6. Material Properties Flashcards

1
Q

Elastic response to tensile stress

A

Full recovery from deformation…
- Metals
- Ceramics
- Polymer Fibres
- Glassy, amorphous, semi-crystalline polymers (below Tg)
- Hard materials w/ high modulus (small deformation)

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2
Q

Rubber elastic response to tensile stress

A

Full recovery…
- Low crosslink density polymer networks
- Soft solid materials
- Low modulus and high reversible deformation

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3
Q

Viscoelastic response to tensile stress

A

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

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4
Q

Energy elasticity in hard materials (and in relation to temperature)

A

Stretching increases inter-atomic distances, potential energy increases - E drops with temperature; increased strain with same applied tensile stress

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5
Q

Key concepts in stress-strain behaviour

A
  • 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
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6
Q

Behaviours above elastic limit

A
  • Plastic deformation:
    Strain does not return to 0 on removal of tensile stress, original shape not fully restored, above ‘yield point’
  • Brittle fracture
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7
Q

Deformation of semi-crystalline polymer above Tg

A
  1. Necking: rapid decrease in stress, local decrease in cross-section of sample, plastic deformation
  2. Cold drawing:
    Stress constant, plastic deformation, viscous flow and breaking of crystalline regions, then chain orientation and re-crystallisation in drawing direction
  3. Strain hardening:
    Stress increase, flow stopped due to oriented, re-crystallised chains, now significantly stiffer and stronger in the drawing direction, 2nd elastic region
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8
Q

Elastomers

A
  • 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.)
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9
Q

Helmholtz free energy (deltaA)

A

DeltaA = Delta’U’ - TDeltaS
U = Internal energy
F = (dA/dL)^V,T

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10
Q

Elastomer strain

A

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

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11
Q

Time dependency of polymer properties

A

Rate of conformational change in polymers is far slower than in small molecules
-> observed mechanical response depends on rate of deformation

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