sifat-sifat polimer
DESCRIPTION
Sifat-sifat PolimerTRANSCRIPT
Pendahuluan
Plastic Products
• Plastics can be shaped into a wide variety of products: – Molded parts– Extruded sections– Films– Sheets– Insulation coatings on electrical wires– Fibers for textiles
9
Polymer Science and Processing Technology • Successful product design requires a knowledge of:
– the requirements of the final product– the behaviour of polymeric materials– commercial polymer processing technology– relevant cost and market factors.
At the heart of polymer science andtechnology is molecular structure. It dictates not only final product properties,but polymer synthesis and processingmethods.
J.S. Parent 10
Polymer Classification: Terminology
• While we have chosen an applications perspective on polymer classification, many alternate schemes are widely used.
• These are usually composition/property specific, as opposed to applications oriented.
Definisi & Klasifikasi Polimer
Polymers: Introduction
• Polymer: High molecular weight molecule made up of a small repeat unit (monomer).– A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A-A
• Monomer: Low molecular weight compound that can be connected together to give a polymer
• Oligomer: Short polymer chain• Copolymer: polymer made up of 2 or more monomers
– Random copolymer: A-B-B-A-A-B-A-B-A-B-B-B-A-A-B– Alternating copolymer: A-B-A-B-A-B-A-B-A-B-A-B-A-B– Block copolymer: A-A-A-A-A-A-A-A-B-B-B-B-B-B-B-B
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Polymer
Poly mer many repeat unit (building blocks)
C C C C C C
HHHHHH
HHHHHH
Polyethylene (PE)
ClCl Cl
C C C C C C
HHH
HHHHHH
Poly(vinyl chloride) (PVC)
HH
HHH H
Polypropylene (PP)
C C C C C C
CH3
HH
CH3CH3H
repeatunit
repeatunit
repeatunit
Carbon chain backbone
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Types of Polymers
• Polymer Classifications– Thermoset: cross-linked polymer that cannot be
melted (tires, rubber bands)– Thermoplastic: Meltable plastic– Elastomers: Polymers that stretch and then return to
their original form: often thermoset polymers– Thermoplastic elastomers: Elastic polymers that can
be melted (soles of tennis shoes)
• Polymer Families– Polyolefins: made from olefin (alkene) monomers– Polyesters, Amides, Urethanes, etc.: monomers linked
by ester, amide, urethane or other functional groups– Natural Polymers: Polysaccharides, DNA, proteins
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Common PolyolefinsMonomer Polymer
Ethylene
H3CCH3
nRepeat unitPolyethylene
CH3
CH3n
CH3 CH3 CH3 CH3 CH3 CH3CH3Propylene
Polypropylene
PhCH3
n
Ph Ph Ph Ph Ph PhPhStyrene
Polystyrene
ClCH3
n
Cl Cl Cl Cl Cl ClClVinyl Chloride
Poly(vinyl chloride)
F2C CF2
Tetrafluoroethylene
F3C
F2C
CF2
F2C
CF2
F2C
CF2
F2C
CF2
F2C
CF2
F2C
CF2
CF3
nPoly(tetrafluoroethylene): Teflon
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18
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Polyesters, Amides, and UrethanesMonomer Polymer
CO2HHO2CHO
OHO O
HO OH2C
H2C O
nTerephthalic acid
Ethyleneglycol
Poly(ethylene terephthalate
H
Ester
HO OH
O O
4H2N NH24
Adipic Acid 1,6-Diaminohexane Nylon 6,6HO N
HNH
H
O O
4 4n
CO2HHO2C
Terephthalic acid
NH2H2N
1,4-Diamino benzene
Kevlar
O
HO
OHN
HN H
n
Amide
HOOH
Ethyleneglycol
H2COCN NCO
4,4-diisocyantophenylmethaneSpandex
H2C
HN
HN
O
HO
O
OH2C
H2C O H
n
Urethane linkage
20
Natural PolymersMonomer Polymer
Isoprenen
Polyisoprene:Natural rubber
O
H
HO
H
HO
H
HOHH OH
OH
Poly(ß-D-glycoside):cellulose
O
H
O
H
HO
H
HOHH OH
OH
H
n
ß-D-glucose
H3N
O
O
RPolyamino acid:protein
H3N
OHN
R1
OHN
Rn+1
O
OH
Rn+2n
Amino Acid
BaseO
OH
OP
O
O
O
oligonucleic acidDNA
NucleotideBase = C, G, T, A
BaseO
O
OP
O
O
O
DNA
DNA
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Rubbers
Polymer ClassificationPolymers are commonly classified based on their
underlying molecular structure.
Polymers
Elastomers ThermosetsThermoplastics
Crystalline Amorphous
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Polymer Classification: Thermoplastic/Thermoset
• One of the most practical and useful classification of polymer compounds is based on their ability to be refabricated.
• Thermoplastic: polymers that can be heat-softened in order to process into a desired form.
