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 1 (Practice) | Registered students can access the homework assignment in the Lesson 1 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Perspective on this Course and what I would like you to take from it
Perspective on this Course and what I would like you to take from it ksc17The name of this course is “Introduction to Polymer Materials”. Let’s break it down.
Introduction:
I assume that this is the first class you have ever had teaches you what a polymer is – no background knowledge about polymers specifically is needed for this course. That being said, this course builds upon basic principles in general chemistry, organic chemistry, and math that you will need to know.
Polymer:
What is it? You’ll find out soon!
Materials:
This class is not a polymer “physics” course, nor is it a polymer “chemistry” course – it’s a polymer materials course. To me, “materials” means that we are going to emphasize an understanding of how the molecular, atomic level structure of a polymer affects its macroscale properties as a material. This structure – functional relationship, as you will see, is especially important and fascinating for polymers. And, we are going to emphasize not just the fundamental science, but also delve into some applications and explore how these unique properties of polymers are useful.
Within the “materials” world, you may hear the distinction “soft” versus “hard” materials. Typically, one would lump inorganic materials like metals or ceramics into “hard” materials that are strong and tough, while polymers and other organic materials evoke thoughts of “soft” materials – materials that are squishy, flexible, and weak. And while maybe this categorization is applicable to many materials, there are numerous cases in which these assumptions fail. For example, mercury is a metal – but it’s a liquid (a soft material). Kevlar is a polymer used for making many products including bullet proof vests, but it is extremely strong – stronger than steel in fact. Diamond, one of the hardest materials known to man, is organic and made entirely of carbon. So dispel any preconceived notions about the physical properties of polymers – in fact, one of the unique aspects of polymers that makes them so useful is how tunable and diverse the physical properties are. We will discuss in detail how the physical properties of a polymer are related to the chemistry and molecular structure of a polymer.
Brief History of Polymers
Brief History of Polymers mjg8Given how ubiquitous polymers are in our lives today, it’s rather incredible to think that the concept of a polymer did not exist until relatively recently. People used to think that polymer materials were actually colloids – they described the material properties they observed by saying that there were “lots of small molecules that were interacting strongly with each other”. If you told scientists 100 years ago that there were actually really long, huge, molecules in there that were strung together with covalent bonds, they would have said you were crazy. The concept of such “macro molecules” just did not exist. So even though people have been using polymers for millennia (wood, silk etc.) and even more recently (do you know those really old telephones made of Bakelite?) – the concept of a polymer did not exist until Staudinger came along in the 1920s – it’s that recent! So it also just goes to show you that a lot of materials science, in terms of applications – you can get pretty far sometimes without understanding the fundamentals, but once people understood polymers on a molecular level, both research and applications exploded.
As stated previously, natural polymers have been used for ages – wood and cotton, for example, are made of natural polymer. But the earliest examples of actual polymer chemistry really start in the 1830s, when people began experimenting with reactions of cotton – cotton, of course, being cellulose. This work led to the discovery of various nitrated cellulose products. Nitrocellulose, also called Celluloid, was used as an early replacement material for billiard balls. At the time, billiard balls were made from elephant ivory, and it was getting really expensive (and environmentally unsustainable), so there was a push to find a suitable substitute. The problem was that the “sound” billiard balls made when they hit each other was really important, and difficult to replicate in other materials. John Wesley Hyatt used one of these modified cellulose polymers to create billiard balls, and it was quite successful! However, there was a slight problem with nitrated cellulose polymers in that there were quite flammable and legend has it that occasionally the billiard balls exploded! So clearly, more work needed to be done. Along came Bakelite – which is the first example of a truly synthetic polymer (the rest were just modifications of cellulose). Bakelite, formed from the condensation reaction of phenol with formaldehyde, became hugely popular – perhaps you have seen products with Bakelite, such as those old telephones. Keep in mind that all this time, people still didn’t really know what a polymer was.
Hermann Staudinger was the first to suggest in 1920 that a polymer is actually a very large molecule, a macromolecule, where the atoms in the molecule were held together by covalent bonds. Recall from general chemistry that a covalent bond is made when atoms share their electrons – this is distinct from a simple attraction between molecules, which is what up until this point, was what everyone thought was what was giving these materials their unique properties. The general consensus was that the materials were simply colloids, where the particles were small molecules held together by attractive intermolecular forces. So this idea that there was actually a giant molecule in there was at the time incomprehensible. It took over a decade for Staudinger’s ideas to fully catch on, and he received the Nobel Prize for his contributions in 1953.
There have been lots of amazing discoveries about polymers since then. For example, even more recently, conductive polymers were discovered – again, at the time, it was difficult for people to believe that an organic material like a polymer could be conductive like a metal, but it's true! Polymers have found even more uses than you could imagine. They are replacing traditional metals and semiconductors, they are being used in solar cells and electronics. There are polymer formulations that are being used in composites for building materials, medicine, drug delivery, adhesives, paints, packaging, clothing. Everywhere.
What is a polymer?
What is a polymer? ksc17As just mentioned, a polymer is a large macromolecule. The word “polymer” can be broken down into the Greek components: poly (many) + mer (part). “One part” would then be called a monomer, “two parts” would be a dimer, “three parts” a trimer, “a few parts” is an oligomer. Polymers can be made of a single repeating unit, over and over, there can be many different monomers in a polymer, you can have ordered repeats, random repeats, there are infinite combinations, and we will talk about the structure of the polymer in detail.
To create a polymer, imagine linking together a bunch of monomer units by sequentially reacting each monomer together. Table 1.1 in the textbook shows examples of chemical structures of common monomers and the polymers that result from their polymerization. Notice the nomenclature for how we name the polymer from the monomer, also pay attention to the notation used for describing the repeat unit of the polymer, which is the structure appearing in the brackets [ ]. Let’s use styrene as an example (Figure 1.5).
Styrene is the name of the monomer, but the repeat unit is the part that is “repeated” (in the brackets) that make up the polymer. The repeat unit is not necessarily the same as the monomer; a repeat unit can be made from multiple monomers for example. If the number of atoms, and hence the molecular weight, of the monomer is the same as the repeat unit, then we call this a polyaddition polymerization. However, the number of atoms in the repeat unit is not always the same as the monomer, if there are chemical byproducts of the polymerization reaction (and we would call this a polycondensation polymerization). A good example of this would be nylon 6,6 produced from the polymerization of hexamethylenediamine and adipic acid (Figure 1.6). Notice that the repeat unit of nylon 6,6 is a combination of both monomers, and that some atoms were lost during the polymerization so that the chemical structure of the repeat unit is not just the simple addition of both monomers; we have lost H2O in this reaction. Can you identify the bond formed between the hexamethylenediamine and the adipic acid in the nylon polymer?
Polymer Classifications
Polymer Classifications mxw142Depending on how many different monomers are combined into a polymer, and in what order and structure, we have different ways of generally classifying polymers (Table 1.2 in text). If the polymer is made up of a single monomer, we call it a homopolymer (Figure 1.7) (e.g., if our monomer is A, the polymer would be poly(A)). If a polymer is derived from the polymerization of multiple different monomers, we call it a copolymer (Figure 1.8) (e.g., if our monomers are A and B, our polymer would be poly(A-co-B). There are many varieties of copolymers. If the positions of monomers is randomly distributed within the polymer, then we call that poly(A-ran-B). Here, “random” does not mean the same thing as “I didn’t intentionally put the monomers in a specific order”; to be random, there truly has to be a random distribution over the entire length of the polymer, which in many cases does not happen even if you do not intentionally control monomer order. More often, “statistical” is correct; since each monomer may have a different reactivity, one monomer may be more readily incorporated in the polymer than the other and so the distribution of each monomer along the polymer MAY be different. So in the cases where the monomers follow such statistical distributions (that are not random) we call them statistical copolymers, poly(A-stat-B). Figure 1.8 shows drawings of alternating copolymers poly(A-alt-B), block copolymers poly(A-block-B), and graft copolymers polyA-graft-polyB. A blend is a mixture of different polymers.
Skeletal Structure
Skeletal Structure mxw142So now we know that monomers can be ‘strung’ together to form a long molecule called a polymer. Perhaps you are imaging that it looks like a tiny piece of string or spaghetti – and in many cases, we can simplify the drawing of the polymer by just drawing the skeletal structure as a squiggly line. In such drawings of skeletal structures, like those shown in Figure 1.9, we don’t draw out the specific chemical structure, but the lines are supposed to represent the polymer backbone and can help us visualize higher order structure. Because a polymer doesn’t just have to be a linear – it can be much more complicated than that. It can be branched – like a tree – or it can be network, where all the strings are connected to each other at linking points called crosslinks. The skeletal structure of a polymer significantly affects its properties. For example, network polymers tend to hold their 3D shape much better than linear polymers; can you imagine trying to build a sculpture out of spaghetti?

Introduction to Polymers, Third Edition, CRC Press, 2011.
In addition to classifying polymers by their chemical structure, we also classify them based on their physical properties (Figure 1.3 in the text). There are three main types: thermoplastics, elastomers, and thermosets. Elastomers are stretchy – think “elastic”, like a rubber band. They can be stretched and deformed and return to their original shape because their 3D structure is held together by crosslinks (i.e. most elastomers are network polymers). Their unique properties are a function of their 3D network structure. Things like crosslink density affect their macroscale material properties. Thermosets are rigid that usually have a very high degree of crosslinking. When they are heated, they don’t often flow or soften, they usually just degrade (i.e., the bonds in the polymer are broken). This is in contrast to thermoplastics or thermosoftening polymers, which do flow upon heating. Thermoplastics are typically linear or branched and do not have that network structure to hold their shape (hence they flow when heated). Most commercial polymers are thermoplastics. They can be crystalline, semi-crystalline, or amorphous. Crystalline phases have a melting temperature (Tm). Amorphous phases can’t really “melt” because they are already amorphous (it’s not considered a phase transition), so we use the term glass transition temperature (Tg) to characterize their softening point. Tg might be a range of temperature over which the transition occurs.
Some polymers have characteristics of more than one of these classes. In a sense, it’s a continuum. For example, some elastomers can also be characterized either as a thermoplastic or thermoset.
PROBLEM 1
If a polymer becomes more flexible, then how do you think Tg will change?
- Increase
- Decrease
- Stay the same
ANSWER
B. Decrease
PROBLEM 2
If intermolecular interactions between polymers increase, then how will Tg change?
- Increase
- Decrease
- Stay the same
ANSWER 2
A. Increase
How big is a polymer?
How big is a polymer? mjg8Usually, "short" polymers are called oligomers. When we start getting to tens, hundreds, thousands of repeat units or more, we have polymers. They can be huge. Remember back to general chemistry, where you learned how to calculate the molar mass of a molecule? Similarly, we can describe the "size" of a polymer using molar mass (or molecular weight) which is typically defined in units of g/mol and abbreviated as "M". Another way of describing the size of a polymer is by its degree of polymerization. Degree of polymerization (described by "x") is the number of repeat units in a polymer. If we know the molar mass of a polymer, how can we figure out the degree of polymerization? Similarly, if we know degree of polymerization, how can we figure out molar mass? All we need to know is the molar mass of the repeat unit!
Let us set up this relationship, where the new variable M0 is the molar mass of the repeat unit:
Where:
- = molar mass
- = degree of polymerization
- = molar mass of the repeat unit
We see that the total molar mass of the polymer is just a function of the degree of polymerization and the molar mass of the repeat unit.
PROBLEM
What is the molar mass of a polymer with degree of polymerization and repeat unit molar mass of 125 g/mol?
ANSWER
=
PROBLEM 2
A polymer with molar mass of 35,200 g/mol. has a degree of polymerization of 800. Which polymer, of the ones shown below, could it be?

ANSWER 2
D. poly(vinyl alcohol)

PROBLEM 3
What is the molar mass of polyethylene (shown below) which has a degree of polymerization of 100?

ANSWER 3
PROBLEM 4
The following monomer is polymerized (condensation polymerization with loss of water). If the degree of polymerization is 100, what is the molar mass of the polymer?

ANSWER 4
= 7,200 g/mol
- First, draw the polymer in terms of the repeat unit:

- Determine the molecular formula of the repeat unit:
3 Carbon, 2 Oxygen, 4 Hydrogen - Calculate the molar mass of the repeat unit, :
3 (12 g/mol) + 2 (16 g/mol) + 4 (1 g/mol) = 72 g/mol - Calculate polymer molar mass, :
What if our polymer has more than one monomer, or more than one type of repeat unit? In that case, we define the mean of the copolymer as just a weighted average of the repeat unit, where the weights are the mole fraction (X) of each type of repeat unit.
Where:
- = molar mass
- = degree of polymerization
- = molar mass of the repeat unit
Example:
What is the mean molar mass of the repeat unit for a copolymer comprised of 20 mol% styrene, 30 mol% methyl methacrylate, and 50% vinyl chloride? The chemical structures of the monomers and the resulting copolymer are shown below.

PROBLEM 5
A statistical copolymer formed from addition polymerization of acrylamide (71 g/mol) and methyl methacrylate (100 g/mol) has a molar mass of 11,955 g/mol with degree of polymerization of 150. What is the molar fraction of acrylamide?
ANSWER 5
= 0.7
- Solve for molar mass of repeat unit using :
- Set up expression to solve for mole fraction of acrylamide:
Molar Mass Distributions
Molar Mass Distributions mjg8When you first learned about the molar mass of molecules, you learned that the molar mass is linked to the identity of the compound; for example, H2O always had a molar mass of 18 g/mol. If the molar mass wasn't 18g/mol, it couldn't be water! The situation is very different for polymers. Take polypropylene, for example:

The molar mass of this polymer could be 420 g/mol (if degree of polymerization is 10) or 21,000 g/mol (if the degree of polymerization is 500). Although vastly different in molar mass, both of these molecules are polypropylene. For polymers, there is almost always a molar mass distribution. An example distribution is given in Figure 1.10. Although this curve looks continuous, we know that in fact it cannot be - the mass of the polymer does change in discreet units, depending on the size of the repeat unit. However, we do typically draw the distributions as continuous function.

Introduction to Polymers, Third Edition, CRC Press, 2011.
Because there is a distribution in molar mass, we have a choice as to how to actually define a characteristic molar mass for a sample. There are three general approaches for calculating the molar mass from a distribution, giving us three different values: (number average molar mass), , (weight average molar mass) and (z-average molar mass). You'll notice from Figure 1.10 that . Each value of molar mass is defined differently.
is defined as the sum of the products of the molar mass of each size of polymer multiplied by its mole fraction (X). Recall from general chemistry that a mole fraction is equal to the ratio of number of moles (or molecules) of a type of polymer (N) divided by the total number of moles (or molecules). Basically, this is the same as your "average" arithmetic mean!
Sometimes it's easier for us to work in weight fractions () rather than mole fractions, since mass is often easier to measure. The weight fraction is defined as the mass of molecules of molar mass divided by the total mass of all the molecules present:
Thus, we can define :
Compare to — do you notice how is a function if squared? Therefore, bigger polymers have a greater influence on than they do on , skewing the value of to be larger than .
Molar Mass Practice Problems
Molar Mass Practice Problems mrs110Dispersity
Dispersity sxr133The dispersity is an indication of the breadth of the molar mass distribution. Consider the two mass distributions shown below in Figure 1.11. The orange curve is broader than the blue, hence we would say that the orange polymer sample has greater dispersity.
Note:
The textbook Introduction to Polymers sometimes uses the term polydispersity index. Recently, the term has been changed to dispersity. IUPAC has deprecated the use of the term polydispersity index, having replaced it with the term dispersity, represented by the symbol Đ (pronounced D-stroke) which can refer to either molecular mass or degree of polymerization. Source Wikipedia: Dispersity

We define the dispersity as the ratio of and :
If your polymer is completely uniform, and every polymer molecule is exactly the same size, your dispersity would be 1. If there is any distribution in molar mass, then dispersity will be greater than 1 because is always greater than .
PROBLEM
What is the dispersity of the polymer mixture described by the data below?
| Ni (mol) | Mi (g/mol) | mi (g) | mi * Mi (g2/mol) (g) |
|---|---|---|---|
| 0.003 | 10,000 | 30 | 300,000 |
| 0.008 | 12,000 | 96 | 1,152,000 |
| 0.011 | 14,000 | 154 | 2,156,000 |
| 0.017 | 16,000 | 272 | 4,352,000 |
| 0.009 | 18,000 | 162 | 2,916,000 |
| 0.001 | 20,000 | 20 | 400,000 |
| ---- | ---- | ---- | ---- |
| 0.049 | 90,000 | 734 | 11,276,000 |
ANSWER
Earlier in the lesson, we learned about degree of polymerization. Well, if there is a distribution in polymer molar mass, then there must also be a distribution of degree of polymerization. So to describe the degree of polymerization for a polydisperse polymer we use degree of polymerization averages, and similarly to molar mass distributions, we have both a number average and a weight average for degree of polymerization.
Summary and Final Tasks
Summary and Final Tasks sxr133Summary
In Lesson One you have learned the very basics of polymers - how we describe the composition (monomer, repeat unit, homopolymer, copolymer, etc.), the skeletal structure (linear, branched, network), and the polymer size (degree of polymerization, number and weight average molar mass). You will have hopefully noticed how different polymer molecules are than molecules you are most familiar with. In particular, the polymer molar mass does not define its composition unlike other molecules, because a polymer have any degree of polymerization. Polymers are also so much higher molar mass than other molecules and as we will see in upcoming lessons, this gives polymers some unique material properties. Next, we will be learning about what is necessary to make a polymer in the first place, because not all molecules are monomers. How do we link together these monomers, and what determines the skeletal structure?
Reminder - Complete all of the Lesson 1 tasks!
You have reached the end of Lesson 1! Review the checklist on the Lesson 1 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 2.
Lesson 2: How Polymers Are Made
Lesson 2: How Polymers Are Made mjg8The links below provide an outline of the material for this lesson. Be sure to carefully read through the entire lesson before submitting your assignments.
Overview/Checklist
Overview/Checklist mrs110Overview
Now that you know what a polymer is, how do we make one, and how do we categorize all the many types of polymers that can be formed? We know that in order to create a polymer, we need to link together monomers, and in this lesson we will begin to discuss how that happens. We will find that there are two general pathways by which monomers can be added together: chain growth and step growth. Each mechanism is characterized by different reactions that take place. In this lesson, you will learn the general characteristics of these polymerization pathways, what is necessary for a molecule to actually be considered a monomer, and how the functionality of the monomer contributes to the skeletal structure of the polymer.
Learning Outcomes
By the end of this lesson, you should be able to:
- describe the principle of equal reactivity;
- define and compare/contrast step growth vs chain growth; condensation with addition polymerization;
- identify functionality of a monomer and how it affects the skeletal structure of polymer formed;
- name the class of polymer formed based on the chemical structure;
- When presented with a polymer, be able to suggest monomers that can be used to produce it.
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 2. | Continue navigating the online material. |
| To Read | Chapter 2 - Principals of Polymerization
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework 2 (Practice) | Registered students can access the homework assignment in the Lesson 2 module. |
Please refer to the Canvas Calendar for specific time frames.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
How is a polymer formed?
How is a polymer formed? sxr133Polymerization requires chemical reactions, and chemical reactions happen as a consequence of collisions of molecules; if monomers never encounter each other, they can never react! Therefore, we would expect that the rate of a reaction has dependence on collision frequency. This is an especially important consideration for polymers, because polymers can be really big which means they diffuse slowly, leading to a lower rate of collision, providing fewer opportunities for reactions. However, because the polymer is large and diffuses more slowly, each encounter between reactants actually has a longer duration, which favors a reaction. These two effects — less overall collisions but longer collision duration — are assumed to balance each other out. Analyses of polymer reaction kinetics suggest that this is a reasonable assumption in most cases. We are therefore going to make this very key assumption called the principle of equal reactivity, which is that reactivity does not vary as a function of polymer size. This assumption underlies all of our future analysis of polymerization, and is important to keep in mind.
Now to actually make a polymer in the first place, you have to have the correct degree of functionality. Clearly, for a polymer to form and grow, 1) there has to be an initial reaction between monomers, and 2) there has to be reaction between monomers and the growing polymer molecule. Consider the two molecules in Figure 2.1, where A and B are able to react together to form a bond. Because each molecule only has one A or B group, once they react, there is no more functionality left to continue the polymerization. Thus, these molecules don’t have enough functionality to form a polymer.
What if instead you had molecules with both an A and B group, as shown in Figure 2.2. Now, after A and B react, there is still enough functionality on the molecules to continue adding monomers to the polymer chain. There is sufficient functionality for a polymer to form.
In Figure 2.2 the monomers have a functionality of two, and so the polymer that forms is a linear polymer (We first learned about skeletal structures in Lesson 1). But what if the monomer had even more functionality? Consider Figure 2.3 where the monomer has a functionality of 4. Now we see that we can get formation of branched polymers and/or network polymers.
So identifying the functionality in a monomer — and whether it has enough to form a polymer in the first place — is going to be key. But let’s say you already know that your monomer can form a polymer — what happens next? How does a monomer actually add to another monomer, or add to a dimer, or add to an existing polymer? There are two general mechanisms for how this can happen: step growth polymerization and chain growth polymerization.
Step growth polymerization
Step growth polymerization sxr133Consider this exercise: you have a bag of pop beads, and each bead represents a monomer. You reach into the bag, pick up two beads, and put them together (they “react”) to form a dimer. Then you put this dimer back into the “solution” of monomers (the bag). Reach in, and grab two more beads at random. Most likely, you pick two single beads - put them together, and throw the dimer back. After you do this a bunch of times, perhaps you reach in and grab a monomer and a dimer. Put them together, you’ve made a trimer. Throw it back! If you do this for long enough, pretty soon your bag will be full of short oligomers, and lots of them, without many monomers left. Only after a long time of doing this exercise will you actually start to piece together these short oligomers to create longer polymers.
This mechanism is characteristic of step growth polymerization. Step polymerization is characterized by:
- loss of monomer early on in the reaction (remember, you turned all those monomers into dimers, trimers, and other short oligomers);
- growth of polymers throughout the reaction;
- the average molar mass increases slowly (for the majority of the exercise, your bag had only very short oligomers in it — only after very long times did you start to get longer polymers);
- high extents of reactions are necessary to get long chain lengths (lots and lots of beads had to be combined into those dimers and trimers before you started to get longer polymers);
- no initiator is used (the bead monomers were inherently reactive with each other).
Chain growth polymerization
Chain growth polymerization sxr133Now try this variation of the bead exercise. In the bag, put a bunch of similarly colored beads (monomers) and a few differently colored beads (which will be our initiator molecules). The difference between this and the previous exercise is that monomer can only add to the initiator or a growing polymer containing the initiator. So reach in and grab two beads until you pull out an initiator and a monomer. Put them together, throw them back! Grab two more; if you grab two monomers, they won’t react with each other. Eventually, you will grab a monomer and a growing polymer fragment that has the initiator bead; keep adding monomers to that. What you find is that, in comparison to the step polymerization exercise, here you are forming relatively few numbers of polymers but each polymer chain that does form will grow longer, faster. You will also not use up your monomer as quickly; even when your polymers grow large, you’ll still have lots of monomer beads left. This exercise is similar to chain growth polymerization. Chain growth polymerization has the following characteristics (compare to step growth polymerization!):
- growth of polymer occurs by adding monomers to relatively few polymer chains;
- monomer remains even at long reaction times;
- average molar mass increases quickly;
- initiation is required.
We will be considering step and chain polymerization independently, and in great depth, in the coming lessons, but for now you should have a good idea of the similarities and differences between these two mechanisms.
Linear Step Polymerization
Linear Step Polymerization sxr133We will first consider polymerization in which a linear polymer is formed, and the mechanism is step growth, i.e., linear step polymerization. We already have seen an example of what this could look like (Figure 2.2). Linear step polymerization occurs from polymerization of either bifunctional or difunctional monomers, which have a functionality of two. A difunctional monomer has two of the same reactive groups capable of forming bonds (e.g. two “A” groups), while a bifunctional monomer has two reactive groups, although they are not the same moieties (but can still react to form bonds, e.g. an “A” and “B” group) (Figure 2.4). We have terminology to describe each of these various combinations of reactions, as depicted in Figure 2.4. For example, if we have monomers that are bifunctional (A-B) and A reacts with B, we call this type of polymerization “ARB” type. (The “R” represents whatever chemical structure is between the reactive functional groups of the monomer). If we have difunctional monomers that react with themselves (A-A reacts with A-A) we call this “RA2”. And if we have difunctional monomers (A-A and B-B) where A reacts with B, then this is an “RA2+RB2” type reaction.

