Polymers- Introduction Flashcards
Homopolymer, random copolymer, block copolymer
Homopolymer has only one type of monomer
Random copolymer has two types of monomer with no order to their arrangement in the polymer chain
Block copolymer has two types of monomer with regions along the chain with many of one type (-M-M-M-N-N-N-)
How many CH2 units does typical molecule of polyethylene have?
Roughly 50,000
Types of natural polymers
Polysaccharides (starch, cellulose)
Polypeptides (muscle, collagen, keratin)
Polynucleotides (DNA, RNA)
Natural rubber, gums, resins
Types of synthetic polymers
Thermoplastics (solid when cooled, viscous liquid when heated)
Thermosets (precursors (viscous liquid) cross link to form infusible solid)
Common types of polymers
See slide 5 to 9
When can polymeric solids crystallise?
When their molecular structures are regular enough. Crystallisation often hampered by irregularities at molecular level
Skeletal structure for crystal or amorphous
Linear polymer more likely to crystallise. Branched has side chains so less likely. Cross-linked likely to be amorphous
Stereo-regularity for crystal or amorphous
Isotactic crystal
Syndiotactic (alternates sides) crystal
Atactic (random sides) amorphous
Why can polyethylene form a random coil?
Rotation around the C-C bonds means planar zigzag conformation changed into random conformation typical of amorphous polymer
Freely jointed chain model
Root mean square distance between the two chain ends is ^1/2. For freely jointed chain:
r sub f= ^1/2=n^1/2 l
n is number of bonds of length l
Blank space is r squared in arrows
Restriction by the valence angle formula
=nl^2[(1-cosθ)/(1+cosθ)]
θ is valence angle between two adjacent bonds (v shape)
Chain stiffness formula
=nl^2σ^2[(1-cosθ)/(1+cosθ)]
σ is steric parameter 1.5 to 2.5
Characteristic ratio
C sub infinity=/rf^2=/nl^2
Measure of chain stiffness/flexibility
Typical values of characteristic ratio for some polymers
Varies with temperature
Range from like 4 to 11
See slide 20
Typical YM values for steel, glass, polymer glass, nylon, polyethylene, rubber
Steel 220 GPa Glass 60 GPa Polymer glass 3-30 GPa Nylon 2 GPa Polyethylene 0.2 GPa Rubber 0.002 GPa
Stress strain plots for various types of polymer
Very steep straight for high modulus polymer fibre.
Steep straight fails at slightly lower stress for glassy polymer.
Straightish fails at lower stress for semicrystalline polymer below Tg.
Less steep for semicrystalline polymer above Tg with peak at failure when below Tg then horizontal for ages until slight increase to failure.
Shallow curve never peak then curves up a bit near end for elastomer
Temperature dependence graph for YM
Log(E) vs T (K). Starts high and near horizontal in glassy region. Curves to steep line down then levels off mostly in leathery region. Curves down bit more in rubbery region. Curves down bit more in rubbery flow region. Curves down bit more in viscous region. All regions similar with (T range) with later one’s getting bit smaller