– Polystyrene, polyethylene– recyclable food containers
• Thermoset: polymers whose individual chains have been chemically crosslinked by covalent bonds and therefore resist heat softening, creep and solvent attack.– Phenol-formaldehyde resins, melamine paints– permanent adhesives, coatings
Thermoplastics and Thermosets• The response of a polymer to mechanical forces at elevated
temperature is related to its dominant molecular structure. • One classification of polymers is according to its behavior and
rising temperature. Thermoplastics and Thermosets are the 2 categories.
• A thermoplastic is a polymer that turns to a liquid when heated and freezes to a very glassy state when cooled sufficiently.
• Most thermoplastics are high-molecular-weight polymers whose chains associate through weak Van der Waals forces (polyethylene); stronger dipole-dipole interactions and hydrogen bonding (nylon).
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• Thermoplastic polymers differ from thermosetting polymers (Bakelite, vulcanized rubber) since thermoplastics can be remelted and remolded.
• Thermosetting plastics when heated, will chemically decompose, so they can not be recycled. Yet, once a thermoset is cured it tends to be stronger than a thermoplastic.
• Typically, linear polymers with minor branched structures (and flexible chains) are thermoplastics. The networked structures are thermosets.
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Thermoplastics and Thermosets
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Examples of Thermoplastics
PTFE
More Examples of Thermoplastics
http://www2.dupont.com/Teflon/en_US/index.html
http://en.wikipedia.org/wiki/Teflon
Polymer
Some engineering polymers (1)
Some engineering polymers (2)
Some engineering polymers (3)
Elastomers (1)
Elastomer (2)
Struktur & sintesa Polimer
Polymer Classification: Chain Architecture
• Linear: A linear polymer chain is one without branches. Its actual conformation may not be “line-like”, but varies with chain stiffness, crystallinity and applied stresses.
• Branched: Chains with an appreciable number of side-chains are classified as branched. These side chains may differ in composition from the polymer backbone.
• Crosslinked: A continuous network of polymer chains is a crosslinked condition. In effect, there is just one polymer chain of infinite molecular weight.
• Chain architecture has a dramatic effect on properties such as viscosity, elasticity and temperature stability.
Polymer Classification: Chemical Microstructure
Homopolymers: polymers derived from a single monomer (can be linear, branched or
crosslinked). poly(ethylene), poly(butadiene).
Random copolymers: two monomers randomly distributed in chain. AABAAABBABAABBA poly(acrylonitrile-ran-butadiene)
Alternating copolymers: two monomers incorporated sequentially ABABABABABABABAB poly(styrene-alt-maleic anhydride)
Block copolymers: linear arrangement of blocks of high mol weight AAAAAAAAAAABBBBBBBBBBBBBBBAAAAAAAA polystyrene-block-polybutadiene-block-polystyrene or
poly(styrene-b-butadiene-b-styrene)
Graft copolymers: differing backbone and side-chain monomers poly(isobutylene-graft-butadiene)
43
Copolymerstwo or more monomers
polymerized together • random – A and B randomly
positioned along chain• alternating – A and B alternate
in polymer chain• block – large blocks of A units
alternate with large blocks of B units
• graft – chains of B units grafted onto A backbone
A – B –
random
block
graft
alternating
Copolymers can be used to tailor functionality or generate new phases and behaviors.
Block copolymer, example: Poly(styrene)-block-poly(butadiene)
Random copolymer, example: Poly(styrene-ran-butadiene)
Graft copolymer, example: Poly(styrene)-graft-poly(butadiene)
Molecular Structures for Polymers
• The physical characteristics of a polymer depend also on differences in the structure of the molecular chains (other variables are shape and weight).
• Linear polymers have repeat units joined end to end in single chains. There may be extensive van der Waals and hydrogen bonding between the chains. Examples: polyethylene, PVC, nylon.
46
Branched Cross-Linked NetworkLinear
secondarybonding
Molecular Structures- Branched
• Where side-branch chains have connected to main chains, these are termed branched polymers. Linear structures may have side-branching.
• HDPE – high density polyethylene is primarily a linear polymer with minor branching, while LDPE – low density polyethylene contains numerous short chain branches.
• Greater chain linearity and chain length tend to increase the melting point and improve the physical and mechanical properties of the polymer due to greater crystallinity.
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Branched Cross-Linked NetworkLinear
Molecular Structures – Cross-linked, Network
• In cross-linked polymers, adjacent linear chains are joined to one another at various positions by covalent bonding of atoms. Examples are the rubber elastic materials.
• Small molecules that form 3 or more active covalent bonds create structures called network polymers. Examples are the epoxies and polyurethanes.
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Branched Cross-Linked NetworkLinear
secondarybonding
49
Chemistry and Structure of Polyethylene
•Polyethylene is a long-chain hydrocarbon. •Top figure shows repeat unit and chain structures. •Other figure shows zigzag backbone structure.
Tetrahedral arrangement of C-H
50
MOLECULAR WEIGHT• Molecular weight, M: Mass of a mole of chains.
Low M
high M
• Polymers can have various lengths depending on the number of repeat units.
• During the polymerization process not all chains in a polymer grow to the same length, so there is a distribution of molecular weights. There are several ways of defining an average molecular weight.
• The molecular weight distribution in a polymer describes the relationship between the number of moles of each polymer species and the molar mass of that species.
Molecular Weight Distribution
The distribution of molecular weights within a polymer is characterized not by a single, unique average, but defined through a number of different ways.
