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Page 1: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polymers

Page 2: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polymers

Steep Slope = 3/5 : Self-Avoiding Walk (Polymer Solution)

Shallow Slope = 1/2 : Gaussian Random Walk(Polymer Melt)

Page 3: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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If we consider a series of chains<R> = 0

RRMS = n1/2 l

Similar to diffusion R ~ Dt1/2

Except when i = j, and there are “n” of these

Page 4: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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The distribution of chain lengths, R, follows almost a Gaussian Distribution:

Boltzman Equation

By Comparison

The energy of an ideal chainas a function of R

Page 5: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Energy of an Ideal Chain

The modulus of rubber is proportional to temperature and

inversely proportional to the molecular weight between

crosslinks.

(Change in energy is force times the change in distance) The ideal chain acts like a spring

Page 6: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Generally Modulus decreases with temperature

http://www.allsealsinc.com/allseals/Orings/or13.htm

Metal For an ideal elastomer it increase with T

This is due to the entropic natureof polymers

Savage K N , Gosline J M J Exp Biol 2008;211:1948-1957

Page 7: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polymer Chains are Mass-Fractals

RRMS = n1/2 l Mass ~ Size2

3-d object Mass ~ Size3

2-d object Mass ~ Size2

1-d object Mass ~ Size1

df-object Mass ~ Sizedf

This leads to odd properties:

density

For a 3-d object density doesn’t depend on size,For a 2-d object density drops with Size

Larger polymers are less dense

Page 8: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Nano-titania from Spray Flame

Random Aggregation (right) df ~ 1.8Randomly Branched Gaussian df ~ 2.3Self-Avoiding Walk df = 5/3

Problem: Disk df = 2 Gaussian Walk df = 2

R/dp = 10, z ~ 220 df = ln(220)/ln(10) = 2.3

z is mass/DOAdp is bead sizeR is coil size

mass = z ~ Rdp

⎝ ⎜ ⎜

⎠ ⎟ ⎟

d f

Balankin et al. (Phys. Rev. E 75 051117

Mass Fractal dimension, df

Page 9: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Nano-titania from Spray Flame

Random Aggregation (right) df ~ 1.8Randomly Branched Gaussian df ~ 2.3Self-Avoiding Walk df = 5/3

Problem: Disk df = 2 Gaussian Walk df = 2

A measure of topology is not given by df.Disk and coil are topologically different. Foil and disk are topologically similar.

z is mass/DOAdp is bead sizeR is coil size

mass = z ~ Rdp

⎝ ⎜ ⎜

⎠ ⎟ ⎟

d f

Balankin et al. (Phys. Rev. E 75 051117

Mass Fractal dimension, df

R/dp = 10, z ~ 220 df = ln(220)/ln(10) = 2.3

Page 10: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

p ~ Rd

⎛ ⎝ ⎜

⎞ ⎠ ⎟ dmin

s ~ Rd

⎛ ⎝ ⎜

⎞ ⎠ ⎟ c

Tortuosity Connectivity

How Complex Mass Fractal StructuresCan be Decomposed

df = dminc�

z ~ Rd

⎛ ⎝ ⎜

⎞ ⎠ ⎟ d f

~ pc ~ sdmin

z df p dmin s c R/d

27 1.36 12 1.03 22 1.28 11.2

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Page 11: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

df = 2.3dmin =1.15c = 2

Balankin et al. (Phys. Rev. E 75 051117 (2007))

A 2-d Sheet has c = 2dmin depends on the extent of crumpling

Consider a Crumpled Sheet

Nano-titania

df = 2.3dmin =1.47c =1.56

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Page 12: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

Disk Random Coil

df = 2dmin =1c = 2

df = 2dmin = 2c =1

Extended β-sheet(misfolded protein) Unfolded Gaussian chain

Page 13: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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For a polymer in solution there is an inherent concentration to the chainsince the chain contains some solvent

The polymer concentration is Mass/Volume, within a chain

When the solution concentration matches c* the chains “overlap”Then an individual chain is can not be resolved and the chains entangle

This is called a concentrated solution, the regime near c* is called semi-diluteand the regime below c* is called dilute

Page 14: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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In concentrated solutions with chain overlap chain entanglements lead to a higher solution viscosity

J.R. Fried Introduction to Polymer Science

Page 15: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

There is a similar behavior in Melt Viscosityas a function of Molecular Weight

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Me is the entanglementmolecular weight

about 10,000 g/mole (10 kDa)

Page 16: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Many Macromolecular Properties Change at Me

Onset of Shear Thinning Behavior in Rheology

Onset of Chain Folding Crystallization

Onset of Robust Mechanical Properties (Organic Powder versus Solid Plastic)

Onset of the ability to draw a fiber (melt strength)

Below the entanglement molecular weight we have an oligomerabove we have a polymer or a plastic material

Page 17: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Page 18: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Viscoelasticity

Page 19: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Viscoelasticity

δ is the phase angle or phase lagit is 0 for Hookean elastic behavior

and 90° (π/2) for Newtonian viscous behavoirWe usually talk about tan δ that varies from 0 to ∞

Page 20: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Dynamic Mechanical Testing

Page 21: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Page 22: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Hookean Elastic

