Difference between revisions of "Tait Liquid Material"
Line 60: | Line 60: | ||
<rho>1</rho> | <rho>1</rho> | ||
<Cv>418.13</Cv> | <Cv>418.13</Cv> | ||
<kCond>0</kCond> | <kCond>0.58</kCond> | ||
</Material> | </Material> |
Revision as of 17:16, 30 December 2013
Constitutive Law
This MPM material as a hyperelastic material. The pressure in the liquid is found from the Tait equation:
[math]\displaystyle{ V(p,T) = V(0,T)\left[1 - C \ln\left(1+{p\over B(T)}\right)\right] }[/math]
where C = 0.0894 is a universal Tait constant, V(0,T) is the temperature dependence of the volume at zero pressure, and
[math]\displaystyle{ B(T) = { K(0,T)\over C } }[/math]
where K(0,T) is the temperature dependence of the bulk modulus at zero pressure. Defining J as relative volume (i.e., determinant of total deformation gradient) and Jres as determinant of deformation gradient due to free thermal expansion, or:
[math]\displaystyle{ J = {V(p,T)\over V(0,T_0)} \qquad {\rm and} \qquad J_{res} = {V(0,T)\over V(0,T_0)} = e^{\beta(0)(T-T_0)} }[/math]
where T0 is the stress free temperature and β0 is the zero-pressure thermal expansion coefficient (which has been assumed to be independent of temperature), the constitutive law for pressure is:
[math]\displaystyle{ p = CK_0\left[\exp\left({1\over C}\left(1 - {J\over J_{res}}\right)\right)-1\right] }[/math]
Here the zero-pressure bulk modulus is K0. and it has been assumed to be independent of temperature.
This material is assume to be a Newtonian fluid, which means that the shear stress is given by
[math]\displaystyle{ \tau = \gamma \nabla \mathbf{v} }[/math]
where [math]\displaystyle{ \nabla \mathbf{v} }[/math] is the velocity gradient. The total stress is given by [math]\displaystyle{ \mathbf{\sigma} = -p \mathbf{I} + \tau }[/math]
Material Properties
The properties for a Tait liquid are:
Property | Description | Units | Default |
---|---|---|---|
K | Zero-pressure, bulk modulus | MPa | none |
viscosity | Liquid viscosity | cP | none |
alpha | Linear thermal expansion coefficient (&beta0 = 2 α) | ppm/K | 0 |
(other) | Properties common to all materials | varies | varies |
History Variables
This material uses history #1 to store the volumetric strain (i.e., the determinant of the deformation gradient).
Examples
The following commands are for water.
<Material Type="27" Name="Water"> <K>.015</K> <viscosity>500</viscosity> <alpha>70</alpha> <rho>1</rho> <Cv>418.13</Cv> <kCond>0.58</kCond> </Material>