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Phenomenological modeling of viscous
electrostrictive polymers
L. Harish (AM13D025)
Group meeting
 Polymers which respond mechanically to electrical input are
termed as electro active polymers(EAPs)
 Large electric field leads to couloumb forces and it termed as
maxwell effect
Introduction
 Electrostatic itself is not enough but also to include the viscosity
of the polymer to consider time dependent effects.
 Large electric field leads to couloumb forces and it termed as
maxwell effect.
Introduction
 It is an electro-viscoelastic coupled problem including
electrostriction and time dependence present in PUelastomers.
 It is assumed that the viscosity is related to the deformation of the
body but not directly to the electromagnetic field quantities.
 Electric loading will make the body deform and there by induces
the viscous deformation.
 Viscoelastic modeling will be based on a multiplicative split of the
deformation. And additive split of the longterm and non-
equilibrium viscous contributions of free energy.
Introduction
 Deformation gradient is multiplicatively split into its volumetric and isochoric
parts
Deformation Tensors
 Consider electro static case
Electromagnetic field quantities
 The electric field and displacements are governed by Maxwell’s equations.
Governing equations
 Material can be described by an energy function and free energy function can
be split into separate contributions.
Constitutive framework
Constitutive models: Energy expressions
 Electric displacements:
Total stresses
Viscosity driving stresses
Mandel type referential stress tensor:
Referential viscous piola Kirchhoff type stresses:
Viscosity driving stresses
Evolution Equations
 Mandel type stresses can conveniently be used to formulate a
thermodynamically consistent model.
 The format of evolution law considered here resembles an approach commonly
used in time dependent plasticity theories.
 Considered function or rather potential:
Evolution Equations
Application to PU elastomer
 For viscous strains the power law type evolution law as well as the Bonet
model are used.
 A good fit to the experimental data can be found by using two viscosity
elements and k=1
Application to PU elastomer
 For viscous strains the power law type evolution law as well as the Bonet
model are used.
Application to PU elastomer
Application to PU elastomer
Application to PU elastomer
Application to PU elastomer

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Phenomenologicalmodelingofviscouselectrostrictivepolymers

  • 1. Phenomenological modeling of viscous electrostrictive polymers L. Harish (AM13D025) Group meeting
  • 2.  Polymers which respond mechanically to electrical input are termed as electro active polymers(EAPs)  Large electric field leads to couloumb forces and it termed as maxwell effect Introduction
  • 3.  Electrostatic itself is not enough but also to include the viscosity of the polymer to consider time dependent effects.  Large electric field leads to couloumb forces and it termed as maxwell effect. Introduction
  • 4.  It is an electro-viscoelastic coupled problem including electrostriction and time dependence present in PUelastomers.  It is assumed that the viscosity is related to the deformation of the body but not directly to the electromagnetic field quantities.  Electric loading will make the body deform and there by induces the viscous deformation.  Viscoelastic modeling will be based on a multiplicative split of the deformation. And additive split of the longterm and non- equilibrium viscous contributions of free energy. Introduction
  • 5.  Deformation gradient is multiplicatively split into its volumetric and isochoric parts Deformation Tensors
  • 6.  Consider electro static case Electromagnetic field quantities
  • 7.  The electric field and displacements are governed by Maxwell’s equations. Governing equations
  • 8.  Material can be described by an energy function and free energy function can be split into separate contributions. Constitutive framework
  • 9. Constitutive models: Energy expressions  Electric displacements:
  • 11. Viscosity driving stresses Mandel type referential stress tensor: Referential viscous piola Kirchhoff type stresses:
  • 13. Evolution Equations  Mandel type stresses can conveniently be used to formulate a thermodynamically consistent model.  The format of evolution law considered here resembles an approach commonly used in time dependent plasticity theories.  Considered function or rather potential:
  • 15. Application to PU elastomer  For viscous strains the power law type evolution law as well as the Bonet model are used.  A good fit to the experimental data can be found by using two viscosity elements and k=1
  • 16. Application to PU elastomer  For viscous strains the power law type evolution law as well as the Bonet model are used.
  • 17. Application to PU elastomer
  • 18. Application to PU elastomer
  • 19. Application to PU elastomer
  • 20. Application to PU elastomer