Viscoelastic

Page 23: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Page 24: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Measure at different frequencies

Combine to make a master curve(Semi-Crystalline Polymer is Shown)

Page 25: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Can also combine frequencies for different temperatures

To yield a master curve in frequency

Page 26: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Temperature and Frequency Plots are directly related

High Frequency => Low TemperatureLow Frequency => High Temperature

Time-TemperatureSuperposition

Page 27: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Williams-Landel-Ferry Shift Factor, aT

Page 28: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Synthesis of Polymers

Polymers are generally produced by organic reactions similar to the organic chemistry you have studied except that the synthesis either involves a

Chain Reaction generally with 3 stages

Initiation: You start the chain reaction

Propagation: You conduct the chain reaction

Termination: You end the chain reaction

Or it involves a Step-Growth Reaction where a simple reaction occurs at two (or more) ends of a growing chain molecule. This type of reaction involves di-functional (or higher functional)

reactants. The reaction proceeds until you run out of reactants or the system becomes too viscous for transport of reacting species to the reacting chain ends.

Condensation Reactionto Make Nylon

Page 29: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Page 30: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Carothers’ EquationsFor Step Growth Polymerization

Page 31: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Chain Vs. Step Growth Polymerization

A. Mechanism

B. Monomer Concentration

C. Polymer Molecular Weight

Distinct and Different-Initiation Step

-Propagation Steps-Termination Step(s)

Chain Growth Step Growth

Distinct and DifferentInitiation, Propagation and

terminationare all the same step

“Termination” is the last reaction that takes place

Monomer is present throughout the

reaction, even at the end

-Early in the reaction the monomer is depleted

-Many dimers and trimers are produced early in the reaction. The

monomer is consumed at early stages of the reaction

Reaction must be driven to 99.9% complete to get a polymer

Page 32: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Nyon 6,10 by interfacial polymerization

Page 33: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polyesters

Polycarbonate (CD’s)bisphenol-A and phosgene

Poly ethylene terephthalate (PET or PETE)

Glyptal Synthesis

Pthalic AnhydrideGlycerol (or Ethylene glycol)

Terephthalic Acid and Ethylene glycol

Page 34: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Gellation/Percolation

Carother’s Method: Percolation occurs when p=2/favg

Page 35: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polyurethane

Page 36: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polyurethane

Page 37: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polyurethane

A step-reaction but not a condensation reaction.

There is no byproduct so this is a useful reaction for coatings and other systems where you

do not want droplets of condensate.

Page 38: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polyurethane Foam

Page 39: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Chain Vs. Step Growth Polymerization

A. Mechanism

B. Monomer Concentration

C. Polymer Molecular Weight

Distinct and Different-Initiation Step

-Propagation Steps-Termination Step(s)

Chain Growth Step Growth

Distinct and DifferentInitiation, Propagation and

terminationare all the same step

“Termination” is the last reaction that takes place

Monomer is present throughout the

reaction, even at the end

-Early in the reaction the monomer is depleted

-Many dimers and trimers are produced early in the reaction. The

monomer is consumed at early stages of the reaction

Reaction must be driven to 99.9% complete to get a polymer

Page 40: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Chain Growth of Poly dimethyl siloxane (PDMS, Silicone)

Termination by Acid

Initiation by Base

Propagation

Page 41: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Sol-Gel Crosslinking

TMOS

Ethoxy is TEOS

Page 42: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Two Free Radical Initiators

AIBN

Benzoyl Peroxide

Both are dissociated by heatAIBN is soluble in organic solvents

BP in water or organic solvents(BP is explosive)

Free Radical Chain Growth

Page 43: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Coupling

Hydrogen Abstraction

Disproportionation

Initiation

Propagation

Termination

Page 44: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Anionic Chain Growth

Initiation

Propagation

There is No Terminationfor Anionic

SBR Rubber

Page 45: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Ziegler-Natta Catalysts (Heterogeneous Catalysts)

1

2

3

Page 46: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Isotactic Polypropyleneby ZN Polymerization

Page 47: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polymers have a Dispersion in All Properties

Molecular Weight (Molar Mass)

Stereochemistry

Block Copolymer Composition

Branch Structure

Page 48: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Polymers have a Dispersion in All Properties

Molecular Weight (Molar Mass)

Stereochemistry

Block Copolymer Composition

Branch Structure

Page 49: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Molecular Weight Distribution

PDI = Mw/Mn

This can be directly related to the Gaussian Distribution

Page 50: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Molecular Weight Distribution

Page 51: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Page 54: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Tacticity

Racemo Diad(Racemic)

rMeso Diad

(Meso)m

Isotactic Triad mm Syndiotactic Triad rr Heterotactic Triad mrrm

Page 55: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

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Atactic Polmer

Has no tacticity

For a random distribution of tacticity: 50% r and 50% m or 25% isotactic, 25% syndiotactic, 50% heterotactic

Higher order groupings are important to crystallinity,Pentads, Heptads, etc.

But there are limits to our ability to resolve tacticity using NMR

Page 56: Polymers - College of Engineering and Applied Sciencebeaucag/Classes/Properties of Materials...Slides5.key Author Gregory Beaucage Created Date 11/9/2011 10:01:07 AM

Polymer Processing

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