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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.

Dec 22, 2015

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Page 1: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

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 Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

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 Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

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 Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

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 Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

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 Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

Stress Relaxation

0

20

40

60

80

100

120

0 50 100 150

Time (sec)

Lo

ad (

N)

Ryan Palmer

Loading of specimensLoading of specimens

Page 7: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

Stress Relaxation

93.7594.75

95.7596.7597.75

98.7599.75

100.75

55 75 95 115 135 155 175

Time (sec)

Lo

ad (

N)

Ryan Palmer

Stress-relaxation CurveStress-relaxation CurveStress Relaxation

0

20

40

60

80

100

120

0 50 100 150

Time (sec)

Lo

ad

(N

)

Page 8: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

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 Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

Maxwell ModelMaxwell Model

Maxwell Model:

Consists of a spring and dashpot in

series.

Page 10: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

Voight ModelVoight Model

Voight Model:

Consists of a spring and dashpot in

parallel.

Page 11: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

Kelvin ModelKelvin Model

Kelvin Model-

Consists of a spring in parallel with a Voight model.

Page 12: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

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 Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

Stress Relaxation

94.00

95.00

96.00

97.00

98.00

99.00

100.00

101.00

60 80 100 120 140 160 180

Time (sec)

Lo

ad

(N

)

Data

Predicted

Ryan Palmer

Stress-relaxation CurveStress-relaxation CurveStress Relaxation

0

20

40

60

80

100

120

0 50 100 150

Time (sec)

Lo

ad

(N

)

Page 14: Mathematical Modeling: Stress Relaxation of Viscoelastic Materials Ryan Palmer Faculty Advisor: Dr. Michael Shaw.

Stress Relaxation

98.00

98.20

98.40

98.60

98.80

99.00

60 65 70 75 80

Time (sec)

Lo

ad (

N)

Data

Predicted

Ryan Palmer

Stress-relaxation CurveStress-relaxation CurveStress Relaxation

94.00

95.00

96.00

97.00

98.00

99.00

100.00

101.00

60 80 100 120 140 160 180

Time (sec)

Lo

ad

(N

)

Data

Predicted

Y error = Σ (Ypred. – Ydata)2

X error = Σ (Xpred. – Xdata)2

X error

Y error