The number average, Mn,considers the number ofmolecules of each size, Mi, in the sample:
The weight average, Mw, considers the mass ofmolecules of each sizewithin the sample:
i
iin n
MnM
i
iiw w
MwM
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xi = number fraction of chains in size range i
MOLECULAR WEIGHT DISTRIBUTION
iiw
iin
MwM
MxM
wi = weight fraction of chains in size range i
Mi = mean (middle) molecular weight of size range i
Mn = the number average molecular weight (mass)__
Polydispersity is the term we use to describe the fact that not all
macromolecules in a given sample have the same “repeat number” x.
size
#
size
#
size
Polydisperse Monodisperse Paucidisperse
Even in a pure sample, not all molecules will be the same.
Nature often does better than people do.
#
MW Requirements of Industrial Polymers
Elastomers amorphous materials operating above Tg physical props derived from chain entanglement, crosslinking
Adhesives range from elastomeric (pressure sensitive) to semi-
crystalline (hot melt) to glassy (epoxy resins)
Plastics broad class of materials whose properties are derived from
an amorphous phase and often from a crystalline phase
Fibres highly crystalline materials physical properties derived from degree of crystallinity
Coatings must be applied as a low viscosity medium and “cure” to
produce satisfactory properties
Composition Distribution
Inclusion of two or more monomers in a material generates a distribution of composition within, and between, polymer chains. Changes to material properties can be pronounced:
Chemical properties: fibre dyeability, hot melt adhesive bonding strength, solvent resistance…
Phase transitions: crystallinity, Tg, Tm, phase separation Mechanical properties: elasticity, modulus, toughness...
“Tailored” polymers can be developed through consideration of: the character of incorporated monomers and,
»polarity of main chain or pendant functionality»potential for crystallization
their sequence distribution within polymer chains.» random chain composition»alternating»block sequencing»graft structure
Random Copolymers
Materials comprised of a random distribution of different monomers are the most widely employed industrial copolymers.
Compositions vary from essentially homopolymers to materials containing equimolar quantities of constituent monomers, depending on the application.
Compare: Poly(acrylonitrile), Poly(butadiene) and Poly(acrylonitrile-co-
butadiene) Poly(ethylene), atactic Poly(propylene) and Poly(ethylene-
co-propylene) Poly(acrylonitrile) and Poly(acrylonitrile-co-methyl acrylate)
Random Copolymer Phase Transitions
Random incorporation of significant amounts of two or more monomers generally:
yields a Tg between the two constituent homopolymers. lowers Tm for crystalline domains, and reduces the extent of
crystallinity.
Shown here is a generic phase diagram for a system of “semi-crystalline” monomers.
Polymer Chain Lengths• Many polymer properties are affected by the length
of the polymer chains. For example, the melting temperature increases with increasing molecular weight.
• At room temp, polymers with very short chains (roughly 100 g/mol) will exist as liquids.
• Those with weights of 1000 g/mol are typically waxy solids and soft resins.
• Solid polymers range between 10,000 and several million g/mol.
• The molecular weight affects the polymer’s properties (examples: elastic modulus & strength). 58
Polymers – Molecular Shape
• Straight (b) and twisted (c) chain segments are generated when the backbone carbon atoms (dark circles) are oriented as in the figure above.
• Chain bending and twisting are possible by rotation of carbon atoms around their chain bonds.
• Some of the polymer mechanical and thermal characteristics are a function of the chain segment rotation in response to applied stresses or thermal vibrations. 59
Polymer Classification: Chemical Class
A popular classification scheme amongst chemists is based on polymer functionality.
Polyesters: poly(ethylene terephthalate) - Dacron
Polyamides: poly(caprolactam) - nylon 6
Urethanes: carbamate linkages through reaction of diisocyanates and diols.
Another (!) classification scheme, again favoured by chemists is based on differences between the polymer and constituent monomer(s).
Condensation polymers: synthesis involves elimination of some small molecule (H2O in the preparation of nylon)
Addition polymer: formed without loss of a small molecule i.e. ethylene polymerization to generate poly(ethylene)
C O
O
N C
OH
N C
O
O
H
Alternating Copolymers
Alternating copolymers are essentially -AB- homopolymers. Condensation polymers are structurally of this class, but are
not considered alternating.
C N
poly(butadiene-ran-acrylonitrile)
C N
poly(butadiene-alt-acrylonitrile)
Alternating Copolymers: Elastomers
Typical stress-strain curves at 0°C for unreinforced rubber vulcanizates:
1: poly(propylene-alt-butadiene) 2: natural rubber: cis-1,4-
polyisoprene
3: synthetic cis-1,4-polyisoprene 4: cis-1,4-polybutadiene
5: poly(styrene-co-butadiene) (25:75)
CHEE 890 J.S. Parent
Segmented Polyurethanes
Schematic morphology of unstretched semicrystalline polyurethane copolymer (segmented block copolymer).
A: hard nylon fibre
B: bicomponent nylon-
spandex
C: mechanical stretch
nylon
D: spandex
E: extruded latex
Graft-Modified Polyolefins
Functionalization of polymers is a cost-effective means of developing specialty materials. Grafting of versatile functional groups to polyolefins can improve blend performance and/or enhance high-temperature properties.