PROBLEM
Consider polycarbonate, formed from the reaction between bisphenol A and phosgene. What “type” of polymerization is this?
- RA2 + RB2
- RA2
- RB2
- ARB
ANSWER
A. RA2 + RB2
So what exactly are A and B? What functional groups can we use to create polymers, and what sorts of polymers do they produce?
Common Classes of Polymers
Common Classes of Polymers ksc17Polymers are often distinguished by the structure of the linkages that are produced. Table 3.1 in the text provides seven common classes of polymers that can be produced by step growth polymerization. We will consider each of these in depth, and identify the functional groups that are needed in the monomers to produce the desired polymers. Be conscious of whether the reactions are polycondensation or polyaddition reactions (refer back to Lesson 1 - What is a Polymer).
Polyesters
Polyesters can be produced from the reaction between carboxylic acids or acid halide groups with alcohols (Figure 2.5). Notice that when a carboxylic acid is used, water is a product; when an acid halide is used, acid is a product.

A very common polyester is polyethylene terephthalate, or PET (Figure 2.6). If you see recycling symbol #1 on your container, it's PET! PET is the most common thermoplastic polymer and is frequently used in synthetic fibers. Even though there are many different polyesters, PET is so common - 18% of world polymer production - that it is often just identified by the general name, "polyester". So if you look on your clothing label and find that it says "polyester", now you know that it's PET. The inclusion of aromatic groups in the backbone lends the polymer more mechanical and thermal stability. University of Liverpool - Chem Tube 3D.

Polyamides
Polyamides are produced from the reaction between carboxylic acids or acid halides with amine groups that creates amide bonds (Figure 2.7).

Nylon is a great example of a polyamide. Nylon 6,6 is shown in Figure 2.8; the "6,6" part comes from the fact that each monomer has 6 carbons; there are many other kinds of nylon as well, depending on the specific monomers used. Nylons have extensive hydrogen bonding between polymer chains which generates a relatively high degree of order (and crystallinity) contributing significantly to nylon's strength and rigidity. This ordering also makes nylon great for fibers. Nylon 6,6 can be easily made from interfacial polymerization, because the adipic acid (or sebacoyl chloride) is water soluble and the hexamethylenediamine is oil soluble. (VIDEO/www.youtube.com/watch?v=VtCBarLbHRM)

Other important examples of polyamides are polypeptides or proteins. Proteins are polypeptides, produced from the polymerization of amino acid monomers. The generic structure of an amino acid is shown in Figure 2.9. Do you see how the polymerization of an amino acid would create an ARB type polymer?

Polyethers
Polyethers are formed from reactions between diols in an RA2 type polymerization.

Polyurethanes
Polyurethanes are formed from the reaction between diisocyanates with diols (Figure 2.11).

Polyurea
Polyurea is formed from the reaction between diisocyanates with diamines (Figure 2.12)

Polymer Matching Game
Polymer Matching Game jls164Directions: Drag the polymer diagrams into the box indicating the proper polymer type. When you have placed all of the polymers, click on the Check button to see how you did.
Hint: You should end up with three polymers in each group.
Note: You may want to zoom out to help you see the whole activity window. Ctrl + – on Windows or Command + – on a Mac. To return to the default zoom level, use Ctrl + 0 on Windows or Command + 0 on a Mac.
Summary and Final Tasks
Summary and Final Tasks sxr133Summary
Hopefully, you now feel comfortable identifying classes of polymers based on the linkages in the backbone and suggesting monomers with appropriate functionality to make polymers of a targeted type and skeletal structure. The various classes of polymers we learned (polyester, polyether, etc.) and the specific reactions we discussed to produce them are all examples of step polymerizations. In Lesson 3, we will continue to dive deeper in step growth mechanisms and especially start to consider the kinetics of polymerization.
Reminder - Complete all of the Lesson 2 tasks!
You have reached the end of Lesson 2! Review the checklist on the Lesson 2 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 3.
Lesson 3: Step Growth Polymerization
Lesson 3: Step Growth Polymerization sxr133The links below provide an outline of the material for this lesson. Be sure to carefully read through the entire lesson before submitting your assignments.
Overview/Checklist
Overview/Checklist mjg8Overview
In this Lesson, we will take a close look at step polymerization. If we know the number of reactive groups in our monomer mixture, and we can control how many groups react, then can we predict the number average degree of polymerization? We can! First we consider if we have stoichiometric balance of reactive groups, then we consider if we have a non-stoichiometric balance and what effects that has on the polymer produced. Finally, we end with a statistical analysis of step polymerization, which gives us insight into the distributions of the molar masses produced.
Learning Outcomes
By the end of this lesson, you should be able to:
- Define extent of reaction and reactant ratio
- Apply Carothers theory to step polymerization reactions
- Calculate the probability of finding a polymer of specific degree of polymerization, and the weight fraction or number fraction of polymers of a specific degree of polymerization
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 3. | Continue navigating the online material. |
| To Read | Chapter 3 - Step Polymerization
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 3 (Practice) | Registered students can access the homework assignment in the Lesson 3 module. |
Please refer to the Canvas Calendar for specific time frames.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Carothers Theory: Stoichiometric Balance of Reactive Groups
Carothers Theory: Stoichiometric Balance of Reactive Groups ksc17We will now consider in greater depth the theoretical treatment of linear step-growth polymerization. Specifically, we will examine the Carothers equation, which relates degree of polymerization to extent of reaction. We learned about degree of polymerization in Lesson 2, but what is extent of reaction?
If we assume equal amounts of mutually reactive groups (e.g., and groups), then we can define the extent of reaction as
Extent of reaction is really just the probability that any single functional group that was present at the start has reacted. Consider the mixture of bifunctional monomers in Figure 3.1.

What is the extent of reaction shown in Figure 3.1? and each represent a functional group, so there were 16 functional groups (2 on each of 8 molecules) initially. Looking at the products, we find that 6 of those functional groups are now part of new bonds, so they reacted. We plug these values our equation for extent of reaction:
But notice, there is another way to represent extent of reaction in terms of number of molecules, where is the number of molecules left after the reaction and is the number of molecules initially. Again, using Figure 3.1, where our initial number of molecules is 8 and our final number of molecules is 5:
Let’s rearrange this new expression for extent of reaction:
This value, , should be familiar, because it’s the same as the number average degree of polymerization!
We combine the equations for extent of reaction with number average degree of polymerization to yield the Carothers equation for stoichiometric balance of reactive groups:
So what does this equation tell us?
If you want polymers of any significant length (i.e., high degree of polymerization, ) you need very high extent of reaction !
Example Problem
Example Problem jls164You would like to make a polyester with by reacting 1 mol butane-1,4-diol and 1 mol of adipic acid. At what value of should you stop your reaction to obtain this size?

Let’s break this down into parts. First, let’s calculate . What is ? To figure that out, we need to draw the polymer that is formed:

What is the repeat unit molar mass of this polymer? We simply add up the molar masses of the atoms:
However, realize that there are 2 monomers in this repeat unit! Thus,
Now we know that , what is ? We set up the following relationship:
Now we know that . What is the extent of reaction you need to obtain this size of polymer?
So now we know Carothers theory for when we have a stoichiometric balance of and reactive groups. But what do we do if we don’t have the same number of reactive groups?
Carothers Theory: Stoichiometric Imbalance of Reactive Groups
Carothers Theory: Stoichiometric Imbalance of Reactive Groups sxr133If there is a stoichiometric imbalance, we consider the reactant ratio, r:
We always have a choice of which groups are and which groups are ; here, we must define the reactant ratio such that it is equal to or less than 1. The way we have defined , then the groups would be in the minority.
Now because we are still confining our analysis to linear polymerization, each monomer has only 2 reactive groups. So, the total number of molecules initially present can be represented as:
Let’s simplify this expression, and try to represent as a function of only the number of groups for instance, but substituting in :
Consider the following example, which is a modification of Figure 3.1. Notice, we now have a different number of and groups:

Our minority functional group is . So our reactant ratio is:
We can still define an extent of reaction:
Let’s keep our eye on the prize: we want to be able to define as a function of and . How can we do this? Similarly to our derivation with the case of stoichiometric balance, we need to have an expression for , the number of molecules remaining. The number of molecules remaining is:
Convince yourself with our example that this is true. There are 10 unreacted and groups, and 2 functional groups per molecule. Thus, we have 5 molecules remaining; and indeed we do! But how can we write as a function of and ? Let’s rewrite our expression for , taking into account that we already know there are 2 functional groups per molecule, and we only have and unreacted groups:
We can define as:
We can define as:
Notice that the because only reacts with , the number of groups that react is the same as the number of groups that react.
Try plugging some numbers in from our example in Figure 3 to convince yourself these expressions hold.
Ultimately, we wanted to write our expression for in terms of and . So:
We can simplify:
Now, finally, we have expressions for and which we substitute into our general expression for
Finally, we have a more general Carothers equation that is now applicable to polymerization with non-stoichiometric balance of reactive groups. And what does this equation tell us? If you want polymers of any significant length (high degree of polymerization) you need VERY HIGH extent of reaction AND to control as close to 1 as possible!
Table 3.1 (Table 3.3 in the text) calculates values of degree of polymerization for varying values of extent of reaction and reactant ratio. Take a look; you may be surprised really how high extent of reaction needs to be in order to get polymers of any significant length, especially as your reactant ratio deviates more greatly from 1.
Introduction to Polymers, Third Edition, CRC Press, 2011.
at | |||||
|---|---|---|---|---|---|
| Reliability ( ) | p = 0.90 | p = 0.95 | p = 0.99 | p = 0.999 | p = 1.000 1 |
| r = 1.000 | 10.0 2 | 20.0 | 100.0 | 1000.0 | infinity |
| r = 0.999 | 10.0 | 19.8 | 95.3 | 666.8 | 1999.0 |
| r = 0.990 | 9.6 | 18.3 | 66.8 | 166.1 | 199.0 |
| r = 0.950 | 8.1 | 13.4 | 28.3 | 37.6 | 39.0 |
| r = 0.900 | 6.8 | 10.0 | 16.1 | 18.7 | 19.0 3 |
1 - As
2 - Only 10 maximum for p=0.9!
3 - Only 19 maximum for r=0.9!
Introduction to Polymers, Third Edition, CRC Press, 2011.
These short chains are barely polymers!
PROBLEM
You’re polymerizing the two monomers shown below. You want to limit your number average degree of polymerization to 39. Assuming you can achieve a quantitative reaction (p approaching 1), and you start with 2 moles of phenolphthalein as your limiting reagent, then how many moles of terephthaloyl chloride should you use?

ANSWER
We are told degree of polymerization, xn is 39. We can therefore use the Carothers equation to solve for reactant ratio:
Once we know the reactant ratio, that tells us the mole ratio of reactive groups that we should use. Since the reactant ratio always has to be 1 or less, and we are told that phenolphthalein is the limiting reagent (and we have 2 moles of it, with 2 functional groups per molecule), we define the reactant ratio as:
We solve for moles of terephthaloyl chloride, which equals 2.1 moles.
Statistical Theory
Statistical Theory mxw142With Carothers theory, we were dealing with number-average quantities. But how do we predict the molar mass distributions? If we treat each reaction between A and B groups in a step of polymerization as a random event, we can start to apply probability and statistics to the reaction and get an estimation of the distribution of the degrees of polymerization of the polymers formed for a given extent of reaction. Essentially, we are trying to find , which is the probability of existence of a molecule containing exactly x units at time t with extent of reaction p. Without going into the derivation here, we find the probability of finding a sequence of x units:
Since is the probability of finding an “x-mer”, it must also be representative of the mole fraction of x-mers:
Where is number of x-mers and is total number of molecules at time . Often, it’s hard to measure the number of molecules present at any given time , but it’s easy to find , which is the number of molecules we initially start with . Can we substitute in ? In order to relate to we use a familiar equation:
If we solve this above equation for , we find . We substitute this relationship into and find an expression for the number of “x-mers” at a given extent of reaction:
We may also be interested in the weight fraction of x-mers, in addition to the number fraction. How do we solve for that? We start with the standard definition of weight fraction:
We substitute into this with and get the weight fraction of x-mers at a given extent of reaction:
PROBLEM
You are polymerizing the below monomers (1 mole of each) by step growth polymerization. When you stop the reaction, there are 0.1 moles of acid chloride groups left. What weight fraction of monomer do you have left?

ANSWER
First, we find the extent of reaction:
Then we can find the weight fraction of monomer (because x=1 is monomer!)
PROBLEM 2
You are polymerizing the below monomers (1 mole of each) by step growth polymerization. You stop the reaction when it's 99% complete. What fraction of the mixture is monomer, on a per mole basis?

ANSWER 2
We can plug directly into the equation:
We can use these relationships we have learned from the statistical theory to plot the most probable distributions for and :

Introduction to Polymers, Third Edition, CRC Press, 2011.
What can we learn from these plots? First, consider the plot of for a few different values of extent of reaction (which is the left graph). Notice that , even for the high extents of reaction, is always larger for the lower values of . This is telling us that even if we go to high extents of reaction, polymers with low degrees of polymerization are still more likely to be found than those with high degrees of polymerization. Now look at the second graph, at right, which is a plot of . In contrast, this plot has a peak, which is actually very close to . As extent of reaction increases, we see that the peak weight fraction moves to high values of – this makes sense, because the polymers with higher degrees of polymerization are formed at higher extents of reaction. We also notice that the breadth of the curve increases as extent of reaction increases, which tells us that the dispersity of the polymer is increasing.
From these distributions, we can solve for the number average molar mass using this relationship:
Doing a series of substitutions (i.e. substitute in , , and then simplify) we find:
Does this look familiar? It’s the same relationship as we got from Carothers theory!
Without going through the derivation, we can apply a similar analysis to get information about the weight average molar mass as well. We find:
and and
Summary and Final Tasks
Summary and Final Tasks sxr133Summary
In Lesson 3, we got a more in depth look at step polymerization. Using the Carothers equation, we now understand the relationship between extent of reaction, reactant ratio, and the degree of polymerization. Out of these relationships, we learned that in order to achieve high degrees of polymerization, we need to go to high extents of reaction and have a reactant ratio as close to 1 as possible. We also used statistical theory to derive expressions for the probability of finding an x-mer, the weight fraction of x-mers, and the number fraction of x-mers. From these, we can learn about the distribution of the polymer molar mass for different extents of reaction.
Reminder - Complete all of the Lesson 3 tasks!
You have reached the end of Lesson 3! Review the checklist on the Lesson 3 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 4.
Lesson 4: Free Radical Polymerization (Part I)
Lesson 4: Free Radical Polymerization (Part I) sxr133Overview / Checklist
Overview / Checklist mjg8Overview
In this Lesson, we are going to learn how free radical polymerization works, what the actual mechanism of the reaction is like, and why it happens. Free radical polymerization is a type of chain growth polymerization, but not the only one – in coming lessons we will cover other kinds of chain growth mechanisms, including ionic polymerization and ring opening polymerization. For now, in Lesson 4 and 5, we are going to focus on free radical, which is one of the most common types of polymerization. We are breaking down the topic of free radical polymerization into two lessons: Lesson 4 focuses on the reaction mechanisms and Lesson 5 focuses on the reaction kinetics.
Learning Outcomes
By the end of this lesson, you should be able to:
- Identify monomers that can undergo free radical polymerization.
- Draw arrow pushing mechanisms for polymerization by free radical polymerization, including initiation, propagation, termination (by combination or disproportionation), and chain transfer.
- Name and describe the stages of the free radical polymerization mechanism.
- Identify the head and tail of a monomer and whether a reaction occurred in a head to tail, head to head, or tail to tail fashion in a polymer and why
- Describe the effects of chain transfer on polymer skeletal structure
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 4. | Continue navigating the online material. |
| To Read | Chapter 4 - Radical Polymerization
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 4 (Practice) | Registered students can access the homework assignment in the Lesson 4 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Introduction
Introduction ksc17Recall from Lesson 2 that we learned about two types of polymerizations: step growth and chain growth. In Lesson 3, we explored in depth the monomers that undergo step growth polymerization and Carothers theory for linear step polymerization. In Lesson 4, we now begin to examine the details of chain growth polymerization. More specifically, in this lesson, we are going to focus on free radical polymerization, which is a specific type of chain growth polymerization.
First, we should probably refresh our memory of what a radical actually is! A radical species is characterized by having an unpaired electron. From general chemistry, we recall that it is much more stable to have electrons paired in orbitals rather than unpaired — so as you may expect, radicals tend to be highly reactive and relatively short-lived. Radicals are denoted by a single dot (representing the electron), such as in Figure 4.1.
Introduction to Polymers, Third Edition, CRC Press, 2011.
The radical is shown as the single dot in Figure 4.1. In (i) the geometry and the hybridization of the central carbon is emphasized. The carbon is sp2 hybridized, and the radical exists in the unhybridized p orbital that is perpendicular to the plane containing the substituents. Usually, the orbital is not drawn, as in (ii) or (iii).
Free radical polymerization makes use of this unstable radical by sequentially adding unsaturated monomers to the active center (radical end) of a growing polymer. Let's break that idea down further. As a refresher, recall that unsaturated molecules are characterized by not having the greatest possible number of hydrogens based on the carbon content. Usually, this means that the molecule contains a double or triple bond. Monomers that are most frequently used for free radical polymerization have a double bond, and more specifically, often a vinyl group or acryloyl group (Figure 4.2). Examples of a few common monomers are shown in Figure 4.3.
We already stated that we are going to use the radical to react with unsaturated monomers and this is going to create a polymer — but how? We can represent this reaction, and where the electrons go within the molecules, by using arrow pushing mechanisms which you learned in organic chemistry. In free radical polymerization, monomers are sequentially added together and the reactive radical end (the active center) attacks double bonds of monomers as shown in Figure 4.4.
There is actually a lot going on in Figure 4.4. First of all, you may want to refresh your memory regarding the conventions of arrow pushing mechanisms. The arrows show where the electrons start (at the arrow tail), and where they go (the arrow head); single headed arrows represent the movement of one electron, while double-headed arrows represent movement of an electron pair. Here, we will be using lots of single headed arrows because we are dealing with radicals, which are unpaired electrons. As shown in Figure 4.4, we have broken down the "overall reaction" into two steps for clarity. Let's look in detail at Step 1 in Figure 4.4. Note that the π bond of the double bond is broken (the σ bond still remains) and that the π bond is broken homolytically. By homolytically, we mean that the two electrons in that bond are split evenly between the two carbons in the bond, one electron going to each carbon. Then, one of those new radicals that is generated can react with the radical on the other monomer, forming a new carbon-carbon bond (step 2). In the future, when writing reaction mechanisms, all you would need to show is the "overall reaction" as shown in bottom of Figure 4.4. Notice that after this reaction takes place, our product now has one additional monomer linked to the polymer chain, and our radical is still at the end of the molecule (this is called the active center). Building upon this general mechanism of free radical polymerization, we move on to more in depth understanding of the process. For example, how do we even get these radicals in the first place? How do we get rid of the radicals if we want to stop our reaction to make polymers of a specific length? These are the sorts of questions that we will soon address.
The Stages of Free Radical Polymerization
The Stages of Free Radical Polymerization ksc17There are three general stages of free radical polymerization: 1) initiation, 2) propagation, 3) termination. Let's consider these stages in the order which they occur.
Initiation
This step involves the creation of the radical, i.e., creation of the active center. Usually, we need to add a special molecule called an initiator to our reaction to generate these radicals in the first place. By using a trigger like an input of light (hv) or heat (Δ), we induce the initiator to homolytically decompose into fragments containing radicals that can be used to initiate polymerization. Common molecules that are used as initiators include peroxides (containing a peroxide bond, -O-O-) and azo compounds (containing R-N=N-R'). Examples of common initiators include benzoyl peroxide, with is thermally triggered, and benzophenone, which is UV triggered. Note that for each bond that is broken, you get two radicals formed.


