6. Material Properties Flashcards
Elastic response to tensile stress
Full recovery from deformation…
- Metals
- Ceramics
- Polymer Fibres
- Glassy, amorphous, semi-crystalline polymers (below Tg)
- Hard materials w/ high modulus (small deformation)
Rubber elastic response to tensile stress
Full recovery…
- Low crosslink density polymer networks
- Soft solid materials
- Low modulus and high reversible deformation
Viscoelastic response to tensile stress
Non-reversible deformation…
- Soft materials
- Polymer melts
- Semi-crystalline polymers
(*outside their elastic range)
Initially react elastically to stress but flow and deform irreversibly under prolonged stress
Energy elasticity in hard materials (and in relation to temperature)
Stretching increases inter-atomic distances, potential energy increases - E drops with temperature; increased strain with same applied tensile stress
Key concepts in stress-strain behaviour
- E (modulus) = stress (sigma) / strain (epsilon)
- STIFF: high modulus, small deformation, vs FLEXIBLE
- HARD withstand high tensile stress vs SOFT
- STRONG absorb high impact energy before breaking (area under curve), vs WEAK
Behaviours above elastic limit
- Plastic deformation:
Strain does not return to 0 on removal of tensile stress, original shape not fully restored, above ‘yield point’ - Brittle fracture
Deformation of semi-crystalline polymer above Tg
- Necking: rapid decrease in stress, local decrease in cross-section of sample, plastic deformation
- Cold drawing:
Stress constant, plastic deformation, viscous flow and breaking of crystalline regions, then chain orientation and re-crystallisation in drawing direction - Strain hardening:
Stress increase, flow stopped due to oriented, re-crystallised chains, now significantly stiffer and stronger in the drawing direction, 2nd elastic region
Elastomers
- Very low E modulus
- Fully elastic strain under low tension
- Stretching is exothermic, contraction is endothermic
- Contract under tension when heat is applied (unstrained rubber shows normal thermal expansion properties)
- Get stiffer w/ increasing temp. (E incr.)
Helmholtz free energy (deltaA)
DeltaA = Delta’U’ - TDeltaS
U = Internal energy
F = (dA/dL)^V,T
Elastomer strain
S = k*ln(omega)
(omega = amount of available chain conf.s)
Since elastomers strain via conformational change i.e entropy/S
Random coil therefore large entropy; chain uncoils, increasingly app-rotational orientation until fully extended
Time dependency of polymer properties
Rate of conformational change in polymers is far slower than in small molecules
-> observed mechanical response depends on rate of deformation