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Linear Viscoelasticity
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Elastic Response
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Viscous Response
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Maxwell Model
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Creep
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Stress Relaxation due to Maxwell
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Voigt Model
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Creep due to Voigt Relaxation
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Combination of Maxwell and Voigt
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Burgers Model
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Generalized Models
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Continues Distribution: Maxwell
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Continues Distribution: Voigt
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Superposition Principle
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Dynamic Response Output: Input: Viscoelastic body For a dashpot:
Stress: Moduli:
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Complex Representation:
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Time Scales
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TTT (if it would be right….) It is because
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Master curve for Polymers
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Composition of Relaxations: phase shift
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Comparison of E(T) and E(t)
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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
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Laplace Transform
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Properties of Laplace Transform
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Linear Viscoelasticity
(no time, so far)
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Laplace… Laplace transform of this function leads to Similarly for m
Finally:
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Examples of Operators Boltzmann kernel Boltzmann without singularity
No infinite rate of deformation
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Homework Pick a Linear viscoelastic moduli Solve the Lame problem
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