Once we generate the radical, it has to be transferred to a monomer to create an active center. It's worth pointing out that not all radicals generated during initiation actually get transferred to the monomer. Some molecules with radicals may further decompose, and the radicals recombine, before they ever get a chance to react with the monomer. But assuming we do have transfer to monomer, there are actually two ways that a radical can add to the double bond of a monomer. There are two ways because the two carbons involved in the double bond may not be equivalent (i.e., they may have different substituents). Figure 4.7 depicts the two ways that the initiator radical can add to a monomer.

The first reaction (Mode I) typically predominates in free radical polymerization. Why do you think this might be the case? Comparing Mode 1 and Mode 2, we notice that difference is whether the initiator radical forms a bond with the carbon attached to the "X" group or not. Remember that for a reaction to occur, two reagents have to be able to get close to each other, which is why consideration of steric effects is important. Hopefully you learned some about steric hindrance in organic chemistry, but to quickly summarize, the basic idea is that bulky substituent groups (i.e., bulky, large "X" groups) prevent the radical from being able to approach the other molecule closely enough to react. Well, in Mode 1, the only substituents on the reacting carbon are hydrogens (since it is a methylene group), which are small, so there's really not much steric hindrance. For Mode 2, "X" could be anything — imagine a tert-butyl group that's big and bulky — the radical will have a harder time approaching that carbon. Thus, Mode 1 tends to be favored based just on steric considerations. But there is another reason as well, which is that the radical in Mode 1 ends up on the carbon with more substituents, which can help to make that radical more stable than the radical on the methylene group.
Propagation
Propagation involves the growth of the polymer chains, where monomers are sequentially added to the active center. The mechanism of propagation looks like what we already discussed in Figure 4.4, so refer back to that if you get confused about the movement of the electrons. Similarly to initiation, there are actually multiple ways in which a monomer can add to the active center (again, because the two carbons in the vinyl group of the monomer may be non-equivalent). Figure 4.8 depicts the two ways in which the monomer can add to the active center. We name these configurations depending on how the "head" or "tail" of the monomer is connected to the active center. The "head" of the monomer is the side where the substituent is attached, while the "tail" is the methylene. Because of the reasons discussed in the section on initiation (sterics, and stabilization of the radical), we expect that the active center is usually found on the "head" group and preferentially reacts with the "tail" of another monomer (i.e., "head to tail"). Less frequently, we would see head to head addition; if head to head addition occurs, it will most likely be followed immediately by a tail to tail addition, such that the active center again ends up on the head side.

CASE STUDY
Consider the polymerization of vinyl fluoride (Figure 4.9). Do you think this monomer will still preferentially add in a head to tail fashion?

The tail (the methylene) is less sterically hindered, so in terms of steric effects, we still expect head to tail addition. But, you may recall from organic chemistry, that fluorine is strongly electron withdrawing which would actually destabilize a radical on the head carbon (which is electron deficient). So, we have competing effects - which wins out? Turns out that 90% of the linkages in poly(vinyl fluoride) are still head to tail, emphasizing the importance of steric considerations.
Termination
Termination involves destruction of the radical active centers, thus preventing any further propagation. But, what happens to those radicals then? There are few different possibilities for where they go. Often, termination occurs via combination of radicals (Figure 4.10).

PROBLEM
In Figure 4.10 a new carbon-carbon bond is formed during termination by combination. What type of linkage is shown?
- Head to tail
- Head to head
- Tail to tail
ANSWER
B. Head to Head
Also notice in Figure 4.10 that upon termination by combination, the final polymer has a final degree of polymerization of x+y, and there are two initiator fragments on each end. Termination by combination is not the only pathway for termination. In termination by disproportionation, an H atom is extracted from the end of a growing chain and the leftover electron combines with another radical, generating a terminal π bond (Figure 4.11).

In termination by disproportionation, we have created two polymers, one with an unsaturated end, and both have one end with an initiator fragment.
Chain Transfer
Chain Transfer sxr133Chain transfer is a process that occurs during polymerization, in which the active center is transferred from one species to another (Figure 4.12).

TA can be initiator, monomer, polymer, the solvent, or something you add to purposefully transfer the radical (i.e., a transfer agent). Often, T is a hydrogen atom or halogen atom
In Figure 4.12, we use T and A to just represent fragments of a molecule that are linked by a single bond. TA can be initiator, monomer, polymer, the solvent, or something you add to purposefully transfer the radical (i.e., a transfer agent). Often, T is a hydrogen atom or halogen atom. Notice that breakage of the single bond in TA happens by homolytic cleavage, as we have seen before, such that the radical has been transferred from one species to another. Chain transfer - the rates at which it happens, and the species between which the radical is transferred - can have dramatic effects on the structure of the resulting polymer. First, we will consider the impact of chain transfer to polymer.
Chain transfer to polymer
Chain transfer to polymer means that the radical is transferred to somewhere in or on a polymer - it can be the same polymer where the radical was initially (intramolecular chain transfer, or backbiting), or the active center can be transferred to a different polymer chain (intermolecular chain transfer). Both of these processes are shown in Figure 4.13.

If we were to polymerize a monomer with a functionality of two (e.g., a monomer with a vinyl group) we expect to create a linear polymer, without branching. But if there is chain transfer to polymer, then we get a very different polymer skeletal structure that does have branching. If there is intramolecular chain transfer to polymer, sometimes called backbiting, the active center is transferred to somewhere else along the same polymer chain where the active center originated. Usually, it's transferred to a position pretty close to the polymer end resulting in the formation of a short branch. If there is intermolecular chain transfer to polymer, then the active center is transferred to another polymer chain. It could be transferred anywhere along the polymer; usually, this mechanism leads to branches that are longer.
Summary and Final Tasks
Summary and Final Tasks sxr133Summary
Free radical polymerization is one of the most important types of polymerizations, and now you should feel comfortable indenting monomers that will undergo free radical polymerization, drawing the free radical polymerization mechanism, and describing how chain transfer affects skeletal structure. It is very key that you understand how the monomers react to give the polymer so that you can draw an accurate repeat unit for any monomer(s) that you start with. Next, we are going to be building upon the foundation we learned in Lesson 4 and apply that to the kinetics of free radical polymerization in Lesson 5.
Reminder - Complete all of the Lesson 4 tasks!
You have reached the end of Lesson 4! Review the checklist on the Lesson 4 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 5.
Lesson 5: Free Radical Polymerization (Part II)
Lesson 5: Free Radical Polymerization (Part II) sxr133Overview/Checklist
Overview/Checklist mjg8Overview
In this Lesson, we continue learning about free radical polymerization, with a focus on the kinetics of the polymerization. We describe the rate of reaction for initiation, propagation, and termination, and how those reactions play into the overall rate of polymerization. Introduction of inhibitors or retarders can be used to modulate the rate or onset of polymerization. We also learn about how to calculate the number average degree of polymerization for free radical polymerization and how it relates to factors such as concentration of monomer, initiator, and chain transfer.
Learning Outcomes
By the end of this lesson, you should be able to:
- Calculate rates of initiation, propagation, and termination, and how these influence rate of polymerization
- Describe the effect of monomer concentration, initiator concentration, radical concentration, and rate of chain transfer on rate of polymerization and degree of polymerization
- Determine the polymer skeletal structure from monomers that can be polymerized by free radical pathways
- Describe steady state conditions
- Describe the effects of inhibitors and retarders on polymerization.
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 5. | Continue navigating the online material. |
| To Read | Chapter 4 - Radical Polymerization
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 5 (Practice) | Registered students can access the homework assignment in the Lesson 5 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Polymerization Kinetics
Polymerization Kinetics jls164Now that we have a working understanding of the reactions and processes that can happen during free radical polymerization, we can begin to discuss the polymerization kinetics for free radical polymerization. We start from the very beginning and define the rate of polymerization:
As shown in Eq. 5.1, we are defining the rate of polymerization as the rate at which monomer M is consumed. Note the negative sign, which is there because we are defining the rate as the disappearance or consumption of monomer.
You may want to refresh your memory of rate equations before going much further!
Rate of Initiation:
We should be able to write a rate equation for each "step" in free radical polymerization: initiation, propagation, and termination. Let's start with initiation; there are actually two parts to initiation: 1) the formation of the radical from decomposition of the initiator and 2) transfer of the radical to a monomer.

The first step of initiation, generation of the radicals, is generally much slower than transfer of the active center to the monomer. Thus, the first step of initiation is the rate determining step, meaning that the rate of initiation is really only a function of the slow step, formation of radicals. Thus, we can represent the rate of initiation as the rate of formation of radicals:
Notice that we don't have anything about monomer concentration in rate of initiation. Because we consume so little monomer during initiation, we neglect any changes in monomer concentration here. But we can make this more specific. Let's say we generate two radicals per initiator molecule, which is common, and that the rate of dissociation of the initiator has a rate constant of kd.

We can thus re-write the rate for first step of initiation as:
However, we also know that not all the radicals that are produced actually get transferred to monomer; only some fraction of them make it through step 2 of initiation. Radicals may combine, react with solvent, etc. To account for the fact that not all radicals produced in step 1 are actually used, we introduce the concept of initiator efficiency, f. For example, If half of our radicals produced actually get used and transferred to monomer, then f =0.5. We can update our description of the rate of initiation:
Rate of Propagation:
Propagation involves the transfer of the radical from one monomer to another monomer, or to polymer. We are using up lots of monomer in this step.

The rate of disappearance of monomer (note the negative sign in the rate!) is a function of the rate constant, the monomer concentration, and concentration of active centers (M·)
Note that this is the only place where we directly account for the rate as consumption of monomer (but NOT the radical species).
Rate of Termination:
Recall that we have two different pathways for termination: combination and disproportionation.

We write the rate equations for these two termination pathways:
The coefficient of two results from the fact that two growing polymers are consumed by either pathway.
Add up these two rates (ktc +ktc = kt ) to get an overall rate equation:
Steady State
Steady State jls164We have now written rate equations for initiation (generation of radicals), propagation (growth of polymer), and termination (consumption of radicals). At the very beginning of the reaction, the rate of formation of radicals is faster than consumption of monomer. But the number of radicals cannot keep growing forever! Eventually, the rate of formation of radicals and consumption of radical monomer/active centers reaches a steady state — radicals are formed as quickly as they are consumed/propagated in the reaction. Radicals are consumed just as fast as they are created. This is called steady state. We work under this assumption for the rest of our derivation of steady state polymerization rates.
The rate of production of radicals is the same as the consumption of radicals:
Substitution of our previous expressions:
Rearrange to solve for the steady state concentration of radicals:
OK great, why do we care? Well, we ultimately want to figure out the rate of polymerization, which recall that we defined at the very beginning of the section. To refresh your memory, we defined rate of polymerization as rate of consumption of monomer. Where else have we seen rate of consumption of monomer? We saw it in the expression for the rate of propagation!
While we can measure the concentration of monomer, it's not easy to measure the concentration of radical. But if we are under steady state conditions, we can substitute for using
Note: the upper limit for is pure monomer. When pure monomer is used, it's called bulk polymerization
PROBLEM 1
What happens to the total radical concentration at steady state if we double the concentration of initiator?
- doesn't depend on so nothing changes
- doubles
- increases by a factor of
- decreases by half
ANSWER 1
C. increases by a factor of
We substitute for in the expression for and find so
PROBLEM 2
What happens to the total rate of polymerization at steady state if we double the concentration of monomer?
- doesn't depend on so nothing changes
- doubles
- increases by a factor of
- decreases by half
ANSWER 2
B. doubles.
Number average degree of polymerization
Number average degree of polymerization jls164We have already introduced the idea of number average degree of polymerization. Recall:
We are going to try to describe number average degree of polymerization using the concentration of monomer and initiator, and for now let's neglect chain transfer. Can we substitute for the numerator, moles of monomer consumed in time ? What's the rate of monomer consumption? We know that, it's the rate of propagation: . What about the denominator, moles of polymer formed in time ? Think about in what step we actually form a complete polymer — it's the termination step. In Figure 5.4, and we noticed that for termination by combination we form one polymer, and for termination by disproportionation we form 2 polymers. Thus the total rate of polymer formation is the sum of formation from combination and disproportionation. We write rate equations for this:
Let's substitute for the numerator and denominator in our number average degree of polymerization. We are going to use the subscript '0' for to denote that this is the degree of polymerization in the absence of chain transfer.
Again, we can't do so much with radical concentrations in that expression. So let's substitute the steady state concentration of radicals, and we get:
is the fraction of termination happening by disproportionation. If there is only termination by combination then . If there is only termination by disproportionation then . We can further substitute with :
This equation looks a little complicated. But importantly, we want to gain insight as to how the number average degree of polymerization is affected by inputs we can control, namely the concentration of monomer and concentration of initiator. We find:
We call the equations for and that we derived instantaneous equations because they apply to a specific concentration of and (which change over time). As a refresher: and . Thus, both go up with increasing , and the expressions are oppositely correlated with . Thus, we can predict how changing and , which we can control, will affect our resulting polymer. Remember is limited to pure monomer in bulk polymerization. So there are constraints on the degrees of polymerization that you can achieve.
How accurate are these expressions as compared to experimental values of ? We find that experimental values of tend to be lower than expected based on these derived relationships. Why? What have we neglected in our derivations? Chain transfer! Chain transfer can contribute significantly to the termination of growing polymer chains. Even though the transferred radical can still continue to react, the chain from which it was transferred is now shorter (lower ) than would have been expected (Figure 5.5). The rate of polymerization may not be so greatly affected if reacts quickly with monomer (Figure 5.5).

We can account for chain transfer, including chain transfer to solvent, monomer, and initiator, in addition to termination by combination and disproportionation by building this into the "moles of polymer formed at time t" part of the denominator in our expression for . We thus update our previous expression, which was , and we alter it:
Notice that the takes into account chain transfer to monomer, is for chain transfer to initiator, and is for chain transfer to solvent. This is a more accurate description of degree of polymerization. Notice that we didn't include a term for chain transfer to polymer in our updated description of degree of polymerization because if the active center is transferred between polymers, then there is actually no effect on "moles of polymer formed at time t". Rearrange, substitute with (which we previously derived without chain transfer) to generate the Mayo Walling Equation:
We have thus introduced transfer constants , , are for each type of chain transfer reaction (transfer to monomer, initiator, and solvent, respectively). Notice that while chain transfer to polymer can greatly affect skeletal structure, it doesn't affect degree of polymerization because the number of polymers before and after chain transfer are the same.
See Table 5.1 below for a list of example transfer constants of various solvents for the free radical polymerization of styrene. Solvents with high transfer constants would prevent propagation and growth of long polymers, but can be added in small quantities to produce smaller polymers if they are desired (i.e., used as a chain transfer agent).
| Compound | Bond Cleaved (T-A) | Transfer Constant CTA=(KtrTA/Kp) |
|---|---|---|
| Styrene | H—C(Ph)=CH2 | 7x10-5 |
| Benzoyl peroxide | PhCOO—OOCPh | 5x10-2 |
| Benzene | H—Ph | 2x10-6 |
| Toluene | H—CH2Ph | 12x10-6 |
| Chloroform | H—CCl3 | 5x10-5 |
| Carbon tetrachloride | Cl—CCl3 | 1x10-2 |
| Carbon tetrabromide | Br—CBr3 | 2 |
| Dodecyl mercaptan | H—SC12H25 | 15 |
PROBLEM
A solution of 100 g/L acrylamide in methanol is polymerized at 25°C with 0.1 mol/L diisobutyryl peroxide whose half life is 9.0 h at this temperature and efficiency in methanol is 0.3. For acrylamide, at 25°C and termination is by coupling alone.
What is the initial steady state rate of polymerization?
(half life for a first order reaction: )

ANSWER
We are looking to solve for the initial steady state rate of polymerization, thus
To solve this equation, we need to substitute for many variables. Can we pull all of that necessary information out of the question? Let's start with the concentration of the monomer, acrylamide. It's density is given, but we need the concentration in mol/L:
Let's move on to . We can get this rate constant for decomposition of the initiator from the half life. We are going to solve for this with the time units of seconds, because in the problem we are given and we want to make sure all our units are going to be consistent throughout the problem.
In order to actually make sure of we are going to have to rearrange our expression for a little.
Now it looks like we have all the numbers we need to plug into this equation!
Inhibitors and Retarders
Inhibitors and Retarders jls164We can add specific molecules to our reaction if we want to prevent or slow down polymerization. For example, when you purchase a commercially available monomer from a supplier, you may read on the bottle that the monomer is stabilized, perhaps by a molecule such as MEHQ (monomethyl ether hydroquinone). Such inhibitors are added to extend the shelf life of the monomer by preventing unwanted, premature polymerization. Inhibitors work by "trapping" any radicals that are generated in a very stable molecule that does not further react. If a "normal" polymerization follows a trajectory such as in Figure 5.6 (Figure 4.7 in the textbook), then that same polymerization with an inhibitor present would follow a trajectory like Figure 5.6 (c); the inhibitor prevents polymerization for a certain amount of time (the induction time), which depends on how much inhibitor is present. As soon as all the inhibitor is used up, then the reaction proceeds as normal.
A retarder works slightly differently than an inhibitor, and serves to slow down a polymerization rather than prevent it, as shown in Figure 5.6 (b). Retarders act in a similar way as inhibitors in that they stabilize radicals, but are not quite as good as preventing further reactions of the radicals as inhibitors. Hence, polymerization can still proceed in the presence of active retarder.
Introduction to Polymers, Third Edition, CRC Press, 2011.
Effects of Temperature
Effects of Temperature jls164Reaction rates typically depend on temperature, so what about polymerization reactions? More specifically, how are rate of polymerization and degree of polymerization dependent on temperature? As with any other reaction, temperature changes the rate constants associated with the polymerization. But there are many rate constants that affect polymerization, so the effect of temperature is not necessarily straightforward. If the temperature increased, we expect there to be more radicals generated in a shorter time frame, so the concentration of active centers will go up. Because rate of polymerization is directly correlated with concentration of radicals, the rate of polymerization will also go up with temperature. Can we simply keep increasing the temperature to increase indefinitely? That's not really an effective strategy, because depolymerization, which is the polymer reverting to monomer, is favored at elevated temperatures. At the ceiling temperature, the rate of polymerization and depolymerization are equal. Also consider that at higher temperatures, with higher concentration of radicals, that also means that termination rates will be higher. As the rate of termination increases, the degree of polymerization decreases, and the polymers will be shorter. Thus, the temperature at which you run a polymerization reaction can have significant impact on the resulting polymer formed and should be considered carefully.
Nonlinear Radical Polymerization
Nonlinear Radical Polymerization jls164Thus far, we have primarily considered free radical linear polymerizations of monomers containing a functionality of 2. With the exception of branching that can occur from chain transfer to polymer, a monomer with a functionality of 2 can only lead to linear polymers. But what if we use a monomer that has a functionality greater than 2? Much like what we discussed for step polymerization, we will get branching and possible formation of crosslinks leading to a network structure. In fact, many monomers for free radical polymerization that have a functionality higher than 2 are often called crosslinkers. Examples of common crosslinkers are shown in Figure 5.7 and Figure 4.2 in the textbook.

PROBLEM
What is the functionality of divinylbenzene?
- 1
- 2
- 3
- 4
ANSWER
- 4
Polymerization of a monomer and crosslinker would create a network polymer, such as diagramed in Figure 5.8. The monomers that have a functionality of 2 form linear polymers, that are linked by the crosslinker.

Introduction to Polymers, Third Edition, CRC Press, 2011
Summary and Final Tasks
Summary and Final Tasks sxr133Summary
We have now completed our lessons focused on free radical polymerization. The reactions, kinetics, and mechanisms you learned in Lessons 4 and 5 will be found elsewhere in the course, however, as radical polymerization is one of the most ubiquitous polymerization mechanisms. Next, we will be moving on to ionic polymerization, which as you will see has quite a few similarities in terms of the reaction mechanism to free radical. A key difference, however, is that the active center is no longer a radical, but an ion - and the fact that it is charged is what is going to give ionic polymerization distinguishing characteristics from free radical polymerization. Pay attention to similarities and difference between these reaction pathways as we move forward in the course.
Reminder - Complete all of the Lesson 5 tasks!
You have reached the end of Lesson 5! Review the checklist on the Lesson 5 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 6.
Lesson 6: Ionic Polymerization
Lesson 6: Ionic Polymerization sxr133Overview/Checklist
Overview/Checklist mjg8Overview
In this Lesson, we will learn about two additional chain growth polymerization mechanisms: cationic and anionic. These ionic polymerization mechanisms have several similarities to the radical chain growth polymerization in terms of the general mechanism (initiation, propagation, termination). An important distinction is that there will be a charged active center in ionic polymerization (while the radical active center is neutral). This charge is what primarily causes any differences we observe between ionic and radical chain growth. The different charge between cationic (positive charge) and anionic (negative charge) further leads to even more variation among ionic polymerization. Try to compare and contrast the three chain growth mechanisms as you go through the lesson to put in perspective and context how the various pathways are related to monomer chemistry, polymer skeletal structure, and reaction mechanism.
Learning Outcomes
By the end of this lesson, you should be able to:
- Predict if a monomer with polymerize via anionic or cationic pathways
- Compare and contrast ionic polymerization with free radical polymerization
- Draw the arrow pushing mechanism for cationic, anionic, and living anionic polymerization
- Describe the characteristics of living anionic polymerization
- Explain how the solvent and counter ions affect ionic polymerization rates
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 6. | Continue navigating the online material. |
| To Read | Chapter 5 - Ionic Polymerization
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 6 (Practice) | Registered students can access the homework assignment in the Lesson 6 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Ionic Polymerization Introduction
Ionic Polymerization Introduction ksc17In Lesson 6, we will continue to talk about chain polymerizations, but we will be exploring new reaction mechanisms: ionic polymerization. In contrast to free radical polymerization, in which the reactive species was a radical (which is neutral), in ionic polymerizations, the active center will be either an anion or a cation, thus carrying charge. Because of the charge associated with ionic polymerization, stabilization of that charge on the active center is going to be a much more critical factor to consider when deciding whether monomers will tend to polymerize with anionic or cationic pathways.

