Difference between revisions of "Isotropic Material"
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| alpha || Thermal expansion coefficient || ppm/M || 40 | | alpha || Thermal expansion coefficient || ppm/M || 40 | ||
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| ([[Common Material Properties|other]]) || Properties common to all materials || varies || varies | |||
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Other combinations are easily derived, but the above examples are the most common. | Other combinations are easily derived, but the above examples are the most common. | ||
== History Variables == | == History Variables == |
Revision as of 10:31, 6 January 2014
Constitutive Law
This MPM material (or FEA material) is a small strain, linear elastic material. The components of 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 coefficient, K is bulk modulus, α is thermal expansion coefficient, ΔT is temperature difference, β is solvent expansion coefficient (MPM only), c is solvent concentration (MPM only), and G is shear modulus. Two other isotropic material properties are modulus, E, and Poisson's ratio, ν.
Material Properties
Although deformation properties of an isotropic MPM material (or FEA material) can be defined by any two of λ, K, G, E, and ν, this material's properties can only be defined by specifying any two (and exactly two) of E, G, and ν. Those three and other properties for this isotropic MPM material (or FEA material) are:
Property | Description | Units | Default |
---|---|---|---|
E | Tensile modulus | MPa | none |
G | Shear modulus | MPa | none |
nu | Poisson's ratio | none | none |
alpha | Thermal expansion coefficient | ppm/M | 40 |
(other) | Properties common to all materials | varies | varies |
If you know K or λ instead of E, G, and ν, they are easily converted to E and ν. Given K and G:
[math]\displaystyle{ E = {9KG \over 3K+G} , \qquad G = G \qquad {\rm and} , \qquad \nu = {3K-2G\over 6K+2G} }[/math]
or given λ and G:
[math]\displaystyle{ E = G\left({3\lambda + 2G \over \lambda + G}\right), \qquad G = G \qquad {\rm and} \qquad {\lambda\over 2(\lambda+G)} }[/math]
or given K and ν:
[math]\displaystyle{ E = 3K(1-2\nu) , \qquad G ={ 3K(1-2\nu)\over 2(1+\nu)}, \qquad {\rm and} \qquad \nu = \nu }[/math]
Other combinations are easily derived, but the above examples are the most common.
History Variables
None
Examples
These commands model copper as an isotropic, elastic material (using scripted or XML commands):
Material "copper","Copper","Isotropic" E 120000 nu .34 alpha 16.5 rho 8.96 kCond 401 Cv 385 Done