MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
TEM of spherulite structure in natural rubber(x30,000).
• Chain-folded lamellar crystallites (white lines) ~10nm thick extend radially.
Chapter 4- Polymer Structures
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
ISSUES TO ADDRESS...
What are the basic
• Classification?
• Monomers and chemical groups?
• Nomenclature?
• Polymerization methods?
• Molecular Weight and Degree of Polymerization?
• Molecular Structures?
• Crystallinity?
• Microstructural features
?
Chapter 4- Polymer Structures
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Poly
mer
= many
mers
Adapted from Fig. 14.2, Callister 6e.
Polymer Microstructure
Polyethylene perspective of molecule
A zig-zag backbone structure with covalent bonds
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Covalent
chain
configurations and strength:
Direction of increasing strength
Adapted from Fig. 14.7, Callister 6e.
Polymer Microstructure
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Common Examples
- Textile fibers: polyester, nylon…
- IC packaging materials.
- Resists for photolithography/microfabrication.
- Plastic bottles (polyethylene plastics).
- Adhesives and epoxy.
- High-strength/light-weight fibers: polyamides,
polyurethanes, Kevlar…
- Biopolymers: DNA, proteins, cellulose…
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Thermoplastics: polymers that flow more easily when
squeezed, pushed, stretched, etc. by a load (usually at
elevated T).
– Can be reheated to change shape.
• Thermosets: polymers that flow and can be molded
initially but their shape becomes set upon curing.
– Reheating will result in irreversible change or decomposition.
• Other ways to classify polymers.
– By chemical functionality (e.g. polyacrylates, polyamides, polyethers, polyeurethanes…).
– Vinyl vs. non-vinyl polymers.
– By polymerization methods (radical, anionic, cationic…). – Etc…
Common Classification
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Common Chemical Functional Groups
Saturated hydrocarbons (loose H to add atoms)
C C H H H H Ethylene (ethene) C C H H C H H H H Propylene (propene) = 1-butene 2-butene trans cis Acetylene (ethyne) H C CH Unsaturated hydrocarbons (double and triple bonds)
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Alcohols
Methyl alcohols
Ethers
Dimethyl Ether
Acids
Acetic acid
Aldehydes
Formaldehyde
Aromatic
hydrocarbons
Phenol
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Some Common Polymers
C C C N H H H Polyacrylonitrile (PAN) C C H H H X C C H H X H
Vinyl polymers (one or more H’s of ethylene can be substituted)
Common backbone with substitutions
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Monomer-based naming: poly________
e.g. ethylene -> polyethylene
if monomer name contains more than one word: poly(_____ ____)
e.g. acrylic acid -> poly(acrylic acid) Monomer name goes here
Monomer name in parentheses
Note: this may lead to polymers with different names but same structure.
C C C C H H H H H H H H … … C C C C H H H H H H H H … … polyethylene polymethylene
Nomenclature
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Polymerization Methods
H H
A. Free Radical Polymerization 1. Initiation
Free radical initiator (unpaired electron) C C H H H H monomer C C H H H R H R Radical transferred C C H H σ bonds π bond R H H C H H C R sp2 carbons sp3 carbon
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Polymerization Methods
A. Free Radical Polymerization2. Propagation C C H H H H C C H H H R H C C H H H C H H H C H H R C C H H H H C C H H H C H H H C H H C H H C H H R H H C H H C R H H C C H H
Both carbon atoms will change from sp2 to sp3.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Polymerization Methods
A. Free Radical Polymerization3. Termination C C H H H R H C C H H H R H R + C C H H H R H R C C H H H R H + C H H C H H C H H C H H R R
Intentional or unintentional molecules/impurities can also terminate.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Polymerization Methods
B. Stepwise polymerization RCOH O N H2 + RCOH O N H2 RCN H O N H2 RCOH O C. Other methodsAnionic polymerization, cationic polymerization, coordination polymerization… RC O N H n HOH + HOH + (n-1) Loses water (condensation)
Proteins (polypeptides have similar composition)
C H C O N H R n Various R groups…
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Molecular Weights
Not only are there different structures (molecular arrangements) …… but there can also be a distribution of molecular weights (i.e. number of monomers per polymer molecule).20 mers 16 mers
10 mers
Average molecular weight =
M
monomer15
.
