Strain energy density function
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A strain energy density function or stored energy density function is a scalar valued function that relates the strain energy density of a material to the deformation gradient.
where
is the (two-point) deformation gradient tensor,
is the right Cauchy-Green deformation tensor, and
is the left Cauchy-Green deformation tensor [1][2].
For an isotropic material, the deformation gradient can be expressed uniquely in terms of the principal stretches or in terms of the invariants of the left Cauchy-Green deformation tensor or right Cauchy-Green deformation tensor and we have
with
A strain energy density function is used to define a hyperelastic material by postulating that the stress in the material can be obtained by taking the derivative of
with respect to the strain. For an isotropic, hyperelastic material the function relates the energy stored in an elastic material, and thus the stress-strain relationship, only to the three strain (elongation) components, thus disregarding the deformation history, heat dissipation, stress relaxation etc.
The strain energy density function relates to the Helmholtz free energy function
[3],
[edit] Examples of strain energy density functions
Some examples of hyperelastic constitutive equations are
- Saint Venant–Kirchhoff
- Neo-Hookean
- Generalized Rivlin
- Mooney–Rivlin
- Ogden
- Yeoh
- Arruda–Boyce model
- Gent
[edit] References
- ^ Bower, Allan (2009). Applied Mechanics of Solids. CRC Press. ISBN 1439802472. http://solidmechanics.org/. Retrieved January 2010.
- ^ Ogden, R. W. (1998). Nonlinear Elastic Deformations. Dover. ISBN 0486696480.
- ^ Wriggers, P. (2008). Nonlinear Finite Element Methods. Springer-Verlag. ISBN 978-3-540-71000-4.
[edit] See also
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