Think back to organic chemistry, where you learned about carbocations and carbanions. How were the carbocations and carbanions best stabilized? By substituents that could help distribute or delocalize charge! A carbocation is stabilized by substituents that donate electron density, since the carbocation is electron deficient. On the other hand, carbanions are best stabilized by substituents that withdraw electrons, since carbanions are electron rich. In most cases, a monomer will have a preference for whether it’s easier to polymerize by anionic or cationic pathways, depending on which active center intermediate is more stable. There are a few monomers, such as styrene, which distribute the charge so well that they can be polymerized by both pathways.
Let’s refresh your memory on electron withdrawing and electron donating groups:
| Electron Withdrawing Groups | Electron Donating Groups |
|---|---|
| -CF3 | -NH2 |
| -CN | -OR |
| -NO2 | -OH |
| -COOH (moderate) | -NHR |
| -COOR (moderate) | -OCOR (moderate) |
| -halides (weak) | -Ph (moderate) |
| - | -R (weak) |
PROBLEM
Do you expect acrylonitrile to proceed via anionic or cationic polymerization?

- Cationic
- Anionic
- Neither, free radical only
ANSWER
B. Anionic
Because –CN is strongly electron withdrawing.
Before diving into the specifics of both anionic and cationic polymerization, here is a general comparison of ionic polymerization with free radical polymerization:
- A propagating chain active center is accompanied by a counter ion (opposite charge) in ionic polymerization, but not with free radical polymerization.
- The counter ion can affect stereochemistry and rate of polymerization in ionic polymerization, which is not a consideration for free radical polymerization.
- The polarity of the solvent is more important in ionic polymerization than in free radical polymerization, because now we have charge to stabilize at the active center.
- Termination can’t occur by reaction between active centers because they are the same charge, whereas in free radical polymerization it is common to have termination by combination of radicals.
Cationic Polymerization
Cationic Polymerization ksc17Let’s first consider cationic polymerization in depth. Cationic polymerization goes through initiation, propagation, chain transfer, and termination, much like free radical polymerization. But cationic polymerization is of course characterized by having an active center that is a positively charged cation. Thus, we look for monomers that have substituents to help stabilize that positive charge and which are electron donating. Example monomers that can be polymerized by cationic polymerization are:

Initiation:
Cationic active centers are created by reaction of the monomer with an electrophile. Examples of good initiators are H2SO4 or HClO4; BF3, AlCl3, SnCl3 with ‘co-catalyst’ (water or organic halide, makes for more stable counter ion). The general steps of initiation are shown in Figure 6.3. As typical, there are two steps in the initiation process.

R+ is an electrophile and A- is the counter-ion. Note that a double headed arrow is used to show the reaction mechanism because we are pushing two electrons (as compared to with reactions in free radical polymerization, where our single headed arrows signified the movement of individual electrons).
Propagation:
Propagation usually takes place by head to tail addition because of the stability of the carbocation and steric considerations. Again, note the double headed arrows in Figure 6.3 and that the counter-ion is always present.

Termination and chain transfer:
Unlike in free radical polymerization, termination by two propagating chains reacting is not possible, because they have the same charge. Instead, termination occurs usually by ion pair rearrangement, releasing H+ and generating a terminal C=C as shown in Figure 6.4. Even though the terminated chain still has a double bond which in principle can continue to polymerize, due to the substitution on that terminal carbon, sterics will reduce the reactivity.

Chain transfer can also occur, similarly resulting in a terminated chain with an end C=C. Again, due to the substitution on the terminal carbon of the terminated chain, even though there is a double bond which can in principle continue to react, sterics will prevent reactivity. The chain that now contains the active center will continue to polymerize. Similar to free radical polymerization, chain transfer to polymer can affect the skeletal structure. Also like free radical polymerization, chain transfer to solvent can still occur and would reduce the degree of polymerization.

Solvent and Counter-ion effects:
Because we now have charge at our active center and have a counter-ion associated with our active center, we have to take into account effects of solvent and that counter-ion that we didn’t have to consider for free radical polymerization. As follows from our general understanding of how added steric bulk prevents reactions, then it’s no surprise that “freer” carbocationic active centers propagate faster (higher kp) than if associated closely with a counter ion. Polar solvents will help to separate ion pairs. Not only can propagation occur faster, but more ion pair separation will also reduce ion pair rearrangement and rate of termination.

PROBLEM
How do you think counter ion size affects kp?
- Larger counter ion size means higher kp
- Smaller counter ion size means higher kp
- Counter ion size has no significant effect on kp
ANSWER
A. Larger counter ion size means higher kp
Larger counter ion size means more physical separation between active center and counter ion, so more space for the monomer to insert and react
Anionic Polymerization
Anionic Polymerization ksc17We now move onto anionic polymerization where we have a negative charge at our active center. To stabilize our active center, we then want to have electron withdrawing substituents on the active center carbon in order to help delocalize the excess charge.
Initiation:
Anionic polymerizations are often initiated by strong nucleophilic initiators, such as potassium amide. As we often see, there are two steps for initiation:

Styrene is one of the monomer most commonly polymerized by anionic polymerization.
Propagation:
Again, looks similar to what we have seen before for propagation but with an anion at the active center. Similarly to initiation, we are showing the propagation for polymerization of styrene.

Termination and Chain Transfer:
Like other chain polymerizations we have seen, we can get chain transfer to solvent. However, for anionic polymerization, we do not see ion pair rearrangement, and there is no formal termination. Why? Well, it would require transfer of a hydride (H-), rather than an H+ which we saw for cationic polymerization; this is unfavorable. Therefore, there is no formal pathway for termination. In order to terminate the polymerization, special molecules would need to be added to cap the polymer with non-reactive functional groups. In the absence of any termination, we call this kind of anionic polymerization a living polymerization.
Kinetics of Living Anionic Polymerization:
It is interesting to compare the kinetics of living polymerization with the free radical polymerization kinetics to see the effect that removing chain transfer and termination have on the kinetics. When carried out in a polar solvent, it is generally true for these anionic polymerizations that ki is much greater than kp since pretty much all our initiator is in the active form very early on. So, the total concentration of carbanionic active centers equals the concentration of initiator used initially . And we can write the rate of propagation:
where is a constant, so we see there is only dependence on , concentration of monomer. We can also easily describe the degree of polymerization:
where c=fractional conversion of monomer and K equals the number of active centers generated per initiator (often, this is 1 for initiators like KNH2 but there are some initiators that generate 2 active carbanions per initiator molecule, which case K=2). We find from this equation that degree of polymerization increases linearly with monomer conversion (which is very different than for free radical polymerization!)
Because the mechanisms for living polymerizations without terminations are quite different from step or chain mechanisms, the derivation for the molar mass distribution is different. (we will not go into depth here). For living polymerization, the molar mass dispersity is given below and a plot of the distributions for various values of is given in Figure 6.10 below (textbook Figure 5.1). Notice that the distributions are relatively narrow, which is different from what we have seen previously for step polymerization and free radical polymerization.

Summary and Final Tasks
Summary and Final Tasks ksc17Summary
Reminder - Complete all of the Lesson 6 tasks!
You have reached the end of Lesson 6! Review the checklist on the Lesson 6 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 7.
Lesson 7: Stereochemistry, Coordination, and Ring-Opening Polymerization
Lesson 7: Stereochemistry, Coordination, and Ring-Opening Polymerization sxr133Overview/Checklist
Overview/Checklist mjg8Overview
In this Lesson, we consider some intricacies of chain polymerization which we have disregarded to this point. For example, you all have learned about the concept of chirality in organic chemistry - is there such a thing for polymers, and how is it controlled? There is, and we call it tacticity - and the tacticity of the polymer has very important ramifications for the polymer properties. What about monomers that are conjugated and can have resonance? We will look at what happens when we polymerize dienes, which have conjugated double bonds, both of which can participate in polymerization. Lastly, we consider a special type of chain growth polymerization where are monomers are actually cyclic, called ring opening polymerization.
Learning Outcomes
By the end of this lesson, you should be able to:
- Identify the tacticity of a polymer.
- Draw the mechanisms for polymerization of dienes leading to 1,2 addition, 3,4 addition, and cis/trans 1,4 addition products.
- Describe the benefits of coordination polymerization and why Ziegler Natta polymerization is used.
- Draw mechanisms and describe the tacticity for cationic and anionic ring opening polymerization.
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read through all of the online lesson material for Lesson 7 | Continue navigating the online material. |
| To Read | Chapter 6 - Stereochemistry and Coordination Polymerization
Chapter 7 - Ring-Opening Polymerization
| The chapter readings come from the textbook, Introduction to Polymers |
| To Do | Homework Assignment 7 (Practice) | Registered students can access the homework assignment in the Lesson 7 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Ring Opening Polymerization
Ring Opening Polymerization jls164Many commercially important polymers that you may use in your daily lives, such as epoxy glue, rely on ring opening polymerization. Ring opening polymerization is characterized by using a monomer that is cyclic (a ring) and the mechanism can proceed by radical, anionic, or cationic pathways depending on the specific monomer and initiator. During polymerization, the ring opens and creates a linear polymer. In many ways, ROP is familiar to our other mechanisms, and we can use it to make many of the same polymers (and some new ones). It still requires initiation, it still goes through propagation and termination, it still follows the same rules for electron donating and electron withdrawing groups as we learned for cationic and anionic polymerization.

Introduction to Polymers, Third Edition, CRC Press, 2011.
So why use a cyclic monomer instead of a non-cyclic one? Well, one important thing going for cyclic monomers (with small rings) is that they have ring strain, which makes them somewhat less stable (and hence more reactive) than non-cyclic monomers. For larger rings, they have less ring strain, but more steric repulsion between the ring substituents, which also makes them unstable.
Let's first look at a cationic ring opening polymerization of epoxides, which are very common cyclic monomers, and are used to produce polyethers. We can use the same initiator molecules. Note the use of double-headed arrows for moving pairs of electrons. We see some equilibrium structures here as well that are new - the cationic intermediates are in equilibrium between the ring open and ring closed state. Termination can occur by rearrangement, just as we saw before in cationic polymerization.

Introduction to Polymers, Third Edition, CRC Press, 2011.
We can also consider ring opening polymerization of epoxides by anionic polymerization, as shown below.

Introduction to Polymers, Third Edition, CRC Press, 2011.
Notice that again we see the same kinds of initiators as was typical for anionic polymerization. We have added an "R" group onto the epoxide to help stabilize the anion, and because of this substitution, the nucleophilic attack will occur on the least hindered carbon. We also see no inherent termination process, unlike cationic polymerization.
In addition to epoxides, another common class of cyclic monomers are lactones:

Introduction to Polymers, Third Edition, CRC Press, 2011.
PROBLEM 1
Of the monomers shown below, which would yield a polyether when polymerized by ring opening polymerization?

- Isotactic polybutadiene
- Syndiotactic polybutadiene
- Atactic polybutadiene
ANSWER 1
A. Isotactic polybutadiene
Isotactic polybutadiene would yield a polyether

PROBLEM 2
Of the monomers shown below, which one would you choose to make this polymer?


ANSWER 2
D.

Tacticity
Tacticity jls164Because we usually draw polymers as flat 2D structures on a piece of paper, it's easy to forget that actually polymers are three-dimensional and the structure often has very important ramifications on the polymer properties and chemistry. For example, in organic chemistry, you learned about chirality or the "handedness" of molecules, where the position of the atoms in 3D space differ by mirror images of one another. Molecules that are chiral have the same connectivity of the atoms, but are not the same molecules - the structures would not be able to be overlaid with each other when the 3D structure is considered. We use a similar concept for polymers, tacticity.

Introduction to Polymers, Third Edition, CRC Press, 2011.
Look at the two repeat units shown in Figure 7.5. Recall from organic chemistry that we used the dashed lines to indicate a bond that goes "into" the page, and a bold line to indicate a bond "coming out of" the page, to give a 3D representation of the molecule. We see in Figure 7.5 that the connectivity of all the atoms is identical between the two structures, but the X and Y substituents are flipped in their 3D orientation. (The carbon that has the X and Y substituents is called an asymmetric carbon.) Therefore, these repeat units are actually not exactly the same; they cannot be overlaid with each other, no matter what orientation you choose. So even though the same monomer could be used to make both of these repeat units, these repeat units are different! In order to describe this difference in 3D structure, we use the concept of tacticity.
There are three terms we use to describe polymer tacticity. Isotactic means that all asymmetric carbons in the polymer have the same configuration. Syndiotactic means that the asymmetric carbons have alternating configuration. Atactic means that the asymmetric carbons have random orientation. Drawings of each of these is shown below. Notice that in order to have tacticity, you must have asymmetric carbons. If X=Y in Figure 7.5, then there is no asymmetric carbon, and no relevant tacticity. Also realize that the entire polymer does not have to be just one of these categories, there may be short stretches along the polymer which can take on any tacticity. Tacticity is important because it can affect the chemistry, reactivity, and mechanical properties of polymers. You can imagine that if the polymer structure is more "regular", such as an isotactic polymer versus an atactic polymer, that the isotactic polymer may be able to pack better, and thus crystallize more easily, which would significantly affect its material properties.

Introduction to Polymers, Third Edition, CRC Press, 2011.
So how does this tacticity arise? To understand this, we have to remember what the 3D structure of our active center looks like. Recall that the radical on our active center is in an unhybridized p orbital that is perpendicular to the plane with the sp2 orbitals bonded to the substituents, as shown in Figure 7.7 below. In a slight oversimplification, we can imagine that the orientation of the next repeat unit will depend on whether the next monomer approaches the active center from above or below. If you are interested, for a more detailed figure depicting how this orientation gets translated to the tacticity, please see Figure 6.2 in the text.

Introduction to Polymers, Third Edition, CRC Press, 2011.
PROBLEM
The polymer below was formed from ring opening polymeriztion of the below monomer. What is the tacticity of this polymer?

- Isotactic
- Syndiotactic
- Atactic
ANSWER
A. Isotactic
Notice that isotactic and syndiotactic refer to the stereoisomerism of the asymmetric carbons, not necessarily the direction those bonds are "pointing". Here, we see the R groups alternate between going into and out of the page, so our first instinct is likely to say that this is a syndiotactic polymer - but also notice that if you were to rotate all the carbons so that they are pointing in the same direction, that in fact, all the carbons with the R group have the same stereochemistry, making it isotactic.
Control of tacticity and stereochemistry
Control of tacticity and stereochemistry jls164There are multiple variables that can affect the resulting stereochemistry of the polymer, such as counter ion, solvent, or temperature. However, it is still very difficult to make highly regular structures by any of the polymerization mechanisms we have discussed thus far. If we need to make highly stereoregular structures, we need a different approach: coordination polymerization. Coordination polymerization involves the addition of monomers to an organometallic active enter.
One of the most important coordination polymerization catalysts is the Ziegler-Natta catalyst. The Ziegler-Natta catalyst allows for the synthesis of highly linear, stereoregular polymers. For example, at the beginning of the course, we introduced both high and low density polyethylene; well, to make the high density polyethylene (HDPE), we noted that you had to have very highly linear polyethylene that packed together well. Such HDPE is often made using coordination polymerization, and cannot be accomplished by other polymerization routes. Similarly, polypropylene can also be produced with a highly steroregular structure (isotactic or syndiotactic) through coordination polymerization. A simplified mechanism of how this works is shown using a Zr catalysts is shown in Figure 7.8.
Since you have not likely taken inorganic chemistry, and for coordination polymerization we are dealing with organometallic molecules, I am not going to expect you to learn or understand exactly how the polymerization mechanism works. But there are a couple important differences to note. First, we see that the organometallic catalyst is located at our active center and "holds on" to the monomer. It holds on to the monomer is a very specific orientation, and so every monomer reacts in the same orientation. Recall how in Figure 7.7, we showed that the stereochemistry is controlled by whether the monomer approaches the active center from above or below? Well, we are basically using this organometallic catalyst to help us control that. But we also see that since the Zr has to coordinate to the monomer that the monomer has to be able to approach the catalyst and that bulky groups are going to prevent this coordination from happening. Therefore, we can't use this technique for every polymer, and those with bulky substituents are going to be less active towards coordination polymerization.
Modes of Addition for Conjugated Monomers
Modes of Addition for Conjugated Monomers jls164Thus far, we have only considered chain polymerization of monomers that have isolated reactive groups. But we also recall from general chemistry and organic chemistry that double bonds are conjugated and can participate in resonance (depending on the molecular structure). So what happens if we have a conjugated monomer? For example, 1,3-butadiene and isoprene are common monomers (shown below) which have conjugated double bonds. How do these monomers react?

Introduction to Polymers, Third Edition, CRC Press, 2011.
There are going to be multiple ways in which these unsaturated bonds can react. To keep track of which carbon is where, we need to number our carbons. Following tradition from the naming of organic molecules, we number our carbons along the carbon chain with the diene and start counting with the carbon nearest the substituent. Take this generic diene as an example, where "R" represents some substituent. We number the carbons as follows:

Introduction to Polymers, Third Edition, CRC Press, 2011.
It is very important that you number your carbons correctly, or you will end up drawing the wrong polymerization products. Please note that you do not necessarily number from left to right, it just depends on where that substituent "R" is located. We see we have two unsaturated bonds that we could polymerize: the 1,2 and 3,4 bonds. Figure 7.11 shows the products we get if we polymerize through those bonds:

Introduction to Polymers, Third Edition, CRC Press, 2011.
We see we get two very different polymer depending on whether we react the 1,2 or 3,4 bond. (Also, don't forget that each of these polymers can have tacticity!) But we aren't quite done, because these dienes have conjugated double bonds, which we know can have resonance. This means, if we generate an active center, that it can move through the molecule via resonance and this will also affect our products. To make things even more complicated, single bonds can rotate, and the bond rotation in the diene will also affect our polymer! As shown in Figure 7.12, because of these resonances and bond rotation we can also get cis 1,4 addition and trans 1,4 addition. (Remember the "cis" and "trans" geometric isomers from general chemistry and organic chemistry?).

Introduction to Polymers, Third Edition, CRC Press, 2011.
Just as tacticity was important to the polymer structure and properties, so is the mode of addition for dienes. Depending on whether you have primarily cis or trans addition, you can have polymers with very different mechanical properties.
PROBLEM
Shown below are (A) trans, (B) cis, and (C) vinyl polybutadiene (from left to right). Which one is most crystalline?

- Trans polybutadiene
- Cis polybutadiene
- Vinyl polybutadiene
ANSWER
A. Trans polybutadiene
The regular zig zag structure of the backbone will allow the polymer to pack better giving it more crystallinity.
Summary and Final Tasks
Summary and Final Tasks ksc17Summary
After this lesson, you should now feel comfortable identifying the tacticity of a polymer, describing how the tacticity impacts the polymer properties, and suggesting methods by which to control tacticity. Additionally, you should be able to draw the products of polymerization of dienes, and describe the mechanism of the various products are formed. Lastly, you now can suggest cyclic monomers to use to create polymer via ring opening polymerization, and notice how many of those polymers you can also make by step growth! Next, we move onto copolymers – where we have not just one type of monomer, but two or more. We will find that when we mix monomers, it’s likely that one monomer is more reactive (and incorporated more quickly into the polymer). How do we measure that, and determine which monomers will actually end up in the polymer? All coming soon, in Lesson 8!
Reminder - Complete all of the Lesson 7 tasks!
You have reached the end of Lesson 7! Review the checklist on the Lesson 7 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 8.
Lesson 8: Copolymerization
Lesson 8: Copolymerization jls164The links below provide an outline of the material for this lesson. Be sure to carefully read through the entire lesson before submitting your assignments.
Overview/Checklist
Overview/Checklist mjg8Overview
You now have a great toolbox of monomers and polymerization mechanisms by which you can make all sorts of exciting polymer materials! You can decide what sorts of monomers and polymerization mechanisms to use, when and how to control tacticity, and how polymerization mechanism impacts skeletal structure for both step growth and chain growth (radical, cationic, anionic, and ring opening). Let’s expand that breadth even more, and think about how we can mix monomers together to create copolymers. In Lesson 1, we learned the difference between homopolymer and copolymer, but most of the polymers we have actually talked about up until now have been homopolymers which incorporate a single type of monomer. In this Lesson, we learn how to predict the ratios in which a monomer will be incorporated into a polymer, and how that composition might drift over the course of a reaction.
Learning Outcomes
By the end of this lesson, you should be able to:
- Explain under what circumstances, and why, the composition of a polymer changes with extent of reaction
- Distinguish between homopropagation and cross propagation reactions
- Describe kinetics of binary chain copolymerization
- Define reactivity ratio
- Apply copolymer composition equations to predict polymer compositions
- Describe, in terms of reactivity ratios, the conditions leading to random copolymerization, azeotropic copolymerization; block copolymers, alternating copolymers, or homopolymers
- Interpret plots of FA vs fA
- Explain composition drift using reactivity ratios
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 8. | Continue navigating the online material. |
| To Read | Chapter 9 - Copolymerization
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 8 (Practice) | Registered students can access the homework assignment in the Lesson 8 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Introduction
Introduction jls164n this lesson, we will consider what happens in terms of kinetics and skeletal structure when we polymerize two or more different monomers together to create a copolymer. We already learned in general what a copolymer is in Lesson 1 “what is a polymer?”. Make sure to refresh your memory on the difference between homopolymer and copolymer, and the definitions of alternating copolymer, block copolymer, random copolymer, and statistical copolymer.
Let’s consider a copolymer formed from reacting two monomers together. We consider a system in which the different monomers can react with each other, and they can also react with themselves. An example would be in the case of chain growth polymerization of two different monomers with vinyl groups. (This is an important point, because we saw some examples of step polymerization in which you could only get an alternating copolymer, RA2+RB2, just because of the specific functional groups that had to react. We are not considering that situation right now.) Consider the situation shown in Figure 8.1 where we have a purple and green monomer, and the purple happens to be incorporated faster into the polymer than the green one. Well, then at the start of our reaction, the polymer we form is going to contain mostly purple monomers. Later in the course of reaction, we find we have used up most of the purple monomers but have lots of green monomers left, so we begin to incorporate the green monomers more often than purple. As you can see, this leads to a distribution of the purple and green monomers along the polymer that is uneven; we have more repeat units of purple at one end of our polymer and more green at the other. You could also imagine that you stop the reaction before getting to a high extent of reaction, and end up with a polymer that has almost no green monomers at all! So what factors influence this distribution of purple and green along the length of the polymer? Can we predict and describe how various monomers will be incorporated when they are polymerized together?