A leading example is the melt grafting of maleic anhydride to polyethylene to generate a material that improves adhesion between polyethylene and nylon phases in toughened nylon parts.
What is the distribution of grafts in the material?
OO O
ROOR
O
O
O
Graft-Modified Materials: Composition Distribution
Silane modified resins are used for enhanced adhesion with siliceous fillers and moisture curing:
Distribution of silane grafts is expected to influence: coupling efficiency to fillers crosslink density of cured articles
Si(OMe)3
Si(OMe)3
ROOR
Polymer Synthesis
There are two major classes of polymer formation mechanisms Addition polymerization: The polymer grows by sequential
addition of monomers to a reactive site»Chain growth is linear»Maximum molecular weight is obtained early in the
reaction Step-Growth polymerization: Monomers react together to
make small oligomers. Small oligomers make bigger ones, and big oligomers react to give polymers.
»Chain growth is exponential»Maximum molecular weight is obtained late in the
reaction
Addition Polymerization
In*A
InitiationIn A* A
Addition Polymerization
Propagation
In*A
InitiationIn A A* A
Addition Polymerization
Propagation
AIn*A
InitiationIn A A A*
Addition Polymerization
Propagation
nAIn A A A A
nA*
A A A A Am
In A A A AnA
*A A A A Am
Combination
*A A A A Am
In A A A AnA
B A A A Am
Disproportionation
TerminationReactive site is consumed
A
In A A A AnA
A*
Chain TransferNew reactive siteis produced
MW kpropagation
k ter mination
MW
% conversion0 100
In*A
InitiationIn A A A A*
7171
Addition (Chain) Polymerization
– Initiation
– Propagation
– Termination
Types of Addition Polymerizations
Ph
Anionic
C3H7 Li C4H9
Ph
Li+ Phn
C4H9
Ph Ph
Li+
n
Ph
Radical
PhCO2•Ph
n
Ph
Cationic
Cl3Al OH2H
PhHOAlCl3
Phn
H
Ph Phn
HOAlCl3
PhCO2
Ph
PhCO2
Ph Phn
Step-Growth Polymerization
Stage 1
Consumptionof monomer
n n
Stage 2
Combinationof small fragments
Stage 3
Reaction of oligomers to give high molecular weight polymer
Step-Growth Polymerization
Because high polymer does not form until the end of the reaction, high molecular weight polymer is not obtained unless high conversion of monomer is achieved.
Xn 11 p
Xn = Degree of polymerizationp = mole fraction monomer conversion
1
10
100
1000
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Mole Fraction Conversion (p)
Deg
ree o
f P
oly
meri
zati
on
Nylon-6,6
Cl Cl
O O
4H2N NH24
Adipoyl chloride 1,6-Diaminohexane
Cl NH
NH
H
O O
4 4
NaOH
HO NH
NH
H
O O
4 4n
6 carbondiacid
6 carbondiamine
Nylon-6,6Diamine, NaOH, in H2O
Adipoyl chloridein hexane
Nylon 6,6
Nylon-6,6
Diamine, NaOH, in H2O
Adipoyl chloridein hexane
Nylon 6,6
Since the reactants are in different phases, they can only react at the phase boundary. Once a layer of polymer forms, no more reaction occurs. Removing the polymer allows more reaction to occur.
Some Common Addition Polymers
8181
Condensation (Step) Polymerization
Condensation polymerization (ex. Polyester)
Some Condensation Polymers
85
Ancient Polymers• Naturally occurring polymers (those derived
from plants and animals) have been used for centuries.– Wood – Rubber– Cotton – Wool– Leather – Silk
• Oldest known uses– Rubber balls used by Incas
Cellulose
• Cellulose is a highly abundant organic compound. Extensive hydrogen bonding between the chains causes native celluose to be roughly 70% crystalline. It also raises the melting point (>280°C) to above its combustion temperature.
• Cellulose serves as the principal structural component of green plants and wood.
• Cotton is one of the purest forms of cellulose and has been cultivated since ancient times.
• Cotton also serves (along with treated wood pulp) as the source the industrial production of cellulose-derived materials which were the first "plastic" materials of commercial importance.
Rubber• A variety of plants produce a sap consisting of a colloidal dispersion of
cis-polyisoprene. This milky fluid is especially abundant in the rubber tree (Hevea); it drips when the bark is wounded.
• After collection, the latex is coagulated to obtain the solid rubber. Natural rubber is thermoplastic, with a glass transition temperature of –70°C.
• Raw natural rubber tends to be sticky when warm and brittle when cold, so it was little more than a novelty material when first introduced in Europe around 1770.
• It did not become generally useful until the mid-nineteenth century when Charles Goodyear found that heating it with sulfur — a process he called vulcanization — could greatly improve its properties.
cis-polyisoprene
Sifat-sifat Polimer
Specific Thermoplastic Properties
Thermoset data
Thermoset Properties
Mechanical properties of Polymers
Hooke’s Law
Young's modulus, also known as the tensile modulus or elastic modulus, is a measure of the stiffness of an elastic material and is a quantity used to characterize materials. It is defined as the ratio of the stress (force per unit area) along an axis to the strain (ratio of deformation over initial length) along that axis in the range of stress in which Hooke's law holds.
