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CHAPTER 4: POLYMER STRUCTURES
ISSUES TO ADDRESS... • What are the basic microstructural features? • How do these features influence properties? 1
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Structures of Polymers
Introduction and Motivation Polymers are extremely important materials (i.e. plastics) Have been known since ancient times – cellulose, wood, rubber, etc.. Biopolymers – proteins, enzymes, DNA … Last ~50 years – tremendous advances in synthetic polymers Just like for metals and ceramics, the properties of polymers Thermal stability Mechanical properties Are intimately related to their molecular structure … End of lecture 1
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Structures of Polymers
Before introducing polymers, let me spend one or two minutes refreshing your memory about hydrocarbons Why? Most polymers are hydrocarbon (e.g. C, H) based Bonding is highly covalent in hydrocarbons Carbon has four electrons that can participate in bonding, hydrogen has only one Saturated v unsaturated Unsaturated – species contain carbon-carbon double/triple bonds Possible to substitute another atom on the carbon Saturated – carbons have four atoms attached Cannot substitute another atom on the carbon End of lecture 1 Unsaturated Saturated
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Structures of Polymers
Hydrocarbons have strong chemical bonds, but interact only weakly with one another (van der Waals’ forces) Isomerism – compounds of the same chemical composition but different atomic arrangements (i.e. bonding connectivity) Chemical formula for both: C4H10 Atomic connectivity different! Isomerism is important as we will see! Aside: Read 4.1 – 4.3! End of lecture 1
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Structures of Polymers
Polymer molecules Ok, what is a polymer? Polymers are molecules (often called macromolecules) formed from a series of building units (monomers) that repeat over and over again As we will see, polymers can be a range of molecular weights There are many monomers Can make polymers with different monomers, etc.. End of lecture 1 n is often a very large number! e.g. can make polyethylene with MW > 100,000!
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Structures of Polymers
End of lecture 1
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Structures of Polymers
Chemistry of polymer molecules (is cool) Basic idea of how you make polymers … Stick with ethylene Gas at STP To polymerize ethylene, typically increase T, P and/or add an initiator (more on initiators later) R* is an initiator that is responsible for activating the monomer to begin chain growth (hence the name) End of lecture 1 After many additions of monomer to the growing chain…
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Structures of Polymers
Polymer chemistry stereochemistry Typical 2D Drawing 3D End of lecture 1
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Structures of Polymers
Polymer chemistry So in polyethylene (or PE) synthesis, the monomer is ethylene Turns out one can use many different monomers Different functional groups/chemical composition – polymers have very different properties! Monomers End of lecture 1
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Structures of Polymers
Polymer chemistry Time for nomenclature related to chemical composition If the polymer is formed from one monomer (i.e. all the repeat units are the same type) – this is called a homopolymer If the polymer is formed from multiple types of monomers (i.e. all the repeat units are not the same type) – this is called a copolymer Also note – the monomers shown before are referred to as bifunctional Why? The reactive bond that leads to polymerization (the C=C double bond in ethylene) can react with two other units Other monomers react with more than two other units – e.g. trifunctional monomers End of lecture 1
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(And these are just the 10 “more common” polymers)
As you can see, there is a very diverse range of chemistries accessible! (And these are just the 10 “more common” polymers) End of lecture 1
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Structures of Polymers
Molecular weight As you might imagine (and will see later), the properties of a polymer depend on how many units (mers) form the chain (i.e. polymer chain length) Nearly all polymer synthesis protocols result in the formation of polymer chains with a distribution of lengths Need way to quantify this – define an “average” molecular weight Two approaches are typically taken Number average molecular weight (Mn) Weight-average molecular weight (Mw) End of lecture 1
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Structures of Polymers
Molecular weight Number average molecular weight (Mn) Basic idea: divide the chains into a series of size ranges and determine the number fraction of chains within each size range, then Hypothetical polymer size distribution based on number fraction of chains Mi – mean (middle) molecular weight (MW) of size range i xi – fraction of the total number of chains within the size range End of lecture 1
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Structures of Polymers
Molecular weight Weight average molecular weight (Mw) Here divide the chains into a series of size ranges and determine the weight fraction of chains within each size range Hypothetical polymer size distribution based on weight fraction of chains Mi – mean (middle) molecular weight (MW) of size range i wi – weight fraction of chains within the size range End of lecture 1
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Structures of Polymers
Molecular weight Are the two different? Yes, one is essentially based on mole fractions, and the other on weight fractions They will only be the same if all the chains are exactly the same MW! Mw > Mn End of lecture 1 Get Mn from this Get Mw from this
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Structures of Polymers
Molecular weight Polydispersity index (not in your book) As mentioned above, inevitably there is a distribution of MWs (the sample will have chains of varying length) Way to quantify this is by the polydispersity of the sample Ratio of the weight and number average molecular weights (polydispersity index, or PI) End of lecture 1 For monodisperse polymers (all chains are the exact same MW), PI = 1 Many commercial polymers have PI values over 10!
