Abstract
This article reviews recent developments in polymer thermomechanics both in theory and experiment. The first section is concerned with theories of thermomechanics of polymers both in rubbery and solid (glassy and crystalline) states with special emphasis on relationships following from the thermomechanical equations of state. In the second section, some of the methods of thermomechanical measurements are briefly described. The third section deals with the thermomechanics of molecular networks and rubberlike materials including such technically important materials as filled rubbers and block and graft copolymers. Some recent data on thermomechanical behaviour of bioelastomers are also described. In the fourth section, thermomechanics of solid polymers both in undrawn and drawn states are discussed with a special focus on the molecular and structural interpretation of thermomechanical experiments. The concluding remarks stress the progress in the understanding of the thermomechanical properties of polymers.
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Abbreviations
- a0 :
-
radius of unstrained sample
- a, a1, a2 :
-
parameters of van der Waals equation of state of a network
- e:
-
uniform (volume) strain
- f:
-
retractive force
- fs :
-
entropy component of retractive force
- fu :
-
energy component of retractive force
- p:
-
number of statistical segments
- r:
-
end-to-end distance of network chains
- rmax :
-
maximum extension of network chains
- 〈r2〉:
-
mean square end-to-end distance of network chains in undeformed sample
- 〈r2〉0 :
-
mean square end-to-end distance of unperturbed chains
- 〈r2〉i :
-
mean square end-to-end distance of network chains in the reference state
- w:
-
degree of crystallinity
- xi :
-
generalized coordinate
- A0 :
-
cross-sectional area of sample
- C:
-
heat capacity
- C:
-
constant in the Gaussian equation of state for-rubber elasticity
- C1, C2 :
-
constants in the Mooney-Rivlin equation
- \(D',D_m ,\bar D_m\) :
-
strain functions in van der Waals equation of state
- E:
-
modulus of elasticity (Young modulus)
- Ec :
-
conformational energy of chains
- E′:
-
modulus of elasticity of filled rubbers
- Ef :
-
internal energy changes in filled rubbers
- E‖ :
-
modulus of elasticity along the draw axis
- E⊥ :
-
modulus of elasticity perpendicular to the draw axis
- Ecr :
-
modulus of elasticity of crystalline lattice
- EAB :
-
modulus of elasticity of amorphous intrafibrillar regions
- EAI :
-
modulus of elasticity of amorphous interfibrillar regions
- F:
-
free energy
- F*:
-
Free energy of deformation of solids
- G:
-
free enthalpy
- G*:
-
free enthalpy of deformation of solids
- G0 :
-
shear modulus
- H:
-
enthalpy
- H*:
-
enthalpy of deformation of solids
- K:
-
modulus of elasticity (volume)
- L0 :
-
length of undeformed samples
- L:
-
length of deformed samples
- Li :
-
length of samples in the reference state
- M:
-
twisting couple
- P:
-
pressure
- Q:
-
heat
- S:
-
entropy
- T:
-
absolute temperature
- V:
-
volume
- U:
-
internal energy
- U*:
-
internal energy of deformation of solids
- W:
-
mechanical work
- X:
-
portion of interfibrillar amorphous regions
- α:
-
volume thermal expansivity
- α* :
-
degree of deformation
- β:
-
linear thermal expansivity
- β‖ :
-
linear thermal expansivity along the orientation axis
- β⊥ :
-
linear thermal expansivity perpendicular to orientation axis
- βcr :
-
linear thermal expansivity of crystalline lattice
- βAB :
-
linear thermal expansivity of intrafibrillar amorphous regions
- βAI :
-
linear thermal expansivity of interfibrillar amorphous regions
- β:
-
linear thermal expansivity under the angle Ï•
- γ:
-
= (∂ ln 〈r2〉0/∂ ln V)T, L
- γS :
-
shear deformation
- γ′:
-
= γ/2
- δ:
-
solubility parameter
- ε:
-
strain (uniaxial)
- η:
-
heat to work ratio
- κ:
-
volume compressibility
- κL :
-
linear compressibility
- λ:
-
elongation (or compression) ratio
- λQ :
-
elongation corresponding to inversion of heat
- λu :
-
elongation corresponding to inversion of internal energy
- λm :
-
limiting elongation
- λf :
-
elongation corresponding to inversion of force
- μ:
-
Poisson's ratio
- ν:
-
number of elastically active network chains
- ξ, ξi :
-
generalized force
- σ:
-
stress
- Ï„:
-
shear stress
- Ï•:
-
angle with the draw direction
- ω:
-
internal energy to work ratio
- θ:
-
twisting angle
- PE:
-
polyethylene
- LDPE:
-
low density polyethylene
- HDPE:
-
high density polyethylene
- PP:
-
polypropylene
- PA:
-
polyamide
- PS:
-
polystyrene
- PET:
-
poly(ethylene terephthalate)
- NR:
-
natural rubber
- PDMS:
-
polydimethylsiloxane
- EPR:
-
ethylene-propylene rubber
- SBR:
-
styrene-butadiene rubber
- PCR:
-
polychloroprene rubber
- NBR:
-
nitrile-butadiene rubber
- PBR:
-
polybutadiene rubber
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Godovsky, Y.K. (1986). Thermomechanics of polymers. In: Dušek, K. (eds) Pharmacy/Thermomechanics/Elastomers/Telechelics. Advances in Polymer Science, vol 76. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-15830-8_2
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