Young's modulus, E, can be calculated by dividing the tensile stress by the extensional strain in the elastic (initial, linear) portion of the stress–strain curve: whereE is the Young's modulus (modulus of elasticity)F is the force exerted on an object under tension;A0 is the original cross-sectional area through which the force is applied;ΔL is the amount by which the length of the object changes;L0 is the original length of the object.
• Young's Modulus =Stiffness = E = Slope of Stress/Strain Curve = = E = Slope of Stress/Strain Curve =s / e
• The steeper the stress/strain relationship (the higher Young's Modulus, E), the more stiff the material. Breaking strain and stress are the amounts of strain and stress observed at the breaking point. The more ductile the material, the more strain at breakage; the stronger the material, the higher the breaking stress.
• Ductile materials will deform more than stiff materials before breaking; however, ductile materials are not usually as strong a stiff materials. Compare, for example, a brittle object, say beach glass, and a ductile object, perhaps a rubber chicken. Glass may be strong (high breaking stress) but it is not ductile (low strain (i.e., little deformation) at breaking). A rubber chicken extends quite a bit before it breaks (long live rubber chickens) but can not withstand as much stress.
Stress
• Stress is "force per unit area" - the ratio of applied force F and cross section - defined as "force per area".
• tensile stress - stress that tends to stretch or lengthen the material - acts normal to the stressed area
• compressive stress - stress that tends to compress or shorten the material - acts normal to the stressed area
• shearing stress - stress that tends to shear the material - acts in plane to the stressed area at right-angles to compressive or tensile stress
Strain
Strain is defined as "deformation of a solid due to stress" and can be expressed asε = dl / lo
= σ / E wheredl = change of length (m, in)lo = initial length (m, in)
ε = unit less measure of engineering strainE = Young's modulus (Modulus of Elasticity) (N/m2 (Pa), lb/in2 (psi))Young's modulus can be used to predict the elongation or compression of an object.
• For many materials, Young's modulus is a constant over a range of strains. Such materials are called linear, and are said to obey Hooke's law. Examples of linear materials include steel, carbon fiber, and glass. Rubber and soil (except at very low strains) are non-linear materials.
Modulus of Elasticity (Young's Modulus)Slope of the stress-strain diagram within the elastic zone is called “Modulus of Elasticity” or “Young’s Modulus”. This parameter depends only on the material type.
In this equation E is the “Modulus of Elasticity”, is the applied stress in psi or ksi within the elastic limit,
and is the corresponding strain. Since strain does not have any units, E has units of psi or ksi. For structural steel E 29,000 ksi. A smaller modulus of elasticity translates to more a flexible (or less rigid) member.
Thermal properties
Permeability
Polymer MorphologyThe ultimate properties of any polymer (plastic, fiber, or rubber) result from a combination of molecular weight and chemical structure. Polymers require a particular MW, which depends largely on the chemical structure, to have desirable mechanical properties.
Molecular Weight
Mechanical Property
Polymer MorphologyThe mechanical properties result from attractive forces between molecules– dipole-dipole interactions, H-bonding, induction forces, London
forces or ionic bonding, ion-dipole interactions
CO
O
R
CO
O
R+
+
-
-
C
HN
O
R
C
HN
O
R
+
+
-
-
A lower MW polyamide will produce good fiber properties as compared to the polyester H-bonding
H-bondingdipole-dipole
• Hydrogen Bonding– A dipole-dipole interaction for hydrogens bonded
to electronegative elements• Electrostatic Interaction
Polymer Morphology
HO
R
HO
R
HO
R
HO
R
Weak bond ~ 5 kcal mol-1 (c-c ~ 81 kcal mol-1 )Require short bond distance ~ 2.5Å (c-c ~ 1.46Å)
very importantin cellulose
Polymer MorphologyIntermolecular forces drop off very rapidly with distance important polymer molecules be able to pack together closely to achieve maximum cohesive strength.
ex. Natural Rubberunstretched state - molecules are randomly distributed
low modulusstretched state - molecules become aligned, at 600%
elongation high modulus(2000 times higher than unstretched)
unstretched - amorphous / stretched - crystalline
OverviewMorphology is a term that has slightly different meaning depending on
the words with which it is used. In general it has to do with the ‘form’ or ‘structure’ of whatever topic it is used to describe.
For our purposes, we will use it to describe the form or structure of the polymer chains of thermoplastic materials when they are in their frozen or solid state.
For thermoplastic resins, there are two basic morphologies:
AMORPHOUS and SEMI-CRYSTALLINE
AmorphousAmorphous polymers appear random and jumbled when allowed to
cool in a relaxed state. They appear very similarly to their molten state, only the molecules are closer together.
They can be described as being similar to a large pot of spaghetti noodles.
Semi-crystallineA portion of the molecular chains in semi-crystalline polymers tend to
‘fold-up’ into densely packed regions called crystals as the polymer cools.
If more than 35% of the polymer chain will form these crystals – the polymer is classified as semi-crystalline.