Chain Growth Binary Copolymerization
Chain Growth Binary Copolymerization jls164Let’s narrow our focus to 1) chain growth polymerization and 2) binary copolymerization. The chain growth part you already know, and for binary copolymerization we mean that there will only be two different monomers, which we will call A and B. Now because we have two different monomers, that means we can also have two different active centers: -A* and –B*. We designate the active enter with an * because it could be any number of species, such as radical, anion, or cation. Since A can react with A, A can react with B, and B can react with B, we have several different modes of addition that can occur:
When an active center on A reacts with another A, or when an active center on B reacts with another B, we call these homopropagation reactions. When an active center on B reacts with A, or when an active center on A reacts with B, these are called cross-propagation reactions. We can describe the rate of monomer consumption for both A and B monomers as the sum of the processes that consume those monomers. For example, A is consumed in reactions (1) and (3) as outlined above. B is consumed in reactions (2) and (4). We then write the rate of consumption for each A and B monomer:
For any point during the reaction, we now have expressions that describe how much A or B is being incorporated. What about the ratio of incorporation? By looking at a ratio of the rates of incorporation of A and B, we can immediately have a sense of which monomer is being preferentially consumed:
This equation for d[A]/d[B] looks a little scary, but if we could just substitute for the concentration of active centers, we could simplify it….. How can we figure out the steady state concentration of active centers?
To start, we can describe the rate of change of [A*] and [B*], which are the active centers, very similarly to how we described the change in [A] and [B]. A* is consumed in reaction (4) but created in reaction (3). (Homopropagation reaction (1) also involves A* but there is no net change in the concentration of A* in reaction (1), thus we do not need to consider it). B* is consumed in reaction (3) and produced in reaction (4). (Again, homopropagation reaction (2) has net zero effect on [B*] so we don’t consider it). Therefore, we can write the change in concentration of active centers:
Let’s apply what we just learned to steady state conditions. Remember our steady state assumption? At steady state, we assume there is no change in the concentration of active centers, so:
When we apply this steady state condition and set d[A*]/dt=d[B*]/dt with the equations above, we get:
This equation gives us the steady state ratio of A and B active centers. We can also now substitute this into Equation 8.3 to get:
Where and . We call Equation 8.7 the copolymer composition equation. The copolymer composition equation is another example of an instantaneous equation, because the concentrations of the monomers change over time. These new variables, rA and rB , are called the monomer reactivity ratios. (Do not confuse the reactivity ratios with the reactant ratio r that we learned for Carothers theory!)
So what does this copolymer composition equation tell us? For any given instant in time, this equation tells us the molar ratio of A and B that is being incorporated into the copolymer. Sometimes, it can also be helpful to express the incorporation of A and B in terms of a fraction: what fraction of monomer being incorporated is A (=FA), or what fraction of monomer being incorporated is B (=FB)? Because we are only considering a binary case with two different monomers, we can express FA and FB as:
To summarize, FA and FB represent the mole fraction of A or B being incorporated into the polymer at a particular time.
What about the mole fraction of A and B monomer left in the reaction? Similarly, we can describe those with fA and fB (note the lowercase to distinguish from FA and FB):
To summarize, fA and fB represent the mole fraction of A and B monomer in the reaction mixture (not in the polymer!)
We can now rewrite our copolymer composition equation (equation 8.7) as a function of fA, fB, FA, FB:
We can use these relationships to predict copolymer composition from the co-monomer composition and reactivity ratios
PROBLEM
You have an equimolar mixture of A and B monomers. rA = 0.9 and rB = 1.2. What is the composition of the copolymer formed at low monomer conversions?
ANSWER
Equimolar ratio means . Using that, we plug in to FA:
This result tells us that 46% incorporation is of A and the rest is B. What is of importance to notice here is that although you start with a 50/50 ratio of monomers, your polymer does NOT have the same monomer ratio! You are incorporating less A than you are B as a result of these reactivity ratios. *side note - Why is “low monomer conversion” specified? It is because as you let the reaction proceed to higher monomer conversions, the ratio of A and B monomer will change! Even though we start with an equimolar ratio of A and B, because here we are using up B faster than A, we are going to deplete our monomer mixture of B. Thus, at higher monomer conversions, the concentration of A will be higher than 0.5, and the concentration of be will be lower than 0.5. By specifying “low monomer conversion” we are assuming that the values of fA and fB are not changing significantly.*
It’s worth taking a more in depth look at these reactivity ratios given how important they are; reactivity ratios dictate the composition of the copolymer formed instantaneously, and influence the overall distribution of A and B groups in the copolymer. Let’s look at their definition again. What do they mean?
Notice that they are the ratio of rate coefficients for homopropagation to cross-propagation for A and B monomer! Let’s try to translate these mathematical relationships into an intuitive understanding.
PROBLEM 2
If rA>1, what does this mean?
- ~A* prefers to add to A
- ~A* prefers to add to B
- ~B* prefers to add to A
ANSWER 2
A. ~A* prefers to add to A
If rA>1, then kAA must be larger than kAB. Thus, ~A* adding to A (homopropagation) is faster than ~A* is adding to B (cross-propagation). No information about ~B* adding to A is given in rA.
Copolymer Equation
Copolymer Equation jls164A useful way of representing information from the copolymer equation is to plot FA as a function of fA. Let’s walk through how to do this using the reactivity ratios from the previous question, rA = 0.9 and rB = 1.2. First, we are going to just choose example values of fA ranging from 0 to 1 (listed in the fA column of the data Table 8.1 for Figure 8.2). Next, we can find fB for each data point, because fB = 1-fA. Then, we plug the given values of rA = 0.9 and rB = 1.2 and the values of fA and fB into the expression:
The values we calculated are shown below in Table 8.1. Plotting FA for each value of fA yields the graph shown below in Figure 8.2. Notice that the answer to the previous problem, which was FA=0.46, in fact corresponds to fA=0.5 as expected.
| fA | fB | FA |
|---|---|---|
| 0 | 1 | 0.00 |
| 0.05 | 0.95 | 0.04 |
| 0.1 | 0.9 | 0.09 |
| 0.15 | 0.85 | 0.13 |
| 0.2 | 0.8 | 0.17 |
| 0.25 | 0.75 | 0.22 |
| 0.3 | 0.7 | 0.27 |
| 0.35 | 0.65 | 0.31 |
| 0.4 | 0.6 | 0.36 |
| 0.45 | 0.55 | 0.41 |
| 0.5 | 0.5 | 0.46 |
| 0.55 | 0.45 | 0.51 |
| 0.6 | 0.4 | 0.57 |
| 0.65 | 0.35 | 0.62 |
| 0.7 | 0.3 | 0.67 |
| 0.75 | 0.25 | 0.73 |
| 0.8 | 0.2 | 0.78 |
| 0.85 | 0.15 | 0.83 |
| 0.9 | 0.1 | 0.89 |
| 0.95 | 0.05 | 0.94 |
| 1 | 0 | 1.00 |

Looking at plots of FA as a function of fA is very helpful in visualizing the relative incorporation of A and B monomers into the polymer. Figure 9.1 in the textbook (and replicated as Figure 8.3 below) shows such plots for varying combination of reactivity ratios. Can you rationalize why each curve as the shape it does? We will spend a significant amount of time considering this graph!

Introduction to Polymers, Third Edition, CRC Press, 2011.
Figure 8.3 is a plot of for various values of reactivity ratios and monomer ratios. This is a key figure illustrating how the reactivity ratios and mole fraction of monomers affect the incorporation of the monomer into the polymer, ultimately determining the polymer composition. The shapes of each of these curves is meaningful, and we will discuss how to interpret this plot.
Take a minute to use the interractive graph below to explore the copolymerization reaction. You can use the sliders to change the values of rA and rB. You can also ust the text entry box to directly enter values for rA and rB. Try adjusting the values to match some of the curves in Figure 8.3 above.
Note: If you hover your mouse over the plot, the X = N/A and Y = N/A boxes will show the coordinates of you cursor.
Note:
If you are unable to interract with the graph above, try opening the page in a different browser.
PROBLEM
“Random” copolymers are defined as having FA=fA for all values of fA. To put that into words, it means that the fraction of A incorporated into the polymer is the same as the fraction of A in the monomer solution for any given monomer fraction of A. What reactivity ratios must we have in order to form a random copolymer?
ANSWER
rA and rB both must equal 1. The random copolymerization conditions correspond to the solid line fA=FA in Figure 8.3. Looking at the key to this figure, we can find that this corresponds to reactivity ratio values of 1. Mathematically, we need values of reactivity ratios that would simplify to FA=fA. This happens when rA=rB=1. Shown below is the substitution and simplification math (don’t forget that fA+fB =1!)
Intuitively, when rB and rA = 1 then both homopropagation and cross-propagation for ~A* and ~B* happen at equal rates. If kAA=kAB (which is the case for rA=1) then ~A* has no preference for adding to A or B. Similarly, if kBB=kBA (which is true for rB=1) then ~B* also has no preference for adding to A or B. Therefore, the relative amounts of A and B incorporated into the polymer simply reflect the distribution of A and B in the monomer solution. There are relatively few copolymerizations that fulfill this requirement. However, also realize that the reactivities of the 2 active centers (~A* and ~B*) don’t have to be the same for random copolymerization.
So we just learned that a random copolymer forms when fA=FA, which can happen when rA=rB=1. What happens when this is not the case? For instance, what if fA<FA, what does that mean? Look at the conditions highlighted below, where an exemplary line for rA=4 and rB=0.1 ( highlighted in blue ). We see that this curve always falls above the line fA=FA indicating that the fraction of A being incorporated into the polymer is greater than the fraction of A in the monomer mixture for all molar fractions of A. This is because both active centers (~A* and ~B*) prefer to add to A monomer, which we know because kAA>kAB and kBA>kBB, based on the given values of reactivity ratios (i.e. rA>1 and rB<1). We can use the same pattern of logic to understand why for the exemplary curve rA=0.1 and rB=10 ( highlighted in yellow ), fA >FA for all molar ratios of A; both active centers prefer to add to B monomer, so we always incorporate less A into the polymer than there is A in the monomer solution.

rA=4 and rB=0.1 ( blue plot )
rA=0.1 and rB=10 ( yellow plot )
Introduction to Polymers, Third Edition, CRC Press, 2011.
Azeotropic Copolymerization
Azeotropic Copolymerization jls164Another special case of copolymerization is that of azeotropic copolymerization, where rA and rB are both less than 1, or, rA and rB are both greater than one (this case is rarer). Two examples are highlighted below. Notice that these curves cross the line fA=FA at a point called the azeotropic composition (fA)azeo. These points have been noted with green dots in figure 8.5. The name “azeotropic” comes from the analogy with phase diagrams of liquid-liquid mixtures, where an azeotropic mixture is characterized by having a vapor phase upon boiling with the same ratio of components as the liquid mixture. Similarly, for copolymerization, at the azeotropic composition, (fA)azeo, we find fA=FA indicating that monomer A is being incorporated into the polymer in the same proportion in which A exists in the monomer solution. Substituting the fact that fA=FA into our copolymer equation (equation 8.8) we can simplify to get an expression for the azeotropic composition:

and the green dots indicate the azeotropic composition.
Introduction to Polymers, Third Edition, CRC Press, 2011.
PROBLEM
A special case of azeotropic copolymerization is where both rA and rB=0. What would be the structure of this polymer?

Introduction to Polymers, Third Edition, CRC Press, 2011.
- Poly(A)-block-poly(B)
- Poly(A)-rand-poly(B)
- Poly(A)-graft-poly(B)
- Poly(A)-alt-poly(B)
ANSWER
D. Poly(A)-alt-poly(B)
Because both reactivity ratios are 0
This means that both kAA and kBB must be zero. Since homopropagations can’t occur, the sequence MUST alternate!
Copolymer Composition Drift
Copolymer Composition Drift jls164For most copolymerizations, fA ≠ FA and so, one monomer is preferentially consumed during polymerization. This means that as the reaction proceeds, the overall composition of the comonomer mixtures changes, i.e., fA and fB change over the course of the polymerization. And if fA and fB change, then FA and FB must also change as a function of monomer conversion! This process, which the monomer composition and polymer composition change over the course of the reaction, is called copolymer composition drift. Copolymer composition drift can lead to synthesis of polymers having very different composition over their lengths, and can become especially significant at higher monomer conversions.

PROBLEM
If rA>1 and rB<1 then fA…
- Increases with higher extents of reaction
- Decreases with higher extents of reaction
- Does not change as a function of extent of reaction
ANSWER
B. Decreases with higher extents of reaction
Because A is preferentially consumed (which we know, because of the reactivity ratios, and in turn fA<FA), A will be used up more quickly than B, and so will become depleted in the commoner mixture at higher extents of reaction.
Given below are some example values of reactivity ratios for pairs of monomers for free radical polymerization. Notice that you need to consider the monomers together, and not individually; the reactivity ratio is not inherent to the monomer, but rather is a function of what you are trying to copolymerize and the conditions of the reaction.
| Monomer A | Monomer B | rA | rB | rArB |
|---|---|---|---|---|
| Styrene | Butadine | 0.78 | 1.39 | 1.08 |
| Styrene | Methyl methacrylate | 0.52 | 0.46 | 0.24 |
| Styrene | Methyl acrylate | 0.75 | 0.18 | 0.14 |
| Styrene | Acrylonitrile | 0.40 | 0.04 | 0.02 |
| Styrene | Maleic anhydride | 0.02 | 0 | 0 |
| Styrene | Vinyl chloride | 17 | 0.02 | 0.34 |
| Vinyl acetate | Vinyl chloride | 0.23 | 1.68 | 0.39 |
| Vinyl acetate | Acrylonitrite | 0.06 | 4.05 | 0.24 |
| Vinyl acetate | Styrene | 0.01 | 55 | 0.55 |
| Methyl methacrylate | Methyl acrylate | 1.69 | 0.34 | 0.57 |
| Methyl methacrylate | n-Butyl acrylate | 1.8 | 0.37 | 0.67 |
| Methyl methacrylate | Acrylonitrile | 1.20 | 0.15 | 0.18 |
| Methyl methacrylate | Vinyl acetate | 20 | 0.0015 | 0.30 |
| trans-Stilbene | Maleic anhydride | 0.03 | 0.03 | 0.001 |
The exact reactivity ratios are often hard to predict, and therefore are mostly determined experimentally. We can get a sense of how well various monomers stabilize the radical active center in comparison to one another based on these reactivity ratios; do the trends match what we predict? Resonance enhances radical stability; if we polymerize a monomer that stabilizes a radical well via resonance with one that doesn’t (such as, styrene with vinyl chloride) we find that the more stabilizing monomer (styrene) is preferentially incorporated (rstyrene>>1, rvinyl chloride <<1). More alkyl substituents also help to stabilize radicals (i.e., a radical on a tertiary carbon is more stable than a secondary carbon), so let’s compare methyl methacrylate versus methyl acrylate. The methyl methacylate should stabilize the radical better on a tertiary carbon, and thus we find that the methyl methacrylate is more readily incorporated into the polymer, as predicted.
PROBLEM 2
Consider the cationic polymerization of nitroethane (monomer A) and chloroprene (monomer B) with rA=33 and rB=0.15. How could you describe the structure of the polymer formed based on these reactivity ratios?
- Random structure is promoted
- Alternating structure is promoted
- “blocky” structure is promoted
ANSWER 2
C. “blocky” structure is promoted
Monomer A is much more reactive than the monomer B, rArB>1. This favors homopolymerization and would lead to formation of blocks.
Summary and Final Tasks
Summary and Final Tasks jls164Summary
This Lesson concludes our in depth discussion of copolymerization and the factors we need to consider when mixing monomers. Its clearly a lot more complicated than you might have imagined, in large part because monomers all have different reactivities. This variability in reactivity leads to monomers being incorporated into the polymer at different rates, which ultimately can lead to composition drift. However, understanding these principles allows us to control the composition of copolymers which is critical for tuning a polymer's properties and structure, which we will be covering soon!
Reminder - Complete all of the Lesson 8 tasks!
You have reached the end of Lesson 8! Review the checklist on the Lesson 8 Overview /Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 9.
Lesson 9: Polymer Conformations
Lesson 9: Polymer Conformations jls164Overview/Checklist
Overview/Checklist mjg8Overview
Up until this point, we have largely been focused on understanding the molecular scale structure and reactivity of polymers. Now, let’s think bigger – how do those polymer behave when you dissolve them in solution? No molecule exists in isolation, so we must consider how polymers interact with other polymers as well as solvent. And, perhaps even before getting to that point, we need to think about the conformations the polymer can adopt in the first place – is it coiled? Is it elongated? Is the polymer flexible, or is it stiff? In Lesson 9, we will address the concept of polymer conformations and discuss ways in which we can represent the “size” of a polymer and how stiff it is. These concepts will be important for characterizing and representing the behavior of a polymer in solution, the thermodynamics of which will be covered in Lesson 10.
Learning Outcomes
By the end of this lesson, you should be able to:
- Calculate contour length and fully extended end to end distance
- Calculate root mean square end to end distance using freely jointed chain, valence angle model, and hindered rotation model
- Predict which polymers will be more sterically hindered to ration than others
- Describe chain stiffness using the characteristic ratio
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 9. | Continue navigating the online material. |
| To Read | Chapter 10 - Theoretical Description of Polymers in Solution
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 9 (Practice) | Registered students can access the homework assignment in the Lesson 9 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Polymer Conformations in Solution
Polymer Conformations in Solution jls164Thus far, we have been primarily considering individual molecules of polymers in isolation. But polymers don’t exist in isolation – they exist amongst other polymers and often dispersed in a solvent. So, how does a polymer behave when it is dispersed in a solution – is the polymer extended? Does it coil up? Is the polymer ordered, or is it randomly oriented? How much volume does the polymer take up in the solution? These are the types of questions that we begin to think about now.

We have previously discussed polymer size in terms of mass (Mw, Mn), but now let’s think in terms of volume – how much space does it occupy, and what is the conformation in solution? There are a few key characteristic parameters that give us some insight into polymer size and conformation.

Contour length is one of the simplest, but also one of the least accurate, descriptors of polymer size. Contour length is defined as the length of the polymer if you were to stretch the polymer out in a line. Disregard bond angles, just pull it as straight as possible, with the constraint being the bond distances. This is of course unrealistic, but it gives the absolute maximum length estimation for polymer size.
Fully extended chain length differs from contour length in that it considers that there are preferred bond angles within the backbone of the polymer. For a backbone consisting of all sp3 hybridized carbons, we expect that angle to be 109.5°. Thus, because we have this zigzag in the backbone, then fully extended chain length for a given polymer will be shorter than the contour length. This fully extended chain model isn’t realistic either, although it’s somewhat better than contour length because at least it includes bond angles.
PROBLEM
For polyethylene with molar mass = 280,000 g/mol, what is the fully extended length? Neglect end groups. Polyethylene is shown below.

ANSWER
The molar mass of the repeat unit of polyethylene (as written above) is 28 g/mol. Therefore we can calculate the degree of polymerization:
And the fully extended length would be:
That’s HUGE! For a point of comparison, the width of a human hair is about a hundred microns – and this 2.5 microns is the length of a single molecule. It would be very unlikely for the polymer to actually exist at this fully extended length.
Now that we have considered one extreme in which the polymer is fully stretched out in a line, what if we now consider the other extreme, which is the polymer coiled up into a sphere? How big would that sphere be?
PROBLEM 2
Consider polyethylene with molar mass = 280,000 g/mol, and that polyethylene has a typical density of 0.9 g/mL. Polyethylene is shown below. If the polyethylene could be packed in a sphere, what would be the radius of one molecule?

ANSWER 2
Let’s now compare these two extremes of the perfectly stretched out polyethylene with a fully extended length of 25,200Å and the perfectly coiled polyethylene with a diameter of 100Å. This size difference is a bit like comparing a tennis ball to a football field – several orders of magnitude difference! So, what conformation does the polymer actually take? And how many different conformations are possible? The polymer takes on these different conformations through the rotation of single bonds in the backbone. In order to address these questions, let’s take a step back and consider a far simpler and smaller molecule than polyethylene, butane:

Butane is not big enough to be considered a polymer, but as you may notice, it looks like a polyethylene dimer! It is a simpler case to consider first, before moving onto polyethylene with hundreds or thousands of repeat units. Butane changes conformation through the rotation around single bonds (Figure 9.3). However, not all conformations are created equal. Newman projections, which you learned in organic chemistry, allow us to visualize how substituents are oriented relative to each other when rotating and “looking” down the bond of a molecule. In Figure 9.4 two examples of Newman projections are shown for the staggered (trans) conformation and the eclipsed conformation of butane. We are “looking down” the center carbon bond between carbons 2 and 3. By drawing the Newman projections shown underneath, it is much easier to visualize how the terminal methyl groups are oriented relative to each other.