3
M
monomer3
10
16
20
=
+
+
This is what is called numberaverage molecular weight.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08 Number average molecular weight:
€ Mn= NjMj j
∑
Nj j∑
€
=
m
oN
jj
j∑
N
j j∑
€ NjMj j∑
=Note: Total weight
€
N
j j∑
=
Total # of polymer chains Weight average molecular weight:€
M
w=
W
jM
j j∑
W
j j∑
=
N
jM
2j j∑
N
jM
j j∑
€
W
j= N
jM
j In general: € M = NjMα+1j j∑
NjMαj j∑
€
M
n If α = 0 then If α = 1 then€
M
w Nj = # of polymer chains with length jMj = jmo mass of polymer chain with length j
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Molecular Weight:
Different Notations
€
M
n
=
N
j
M
j
j
∑
N
j
j
∑
€
M
n
=
x
i
M
i
i
∑
€
x
i=
N
iN
j j∑
€
M
w
=
N
j
M
2
j
j
∑
N
j
M
j
j
∑
€
M
w
=
w
i
M
i
i
∑
€
w
i
=
N
i
M
i
N
j
M
j
j
∑
In Lecture Notes In Callister Textbook
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08 Examples –
Light scattering: larger molecules scatter more light than smaller ones. Infrared absorption properties: larger molecules have more side groups and light absorption (due to vibrational modes of side groups) varies linearly with number of side groups.
Molecular Weights
Why do we care about weight average MW?-some properties are dependent on MW (larger MW polymer chains can contribute to overall properties more than smaller ones).
Distribution of polymer weights
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Polydispersity and Degree of Polymerization
Polydispersity:
€
M
w
M
n
≥ 1
When polydispersity = 1, system is monodisperse.
Degree of Polymerization:
€
n
n
=
M
n
m
o
Number avg degree of polymerization
n
w
=
M
w
m
o
Weight avg degree of polymerization
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Compute the number-average degree of polymerization for polypropylene, given that the number-average molecular weight is 1,000,000 g/mol. What is “mer” of PP?
Mer molecular weight of PP is
Example 1
C
3H
6m
o=3A
C+6A
H=3(12.01 g/mol)+6(1.008 g/mol)
= 42.08 g/mol
Number avg degree of polymerization
n
n=
M
nm
o=
10
6g /mol
42.08g /mol
= 23,700
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Example 2 (a, b, and c)
A. Calculate the number and weight average degrees of polymerization and polydispersity for a polymer sample with the following distribution.
Avg # of monomers/chain Relative abundance
10 5 100 25 500 50 1000 30 5000 10 50,000 5 nn= Mn mo =m0 m0 jNj j
∑
Nj j∑
= jNj j∑
Nj j∑
=5 *10 + 25 *100 + 50 * 500 + 30 *1000 + 10 * 5000 + 5 * 50000 5 + 25 + 50 + 30 + 10 + 5 = 2860.4 nw= Mw mo = 1 mo ( jmo) 2N j j∑
Nj( jmo) j∑
= j2N j j∑
jNj j∑
=5 *10 2 + 25 *1002 + 50 * 5002 + 30 *10002 + 10 * 50002 + 5 * 500002 5 *10 + 25 *100 + 50 * 500 + 30 *1000 + 10 * 5000 + 5 * 50000 = 35, 800Note: m0 cancels in all these!
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Example 2 (cont.)
B. If the polymer is PMMA, calculate number and weight average
molecular weights.
Mw if monomer is methylmethacrylate (5C, 2O, and 8H)
So m0= 5(12)+2(16)+8(1)= 100 g/mol CH3 | | CO2CH3
€
M
n =
n
n
m
o = 2860.4(100
g
/
mol
) = 286,040
g
/
mol
M
w =
n
w
m
o = 35,800(100
g
/
mol
) = 3,580,000
g
/
mol
€
M
wM
n= 3,580,000 286,040 ~ 12.52 Polydispersity:MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Example 2 (cont.)
C. If we add polymer chains with avg # of monomers = 10 such that their relative abundance changes from 5 to 10, what are the new number and weight average degrees of polymerization and polydispersity?
