Difference between revisions of "Isotropic Material"
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== Constitutive Law == | |||
This [[Material Models|MPM material]] (or [[FEA Material Models|FEA material]]) is a [[Material Models#Linear Elastic Small Strain Materials|small strain, linear elastic material]]. The components of stress are related to components of strain by | |||
| |||
<math>\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 [[Material Models|MPM material]] (or [[FEA Material Models|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 [[Material Models|MPM material]] (or [[FEA Material Models|FEA material]]) are: | |||
{| class="wikitable" | |||
|- | |||
! Property !! Description !! Units !! Default | |||
|- | |||
| E || Tensile modulus || [[ConsistentUnits Command#Legacy and Consistent Units|pressure units]] || none | |||
|- | |||
| G || Shear modulus || [[ConsistentUnits Command#Legacy and Consistent Units|pressure units]] || none | |||
|- | |||
| nu || Poisson's ratio || none || none | |||
|- | |||
| alpha || Thermal expansion coefficient || ppm/K || 40 | |||
|- | |||
| ([[Common Material Properties|other]]) || Properties common to all materials (but only allowed for MPM Calculations) || 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> 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> E = G\left({3\lambda + 2G \over \lambda + G}\right), \qquad G = G \qquad {\rm and} \qquad \nu = {\lambda\over 2(\lambda+G)}</math> | |||
or given K and ν: | |||
| |||
<math> 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 |
Latest revision as of 13:50, 2 June 2015
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 | pressure units | none |
G | Shear modulus | pressure units | none |
nu | Poisson's ratio | none | none |
alpha | Thermal expansion coefficient | ppm/K | 40 |
(other) | Properties common to all materials (but only allowed for MPM Calculations) | 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 \nu = {\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