Difference between revisions of "Isotropic Material"
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== Material Properties == | == Material Properties == | ||
Although an isotropic [[Material Models|material]] can be defined any two of λ, K, G, E, and ν, the only properties allowed for defining this material are E and ν. | Although an isotropic [[Material Models|material]] can be defined any two of λ, K, G, E, and ν, the only properties allowed for defining this material are E and ν. Those two and other properties are: | ||
== History Data == | == History Data == | ||
None | None | ||
Revision as of 13:11, 27 March 2013
This material is a small strain, linear elastic material. The components stress are related to components of strain by
[math]\displaystyle{ \sigma_{ij} = \bigl(\lambda\varepsilon_{ii} - 3K(\alpha \Delta T+\beta c)\bigr)\delta_{ij} + 2G\varepsilon_{ij} }[/math]
where λ is the Lame, K is bulk modulus, α is thermal expansion coefficient, ΔT is temperature difference, β is solvent expansion coefficient, c is solvent concentration, and G is shear modulus. Two other isotropic material properties are modulus, E, and Poisson's ratio, ν.
Material Properties
Although an isotropic material can be defined any two of λ, K, G, E, and ν, the only properties allowed for defining this material are E and ν. Those two and other properties are:
History Data
None