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Structures of Polymers
Molecular weight Other ways to define polymer MW Degree of polymerization Represents the average number of mers in a chain. The number and weight average degrees of polymerization are m is the mer MW in both cases. In the case of a copolymer (something with two or more mer units), m is determined by End of lecture 1 fj and mj are the chain fraction and molecular weight of mer j
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Structures of Polymers
Example Problem 4.1 Given the following data determine the Number average MW Number average degree of polymerization Weight average MW Polydispersity Number average MW (Mn) How to find Mn? Calculate xiMi Sum these! End of lecture 1
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Structures of Polymers
Example Problem 4.1 Number average degree of polymerization (MW of H2C=CHCl is g/mol) Weight average molecular weight (Mw) How to find Mw? Calculate wiMi Sum these! End of lecture 1
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Structures of Polymers
Molecular shape The pictures I have drawn so far of polymers are in a way misleading How – I have always drawn them as highly elongated (straight) chains – in practice this is almost never the case Why? C-C bonds are typically 109° (tetrahedral, sp3 carbon) If you have a macromolecule with hundreds of C-C bonds, this will lead to bent chains End of lecture 1
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Structures of Polymers
Molecular shape Taking this idea further, can also have rotations about bonds Leads to “kinks”, twists Take home message – the end-to-end distance of a polymer chain in the solid state (or in solution) is usually much less than the distance of the fully extended chain! This is not even taking into account that you have numerous chains that can become entangled! End of lecture 1
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Structures of Polymers
Molecular structure Physical properties of polymers depend not only on their molecular weight/shape, but also on the difference in the chain structure For the purposes of this class, the four main structures we will consider are Linear polymers Branched polymers Crosslinked polymers Network polymers End of lecture 1
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Structures of Polymers
Molecular structure Linear polymers – polymers in which the mer units are connected end-to-end along the whole length of the chain These types of polymers are often quite flexible Van der waal’s forces and H-bonding are the two main types of interactions between chains Some examples – polyethylene, teflon, PVC, polypropylene End of lecture 1
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Structures of Polymers
Molecular structure Branched polymers – exactly what it sounds like Have chains off the main chain (backbone) These are often (though not always!) quite a bit shorter than the main chain This leads to inability of chains to pack very closely together These polymers often have lower densities These branches are usually a result of side-reactions during the polymerization of the main chain Most linear polymers can also be made in branched forms End of lecture 1
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Structures of Polymers
Molecular structure Crosslinked polymers – polymers where adjacent chains are attached to one another at various positions via covalent bonds Often carried out during polymerization or by a non-reversible reaction after synthesis (referred to, surprisingly, as crosslinking) These materials often behave very differently from linear polymers Many “rubbery” polymers are crosslinked to modify their mechanical properties; in that case it is often called vulcanization End of lecture 1 picture
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Structures of Polymers
Molecular structure Network polymers – these are polymers that are “trifunctional” instead of bifunctional (see earlier slides) There are three points on the mer that can react This leads to three-dimensional connectivity of the polymer backbone Highly crosslinked polymers can also be classified as network polymers Examples: epoxies, phenol-formaldehyde polymers End of lecture 1
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Structures of Polymers
Molecular configuration For polymers with side chain groups (besides Hydrogens), the arrangement of these groups can strongly modify their properties Consider Where R is not hydrogen (e.g. –CH3) There are two “well-defined” arrangements of the R group Head-to-tail Head-to-head Here the R groups alternate End of lecture 1 Here the R groups are adjacent
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Structures of Polymers
Molecular configuration Typically the head-to-tail configuration dominates (why?) This is a specific example of how mers are connected – as we will see it will have significant influence on polymer properties More general is the issue of isomerism – different molecular configurations for molecules (polymers) of the same composition We will focus on two Stereoisomerism Geometrical Isomerism End of lecture 1
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Structures of Polymers
Stereoisomerism Denotes when the mers are linked together in the same way (e.g. head-to-tail), but differ in their spatial arrangement This really focuses on the 3D arrangement of the side-chain groups Three configurations most prevalent Isotactic Syndiotactic Atactic End of lecture 1
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Structures of Polymers
Stereoisomerism Isotactic polymers All of the R groups are on the same side of the chain Isotactic configuration End of lecture 1 Note: All the R groups are head-to-tail All of the R groups are on the same side of the chain Projecting out of the plane of the slide This shows the need for 3D representation to understand stereochemistry!