In terms of energy, it is more favorable (lower energy) to have the methyl groups far away from each other, and to have substituents not overlapping with each other, due to sterics. We can draw a plot to show the relationship between the rotation angle and the potential energy of the molecule. Notice that there are three potential energy minima for butane that correspond to the trans and gauche conformations (Figure 9.5). The molecule is most likely to exist in these conformations that minimize potential energy.

Introduction to Polymers, Third Edition, CRC Press, 2011.
What if you add more carbons now – how many conformations are there of pentane? Hexane? Poly(ethylene)? As you add additional carbons to the chain, each of those additional bonds can now have these various rotation angles and the problem of describing the molecular conformation becomes exponentially more complex. We can still have Newman projections along each bond in polyethylene, and it looks very similar to butane except that instead of methyl groups there are now polymer chains:

Consider a polyethylene molecule having 10,000 bonds, and if each of those bonds has 3 preferred orientations – how many different conformations of the polymer would there be? 310,000, which is a huge number! The probability that the chain exists in any specific one of these confirmations is incredibly small. We can’t predict exactly what conformation the polymer will have at any given instance. The conformation actually fluctuates, at some intermediate between fully extended and spherical. We can use statistics to think about the polymer conformation and size in terms of averages, and what dimensions might be most likely.
Freely Jointed Chain
Freely Jointed Chain jls164One way to think of polymer conformations is to treat the polymer like a freely jointed chain where every bond is free to rotate to any angle, but the bond distances are fixed (“l”) and the number of bonds in the chain is fixed (“n”). We can then think of the polymer conformation as that of a “random walk”. What do we mean by that? Imagine you stand in one place, representing the end of the polymer, and take a step of length “l” in any direction. This corresponds to one bond distance and the position of the second atom in the polymer backbone. Take another step of length “l”, in any direction. You now stand in the position of the third atom in the polymer backbone. Continue for “n” steps, however many bonds are in the backbone of the polymer. Your path may look something like this:

A good way of characterizing this “walk” is the distance from the start to the finish, which we labeled as “r” and call the “end to end distance”. There are many different possibilities for r given values of l and n, just depending on the specific path you take. Similarly, the polymer is constantly fluctuating in conformation and changing end to end distance. While we cannot specify the exact conformation at any given instance, we can know something about the distribution for r values and can use an “average” value of r reflective of that distribution: root mean square (RMS) end to end distance, which is given by the equation 9.1:
Note:
"" is the number of "steps" (i.e., number of bonds in the polymer backbone) and "" is the length of each "step" (i.e., bond).
Although RMS end to end distance of a freely jointed chain is a better representation of the polymer conformation than either the contour length or fully extended chain length, it’s still not great – after all, we made an assumption that the bond angles and positions could be anywhere, which is definitely not representative of actual polymer molecules. We can try to alter our model to take that into account.
Valence Angle Model (freely rotating)
Valence Angle Model (freely rotating) jls164
In the valence angle model, we try to account for the fact that the bonds along the backbone of the polymer will have a preferred bond angle. For a fully singled bonded carbon backbone in which all carbons are sp3 we expect those bonds angles to be 109.5°. In this model, although we fix the bond angle, we will still consider each single bond to freely rotate.
We can alter our formula for the mean square end to end distance with that fixed bond angle:
Notice that the subscript “fa” here is to indicate that this is free rotation around a fixed angle. Also notice that this formula is for the mean square end to end distance, not the root mean square. You’d have to take the square root to find RMS end to end distance.
Valence Angle Model with Hindered Rotation
Valence Angle Model with Hindered Rotation jls164
In the valence angle model, we initially assumed that single bonds can freely rotate. But we know that not all orientations are created equal (recall Newman projections?) How can we account for that? In the valence angle model with hindered rotation, we not only account for the bond angles but also account for the fact that single bonds do not freely rotate to any angle, and depending on the substituents on the polymer, some bonds may be more hindered than others. We thus define the mean square end to end distance with a subscript of “0” meaning hindered rotation round a fixed bond angle:
Notice we have introduced a new variable, σ, which is called the steric parameter. Steric parameters are usually determined experimentally from measured values of . The steric parameter represents how stiff or flexible the polymer is. A stiffer polymer with more hindered rotation will have a high steric parameter, and a more flexible polymer with freer rotation will have a lower steric parameter.
PROBLEM
Which polymer would you expect to have the highest steric parameter σ at a given temperature?

ANSWER
B. The bulkiest substituent will give the most hindered rotation and largest steric parameter.

Chain Stiffness
Chain Stiffness jls164We can get a sense of how stiff a polymer chain is from the characteristic ratio, C∞
PROBLEM
Do you expect a “stiffer” polymer to have a C∞ that is higher or lower than a “flexible” polymer?
- Stiffer polymer will have a C∞ that is higher than that of a flexible polymer
- Stiffer polymer will have a C∞ that is lower than that of a flexible polymer
ANSWER
A. Stiffer polymer will have a C∞ that is higher than that of a flexible polymer
Higher steric parameter corresponds to a higher characteristic ratio (all else equal) because a higher steric parameter will give a higher value of . So polymers that do not rotate as freely are more stiff and have longer end to end distances. The denominator, is the mean square end to end distance based on the “random walk” with free rotation and no restrictions to bond angles (i.e., the denominator represents the most flexible polymer possible!). The numerator is the valence bond model including hindered rotation; this value will be higher for stiffer polymers. Think of the two extremes: an infinitely stiff polymer is just a rod. It can’t coil at all, and the end to end distance is the same as the contour length. Compare that to a very flexible polymer, which will have the ability to coil, and thus will have a much lower end to end distance.
A table of some characteristic ratios and steric parameters is given below (textbook table 10.3)
| Polymer | Temperature / °C | σ | C∞ |
|---|---|---|---|
| Polyethylene | 140 | 1.8 | 6.8 |
| Isotactic polypropylene | 140 | 1.6 | 5.2 |
| Poly(vinyl chloride) | 25 | 1.8 | 6.7 |
| Polystyrene | 25 | 2.3 | 10.8 |
| Polystyrene | 70 | 2.1 | 9.2 |
| Poly(methyl methacrylate) | 25 | 2.1 | 8.6 |
| Poly(methyl methacrylate) | 72 | 1.8 | 6.6 |
As expected, bulkier groups correspond to higher steric parameters and higher characteristic ratios. Temperature also plays a role; at higher temperatures there is more energy available to overcome those barriers to rotation, so it becomes easier for single bonds to rotate. If it’s easier for bonds to rotate, then the polymer is overall more flexible, and we therefore see a decrease in the steric parameters and characteristic ratio as we go to higher temperatures.
Summary and Final Tasks
Summary and Final Tasks jls164Summary
Because polymers are such large molecules, they really can take on nearly infinite dramatically different conformations, which makes it difficult to fully describe their conformation at any given time. But we can use the concepts of end to end distances and chain stiffness to help us describe the conformations of polymers and to compare properties across different chemical structures. These same concepts are going to still be useful in our next lesson, Lesson 10, where we will begin to learn about thermodynamics of polymers in solution. We will need to start to take into account interactions between polymers and solvent, and figure out how those interactions actually affect polymer conformations and the properties of polymer solutions.
Reminder - Complete all of the Lesson 9 tasks!
You have reached the end of Lesson 9! Review the checklist on the Lesson 9 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 10.
Lesson 10: Polymer Solutions
Lesson 10: Polymer Solutions jls164Overview/Checklist
Overview/Checklist mjg8Overview
In this Lesson, we continue to consider how polymers behave in solution, but more so focus on the thermodynamics of the mixing process. What are the driving forces for mixing, and how can we predict if a polymer and solvent will mix spontaneously? We will begin with ideal solution theory and build a framework for thinking about polymers in solution, and later move on to Flory Huggins theory, which is more accurate but slightly more complex. Keep in mind as you go through the lesson the situations in which these various parameters and theories are most accurate, and in which cases they may fail to accurately describe polymer solution behavior.
Learning Outcomes
By the end of this lesson, you should be able to:
- Explain how and why polymer solutions differ from ideal solutions
- Describe what the parameters in Flory Huggins represent
- Define solubility parameters and use them to predict good and bad solvents for polymers
- Discuss limitations of solubility parameters
- Relate solubility parameters to the Flory parameter
- Predict the behavior of a polyelectrolyte in solution with varying ionic strength
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 10. | Continue navigating the online material. |
| To Read | Chapter 10 - Theoretical Description of Polymers in Solution
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 10 (Practice) | Registered students can access the homework assignment in the Lesson 10 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Thermodynamics and Mixing in Polymer Solutions
Thermodynamics and Mixing in Polymer Solutions jls164Now that you have a sense of the various conformations that a polymer may assume in solution, let’s consider the thermodynamics of that mixing process. Will the polymer actually dissolve in the solvent? How do the solvent-polymer interactions affect the chain conformations? What about polymer-polymer interactions?
We begin to think about the thermodynamics of polymers in solution by starting with a far simpler solution, an ideal solution. This is a simplistic way of thinking of a solution, in which we mix a solute and solvent, but every molecule of solvent and solute is exactly the same in terms of size and intermolecular interactions. This is of course very idealistic and not representative of real solutions, but it’s a good place to start in terms of building a framework for thinking about enthalpy and entropy of mixing.

Brief review of fundamental thermodynamics and free energy:
In previous courses, you have been introduced to the concepts of enthalpy (H) and entropy (S). Enthalpy is a measure of the potential to take up or give off energy in the form of heat, and entropy is a measure of disorder. Both properties are directly related to Gibbs free energy according to the following equation, in which is the temperature in Kelvin:
Enthalpy and entropy, like Gibbs free energy, describe properties of a system at a given state. Like Gibbs free energy, the absolute amount of entropy or enthalpy in a system is not directly measurable; instead, we typically discuss changes in these values as a system moves from one state to another:
If a process is spontaneous, then and if it is non-spontaneous, then .
PROBLEM 1
What is true of the enthalpy of mixing, for an ideal solution?
ANSWER 1
C.
All intermolecular interactions are equivalent, thus there can be no change in enthalpy upon mixing.
PROBLEM 2
What is true of the entropy of mixing, for an ideal solution?
ANSWER 2
A.
Entropy is a measure of disorder. If we go from two pure substances (solvent and solute) and mix them together, there will be more disorder, as now we have to account for all of the different arrangements of the solvent and solute in space.
PROBLEM 3
What is true of the Gibbs free energy of mixing, for an ideal solution?
ANSWER 3
B.
If and , then by using , we know must be negative and mixing for an ideal solution will always be spontaneous.
So we know that entropy increases in an ideal solution, and this is what drives the spontaneous mixing. But what is the entropy exactly? In our simple model, imagine an array like that pictured (figure 10.2) in which you place the solvent and solute molecules in various spaces. How many different distinguishable arrangements of the solvent and solute molecules in this array can there be?

Entropy is related to the “”, where and are the numbers of solvent and solute molecules:
Entropy is related to through the Boltzmann equation, where is entropy and is the Boltzmann constant:
If we substitute the expression for into the Boltzmann equation, we get :
…where have now switched from using “number of molecules” and to using mole fractions and (i.e. and ). Notice the switch from to (the gas constant) as well; the use of vs depends on whether you are dealing with individual molecules or moles of molecules, because where is Avogadro’s number. (Usually we deal with moles, and we have introduced mole fractions into our expression for entropy, thus we are using ).
Because we know that in an ideal solution, we can also write an expression for the change in free energy:
Now we have a good understanding of the thermodynamics of ideal solutions. Do polymer solutions behave like ideal solutions? Usually, they do not! In that case, what’s wrong with the theory of ideal solutions? There are two major flaws in the assumptions made for an ideal solution: 1) the assumption that all solvent and solute molecules are the same size is very wrong, especially in the case of polymer solutions because polymers are very large compared to solvent; 2) intermolecular interactions do occur, and they are usually different between solvent-solvent, solute-solute, and solute-solvent. After all, what if you choose a “bad” solvent for the polymer, like trying to dissolve polyethylene (a hydrophobic polymer) in water? Well, we know that won’t work. So intermolecular interactions are definitely important in determining whether two components will mix!
Flory-Huggins Solution Theory
Flory-Huggins Solution Theory jls164Flory-Huggins solution theory attempts to describe the thermodynamics of polymer solutions in a more accurate way than ideal solution theory. We noted the two important flaws with ideal solution theory, namely the fact that polymers are large in comparison to solvent and that there are intermolecular interactions to account for. Let’s tackle the size issue first. How can we account for the fact that polymers are very large in comparison to the size of the solvent? We are going to imagine that a polymer has a bunch of segments, where each segment is the size of the solute. So in this picture (Figure 10.3) for example, each blue dot is a segment of a polymer, and all those blue dots are connected to make up one polymer molecule.

Flory’s result for the combinatorial entropy of mixing is then:
where and are the volume fractions (not mole fractions) of the two components (i.e., solvent and polymer), respectively.
EXAMPLE
In the picture above (Figure 10.3), what is the mole fraction (or number fraction) of polymer?
There is 1 molecule of polymer and 75 molecules of solvent, thus the total number of molecules is 76. .
What is the volume fraction of polymer in the picture above?
→ The volume of the polymer is 25 times larger than the volume of the solvent. The total volume is 100. Thus the volume fraction of polymer is .
What is for the above picture using ideal solution theory?
What is for the above picture using Flory-Huggins theory?
PROBLEM
Determine the entropy change that takes place when mixing 10 g of toluene with 10 g of a polystyrene sample with Mn = 100 000 g/mol. Assume the volume of a monomer is approximately the same as a solvent molecule. Molar mass of toluene = 92 g/mol, molar mass of styrene = 104 g/mol. R = 8.314 J/(K mol)
ANSWER
First, let’s solve for the number of moles of solvent and polymer:
We need to find the degree of polymerization of the polystyrene so we can figure out the “volume” of the polymer in relation to the solvent:
Next, we will tackle the intermolecular interactions and their contribution to mixing. We are going to first make a “nearest neighbor” assumption, which is to say that we are going to neglect long range interactions and only consider the interactions between molecules that are closest to each other. In the pure solvent before mixing, we have solvent-solvent interactions, and let’s call the free energy of this interaction g11. In the pure polymer before mixing, we have polymer-polymer interactions, which we will call g22. When we mix the solvent and polymer, we must break the solvent-solvent interaction, and break the polymer-polymer interaction, before forming a new solvent-polymer interaction, g12. The change in energy per each new solvent-polymer pair formed is thus:
Flory defined the following interaction parameter, which he made dimensionless by dividing by , and it represents polymer-solvent interactions using this value of ∆g12 and “”, which is the number of surrounding “sites” or “cells” around each position in our matrix:
We use this interaction parameter as a contribution to the free energy of mixing. It is a way of trying to account for the change in enthalpy that can occur when the polymer and solvent mix:
Now even though this model is still relatively simplistic – after all, we are still considering that the molecules are organized in this matrix which is of course unrealistic – it is still much better than ideal solution theory.
PROBLEM 2
Which is more favorable for mixing, a high or low Flory-Huggins parameter?
ANSWER 2
Low. For favorable, spontaneous mixing, we need ∆Gm to be negative. We thus want χ to be small.
Case Study: poly(N-isopropylacrylamide)
Case Study: poly(N-isopropylacrylamide) jls164Most of us have the intuition that if you want to get two things to mix better, we should heat them. For instance, if you want to be able to dissolve more salt or sugar in water, you heat the water. And usually this makes sense because when you mix two different pure substance together we normally expect the entropy term to be positive (more disorder), and therefore, increasing T just makes that term even more favorable. However, not all solutions behave in this way! Poly(N-isopropylacrylamide), or PNIPAAm, is an interesting example of a polymer in solution that actually shows the reverse behavior and is less soluble, and phase separates, upon heating. The temperature at which this phase separation occurs is called the lower critical solution temperature (LCST). In the video below, we can see when we reach the LCST because the solution turns white, which is indicative of the polymer phase separating out of the water.
Please watch the following (45 second) video. Note that the video has no sound.
Can we understand this interesting behavior in terms of entropy and enthalpy?
PROBLEM 1
Which interactions occur when you dissolve PNIPAAm in water?

- Dispersion forces
- Hydrogen bonding
- Ion-ion interactions (Coulombic forces)
- A and B
- A, B and C
ANSWER 1
D. A (Dispersion forces) and B (Hydrogen bonding)
for dissolving PNIPAAm in water is negative.
PROBLEM 2
Given that is negative, and the observation that phase separation occurs upon heating, what does this tell you about of mixing? ?
- is positive
- is negative
- Not enough information
ANSWER 2
B. is negative
If we know that is negative (favorable), but we observe phase separation upon heating , then what can be said about ? How does temperature play a role in all this? Well, must be negative! As increases, the entropy term starts to dominate over the enthalpy term. Given the observation that mixing becomes less favorable, the entropy upon mixing must be unfavorable, and therefore negative. WHY? This mixing of polymer and solvent actually gives rise to a more ordered system, in part because of the hydrogen bonding and ordered interacts of the water around the polymer. This is great example of a mixture that does not follow ideal mixing behavior.
Another consequence of polymers not “liking” to mix and giving rise to some unusual behavior– consider aqueous multiphase systems. Normally, we think that if two different solutes are soluble in a solvent, such as water, then those solutes should all be able to be mixed together in one solution. For example, salt and sugar both dissolve in water, so we can easily make a solution of salt and sugar together in water. But with some polymers, this is not the case! Even though several different polymers are soluble in water, they can phase separate from each other, even in an entirely aqueous system! The thermodynamics treatment is far more complicated – we need extra terms for the polymer interactions – but similar principles apply, and also gives some motivation for why we care which phases mix and which don’t.
Now that we have established the importance of intermolecular interactions, can we try to quantify, or estimate, the changes in enthalpy of mixing a bit more? One framework to consider these interactions is the cohesive energy density (CED), which is the energy required to separate molecules from their nearest neighbors to infinite distance. If the interactions between molecules are strong, then we expect a high CED, whereas if interactions are weak, the CED will be lower. Keep in mind that this is defined as the CED for a pure substance (i.e., the solute or solvent). CED is equivalent to the solubility parameter squared:
For any compound, the solubility parameter can be determined experimentally, where and :
We build these solubility parameters into an expression for enthalpy of mixing, as shown, where :
This model predicts that mixing becomes more favorable (i.e., becomes less positive) as the difference between the solubility parameters of the two components decreases. We cannot get negative values of using this model because we square the difference in solubility parameters, and there are no negative terms. Thus, the most favorable we can ever predict is 0. In effect, we want to minimize the difference in the solubility parameters in order to try to get the most favorable possible. This is basically a way of saying “like dissolves like”. Polar solvents will have higher solubility parameters while nonpolar substances have lower solubility parameters. We will tend to mix polar and polar, nonpolar and nonpolar, in order to minimize the difference in solubility parameters. This falls in line with our intuition.
The fact that you cannot get negative values of highlights a shortcoming of this model, which is that it is unable to account for new, intermolecular interactions that occur as a result of mixing. For example, in the case of PNIPAAm that we considered, we formed strong hydrogen bonds between polymer and water, and was negative; those new hydrogen bonding interactions are not captured in this model. The solubility parameters come from separation of “like” molecules, but nowhere here do we account for new, different, interactions that may occur as a result of the specific choice of compounds to mix. Some example solubility parameters are given:
| Polymer | δ (cal/cm3)1/2 | Solvent | δ (cal/cm3)1/2 |
|---|---|---|---|
| Poly(tetraflouroethylene) | 6.2 | n-Hexane | 7.3 |
| Poly(dimethylsiloxane) | 7.4 | Cyclohexane | 8.2 |
| Polyisobutylene | 7.9 | Carbon tetrachloride | 8.6 |
| Polyethylene | 7.9 | Toluene | 8.9 |
| Polyisoprene | 8.1 | Ethyl acetate | 9.1 |
| 1,4-Polybutadiene | 8.3 | Tetrahydrofuran | 9.1 |
| Polystyrene | 9.1 | Chloroform | 9.3 |
| Atactic polypropylene | 9.2 | Cadbon disulfide | 10.0 |
| Poly(methyl methacrylate) | 9.2 | Dioxane | 10.0 |
| Poly(vinyl acetate) | 9.4 | Ethanol | 12.7 |
| Poly(vinyl chloride) | 9.7 | Methanol | 14.5 |
| Poly(ethylene oxide) | 9.9 | Water | 23.4 |
Looking at these example values of solubility parameters, we see some trends; water, a very polar solvent with strong intermolecular interactions, has a high solubility parameter, and hence a high CED. Non-polar substances, like hexane or polyethylene, have low solubility parameters and a low CED. This follows the trends as we expect.
PROBLEM 3
Which would you predict is a better solvent for poly(ethylene oxide)? Use solubility parameters in Table 10.1 above.
- n-hexane
- dioxane
- water
ANSWER 3
B. dioxane
Using solubility parameters, we would choose dioxane <!-- -->(δ=10(cal/cm3)1/2), because it would minimize the difference in solubility parameters (for<PEO, <!-- --> (δ=9.9(cal/cm3)1/2)). However, in reality, the best solvent for PEO is water, because it can participate in hydrogen bonding with the polymer and has much more favorable enthalpy of mixing. You would never choose water as the solvent based on solubility parameters however, which highlights a significant shortcoming of this method – which is that it cannot account for any new interactions, like hydrogen bonds, that occur between the polymer and solvent because the solubility parameters are only for the pure substances.
The solubility parameters are also helpful in estimating the enthalpic contribution to the Flory-Huggins interaction parameter where is molar volume of solvent:
PROBLEM 4
If the difference in solubility parameters increases (i.e the solvent is not as good for your polymer) then what can be said about ΔGm? Recall,
- increases
- decreases
- We can't tell from this information
ANSWER 4
A. increases
The Flory parameter will increase. This means mixing is less favorable. And that’s certainly the quantitative way to think about this problem…..But does this make sense conceptually to you? If we increase the difference between the solubility parameters then this means the solvent is increasingly not very good for the polymer. We expect mixing to become less favorable, and therefore we expect to become less favorable as well. Hence, we expect to go up!
PROBLEM 5
If we increase the difference in solubility parameters, how would we expect the conformation of the polymer to change?
- The polymer becomes more coiled, favoring polymer-polymer interactions
- The polymer elongates, favoring solvent-polymer interactions
- The polymer conformation isn’t affected by
ANSWER 5
A. The polymer becomes more coiled, favoring polymer-polymer interactions
As the difference in solubility parameters increases, this means the solvent is becoming “worse” for the polymer. Eventually, if the solubility is different enough, you may not be able to have spontaneous mixing and would instead get phase separation.
Recall when we talked about polymer conformations that there are the two extremes: a coiled up, spherical polymer globule, and the fully elongated polymer. Well, each of these have very different surface contact area with the solvent; the coiled polymer reduces contact area between polymer and solvent, while the elongated polymer has increased contact area with the solvent. If solvent-polymer interactions are favorable, then the polymer would elongate to maximize those favorable interactions. But if the interactions are not good, such as between a polymer and poor solvent, then probably polymer-polymer interactions are going to more favorable. This would induce the polymer to coil.
Polyelectrolytes
Polyelectrolytes jls164Polyelectrolytes are a class of polymers that have rather special and useful properties when dissolved in solution. Polyelectrolytes are characterized by having a charged backbone. A few considerations:
- There are counter ions – how do they affect things?
- The polymer backbone is charged, what does that do?
What about osmotic pressure? (Remember what it is??)
Recall that osmosis is the movement of molecules through a semi-permeable membrane from a region of low solute concentration to a region of high solute concentration. Osmotic pressure is then the minimum pressure that is required to prevent the flow of solvent across the membrane, and in effect is a measure of the tendency of the solution to take up solvent.
PROBLEM
Which of these polymers would be a polyelectrolyte when dissolved in water?

