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Linear Viscoelasticity. Elastic Response. Viscous Response. Maxwell Model. Creep. Stress Relaxation due to Maxwell. Voigt Model. Creep due to Voigt. Relaxation. Combination of Maxwell and Voigt. Burgers Model. Generalized Models. Continues Distribution: Maxwell.
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Creep due to Voigt Relaxation
Dynamic Response Output: Input: Viscoelastic body For a dashpot: Stress: Moduli:
TTT (if it would be right….) It is because
General Constitutive Law We can re-write this in the form: than we generalize the Elastic law: If we define and, for example: It might be shown that
Linear Viscoelasticity (no time, so far)
Laplace… Laplace transform of this function leads to Similarly for m Finally:
Examples of Operators Boltzmann kernel Boltzmann without singularity No infinite rate of deformation
Homework • Pick a Linear viscoelastic moduli • Solve the Lame problem