Amorphous regions
Semi-crystalline regions
ExampleThink of Semi-crystalline materials like ramen noodles. When in their solid state, they have a compact ordered arrangement
The dense arrangement makes them stiffer and they resist flowing in that state
ExampleAmorphous materials are like cooked ramen noodles in that there is a random arrangement of the molecules and there are no crystals present to prevent the chains from flowing
It is important to remember that both materials have the random, unordered arrangement when molten
Degree of CrystallinityThere are many different factors that can determine the amount of
crystals or degree of crystallinity of a plastic component.• Cooling rate – it takes time for the polymer chains to fold up. If we
cool the polymer more quickly, we form fewer crystals• Additives – some additives can be put into plastics to increase the
degree of crystallinity while others can disrupt the formation of the crystals giving us a lower degree of crystallinity
• Polymer type – different materials can form higher or lower levels of crystallinity depending on their molecular structure
Temperature• As matter heats up, the molecules vibrate faster due to the
addition of the heat energy.• This faster vibration causes the molecules to move
further apart increasing the space or free volume between the molecules
• At some point the molecules get so far apart, they are no longer solid, they behave like a liquid.
• If you continue to heat the matter, the molecules get so far apart they turn into a gas (evaporate)
• With plastic materials, it is very difficult if not impossible to get them to evaporate because of their degree of entanglement.
TemperatureFor most materials, we are concerned with the melting point and boiling point. These are the temperatures at which the matter experiences a ‘change of state’
oSolid to Liquid
oLiquid to Gas
For thermoplastic materials, we are concerned with:
oGlass Transition Temperature
oMelting Temperature
Glass Transition Temperature (Tg)The Tg is important to both morphologies of thermoplastics
In amorphous materials, it is the temperature at which the molecules have enough absorbed enough energy and have moves far enough apart that the material behaves more rubber-like than glass-like.
The material stretches further when pulled
The material absorbs more impact energy without fracturing when struck
When the material does fail, it fails in a ductile manner as opposed to a brittle manner. (If a material fails in a ductile manner, it yields before it fails. In a brittle manner, it fails or ruptures before it yields)
The sample to the left experienced a brittle failure
•The material did not yield before failure
•The material broke like glass
The sample to the right broke in a ductile manner
•The material yielded (stretched) before failure
•The material behaved more like a rubber
Glass Transition Temperature (Tg)
Glass Transition Temperature (Tg)Because a semi-crystalline material has a portion of its chain that remains in an amorphous state, it is also affected by the Tg
- When a S/C material is above its Tg, it can form crystals – once it dips below the Tg crystal formation stops
-The amorphous portions of the chains have enough energy and the molecules are far enough apart, that the molecules can continue to fold up and unfold.
- The crystals are more easily pulled apart- The material is more flexible
Ex. Polyethylene and Polypropylene both have low Tg’s. They are way below room temperature. That is why milk jugs and yogurtcontainers are flexible when you take them out of the refrigerator.
Melt Temperature (Tm)Amorphous materials don’t truly have a Tm. They just continue to soften more until they behave more like a liquid.
The molecules absorb enough energy and move far enough apart (increase the free volume) that the material can flow.
When we refer to the melt temperature for amorphous materials, it is usually the temperature at which we can process it.
Melt Temperature (Tm)For S/C materials, the Tm is the temperature at which the crystals melt.
Once the crystals are melted the material generally flows very easily.
The ideal temperature for growing crystals is approximately 2/3 of the way between the Tg and the Tm.
Not in all cases, but in many, the degradation temperature for S/C materials is not much higher than the melt temperature.
OrientationWhen we talk about orientation in respect to polymer materials, we are talking about the alignment of the molecules.
Think of a polymer molecule like a broken rubber band sitting on your desk.
- As it flows, the molecule straightens out and stretches
Orientation-When it stops flowing, it wants to return to its random state.-As it cools, it will either start to fold up into a crystal or just move closer to the other molecules.
-If we cool the molecule quickly, before it has a chance to relax, we lock in that molecular alignment or orientation.
-When the molecules are aligned – the material is stronger in the direction of the alignment, but weaker transverse to it.
PropertiesYou have already seen that there is a big difference between the two basic morphologies of thermoplastic materials.
These differences cause the different types of materials to experience property differences.
Although the properties are mainly dependent on a specific polymer’s structure, there are tendencies that go with the specific morphologies.
This is why material selection is so important to the plastics field.
If the wrong material is used for a specific application, it can fail and cause damage or worse – personal injury or death.
PropertiesChemical Resistance
Plastic materials are used in virtually every aspect of today’s activities and they come into contact with a wide variety of chemical substances that they need to resist.
As a general rule S/C materials are more resistant to chemical attack than amorphous materials.
It is more difficult for the chemical media to penetrate the dense crystalline structure to damage the polymer chains.
Polyethylene is used to store everything from detergent to mineral spirits to gasoline. Polypropylene is only slightly less chemically
resistant than Polyethylene.
PropertiesChemical Resistance
Of the amorphous materials PVC is probably the best in chemical resistance, mainly due to the large chlorine atom that helps to protect the main polymer chain.