Add 5 more monomers of length 10 …. nn= Mn mo =
∑
jjNj Nj j∑
=10 * 10 + 25 * 100 + 50 * 500 + 30 * 1000 + 10 * 5000 + 5 * 50000 10 + 25 + 50 + 30 + 10 + 5 = 2750 Mw Mn =3, 580, 000 275000 ~ 13 Polydispersity: € nw =M w mo= j2N j j ∑ jN j j ∑ = 35,800Note: significant change in number average (3.8 %) but no change in weight average!
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08 For an asymmetric monomer
T H + T H T H T H T H H T H T T H C H F C H H C F H C H H C H F C H H C H H C F H e.g. poly(vinyl fluoride):
H to T T to T H to H Random arrangement e.g. PMMA C C CH3 C H H C C CH3 C H H O O C H3 H3C O O C C CH3 C H H C C CH3 C H H O O C H3 O C H3 O H to T H to T H to T
Exclusive H to T arrangement (Why?)
Sequence isomerism
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Regularity and symmetry of side groups affect properties
• Stereoisomerism: (can add geometric isomerism too)
Polymer Molecular Configurations
Isotactic On one side Syndiotactic Alternating sides Atactic Randomly placed
- Conversion from one stereoisomerism to another is not possible by simple rotation about single chain bond; bonds must be severed first, then reformed!
Polymerize Can it crystallize?Melting T?
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Regularity and symmetry of side groups affect properties
Polymer Geometrical Isomerism
cis
-structure
trans
-structure
with R= CH
3to form rubber
Cis-polyisoprene
trans-polyisoprene
H H-Conversion from one isomerism to another is not possible by simple
rotation about chain bond because double-bond is too rigid! -See Figure 4.8 for taxonomy of polymer structures
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Polymer Structural Isomerism
Some polymers contain monomers with more than 1 reactive sitee.g. isoprene C H2 C C H CH2 CH3 trans-isoprene trans-1,4-polyisoprene C H2 C C H C H2 CH3 1 4 2 trans-1,2-polyisoprene n C H2 C CH C H2 C H3 n 3 3,4-polyisoprene C H2 C H C C H2 CH3 n
Note: there are also cis-1,4- and cis-1,2-polyisoprene
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Covalent
chain
configurations and strength:
Direction of increasing strength
Adapted from Fig. 14.7, Callister 6e.
Polymer Microstructure
Van der Waals, H More rigid
Short branching
Long branching
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Random, Alternating, Blocked, and Grafted
CoPolymers
• Synthetic rubbers are often copolymers. e.g., automobile tires (SBR)
Styrene-Butadiene Rubber random polymer
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Molecular Structure
How do crosslinking and branching occur in polymerization?1. Start with or add in monomers that have more than 2 sites that bond with other monomers, e.g. crosslinking polystyrene with divinyl benzene
… … stryene polystyrene Control degree of crosslinking by styrene-divinyl benzene ratio + … … styrene
divinyl benzene crosslinked polystyrene Monomers with trifunctional groups lead to network polymers.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Molecular Structure
Branching in polyethylene (back-biting)C H2 CH2 R C H2 C H2 C H2 C H2 C H2 C H H R C C H2 CH2 CH2 C H H H H Same as
Radical moves to a different carbon
(H transfer) R C C H2 CH2 CH2 C H H H H
Polymerization continues from this carbon
Process is difficult to avoid and leads to (highly branched) low-density PE . When there is small degree of branching you get high-density PE.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Example 3
Nitrile rubber copolymer, co-poly(acrylonitrile-butadiene), has
Calculate the ratio of (# of acrylonitrile) to (# of butadiene).
€
M
n
= 106,740g /mol
€
n
n = 2000 3 C = 3 x 12.01 g/mol 3 H = 3 x 1.008 g/mol 1 N = 1 x 14.007 g/mol m0= 53.06 g/mol 4 C = 4 x 12.01 g/mol 6 H = 6 x 1.008 g/mol m0= 54.09 g/mol 1,4-addition product € mo =Mnn n = 106,740 2000 = 53.57g/mol We need to use an avg. monomer MW: € mo= f1m1+ f2m2= f1(m1− m2) + m2 € f1=mm0− m2 1− m2= 53.37 − 54.09 53.06 − 54.09= 0.7 € f2 = 1−f1 = 0.3 € f2 f1= 0.7 0.3→ 7 : 3MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Crosslinking in elastomers is called vulcanization, and is achieved by
irreversible chemical reaction, usually requiring high temperatures.
