Hyperfoam Options

You can create a hyperfoam material model to describe a cellular solid whose porosity permits very large volumetric changes.

In the elastomeric foam (hyperfoam) material model the elastic behavior of the foams is based on the strain energy function.

U=i=1N2μiαi2[λ^1αi+λ^2αi+λ^3αi3+1βi((Jel)αiβi1)],

where N is a material parameter; μi, αi, and βi are temperature-dependent material parameters;

λ^i=(Jth)13λi       λ^1λ^2λ^3=Jel;

and λi are the principal stretches. The elastic volume ratio, Jel, relates the total volume ratio (current volume/reference volume), J, and the thermal volume ratio, Jth:

Jel = JJth.

Jth is given by

Jth = (1+εth)3,

where εth is the linear thermal expansion strain that is obtained from the temperature and the isotropic thermal expansion coefficient.

The coefficients μi are related to the initial shear modulus, μ0, by:

μ0 = i=1Nμi,

where the initial bulk modulus, Κ0, follows from

Κ0 = i=1N2μi(13+βi).

For each term in the energy function, the coefficient βi determines the degree of compressibility. βi is related to the Poisson's ratio, νi, by the expressions

βi = (νi12νi),νi = (βi1+2βi).

Thus, if βi is the same for all terms, we have a single effective Poisson's ratio, ν. This Poisson's ratio is valid for finite values of the logarithmic principal strains ε1,ε2,ε3; in uniaxial tension ε2=ε3=νε1.

Input DataDescription
Strain energy potential orderNumeric order, N.
mu1μ1
alpha1α1
nu1ν1
Use temperature-dependent dataSpecify material parameters that depend on temperature. A Temperature field appears in the data table.
Moduli time scaleSelect Instantaneous or Long Term for the application of viscoelastic effects.