
doi: 10.1122/1.549591
When subjected to creep test, aluminum exhibits characteristics which are analogous to those of thermorheologically simple material in the sense that on a plot of logarithm of creep function versus logarithm of time the curves corresponding to different stresses have the same shape so that they all could be shifted to form a master curve. Based on this observation and in analogy with the idea of time‐temperature superposition, a theory for viscoelastic materials is developed in which the natural time appearing explicity in the argument of relaxation or creep function is replaced by a suitable scalar‐valued function of stress tensor.
elastic- viscoplastic materials, constitutive equations, isotropy, Materials of strain-rate type and history type, other materials with memory (including elastic materials with viscous damping, various viscoelastic materials), linearization, virtual work, BZK theory, creep-compliance, temperature-dependent intrinsic time, yield phenomena, stress clock function, Volterra's integral equations, Viscoelastic fluids, Plastic materials, materials of stress-rate and internal-variable type, strain- relaxation modulus
elastic- viscoplastic materials, constitutive equations, isotropy, Materials of strain-rate type and history type, other materials with memory (including elastic materials with viscous damping, various viscoelastic materials), linearization, virtual work, BZK theory, creep-compliance, temperature-dependent intrinsic time, yield phenomena, stress clock function, Volterra's integral equations, Viscoelastic fluids, Plastic materials, materials of stress-rate and internal-variable type, strain- relaxation modulus
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