- sodium polyacroylate
- polyacrylic acid
- poly(methyl acrylate)
ANSWER
A and B

A is a salt and B is an acid that would be dissociated in water.
Let’s say we start with a polyelectrolyte that is a salt, like sodium polyacrylate. When the polymer not in water, the counter ion is electrostatically attracted and tightly associated with the ion on the polymer backbone. In this picture (figure 10.3), the blue negative charge is on the polymer and the red positive charge is the counter ion. When we add water – pure water, with limited ions in it – we have now created an environment in which there is osmotic pressure. We have lots of ions around the polymer, no ions in the surrounding water. The water diffuses near the polymer and the counter ions diffuse away from the polymer some distance due to the osmotic pressure. As the counter ions drift further away, the charge on the polymer backbone is less shielded and so the charges repel each other and the coil expands. This is called the polyeletrolyte effect.

Polyelectrolytes are very important commercially. Some of them, such as the sodium polyacrylate that is pictured below, can absorb and “trap” hundreds of times their weight in water. This is how diapers work! Other great examples of where superabsorbent polymers like sodium polyacrylate are used include “instant snow” and “moisture control” potting soil.

If the polyelectrolyte is a linear polymer, when you keep adding water to it, it will eventually become completely diluted. Imagine dumping a bowl of spaghetti into the ocean – the noodles will all float away from each other. But if you have a network – where all the polymers are connected – then this network will retain its shape and can’t get infinitely diluted. If you throw a net into the ocean, it remains a net! If the polymer is swollen in water and it is crosslinked, we refer to this as a hydrogel. Some examples of hydrogels are those water beads that you put in candles which are popular at weddings – they look like solid beads when you buy them, but after soaking in water, they swell up into large hydrogel spheres. Even if you left them in water forever, they would never get any larger than their equilibrium swelling volume because the polymer is crosslinked. Another example is contact lenses; obviously, you don’t want your contacts to dissolve into your eye, so it has to be crosslinked!

PROBLEM 2
If you added NaCl to an aqueous solution of sodium polyacrylate, how would the polymer conformation change?

- Nothing would change
- The polymer would be more extended (swell)
- The polymer would become more coiled (shrink)
ANSWER 2
C. The polymer would become more coiled (shrink)
The added salt ions will reduce the osmotic pressure and will help shield the charges on the polymer backbone from each other, both will drive the polymer to “shrink”.
We can use polyelectrolytes to make pH-responsive polymers. Consider the polyacrylic acid, shown below. Here, we are basically switching between a polyelectrolyte and non-polyelectrolyte; in base, the backbone of the polymer is charged, and this polymer would then swell in water as we expect. But when acid is added, and the polymer is fully protonated and has no charge, then it is not a polyelectrolyte, it is not affected by the osmotic pressure, and shrinks in volume.

Summary and Final Tasks
Summary and Final Tasks jls164Summary
In this lesson, we began to think in depth about how a polymer behaves when it is mixed with a solvent to make a solution and have described the entropy, enthalpy, and free energy of mixing. We started with ideal solution theory, and discussed in what instances and why polymer solutions are not well described by this theory. We then introduced Flory-Huggins theory to try to address some of those false assumptions. We covered cohesive energy density and solubility parameters and how these can be used to predict which solvents might be best for which polymers, but also realize the limitations of that model as well! Specifically for polymers in water, we saw some examples of polyelectrolytes which have some very useful and interesting properties due to the charged polymer backbone.
Reminder - Complete all of the Lesson 10 tasks!
You have reached the end of Lesson 10! Review the checklist on the Lesson 10 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 11.
Lesson 11: Polymer Characterization Methods
Lesson 11: Polymer Characterization Methods jls164Overview/Checklist
Overview/Checklist mjg8Overview
In this Lesson we are going to begin learning about the various characterization methods that are commonly used to analyze polymers. What methods are useful to analyze the molar mass, the dispersity, the crystallinity, etc.? There are many properties of polymers that we learned about so far, and we have to figure out how to actually measure them! We will begin by getting a general overview of the broad categories of characterization methods and the types of properties they can be used to measure. From there, we will go more in depth on a few select characterization methods: differential scanning calorimetry, size exclusion chromatography, end group analysis, and osmometry.

Figure 11.01 is an overview of some of the key polymer characterization approaches and the properties they are used to measure. Spectroscopy, such as UV-VIS, FTIR, NMR, Raman, and mass spectrometry are used primarily analyze the chemical composition and molecular structure of polymers. For example, we can confirm using these techniques that we in fact made the chemistry of polymer we intended, we can determine the tacticity, or we can figure out end group concentration. Light scattering and diffraction are used to determine the conformations of polymers in solution and crystal structure. To analyze the thermal transitions in polymers, such as the glass transition, melting temperature, or heat capacity, we can use differential scanning calorimetry (DSC). Dilatometry also can provide insight into thermal transitions by measuring changes in free volume. Size exclusion chromatography (SEC) is an important tool that can tell us about the molar mass distributions of polymers. Osmometry and end group analysis are techniques that help us count the “number” of molecules in solution, which yields insight as to the number average molar mass. Osmometry can also be used to measure the Flory-Huggins interaction parameter. Of these techniques, we will not be covering spectroscopy or light scattering or diffraction in much more depth. The others we will discuss how the technique works, what it measures and how, and what are the advantages and limitations of the various approaches.
Learning Outcomes
By the end of this lesson, you should be able to:
- List the polymer characteristics that that can be analyzed using:
- osmometry
- end group analysis
- size exclusion chromatography
- differential scanning calorimetry
- Analyze results from:
- osmometry
- end group analysis
- size exclusion chromatography
- differential scanning calorimetry
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 11. | Continue navigating the online material. |
| To Read | Chapter 11 - Number-Average Molar Mass
Chapter 14 - Molar Mass Distribution
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 11 (Practice) | Registered students can access the homework assignment in the Lesson 11 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Osmometry
Osmometry jls164The first characterization methods we will address are those that can help us figure out the polymer number average molar mass. was one of the first characteristics of polymers we learned about in this class. Recall this fundamental relationship:
The number average molar mass is just a function of the molar mass of the repeat unit and how many repeat units there are (i.e., the degree of polymerization). We, of course, know the molar mass of the repeat unit, that just is a function of what polymer we are trying to make. So, how do we figure out ? Well, if we could just figure out that would be easy….
Now, recall this expression we learned very early on as well, that related the total number of molecules at the start and end of the reaction to degree of polymerization:
We can easily find because this is just the total number of monomers we started with. If we could just figure out , the number of molecules at the end of the reaction, then this would allow us to solve for degree of polymerization. And then we could use degree of polymerization to solve for !
It turns out, there are a number of measurable physical properties of solutions that depend primarily on the number of solute molecules per unit volume; these are called colligative properties. Examples include boiling point elevation, freezing point depression, osmotic pressure, and vapor pressure. If we can use these techniques to quantify the number of polymer molecules in solution, then we can use these to determine and . We will focus on osmotic pressure, because this is the only colligative property that is most accurately measured for polymers of higher molar mass. But there is still a limit – if the polymer is too big and solvent too dilute, it’s hard to measure osmotic pressure, and if the polymer is too small, then the membrane may have a hard time keeping out the polymer solute. But those concerns aside, we will be considering osmometry in depth first!
As a quick review, recall that osmosis is the movement of molecules through a semi-permeable membrane from a region of low solute concentration to a region of high solute concentration. Osmotic pressure is then the minimum pressure that is required to prevent the flow of solvent across the membrane, and in effect is a measure of the tendency of the solution to take up solvent. Review the Wikipedia: Osmotic Pressure page for more information.

Introduction to Polymers, Third Edition, CRC Press, 2011.
The difference in height between the solutions in the two sides of the chamber, is related to the osmotic pressure (), where is acceleration due to gravity and is the solvent density:
And we can relate the osmotic pressure to the Flory-Huggins parameter () where is the polymer concentration (mass/volume) in the mixture, is molar volume of solvent, and is polymer density:
The quantity is called the reduced osmotic pressure.
PROBLEM
Consider the experimental data plotted below and the relationship between reduced osmotic pressure and concentration of polymer. What does the Y intercept of the plot represent?

Introduction to Polymers, Third Edition, CRC Press, 2011.
(Data taken from Kamide, K. et al., Br. Polym. J. 15,91, 1983.)
- The density of polymer
- χ
- The molar volume of polymer
ANSWER
C.
The plot has reduced osmotic pressure, , on the Y axis and is on the X axis. Looking at the equation:
We see that the quantity thus corresponds to the Y intercept and corresponds to the slope. We can use the slope to therefore measure the Flory Huggins parameter and the Y intercept to measure the number average molar mass.
PROBLEM 2
Consider the experimental data plotted below for two different sizes of polystyrene in toluene, and the relationship between osmotic pressure and concentration of polymer. Which sample has higher ?

Introduction to Polymers, Third Edition, CRC Press, 2011.
(Data taken from Kamide, K. et al., Br. Polym. J. 15,91, 1983.)
- Sample (a)
- Sample (b)
ANSWER 2
A. Sample (b)
We know that is the Y intercept. Thus, as increases, the intercept decreases. Sample (b) has the lower intercept, and higher Thus, the intercept helps us measure number average molar mass.
End group analysis
End group analysis jls164If we know the skeletal structure of a polymer (i.e., how many end groups there are per molecule of polymer) and the end groups are in some way distinguishable from other chemical moieties on the polymer, then end group analysis can be a powerful tool to allow us to “count” the number of molecules in a sample and hence solve for .Alternatively, if we know from some other method, then end group analysis can actually help us figure out how many end groups there were on average per molecule. There are a variety of analytical methods that could facilitate quantification of the end groups, such as spectroscopic methods, elemental analysis, and titration. We will not be going into depth regarding spectroscopic analysis, but in this lesson we will go over examples for which acid-base titrations and elemental analysis can be used.

End group analysis would be like counting the stars on these polymers (6) and knowing there are 2 end groups per molecule – we can use that information to figure out that there are 3 polymer molecules.
There are several requirements that must be met in order for end group analysis to be useful:
- There has to be some way to quantify the end group functionality in the first place, usually by titration, elemental analysis, or spectroscopy.
- Other functional groups on the polymer or in the solution can’t interfere with measurement of your target end groups.
- The concentration of end groups has to be sufficient to get an accurate measurement (so may not be good for very high molecular weight samples).
- You have to know how many end groups there are per molecule (to find molar mass), OR you know the molar mass, and want to know the number of end groups per molecule.
PROBLEM
Generally speaking, for which mechanism of polymerizations listed below is end group analysis least useful?
- Step polymerization
- Free radical polymerization
- Living anionic polymerization
ANSWER
B. Free radical polymerization
Step polymerizations are amenable to end group analysis because their reactivity and skeletal structure are well defined. Many chain polymerizations, such as free radical, are likely to undergo chain transfer to polymer which causes the architecture of the polymer to not be well defined and would therefore not be suitable. Living anionic polymerizations would be suitable, provided you can distinguish the end group functionality, because anionic polymerization are not prone to chain transfer mechanisms.
Counting the number of end groups: Acid-base titrations
Counting the number of end groups: Acid-base titrations jls164Recall from general chemistry laboratory those titration experiments? This analysis method works by neutralizing an unknown concentration of acid or base with a known concentration of acid or base. For example, we may have a polymer that has terminal carboxylic acid groups, which would give an acidic solution when dissolved in water. We could add a strong base, like NaOH, to our sample and neutralize the carboxylic acid groups. If we know how much NaOH is required to neutralize the acid, then we can figure out how many carboxylic end groups there must have been in the first place. Usually, a colorimetric pH indicator is used to determine the end point of the titration. Easy groups to distinguish by acid-base titration are carboxylic acids and amines. Sometimes the polymer as its originally produced does not have an acidic or basic end group, but we can do a reaction to make that functional group amenable to titration. An example would be terminal hydroxyl groups, which are not distinguishable by acid-base titration but can be converted via multiple pathways to carboxylic acids:

PROBLEM
For end-group analysis, 0.8632 g of a carboxyl terminated polybutadiene sample of the general structure shown below, dissolved in a mixture of ethanol and toluene, consumed 5.2 mL of 0.1242 M alcoholic potassium hydroxide solution in titration using phenolphthalein as the indicator. Calculate the molar mass of the polymer.

ANSWER
First we find the number of carboxylic acid groups, which we know must equal the number of hydroxyl groups:
Given the structure of the polymer, we see there are 2 carboxylic acid groups per molecule. Since we know how many carboxylic acids there are, we can figure out how many polymer molecules there are:
To find the number average molar mass, we simply divide:
Counting the number of end groups: Elemental analysis.
Counting the number of end groups: Elemental analysis. jls164If we can functionalize the end groups of the polymer with an element that is not found elsewhere in the polymer, such as a halogen, then we can use elemental analysis to figure out what mass or atom percentage of that element is in the sample. Working backwards, we can then figure out how many of those atoms there are in total, and hence how many end groups there are in the sample.
PROBLEM
1 g of a sample of polyester polyol of Mn = 3,000 g/mol was treated with bromoacetyl bromide to convert the hydroxyl end groups to bromoacetyl end groups as shown below. The treated polymer was found to contain 4.88% by weight Br by elemental analysis. Estimate the average number of hydroxyl groups on each molecule of the polyol. Bromine = 79.9 g/mol.

ANSWER
For every OH group reacted, the molar mass changes, because the –OH loses the H but gains the two carbons, an oxygen, bromine, and two more hydrogens. Thus, the molar mass of polymer for each hydroxyl group that reacts increase by: (79.9+24+16+2-1)g/mol = 120.9 g/mol
If “x” is the average number of OH groups per polymer molecule that reacted with the bromoacetyl bromide, then:
Mass percentage of bromine content found would then be:
There are about 2 hydroxyl groups per polymer molecule.
Size Exclusion Chromatography (SEC)
Size Exclusion Chromatography (SEC) jls164SEC helps us answer the question, what is the molar mass distribution of the polymer? In general, to analyze the sample, you pass a solution (polymer plus solvent) through a column that is packed with porous beads. A detector “watches” when polymer comes out the other end of the column (often by change in refractive index or UV absorption). The software generates a plot of polymer concentration vs. time, which gives you an indication of the molar mass dispersity of the polymer.

Importantly, as shown in the figure above, larger polymers exit the column (i.e., elute) faster than smaller polymers. This is a bit counterintuitive for most people. It has to do with the fact that larger molecules have a shorter path length in the column than the smaller polymers. The packing material in the column has a range of pore sizes; the larger polymers cannot fit into the smaller pores, and hence they are more limited in the paths that they can take through the column, and elute faster. Smaller polymers that can go into the smallest pores will ultimately travel greater distances within those pores and hence elute more slowly.
Often, SEC data is not plotted as a function of time, but rather as a function of elution volume. Elution volume (Ve) is the volume of solvent required to move the polymer from the point of injection (one end of the column) to the detector (other end of the column). A small elution volume means that little solvent is required to flush the polymer out of the column (this would correlate to “fast” elution) while a large elution volume means that more solvent is required (correlating with a “slower” elution). Data you collect might look something like this:

Now even though we say SEC can be used to measure molar mass distributions, in fact, as you may have noticed, it actually is separating polymers by their “size” rather than mass. More precisely, SEC is separating polymers by their hydrodynamic volume or hydrodynamic radius – which is affected by various things, in particular the polymer (chemistry and structure), solvent, solvent/polymer interactions, and temperature.

Unfortunately, molar mass does not always correlate with polymer hydrodynamic volume. After all, when we were considering polymer conformations in solution, the polymer “size” could vary widely depending on whether it was coiled or extended. These considerations of polymer conformations in solution are relevant when we try to interpret data from SEC experiments. This means a polymer with the smaller hydrodynamic radius will require a higher elution volume than a polymer with a larger hydrodynamic radius, even if the sample with small hydrodynamic radius has the higher molar mass!
PROBLEM
Consider polystyrene of the same molar mass in methanol, chloroform, and n-hexane. Which would you expect (using the table below) to have the largest hydrodynamic volume, of the options given?
| Polymer | δ (cal/cm3)1/2 | Solvent | δ (cal/cm3)1/2 |
|---|---|---|---|
| Poly(tetraflouroethylene) | 6.2 | n-Hexane | 7.3 |
| Poly(dimethylsiloxane) | 7.4 | Cyclohexane | 8.2 |
| Polyisobutylene | 7.9 | Carbon tetrachloride | 8.6 |
| Polyethylene | 7.9 | Toluene | 8.9 |
| Polyisoprene | 8.1 | Ethyl acetate | 9.1 |
| 1,4-Polybutadiene | 8.3 | Tetrahydrofuran | 9.1 |
| Polystyrene | 9.1 | Chloroform | 9.3 |
| Atactic polypropylene | 9.2 | Cadbon disulfide | 10.0 |
| Poly(methyl methacrylate) | 9.2 | Dioxane | 10.0 |
| Poly(vinyl acetate) | 9.4 | Ethanol | 12.7 |
| Poly(vinyl chloride) | 9.7 | Methanol | 14.5 |
| Poly(ethylene oxide) | 9.9 | Water | 23.4 |
ANSWER
Chloroform
A smaller difference in solubility parameters means better solvent for the polymer → more polymer-solvent interactions, more elongated polymer.
Now that we know that SEC is actually separating polymers by their hydrodynamic volume, how do we go about actually correlating that with the molar mass? The best way to do this is with a calibration curve made using standards which are expected to behave like your sample. To make such a calibration curve, you get a series of low dispersity polymers of known molar mass and run them through the SEC to yield a plot that could look something like the top plot of the figure below, where each peak corresponds to the elution of one of the standards:

Since you know the molar mass of each of your standards, you can correlate each of those peaks with a specific elution volume. This allows you to make the calibration curve (bottom plot of the figure above). Now you can use this calibration curve to correlate the elution volume to molar mass for any sample that you expect to elute similarly in the SEC column (i.e., sample chemistry of polymer, same solvent).
So we can figure out now how to correlate elution volume to molar mass, but how do we get the molar mass distribution of the sample?

First, we normalize the area under the SEC data curve to 1, because presumably all our polymer is somewhere on that plot. Then we can slice it into sections of arbitrarily small widths (vi). Each slice has a weight fraction (wi) associated with it, according to the area within that slice. Each slice also has a molar mass which you can figure out using the calibration curves we just learned about:

Therefore, if you know the weight fraction of polymer with a specific molar mass, we can use that to create our molar mass distribution curve.
PROBLEM 2
Here are two calibration curves for two standards of a polymer with the same chemical composition, same (good) solvent, and same temperature... But different shapes! Which polymer is branched and which one is linear?