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Structures of Polymers
Stereoisomerism Syndiotactic polymers The R groups occupies alternate sides of the chain End of lecture 1 Syndiotactic configuration Note: The R groups are still head-to-tail R groups alternate – one of out of the plane, one into the plane
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Structures of Polymers
Stereoisomerism Atactic polymers The R groups are “random” Atactic configuration End of lecture 1 R groups are both into and out of the plane, no real registry Two additional points Cannot readily interconvert between stereoisomers – bonds must be broken Most polymers are a mix of stereoisomers, often one will predominate
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Structures of Polymers
Geometrical Isomerism These typically occur when one has double bonds (cis/trans) Consider the mer of isoprene cis configuration End of lecture 1 The methyl group and hydrogen are on the same side of the C=C double bond This is referred to as the cis structure cis-polyisoprene is a natural rubber
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Structures of Polymers
Geometrical Isomerism Now consider the other isomer trans configuration The methyl group and hydrogen are on opposite sides of the C=C double bond This is referred to as the trans structure trans-polyisoprene (gutta percha) has very different physical properties! Note – cannot simply interconvert between the cis and trans isomers Why? End of lecture 1
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End of lecture 1
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Structures of Polymers
Thermoplastic polymers Another way to categorize polymers – how do they respond to elevated temperatures? Thermoplastics – these materials soften when heated, and harden when cooled – this process is totally reversible This is due to the reduction of secondary forces between polymer chains as the temperature is increased Most linear polymers and some branched polymers are thermoplastics End of lecture 1
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Structures of Polymers
Thermosetting polymers Thermosets – these materials harden the first time they are heated, and do not soften after subsequent heating During the initial heat treatment, covalent linkages are formed between chains (i.e. the chains become cross-linked) Polymer won’t melt with heating – heat high enough it will degrade Network/crosslinked polymers are typically thermosets End of lecture 1
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Structures of Polymers
Copolymers Idea – polymer that contains more than one mer unit Why? If polymer A has interesting properties, and polymer B has (different) interesting properties, making a “mixture” of polymer should lead to a superior polymer “Random” copolymer – exactly what it sounds like End of lecture 1 “Alternating” copolymer – ABABABA…
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Structures of Polymers
Copolymers Idea – polymer that contains more than one mer unit Why? If polymer A has interesting properties, and polymer B has (different) interesting properties, making a “mixture” of polymer should lead to a superior polymer “Block” copolymers. Domains of “pure” mers End of lecture 1 “Graft” copolymers. One mer forms backbone, another mer is attached to backbone and is a sidechain (it is “grafted” to the other polymer)
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Structures of Polymers
Polymer crystallinity Polymers can be crystalline (i.e. have long range order) However, given these are large molecules as compared to atoms/ions (i.e. metals/ceramics) the crystal structures/packing will be much more complex End of lecture 1
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Structures of Polymers
Polymer crystallinity (One of the) differences between small molecules and polymers Small molecules can either totally crystallize or become an amorphous solid Polymers often are only partially crystalline Why? Molecules are very large Have crystalline regions dispersed within the remaining amorphous materials Polymers are often referred to as semicrystalline End of lecture 1
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Structures of Polymers
Polymer crystallinity Another way to think about it is that these are two phase materials (crystalline, amorphous) Need to estimate degree of crystallinity – many ways One is from the density End of lecture 1
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Structures of Polymers
Polymer crystallinity What influences the degree of crystallinity Rate of cooling during solidification Molecular chemistry – structure matters Polyisoprene – hard to crystallize Polyethylene – hard not to crystallize Linear polymers are easier to crystallize Side chains interfere with crystallization Stereoisomers – atactic hard to crystallize (why?); isotactic, syndiotactic – easier to crystallize Copolymers – more random; harder to crystallize End of lecture 1
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Structures of Polymers
Polymer crystals Chain folded-model Many polymers crystallize as very thin platelets (or lamellae) Idea – the chain folds back and forth within an individual plate (chain folded model) End of lecture 1
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Polymer crystals More commonly, many polymers that crystallize from a melt form spherulites One way to think of these – the chain folded lamellae have amorphous “tie domains” between them These plates pack into a spherical shape Polymer analogues of grains in polycrystalline metals/ceramics End of lecture 1
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POLYMER MICROSTRUCTURE
• Polymer = many mers Adapted from Fig. 14.2, Callister 6e. • Covalent chain configurations and strength: Direction of increasing strength Adapted from Fig. 14.7, Callister 6e. 2
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THERMOPLASTICS VS THERMOSETS
--little cross linking --ductile --soften w/heating --polyethylene (#2) polypropylene (#5) polycarbonate polystyrene (#6) • Thermosets: --large cross linking (10 to 50% of mers) --hard and brittle --do NOT soften w/heating --vulcanized rubber, epoxies, polyester resin, phenolic resin Adapted from Fig , Callister 6e. (Fig is from F.W. Billmeyer, Jr., Textbook of Polymer Science, 3rd ed., John Wiley and Sons, Inc., 1984.) 3
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MOLECULAR WEIGHT & CRYSTALLINITY
• Molecular weight, Mw: Mass of a mole of chains. • Tensile strength (TS): --often increases with Mw. --Why? Longer chains are entangled (anchored) better. • % Crystallinity: % of material that is crystalline. --TS and E often increase with % crystallinity. --Annealing causes crystalline regions to grow. % crystallinity increases. Adapted from Fig , Callister 6e. (Fig is from H.W. Hayden, W.G. Moffatt, and J. Wulff, The Structure and Properties of Materials, Vol. III, Mechanical Behavior, John Wiley and Sons, Inc., 1965.) 4
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ANNOUNCEMENTS Reading: Chapter 4 HW # 3. Due Friday February 9th
3.72; 3.75; 3.81; 3.83; 4.1; 4.2; 4.3; 4.7; 4.10; 4.18; 4.23; 4.27 29
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