Polycarbonate, Acrylic, Polystyrene and the other styrenics are all very susceptible to chemical attack, especially to mineral spirits and solvents like lacquer and paint thinners, alcohol, and gasoline.
PropertiesOptical Properties
Amorphous materials have a much higher clarity than S/C materials.
The crystals that form in the material diffract the light as it passes through giving the material a translucent to opaque appearance.
If the crystallinity is disrupted by adding a copolymer or other additive or by quenching the material so quickly the crystals don’t have enough time to form, the material may appear somewhat clear.
Amorphous Acrylic more commonly known as Plexiglas and Polycarbonate used in safety glasses and optical lenses are far superior in terms of optical properties.
PropertiesImpact Resistance
The material structure determines the impact resistance, but as a general rule, S/C materials are more brittle than Amorphous.
The chain portions that are folded up in the crystal restrict the polymer chains as they try to move past one another when a force is applied making the S/C materials more brittle.
Polycarbonate is used in safety glasses, but General Purpose Polystyrene (GPPS) is very brittle – both are amorphous, but have different polymer structures.
On the S/C side, Polyethylene is very ductile at room temperature because it is above its Tg, but Nylon and Polyester are brittle at room temperature.
PropertiesViscosity
S/C materials by their very nature flow more easily than Amorphous materials.
The same mechanism that allows the material to fold up into dense crystals allows the polymer chains to slide past one another easily in the melted state.
For this reason materials like Nylon require very tight tolerances on their tooling to prevent melted plastic from leaking out of the cavities causing flash.
Flash
PropertiesWeather Resistance
When it comes to weather resistance, the most damaging aspect of weathering is generally considered to be Ultraviolet light.
The UV light breaks down the chains of the polymers making them more brittle, causing colors to fade or yellow, and causing additives in the polymers to migrate to the surface (chalking).
PropertiesWeather Resistance
Amorphous polymers have better chemical resistance to weathering effects than S/C polymers.
The crystals in the S/C polymers diffract the light so the UV rays spend more time within the polymer structure and do more damage. The clear amorphous polymers allow the damaging radiation to pass through doing less damage.
PropertiesShrinkage
Because they fold up into crystal structures, S/C materials have higher shrinkage rates when compared to Amorphous materials.
In injection molding most amorphous materials will shrink between 0.003-0.007 in/in (0.3-0.7%)
S/C materials shrink differently depending upon the level of crystallinity that they achieve.
Some will shrink over 0.025 in/in depending on processing variables, part thickness, and additives.
Material TypesAmorphous
Polyvinyl Chloride (PVC)
General Purpose Polystyrene (GPPS)
Polycarbonate (PC)
Polymethylmethacrylate (PMMA or Acrylic)
Acrylonitrile Butadiene Styrene (ABS – a terpolymer)
Material TypesSemi-crystalline
Polyethylene (PE, HDPE, LDPE, etc.)
Polypropylene (PP)
Polyamides (PA – Nylon)
Polyesters
Polyethylene Terephthalate (PET)
Polybutylene Terephthalate (PBT)
Polyoxymethylene (POM - Acetal)
Polytetrafluoroethylene (PTFE – Teflon)
Morphologies
• Amorphous structure random, unordered ex. Polystyrene• Crystalline structure regular, order ex. Polyethylene, Polypropylene
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Polymer Microstructure
Polyolefins with side chains have stereocenters on every other carbon
CH3n
CH3 CH3 CH3 CH3 CH3 CH3CH3
With so many stereocenters, the stereochemistry can be complex. There are three main stereochemical classifications for polymers.
Atactic: random orientation
Isotactic: All stereocenters have same orientation
Syndiotactic: Alternating stereochemistry
Capable of crystallizing
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Why is this important?
• Tacticity affects the physical properties– Atactic polymers will generally be amorphous, soft,
flexible materials– Isotactic and syndiotactic polymers will be more
crystalline, thus harder and less flexible
• Polypropylene (PP) is a good example– Atactic PP is a low melting, gooey material– Isoatactic PP is high melting (176º), crystalline, tough
material that is industrially useful– Syndiotactic PP has similar properties, but is very
clear. It is harder to synthesize
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Polymer CrystallinityPolymers are rarely 100% crystalline• Difficult for all regions of all chains to
become aligned
• Degree of crystallinity expressed as % crystallinity. -- Some physical properties depend on % crystallinity. -- Heat treating causes crystalline regions to grow and % crystallinity to increase.
crystalline region
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The effect of temperature on the structure and behavior of thermoplastics.
ThermoplasticsThe crystalline phases of such polymers are characterized by their melting temperature (Tm).Many thermoplastics are completely amorphous and incapable of crystallization, these amorphous polymers (and amorphous phases of semicrystalline polymers) are characterized by their glass transition temperature (Tg).
– the temperature at which they transform abruptly from the glassy state (hard) to the rubbery state (soft).
Thermoplastics
Glass transition temperature (Tg)This transition corresponds to the onset of chain motion
•below the Tg the polymer chains are unable to move and are “frozen” in position.
Both Tg and Tm increase with increasing chain stiffness and increasing forces of intermolecular attraction
ThermosetsThermosets - normally rigid materials - network polymers in which chain motion is greatly restricted by a high degree of crosslinking
As with elastomers, they are intractable once formed and degrade rather than melt upon the application of heat.