Vulcanization
• Sulfur compounds are added to form chains that bond adjacent
polymer backbone chains and crosslinks them.
• Unvulcnaized rubber is soft and tacky an poorly resistant to wear.
e.g., cis-isoprene Stress-strain curves
+ (m+n) S
(S)
n(S)
mSingle bonds
Double bonds
See also sect. in Chpt. 8
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
•
Molecular weight
, M
w:
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 increasewith % crystallinity. --Annealing causes crystalline regions to grow. % crystallinity increases.
crystalline region
amorphous region Adapted from Fig. 14.11, Callister 6e.
Molecular Weight and Crystallinity
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Polymer Crystallinity
polyethylene
• Some are amorphous.• Some are partially crystalline (semi-crystalline). • Why is it difficult to have a 100% crystalline polymer?
%crystallinity =
ρ
c(
ρ
s−
ρ
a)
ρ
s(
ρ
c−
ρ
a)
× 100%
ρs = density of specimen in question ρa = density of totally amorphous polymer ρc = density of totally crystalline polymer
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
€
%crystallinity =
M
crystallineM
total× 100% =
ρc
V
cρs
V
s× 100% =
ρc
ρs
f
c× 100%
Volume fraction of crystalline component.
€
Mtotal= Mcrystalline+ Mamophous Ms= Mc+ Ma ρsVs=ρcVc+ρaVa ρs=ρcVVc s+ρa Va Vs = ρcfc+ρafa=ρcfc+ρa(1−fc) = fc(ρc−ρa) + ρa Using definition of volume fractions:
€ fc =Vc Vs € fa =VVa s
€
f
c=
ρ
s−
ρ
aρc
−
ρa
Substituting in fc into the original definition:
%crystallinity =
ρ
c(
ρ
s−
ρ
a)
ρ
s(
ρ
c−
ρ
a)
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Polymer Crystallinity
Degree of crystallinity depends on processing conditions (e.g. cooling rate) and chain configuration.Cooling rate: during crystallization upon cooling through MP,
polymers become highly viscous. Requires sufficient time for random & entangled chains to become ordered in viscous liquid.
Chemical groups and chain configuration: More Crystalline
Smaller/simper side groups Linear Isotactic or syndiotactic
Less Crystalline Larger/complex side groups
Highly branched Crosslinked, network
Random
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Semi-Crystalline Polymers
Fringed micelle model: crystalline region embedded in amorphous region. A single chain of polymer may pass through several crystalline regions as well as intervening amorphous regions.
€
f
c=
ρ
s−
ρ
aρ
c−
ρ
aCrystalline volume fractions Important
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Semi-Crystalline Polymers
Chain-folded model: regularly shaped platelets (~10 – 20 nm thick) sometimes forming multilayers.Average chain length >> platelet thickness.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Semi-Crystalline Polymers
Spherulites: Spherical shape composed of aggregates of chain-folded crystallites.
Natural rubber
Cross-polarized light through spherulite structure of PE.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Diblock copolymers
Representative polymer-polymer phase behavior with different architectures:
A) Phase separation with mixed
LINEAR homopolymers. B) Mixed LINEAR homopolymers and
DIBLOCK copolymer gives surfactant-like stabilized state. C) Covalent bond between blocks in
DIBLOCK copolymer give microphase segregation. F. Bates, Science 1991.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
•
Thermoplastics
:
--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
Callister, Fig. 16.9
T
Molecular weight
Tg
Tm
mobile liquid viscous liquid rubber tough plastic partially crystalline solid crystalline solidAdapted from Fig. 15.18, Callister 6e.
Thermoplastics vs Thermosets
Tm: melting over wide range of T depends upon history of sample consequence of lamellar structure thicker lamellae, higher Tm.
Tg: from rubbery to rigid as T lowers
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Packing of “spherical” atoms as in ionic and metallic crystals led to crystalline structures.
• How polymers pack depend on many factors: • long or short, e.g. long (-CH2-)n.
• stiff or flexible, e.g. bendy C-C sp3.
• smooth or lumpy, e.g., HDPE. • regular or random
• single or branched
• slippery or sticky, e.g. C-H covalent (nonpolar) joined via vdW.
Analogy:
Consider dried (uncooked) spaghetti (crystalline) vs.cooked and buttered spaghetti (amorphous).
• pile of long “stiff” spaghetti forms a random arrangement. • cut into short pieces and they align easily.
