meen 53301 stress analysis in viscoelastic materials meen 5330, fall 2006 presented by: suresh kumar...

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MEEN 5330 1 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI JAMAL MOHAMMED SUBRAHMANYA SRI VITTAL CHEDERE

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Page 1: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 1

Stress Analysis in Viscoelastic Materials

MEEN 5330, Fall 2006

Presented by:SURESH KUMAR ANBALAGANSAI PRASEN SOMSETTYVEERABHADRA REDDY KAJULURIJAMAL MOHAMMEDSUBRAHMANYA SRI VITTAL CHEDERE

Page 2: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 2

Introduction

Hooke’s LawViscoelastic MaterialRelation with Hooke’s LawExamples

Page 3: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 3

Some phenomena in viscoelastic materials

A) Instantaneous elasticityB) Creep under constant stressC) Stress relaxation under constant

strainD) Instantaneous recoveryE) Delayed recoveryF) Permanent set

Page 4: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 4

CREEP

Slow progressive deformation of a material under constant stress

Anelastic Material

Page 5: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 5

THREE STAGES OF CREEP

Page 6: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 6

STRESS RELAXATION

Page 7: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 7

Basic Elements

These models allow the mathematical representation of viscous and elastic properties of viscoelastic materials.Basic elements: (Spring and Dashpot)F = -KXF is restoring force by spring, K is spring constant and X is spring elongation.F/A = -(K/A)*Xσ = E ε E is modulus of elasticity.

Spring.

Page 8: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 8

Basic Elements

Piston cylinder arrangement with a perforated bottom A viscous lubricant between the cylinder and piston walls force ‘F’ is proportional to the velocity F = K (dX/dt) σ = η (dε / dt) η is Viscosity coefficient Dashpot

Page 9: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 9

Maxwell model

For series connection the total strain is given byε = ε1 + ε2 strain rate is given by ε *=ε1*+ε2*ε *= σ*/E + σ /ηε * is (dε/dt)

Spring and dashpot in series

Page 10: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 10

Kelvin/Voight Model

σ = σ1+ σ2 (total stress)σ1 = E ε (for spring)σ2 = η ε* (for dashpot)σ = E ε + η ε*

Spring and Dashpot in parallel

Page 11: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 11

Generalized Maxwell model

The generalized Maxwell model consists of a series of Maxwell model as shown below,

Page 12: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 12

Generalized Maxwell model cont’d

The total strain is given by

N

i i

N

i

G11

.. 11

Page 13: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 13

Generalized Maxwell model cont’d

Consider the following setup of Maxwell model units,

Page 14: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 14

Generalized Maxwell model cont’d

The above diagram shows a generalized model of Maxwell model units connected in parallel.The total strain is given by,

N

i

ii

tG

1

.

1

Page 15: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 15

Example for a Generalized Maxwell model

consider the following arrangement of Maxwell model units. Determine the stress-strain relations for the given arrangement.

Page 16: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 16

Example for a Generalized Maxwell model cont’d

SolutionFor a generalized Maxwell model, we have the stress – strain relation as follows

N

i

ii

tG

1

.

1

Page 17: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 17

Example for a Generalized Maxwell model cont’d

For N=2, the above equation becomes,

We know the relaxation time relation as,

222111 /1///1//

GG

111 /1/ G

Page 18: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 18

Example for a Generalized Maxwell model cont’d

Using the above relation the equation for the strain changes to,

Which when expanded becomes

122112 /1/1)/(/1 ttt GG

)//()(//)( 221121212121 GGGG

Page 19: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 19

Generalized Kelvin Model

The generalized Kelvin model is represented using a number of Kelvin model units connected in series as shown

Page 20: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 20

Generalized Kelvin Model cont’d

The total strain, for an N number of Kelvin model units is given as follows

N

i tiiG1

Page 21: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 21

Standard Linear Solid

For a spring,σ = E1 ε1ε1* = σ*/E1For the Kelvin model,σ = E2 ε2 + η2 ε2*η2 ε2* = σ - E2 ε2ε2* = 1/ η2 (σ – E2ε2)

three parameter linear solid model

Page 22: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 22

Standard Linear Solid cont’d

for a series combination of linear solid,ε = ε1 + ε2strain rate ε* = ε1* + ε2*ε* = σ*/E1 + 1/ η2 (σ – E2ε2)

Page 23: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 23

Three parameter Viscous model

For a dashpotσ = η ε*ε1* = σ/ η1For the Kelvin model,σ = E2 ε2 + η2 ε2*η2 ε2* = σ - E2 ε2ε2* = 1/ η2 (σ – E2ε2)

three parameter viscous model

Page 24: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 24

Three parameter Viscous model cont’d

for a series combination of the viscous model,ε = ε1 + ε2strain rate ε* = ε1* + ε2*ε* = σ/ η 1 + 1/ η2 (σ – E2ε2) ε* = σ (1/ η 1 + 1/ η2) - E2ε2/ η2

Page 25: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 25

CONCLUSION

The study of the stress-strain analysis of viscoelastic materials helps us understand the procedure and the steps involved in determining the stress-strain relations for a whole bunch of different models.

This in time will prove to be useful in solving any kind of stress-strain analysis problems that exhibit the kind of behavior as discussed in this report.

Page 26: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 26

Homework problem

Determine the stress - strain equation for a four parameter model (four parameter model is a Maxwell and a Kelvin/Voight Model connected in series).

Page 27: MEEN 53301 Stress Analysis in Viscoelastic Materials MEEN 5330, Fall 2006 Presented by: SURESH KUMAR ANBALAGAN SAI PRASEN SOMSETTY VEERABHADRA REDDY KAJULURI

MEEN 5330 27

REFERENCES