ElastomersElastomers - crosslinked rubbery polymers - rubber networks - that can be easily stretched to high extensions (3x to 10x original dimensions) – the rubbery polymer chains become extended upon
deformation but are prevented from permanent flow by crosslinking, and driven by entropy, spring back to their original positions on removal of the stress.
PolysaccharidesThe size of polysaccharide molecules can vary, occurring as polydispersed molecules that have a range of 100 to 100,000 monosaccharide units
– MW 16,000 - 16,000,000 daltons
There are a number of methods used to determine the molecular weight of polysaccharides
– viscosity*, light scattering, ultracentrifugation, osmometry and titration are most common
(*viscosity is routinely used, but is not an absolute method and can be used only in conjunction with one of the other methods)
Molecular Weight DistributionThe simplest, most common molecular weight is the number-average molecular weight (n)
– end-group analysis or colligative properties (b.p. elevation, osmotic pressure, etc)
others commonly used are weight-average molecular weight (w), z-average molecular weight (z) and viscosity-average molecular weight (u)
– light scattering (w), sedimentation equilibrium (z) and solution viscosity (u)
Number-average molecular weight (n)– based on methods of counting the number of
molecules in a given weight of polymer• the total weight of a polymer sample, w, is the sum of
the weights of each molecular species present
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NM
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Weight-average molecular weight (w)determination of molecular weight based on size rather than the number of molecules
– the greater the mass, the greater the contribution to the measurement
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2
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iii
ii
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w
MwM
w = weight fractionM = molecular weight N = number of molecules
Z-average molecular weight (z)some molecular weight determination methods (e.g. sedimentation equilibrium) yield higher molecular weight averages - z
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2
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2
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z
Mw
Mw
MN
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w = weight fractionM = molecular weightN = number of molecules
Example - a polymer sample consists of 9 molecules of mw 30,000 and 5 molecules of mw 50,000
000,37)59(
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n
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NMM
Number-average molecular weight (n)
Consider the previous example - 9 molecules of molecular weight 30,000 and 5 molecules of molecular weight 50,000
000,40)000,50(5)000,30(9
)000,50(5)000,30(9 22
wM
Weight-average molecular weight (w)
Consider the previous example - 9 molecules of molecular weight 30,000 and 5 molecules of molecular weight 50,000
136,42)000,50(5)000,30(9
)000,50(5)000,30(922
33
zM
Z-average molecular weight (z)
A Typical Molecular Weight Distribution Curve
200 000 400 000 600 000 800 000 1 000 000Mi (g mol-1)
104 wi
1.0
2.0
3.0
4.0n = 100 000 g mol-1
w = 199 900 g mol-1
z = 299 850 g mol-1
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Molecular Weight of PolymersUnlike small molecules, polymers are typically a mixture of differently sized molecules. Only an average molecular weight can be defined.
• Measuring molecular weight• Size exclusion chromatography• Viscosity
• Measurements of average molecular weight (M.W.)• Number average M.W. (Mn): Total
weight of all chains divided by # of chains
• Weight average M.W. (Mw): Weighted average. Always larger than Mn
• Viscosity average M.W. (Mv): Average determined by viscosity measurements. Closer to Mw than Mn
# o f m o l e c u l e s
Mn
Mw
increasing molecular weight
Mv
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What the Weights MeanMn: This gives you the true average weight
Let's say you had the following polymer sample:2 chains: 1,000,000 Dalton 2,000,0005 chains: 700,000 Dalton 3,500,00010 chains: 400,000 Dalton 4,000,0004 chains: 100,000 Dalton 400,0002 chains: 50,000 Dalton 100,000
10,000,00010,000,000/23 = 435,000 Dalton
1 Dalton = 1 g/mole
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Weight Average Molecular Weight
Mw: Since most of the polymer mass is in the heavier fractions, this gives the average molecular weight of the most abundant polymer fraction by mass.
2,000,00010,000,000
0.201,000,000 200,000
3,500,00010,000,000
0.35700,000 245,000
4,000,00010,000,000
0.40400,000 160,000
400,00010,000,000
0.04 100,000 4,000
100,00010,000,000
0.0150,000 500
Total 609,500
Polymer Solution Viscosity
When a polymer is dissolved in a solvent and then subjected to flow through a narrow capillary it exerts a resistance to that flow. This resistance is very informative. •It provides information on the size of the polymer•Its Flexibility and shape in solution •Its interactions with the solvent it is disolved in.
Polymer Melts
• To shape a thermoplastic polymer it must be heated so that it softens to the consistency of a liquid
• In this form, it is called a polymer melt • Important properties:
– Viscosity– Viscoelasticity
Viscosity of a polymer melt decreases with temperature, thus the fluid becomes thinner at higher temperatures
Figure 13.2 ‑
Viscosity as a function of temperature for selected polymers at a shear rate of 103 s-1
Viscoelasticity
Combination of viscosity and elasticity• Possessed by both polymer solids and polymer
melts• Example: die swell in extrusion, in which the
hot plastic expands when exiting the die opening
Various Fillers