Candle wax more crystalline than PE, even though same
chemical nature.
Packing of Polymers
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Would you expect melting of
nylon 6,6
to be lower thanPE
?What Are Expected Properties?
€ − N | H − H | C | H 6 − N | H − O || C− H | C | H 4 − N | H − O || C− € − N | H − H | C | H 6 − N | H − O || C− H | C | H 4 − N | H − O || C− + + + + + + € − H C H − H C H − € − H C H − H C H − + + + + + + nylon 6,6 polyethylene
a) What is the source of intermolecular cohesion in Nylon vs PE? b) How does the source of linking affect temperature?
Hydrogen bonds Van der Waals bonds
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Which polymer more likely to crystallize? Can it be decided?
What Are Expected Properties?
Linear syndiotactic polyvinyl chloride Linear isotactic polystyrene• Linear and syndiotactic polyvinyl chloride is more likely to crystallize. • The phenyl side-group for PS is bulkier than the Cl side-group for PVC. • Generally, syndiotactic and isotactic isomers are equally likely to crystallize.
• For linear polymers, crystallization is more easily accomplished as chain alignment is not prevented.
• Crystallization is not favored for polymers that are composed of chemically complex mer structures, e.g. polyisoprene.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Which polymer more likely to crystallize? Can it be decided?
What Are Expected Properties?
Linear and highly crosslinkcis-isoprene
• Not possible to decide which might crystallize. Both not likely to do so. • Networked and highly crosslinked structures are near impossible to reorient to favorable alignment.
H
+
+ H20 Networked Phenol-Formaldehyde (Bakelite)MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Which polymer more likely to crystallize? Can it be decided?
What Are Expected Properties?
alternating Poly(Polystyrene-Ethylene) Copolymer random poly(vinyl chloride-tetra-fluoroethylne) copolymer• Alternating co-polymer more likely to crystallize than random ones, as they are always more easily crystallized as the chains can align more easily.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08 • Soap is a detergent based on animal or vegetable product, some contain petrochemicals
Detergents
grease water detergent
• What properties of soap molecules do you need to remove grease? • “green” end must be “hydrophilic”. Why?
• Opposite end must be hydrocarbon. Why?
Water must be like oxygen (hoard electrons and promote H-bonding)
grease
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Simple polymer: Elmers glue + Borax
SLIME!
Chemistry Elmer’s glue is similar to “poly (vinyl alcohol)” with formula:
Borax is sodium tetraborate decahydrate (B4Na2O7 • 10 H2O).
The borax actually dissolves to form boric acid, B(OH)3.
This boric acid-borate solution is a buffer with a pH of about 9 (basic). Boric acid will accept a hydroxide OH- from water.
B(OH)3 + 2H2O B(OH)4- + H3O+ pH=9.2
OH OH OH OH OH OH OH OH OH OH OH OH OH OH OH
this is a SHORT, n=15 chain of poly(vinyl alcohol)
Hydrolyzed molecule acts in a condensation reaction
with PVA,
crosslinking
it.
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Simple polymer: Elmer’s glue + Borax
SLIME!
Hydrolyzed molecule acts in a condensation reaction with PVA, crosslinking it.
B(OH)3 + 2H2O B(OH)4- + H3O+ pH=9.2
Crosslinkingties chains via weak non-covalent
(hydrogen) bonds, so it flows slowly. Crosslinked
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
Range of Bonding and Elastic Properties
Is “slime” a thermoset or thermoplastic, or neither?
Thermoset
bonding
Thermoplastic
bonding
• Induced dipolar bonds form crosslinks
Slime?
Stiffness increases
Where is nylon?
• Covalent bonds
form crosslinks • H-bonds form crosslinks
MatSE 280: Introduction to Engineering Materials ©D.D. Johnson 2004, 2006, 2007-08
• Polymers are
part crystalline
and
part amorphous
.
• The more
“lumpy” and branched
the polymer, the
less
dense and less crystalline
.
• The more
crosslinking
the
stiffer
the polymer. And,
networked
polymers are like heavily crosslinked ones.
• Many
long-chained polymers crystallize with a Spherulite
microstructure
- radial crystallites separated by
amorphous regions.
• Optical properties: crystalline -> scatter light (Bragg)
amorphous -> transparent.
Most covalent molecules absorb light