Difference between revisions of "Clamped Neo-Hookean Material"

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== Constitutive Law ==
== Constitutive Law ==


This  [[Material Models|MPM Material]] is an isotropic, elastic-plastic material in large strains using a hyperelastic formulation. The elastic part is a [[Neo-Hookean Material|neo-Hookean material]]. Plasticity occurs when the elongation in either tension of compression reaches a critical value. This material is based on similar material using in a paper to animate snow mechanics.
This  [[Material Models|MPM Material]] is an isotropic, elastic-plastic material in large strains using a hyperelastic formulation. The elastic part is a [[Neo-Hookean Material|neo-Hookean material]]. Plasticity occurs when the elongation in either tension of compression reaches a critical value. This material is based on similar material using in a paper to animate snow mechanics<ref>A. Stomakhin, C. Schroeder, L. Chai, J. Teran, and A. Selle, "A material point method for snow simulation," ACM Trans. Graph., Vol. 32, No. 4, Article 102, July 2013.</ref>.


== Material Properties ==
== Material Properties ==

Revision as of 12:44, 3 February 2015

Constitutive Law

This MPM Material is an isotropic, elastic-plastic material in large strains using a hyperelastic formulation. The elastic part is a neo-Hookean material. Plasticity occurs when the elongation in either tension of compression reaches a critical value. This material is based on similar material using in a paper to animate snow mechanics[1].

Material Properties

The material properties are given in the following table.

Property Description Units Default
CritComp Critical compression extension none 0.025
CritComp Critical tensile extension none 0.0075
Hardening Hardening coefficient none 10
(other) Properties to define underlying Neo-Hookean material varies varies
  1. A. Stomakhin, C. Schroeder, L. Chai, J. Teran, and A. Selle, "A material point method for snow simulation," ACM Trans. Graph., Vol. 32, No. 4, Article 102, July 2013.