ANSWER
2 is branched and 1 is linear.
They are in a good solvent, so the linear polymer will have the larger hydrodynamic volume. (Branching will make the polymer more compact as compared to a linear polymer with the exact same mass, all else equal). The linear polymer will therefore elute faster, with lower Ve, for a given molar mass
Summary of strengths and weakness of SEC
Strengths of SEC
- Can be used for a pretty wide range of polymers and solvents systems – can be used for sensitive biological systems in aqueous solutions as well as synthetic polymers in organic solvents.
- Can get information about molar mass, distribution of molar mass, and dispersity (and also Mn).
Limitation of SEC
- We are using hydrodynamic volume as an analog to molar mass. Depending on your polymer system, you may or may not be able draw an accurate correlation between the two.
- If there is interaction between the column packing material (the stationary phase) and your polymer, this will cause longer elution times and will mimic smaller polymers.
Thermal Transitions and Differential Scanning Calorimetry
Thermal Transitions and Differential Scanning Calorimetry mxw142The glass transition temperature (Tg) or melting temperature (Tm) of polymers are important characteristic properties. How do we measure those thermal transitions or phase transitions? Now, we will discuss a common approach to quantifying Tg and Tm, called differential scanning calorimetry (DSC). DSC is a technique that measures heat required to change the temperature of a sample and a reference of known heat capacity. The direction of heat flow is very important in DSC, as that will tell us whether we have an exothermic or endothermic transition, and this is often a point of confusion when analyzing data from DSC.
To prepare for our discussion of DSC, let’s first review heat flow and how it relates to phase transitions, which is something you first learned in introductory chemistry. You likely saw a plot something like this, which depicts the heat associated with temperature transitions for one mole of H2O:

Notice that while the material undergoes a phase transition, the temperature does not change even though heat is being added. For example, look at ΔHfus in which H2O goes from solid ice to liquid water. We have to add 6 kJ of heat to cause this transition to happen for 1 mole of water (so it is an endothermic phase transition), but the temperature remains constant at 0°C during this phase transition. Once we get liquid water, as we add heat, the temperature goes up linearly; how much heat you have to add to increase the temperature is a function of the material’s heat capacity.
When we do DSC analysis, we are going to be heating our sample to specific temperatures at a specific rate and looking at how much heat is required to get us to that temperature. In a way, it has a lot of similarities to this plot, except instead of tracking absolute values of heat added, we measure the heat flow. If the heat flow goes up, that means we will be adding more heat to the system to raise it to a given temperature, whereas if heat flow decreases, heat is released from the system to the surroundings. Let’s look at some sample data you might collect from DSC and try to interpret it.
Look at the graph in Figure 11.12. The Y axis is important, and identifying which “direction” is endothermic vs exothermic is key. In this class, I will keep the axis the same, as in what is shown in Figure 11.12 (but be wary that you may see examples in other books or papers that define the axis in the opposite direction). Here, an increase in heat flow means that the DSC machine is putting in extra heat to try to raise the sample temperature – and it has to do this, because the material is undergoing an endothermic phase transition or a change in heat capacity. In the plot in Figure 11.12 below, we see that initially the heat flow is constant while the temperature is increasing. This means the sample has a constant heat capacity. Suddenly, we see a spike in heat flow; this spike corresponds to a phase transition. During a phase transition, heat is either input or released, but there is no change in temperature (recall our phase diagram for water?) This is why you see that sudden increase in the DSC trace – the machine has to put in a lot more heat in order to get the temperature to rise above the transition temperature. In this specific example, the peak is pointing upward, which means we are inputting heat, and thus the phase transition must be endothermic. Thus, if this was a polymer sample, this would be the melting temperature (Tm). (Vaporization is also endothermic, but for polymers, it’s unlikely that we would be vaporizing them).

PROBLEM
A DSC trace is shown below. What is happening at the temperature marked?

ANSWER
The polymer is crystallizing. Notice that this peak is pointing down; at the temperature marked (T), heat flow to the sample is decreased, and that’s because the sample is undergoing an exothermic phase transition. Crystallization is the relevant phase transition for polymers.
Another DSC trace is shown below in Figure 11.13. This one looks slightly different than the melting and crystallization curves we saw before. Here, we notice that the heat flow increased, but never came down again! Therefore, this feature cannot correspond to a phase transition, but must be indicative of something else – such as, a change in the heat capacity (ΔCp). This change in heat capacity is correlated to the glass transition temperature (Tg), in which the polymer is going from a glassy solid state to a more viscous state.

Putting it all together could look something like the DSC trace shown below in Figure 11.14:

Not all polymers will have all of these transitions, and there are a number of factors that can affect the DSC trace. For example, some polymers do not crystallize, so keep in mind which curves you might expect or not expect to see depending on the polymer chemistry and skeletal structure. It can often be very difficult to define a specific temperature for these transitions, as the peaks may be quite broad or happen over a range of temperatures. The thermal history of the polymer can also affect the measurements of melting (Tm) and crystallization (Tc) and glass transition (Tc) temperatures, because of hysteresis. Heating rates and cooling rates can also affect these measurements. However, in general, DSC is a very powerful technique that helps us to probe the thermal properties of polymers.
Summary and Final Tasks
Summary and Final Tasks mrs110Reminder - Complete all of the Lesson 11 tasks!
You have reached the end of Lesson 11! Review the checklist on the Lesson 11 Overview / Checklist page to make sure you have completed all of the activities listed there before you begin Lesson 11.
Lesson 12: Mechanical Properties of Polymers
Lesson 12: Mechanical Properties of Polymers jls164Overview/Checklist
Overview/Checklist mjg8Overview
Our last lesson of this course is focused on the mechanical properties of polymers. While we will be largely discussing the macroscale properties of polymers, always be mindful of how those bulk properties are actually derived from the molecular scale structure and chemistry of the polymer. In order to motivate how important it is to understand the mechanical properties of polymers and how that relates to molecular scale polymer structure and dynamics, consider the tragic accident of the Challenger explosion. Polymeric O-ring seals, which are flexible and elastic, were used in the space shuttle at joints where it was necessary to contain and compartmentalize explosive propellant. The day of the shuttle launch, it was quite cold, with temperatures dropping below the glass transition temperature of the polymer O-rings. The low temperatures caused the O-rings to become brittle, non-elastic, and glassy, as we well know should happen when a polymer is below . Thus, the O-rings could not form a tight seal, and upon launch, the joints failed and the Challenger exploded. This accident highlights how critical it is for you – the future scientists and engineers – to learn the fundamental chemistry and mechanics of the materials you work with. For more information, read the O-ring Concerns section of the Wikipedia Space Shuttle Challenger Disaster page
Polymers are a unique class of materials in terms of their mechanical properties because they may possess some characteristics of a fluid and some characteristics of a solid. While ideal elastic solid materials store all the energy from stress in the bonds, so that the material will restore itself upon release of stress, ideal viscous fluids dissipate all the stress in flow. Polymers, as we will see, tend to be somewhere in the middle. We have a special term to describe this combination of fluid and solid properties: viscoelasticity.

Learning Outcomes
By the end of this lesson, you should be able to:
- Describe the stress-strain characteristics of elastomers, glassy polymers, semi-crystalline polymers.
- Correlate chemical structure with mechanical properties.
- Explain the changes in entropy and enthalpy that occur during elastomer deformation.
- describe strain induced crystallization and hysteresis.
- Draw time dependent strain plots for viscoelastic material.
- Analyze modulus vs time plots and identify glass region, glass transition, rubbery plateau.
- Compare mechanical properties for low and high molecular weight polymers; crosslinked and non-crosslinked polymers.
- Describe how mechanical properties of polymers depend on temperature.
- Define shear thinning and shear thickening polymers.
- Describe how molecular weight affects viscosity.
Lesson Checklist
| Activity | Content | Access / Directions |
|---|---|---|
| To Read | Read all of the online material for Lesson 12. | Continue navigating the online material. |
| To Read | Chapter 16 - The Amorphous State
| The chapter readings come from the textbook, Introduction to Polymers. |
| To Do | Homework Assignment 12 (Practice) | Registered students can access the homework assignment in the Lesson 12 module. |
Please refer to the Canvas Calendar for specific timeframes.
Questions?
If you have questions, please feel free to post them to the General Questions and Discussion forum. While you are there, feel free to post your own responses if you, too, are able to help a classmate.
Polymers as Solids
Polymers as Solids jls164First, let’s consider polymers as solids. When we treat a polymer like a solid, we consider things like the strength, stiffness, and toughness of a material. Hooke’s law is relevant here (stress = Young’s modulus x strain):
Stress, , the load on an object divided by its cross-sectional area, is a measure of the force at any point inside a material (much like how we describe the pressure exerted by a gas on the walls of its container). Stress therefore equals force divided by area:
Strain is defined as the normalized extension, the change in length () divided by the original length of the object ().
Stress is proportional to the stain and independent of loading rate. If we plot stress versus strain, then the modulus of the material is the slope of the curve, toughness is the area under the curve, and strength is the stress at breaking. This relationship for an ideal elastic solid is shown below.

Think about how these properties could tie back to the molecular scale. We basically have a series of atoms linked up together by a network of bonds, which are a little like tiny springs (and thus we can more easily visualize how Hooke’s law is relevant here). Stiffness or modulus of a solid material is related to the stiffness of the chemical bonds within the system (how much does the spring stretch?). Strength of an ideal solid material is related to the cohesive strength of the bonds, which is proportional to the depth of the potential energy well of the bonds.
For an ideal elastic solid, if we apply and subsequently remove a force on the material, it should go back to its original shape without any permanent deformation. There is no perfectly elastic material. When it comes to polymers, probably the closest we can come are single crystals of polymers, which are rare. “Real” solid materials deviate from such ideal behavior.

Introduction to Polymers, Third Edition, CRC Press, 2011.
Above are some examples of how varied the mechanical properties of polymers can be. The breaking points for materials on this plot is shown with the “x”. Polymer fibers which are crystalline can be high modulus, and so can glassy polymers below . But semi-crystalline polymers and elastomers (above ) are “softer” and certainly have lower modulus. Thus, the mechanical properties are highly tunable and span orders of magnitude in scale. Comparing the modulus of some common polymers to other materials (Table 12.1 below) we see that polymers, in comparison, are not very stiff! Even a glassy polymer like atactic polystyrene has a modulus of only about 3,000 MPa (about 1/20th that of window glass).
| Material | E(MPa) |
|---|---|
| Rubber | 7 |
| Polyethylene - High Density | 830 |
| Polyethylene - Low Density | 170 |
| Poly(Styrene) | 3,100 |
| Poly(methyl methacrylate) (Plexiglas) | 4,650 |
| Wood | 14,000 |
| Concrete | 17,000 |
| Glass | 70,000 |
| Steel | 210,000 |
| Diamond | 1,200,00 |
Why are the mechanical properties of polymers so variable, and why so different than other solid materials? Polymers are unique in that they are made of giant molecules – these molecules interact very differently than small molecules. Many factors affect polymer mechanical properties. Some of these we already discussed in detail. for example, by definition, is a change in the mechanical properties. Above the glass transition, polymers can flow and deform with lower modulus, but below the glass transition, polymers are glassy solids and are more brittle. Cross-linking most definitely affects mechanical properties; thermosets are characterized by very high levels of crosslinking, and they tend to be more rigid and higher modulus than a low-crosslinking elastomer. Crystallinity is a big factor as well. Consider the difference in modulus between and high and low density PE in the table above. Recall that HDPE is linear, and the chains pack together much more easily. Whereas for LDPE, there is branching which prevents close packing, and prevents crystallization, of the PE. Because HDPE has more crystallinity, we find that its modulus is much higher.
We have already stated that single-crystal polymers are very rare; semi-crystalline polymers, which have some amorphous and some crystalline regions, are much more common. If the polymer is semi-crystalline, then it has some regions that are crystalline and some that are amorphous and the mechanical properties of the bulk tend to be a combination or “average” of the properties associated with each. So for example, we expect crystalline polymers to have higher modulus and amorphous polymers to have lower modulus, thus as we increase the degree of crystallinity, we find that the modulus also increases:

Introduction to Polymers, Third Edition, CRC Press, 2011.
Even within polymers that are the same “chemically”, i.e., polyisoprene, we can still have geometric isomers and/or different skeletal structure that influence the mechanical properties. For example, “cis” isomers tend to not pack together well, and therefore do not crystallize to a significant degree. Thus, polyisoprene that is predominantly in the “cis” conformation is an elastomeric material. But the “trans” form does pack better, induces more crystallization, and causes the material to be more rigid. You could thus imagine tuning the overall mechanical properties of this polymer by just varying the ratio of cis and trans bonds in the polymer.

Given the unique mechanical properties of elastomers, it’s worth considering the thermodynamics associated with mechanical deformation. Try this at home! Hold a rubber band to your lips and stretch it, then release it. Do you feel a change in temperature? When you stretch the rubber band, you should feel heat (exothermic, is negative). When you release the rubber band, you feel cool (endothermic, positive). What’s going on, and can we explain it in terms of entropy and enthalpy?
PROBLEM
When you stretch a rubber band, does the entropy of the elastomer change and how?
Recall,
ANSWER
Entropy decreases.
for stretching is positive (it is a non spontaneous process!) and we also know that is negative (exothermic). So, must be negative. What does this mean conceptually? When you stretch an elastomer, you are creating order – you are aligning the polymer chains. By applying strain, you actually are creating order and can even possibly induce crystallization.
Strain induced crystallization means that polymer chains become more aligned when stretched, facilitating crystallization (which contributes to the exothermic nature of the rubber band stretching!) This isn’t necessarily a good property….. We know that the degree of crystallinity of a polymer can have dramatic impact on its mechanical properties. So if the degree of crystallinity changes, then the properties, change, perhaps in undesirable ways. It also means the polymers behave differently upon application and release of stress (hysteresis) (see Figure 12.6 below).

Introduction to Polymers, Third Edition, CRC Press, 2011.
(Data taken from Andrews, E.H., Fracture in Polymers, Oliver and Boyd Ltd. London, 1968)
Polymers as liquids
Polymers as liquids jls164Previously, we treated polymers as solid. Now, we are focusing on polymers as liquids. Viscosity is a characteristic property of fluids; a less viscous fluid has low resistance to shear stress, while a highly viscous fluid has higher resistance to shear stress. We have intuition about this – water we would consider to have low viscosity, while something like toothpaste would be highly viscous. The viscosity of a fluid is a measure of its resistance to gradual deformation by shear stress. Imagine a sandwich with two plates on either side and a fluid in between. If you push one plate and keep the other static, what happens to the liquid? The plates do not simply slide past the fluid – but rather the liquid is “stuck” at the walls, and is “sheared” when you slide the plates past each other. There is some frictional force in the fluid. This is viscosity.
Ideal viscous fluids, i.e. Newtonian fluids, have a viscosity () that is independent of shear rate () such that this relationship between shear stress (), viscosity, and shear rate would yield a constant value of viscosity no matter what shear is applied:

Many liquids that consist of small molecules, like water for example, may not be “perfect” Newtonian fluids, but they come pretty close. When we consider polymeric fluids, which could be a polymer melt or a polymer solution, the fact that there are very large polymer molecules now impart significantly different properties to the fluid; most polymer melts are therefore non-Newtonian fluids.
If a fluid is non-Newtonian, then there clearly must be some dependence of the viscosity on the shear rate. There are two general possibilities for how the fluid might behave: either the material increases in viscosity with increasing shear rate, or the viscosity decreases with an increasing shear rate. These are called shear thickening or shear thinning fluids, respectively. A diagram that considers how the shear stress - shear rate curves for shear thinning and shear thickening polymers might look is shown in Figure 12.9. The slope of these shear stress – shear rate curves is called the apparent viscosity, .

An example of a shear thickening material is Ooobleck (which is cornstarch in water) or wet sand. But actually most polymer melts and solutions are shear thinning. Ketchup is a great example of a shear thinning fluid; it will almost certainly never come out of the bottle in any reasonable time if you just turn it upside down, but if you give the bottle a good shake (=shear) suddenly it starts to flow!
PROBLEM
Which plot below shows a shear thinning fluid?

ANSWER
Plot C.

The viscosity is just the slope of the shear stress – shear rate plot. A fluid that increases viscosity with increasing shear rate is shear thickening, while a fluid that decreases viscosity with increasing shear rate is shear thinning. Shear thinning is common in polymers.
Looking back at the plots of shear stress vs shear rate in Figure 12.9, we notice that while at higher shear rates, the apparent viscosity changes rapidly, at low shear rates, the viscosity can actually be relatively constant. The constant apparent viscosity in the low-shear region is known as the zero shear viscosity, .
The viscosity of polymer melts depends on a number of factors. An important factor is the molar mass. The plot below shows the vs for a range of different polymers.

You’ll notice that viscosity increases with molecular weight (which is directly related to degree of polymerization) – by orders of magnitude. Now at first glance, given that the viscosity of the polymers increases so dramatically with molecular weight, we might think that high molecular weight polymers are orders of magnitude harder to process. Actually, because of shear thinning, it’s not as difficult as you might think. Which brings us to the question of why is a polymer shear thinning in the first place? Again, we come back to entanglements! As you shear a polymer along a specific direction, the polymers slip past each other and there is some disentanglement and actually the polymer chains align in the direction of shear. This polymer alignment during shear actually is very important to the mechanical properties of the polymer products being manufactured because it can impart different mechanical properties along different axes of a material. For example, if you have ever tried ripping a plastic grocery bag along different directions, you’ll notice that in one direction it tears easily, while along the perpendicular direction it is much more difficult – and it is because of polymer alignment during shear imposed during the manufacturing of the bag itself.

PROBLEM 2
Sample A and Sample B are the same type of linear polymer but different molar weight. You analyze the samples with SEC and obtained the chromatogram below. Which sample has higher viscosity?

ANSWER 2
Sample A
Recall learning about SEC and how higher molecular weight polymers will elute faster than lower molecular weight polymers (all else equal). Thus, Sample A is the higher MW polymer and we would expect it to have the higher viscosity.
Polymers as Viscoelastic Materials
Polymers as Viscoelastic Materials jls164Viscoelasticity combines a little bit of both solid behavior and fluid behavior. While ideal elastic materials store all the energy from stress in the bonds, so that the material will immediately restore itself upon release of stress, ideal viscous fluids dissipate all the stress in flow. Viscoelastic materials are somewhere in the middle, and many polymers are viscoelastic. An important characteristic of viscoelastic materials is that timescale matters. For ideal elastic solids and ideal viscous liquids, time doesn’t matter – whether you apply a stress fast or slow, the response of the material should be identical. But this isn’t so for most polymers, which show time-dependent behavior. Two important time-dependent properties of polymers are creep and stress relaxation.
Creep is a property of viscoelastic materials in which the strain of the material changes over time while under a constant load (stress) (Figure 12.12). Creep is not something that happens in a perfectly elastic solid. For an ideal elastic material, under constant stress, it would instantaneously deform and would also instantaneously go back to original shape after removal of stress.

A strain vs. time plot for a viscoelastic material with creep would likely look something like this:

The creep can be non-linear, as shown, where the strain changes in a non-linear fashion with time. Upon release of the stress, the polymer can recover some, but usually undergoes some amount of permanent deformation.
In comparison to creep, which is a constant stress experiment, stress relaxation is a constant strain experiment. You deform the material to a given strain, and measure the stress required to maintain that deformation over time (Figure 12.14).

The data for stress relaxation experiments are usually reported as a modulus vs time plot. This time dependent modulus, called the relaxation modulus, , is simply the time dependent stress , divided by the (constant) strain, :
Importantly, stress relaxation is also temperature dependent. The graph shows how PMMA relaxation modulus varies as function of both time and temperature. As expected, the relaxation modulus goes down with time – after all, if at constant strain the stress is decreasing, then the modulus must be decreasing too. We also see that at higher temperatures, the modulus is also lower. This makes sense, as we are heating the polymer, we supply more energy for those bonds to rotate, for the polymers to move past each other, to overcome intermolecular interactions – thus, the modulus will decrease.

An important characteristic of viscoelastic materials is the time-dependent mechanical properties. At short time scales, a polymer may behave as a glassy solid, but at longer time scales, it could flow more like a liquid. This time dependence is influenced by things like molecular weight which affects entanglements, as we touched on in the “polymers as liquids” section (Figure 12.16 below). If you have a low molecular weight polymer it will form less entanglements and so “untangles” more quickly. Larger polymers take longer to relax and untangle, and we see this in the “rubbery plateau” region of the plot below. A nice example of the impact of these time-dependent properties is silly putty. Silly putty behaves like an elastic solid on short time scales – you can bounce it like a rubber ball. But at long time scales, for instance if you just leave it out on the table, it flows like a liquid and will spread.

The plots above are a function of time, but we also know that stress relaxation should also be affected by temperature.
PROBLEM
In the figure below, we consider the effect of temperature on the modulus for polymers at a given time and strain. We already know that going from below to above the glass transition temp will have a dramatic effect on the modulus – below the polymer is rigid glassy solid, but above it begins to flow and the modulus decreases significantly. Both plots shown are for high molar mass polymer, and hence both have a rubbery plateau, but one sample is crosslinked and one is linear. Which one is which?

ANSWER
Plot (a) is linear and plot (b) is crosslinked. The crosslinked polymer reaches a limit of lower modulus because it is being held together by crosslinks that prevent the network from deforming indefinitely.
Polymer Processing
Polymer Processing jls164So how do we turn polymers into the products that we use in our daily lives, and how do these mechanical properties influence the processability of polymers? Definitely, we need to keep in mind how the skeletal structure of the polymer will affect the general mechanical properties (i.e., a highly crosslinked thermoset is going to be processed somewhat differently than a linear thermoplastic). But, in general, processing methods have three phases:
- heating to soften or melt
- shaping/forming under constraint
- cooling to retain shape
The most common processing approaches are injection molding, extrusion, blow molding (these three are mostly useful for thermoplastics) and compression molding (more useful for thermosets). Because it is so much easier to see how processing is done through video, please watch this video (6:08) which summarizes the most common approaches to polymer processing:
Most polymer products you use on a day to day basis are made by injection molding. If you are interested, I highly suggest watching this interesting video (9:36):
Summary and Final Tasks
Summary and Final Tasks jls164Summary
In this lesson, we have covered many of the common characterization techniques (DSC, SEC, end group analysis, etc.) that are used to analyze various properties of polymers (thermal transitions, molar mass distributions, number average molar mass, etc.). These techniques are by no means the only ones and in particular, we did not discuss spectroscopy, which encompasses so many important characterization techniques.
In the next lesson, we will be learning about mechanical properties of polymers. Polymers have some very unique mechanical properties and can differ significantly from materials you likely learned about in MatSE 201. Even though we will be talking mostly about properties of “bulk” polymers, don’t forget that the molecular scale chemistry, bonding, and intermolecular interactions, and chain conformations that we spent so much time learning about – these things are all at the core of WHY polymers have certain bulk properties.
Reminder - Complete all of the Lesson 12 tasks!
You have reached the end of Lesson 12! Review the checklist on the Lesson 12 Overview / Checklist page to make sure you have completed all of the activities.

