Difference between revisions of "Isotropic, Hyperelastic-Plastic Material"
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| UJOption || Set to 0, 1, or 2, to select the energy term from [[#Constitutive Law|above]]. || none || 0 | | UJOption || Set to 0, 1, or 2, to select the energy term from [[#Constitutive Law|above]]. || none || 0 | ||
|- | |- | ||
| alpha || Thermal expansion coefficient || ppm/ | | alpha || Thermal expansion coefficient || ppm/K || 0 | ||
|- | |- | ||
| Hardening || This command selects the [[Hardening Laws|hardening law]] by its name or number. It should be before entering any yielding properties. || none || none | | Hardening || This command selects the [[Hardening Laws|hardening law]] by its name or number. It should be before entering any yielding properties. || none || none | ||
Revision as of 07:53, 12 March 2015
Constitutive Law
This MPM Material is an isotropic, elastic-plastic material in large strains using a hyperelastic formulation. The elastic regime for this material is identical to a Mooney except that it only allows a Neohookean elastic regime (with G = G1 and G2 = 0).,
The formulation of finite strain plasticity is based on the notion of a stress free intermediate configuration and uses a multiplicative decomposition of the deformation gradient F given by:
[math]\displaystyle{ \mathbf{F} = \mathbf{F}_{e}. \mathbf{F}_{p} }[/math]
Where Fe and Fp are the elastic and plastic deformation gradient tensors respectively, with det (Fp), that supposes the plastic flow to be isochoric. The Neo-Hookean elastic stored energy, represented by its uncoupled volumetric-deviatoric internal energy form, is consistent with the fundamental idea that the elastic-plastic deviatoric response is assumed to be uncoupled from the elastic volumetric response
In finite strain plasticity, the stored energy is based on the additive decomposition of the stored energy into elastic We and plastic Fp internal energies. The elastic stored energy is related to the intermediate configuration and the plastic stored energy is expressed in term of plastic state variables α.
[math]\displaystyle{ W =W_{e} (\mathbf{B}_{e}) + W_{p} (\alpha) }[/math]
The stored Neo-Hookean stored energy, We, is identical to the Mooney Energy W and dependent on entered small-strain, bulk modulus (κ), small-strain, shear modulus (G = G1), and dilation energy option (UJOption). The value of G2 is always zero in this material.
In associative plasticity, the plastic storage energy is represented by the plastic flow condition. The plastic flow model considered here is isotropic hardening. It is handled by any hardening law available in the code (see Hardening Laws). The associative flow rate is defined by the principle of maximum plastic dissipation.[1][2] It is given, in the present context, by:
[math]\displaystyle{ L_{v} \mathbf{B}^e = \mathbf{F} {\delta\over t} (\mathbf{\bar C}{^{p-1}}) \mathbf{F^T} = - {2\over 3} {\gamma} {\rm Tr}(\mathbf{B}_{e})\mathbf{n} \qquad {\rm with} \qquad \mathbf{n} = {\mathbf{\tau^{d}}\over ||\mathbf{\tau^{d}}||} }[/math]
Where Lv is the Lie derivative of the deviatoric part of the elastic left Cauchy-Green strain tensor [math]\displaystyle{ \bigl(\mathbf{\bar B}_{e}\bigr) }[/math]. It represents the plastic strain rate that is a tensor normal to the yield surface in the stress space; n is a normal to the yield surface and γ is the consistency parameter also called the plastic multiplicator. In addition, a isotropic hardening law is needed. It is represented by the rate equation, as in the linear theory:
[math]\displaystyle{ {d {\alpha}\over dt } ={\gamma} \sqrt{2\over3} }[/math]
Material Properties
The material properties are set using
| Property | Description | Units | Default |
|---|---|---|---|
| K | Low-strain bulk modulus | MPa | none |
| G1 (or G) | Low-strain shear modulus | MPa | none |
| UJOption | Set to 0, 1, or 2, to select the energy term from above. | none | 0 |
| alpha | Thermal expansion coefficient | ppm/K | 0 |
| Hardening | This command selects the hardening law by its name or number. It should be before entering any yielding properties. | none | none |
| (yield) | Enter all plasticity properties required by the selected hardening law. | varies | varies |
| (other) | Properties common to all materials | varies | varies |
See these relations to covert other properties (such as modulus and Poisson's ratio) to bulk and shear moduli.
History Variables
The selected hardening law will create one or more history variables. This material uses the next history variable (after the hardening laws history variables) to store the volumetric change (i.e., J or the determinant of the deformation gradient). The total strain is stored in the elastic strain variable, while the plastic strain stores the elastic left Cauchy Green tensor.
Examples
These commands model a polymer as an isotropic hyperelastic-plastic material with a particular linear isotropic hardening:
Material "polymer","polymer","HEIsotropic" K 5000 G1 1100 alpha 60 rho 1.2 yield 72 Ep 1000 Done
References
- ↑ J. C. Simo, "Framework for finite elastoplasticity. Part I", Computer Methods in Applied Mechanics and Engineering, 66, 199-219 (1988).
- ↑ J. C. Simo, "Framework for finite elastoplasticity based on maximum dissipated energy and the multiplicative decomposition. Part II: Computational aspects", Computer Methods in Applied Mechanics and Engineering, 68, 1-31 (1988)