Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

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Mathematical Modeling: Mathematical Modeling: Stress Relaxation of Stress Relaxation of Viscoelastic Materials Viscoelastic Materials Ryan Palmer Faculty Advisor: Dr. Michael Shaw

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Mathematical Modeling: Stress Relaxation of Viscoelastic Materials. Ryan Palmer Faculty Advisor: Dr. Michael Shaw. The Main Objective. Understand the viscoelastic material properties of skin Apply knowledge towards healing chronic wounds. Pictures provided by Dr. Garner (USC). - PowerPoint PPT Presentation

Transcript of Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Page 1: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Mathematical Modeling:Mathematical Modeling:Stress Relaxation of Stress Relaxation of

Viscoelastic MaterialsViscoelastic Materials

Ryan Palmer

Faculty Advisor: Dr. Michael Shaw

Page 2: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

The Main ObjectiveThe Main Objective Understand the viscoelastic material properties of

skin Apply knowledge towards healing chronic wounds

Pictures provided by Dr. Garner (USC)

Page 3: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

ViscoelasticityViscoelasticity

Viscous: Fluid-like motion with high resistance to flowExample: Glass

Elastic: Spring-like motionExample: Rubber band

Page 4: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Gelatin Specimen Preparation at Gelatin Specimen Preparation at CLUCLU

R. Palmer, G. Toland

Experimental variables:– u*– du/dt– gelatin concentration Pictures and graphs provided by

Dr. Shaw (CLU)

Page 5: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Force-displacement-time Force-displacement-time schematic of experimentschematic of experiment

Force, F

Time, t(sec)

Displacement, u(mm)

t=0

t=180

u*=2.0 mmt=60

1. Apply controlled displacement until reach peak displacement, u*; monitor load

2. Hold peak displacement u*; monitor load relaxation

Force, F

Indentation displacement,

u

Indenter diameter = 12 mmGel diameter = 23 mmGel thickness ~ 4 mmPictures and graphs provided by Dr. Shaw (CLU)

Page 6: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Stress Relaxation

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Loading of specimensLoading of specimens

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Stress Relaxation

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Page 8: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Viscoelastic modelsViscoelastic models

Viscoelastic materials have been modeled by a mixture of Maxwell, Voight and Kelvin models3.

These models consist of spring and dashpot setups.

Dashpot: A pneumatic or hydraulic cushion for a falling weight, to prevent shock5.

Page 9: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Maxwell ModelMaxwell Model

Maxwell Model:

Consists of a spring and dashpot in

series.

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Voight ModelVoight Model

Voight Model:

Consists of a spring and dashpot in

parallel.

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Kelvin ModelKelvin Model

Kelvin Model-

Consists of a spring in parallel with a Voight model.

Page 12: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Viscoelasticity and RC Viscoelasticity and RC CircuitsCircuits

Dashpot Resistor

Spring Capacitor

RC circuits are often used to simplify viscoelastic systems.Which help attain an equation to model its properties.

Page 13: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Stress Relaxation

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Stress-relaxation CurveStress-relaxation CurveStress Relaxation

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Page 14: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials

Stress Relaxation

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Stress-relaxation CurveStress-relaxation CurveStress Relaxation

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X error = Σ (Xpred. – Xdata)2

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