8.15.6. Formulation and Parameters for a Hyper Elastic Material

A hyper elastic material has four available models: NEO-HOOKIAN, ARRUDA-BOYCE, OGDEN and MOONEY-RIVLIN. The parameters for a hyper elastic material are shown in the figure and table below.

Figure 8.84: Properties of a hyper elastic material

Properties of a hyper elastic material

Figure 8.85: Properties of a hyper elastic material

ParameterSymbolDescriptionDimension (Range)
1. C10
Properties of a hyper elastic material
Use to set the elastic constant which corresponds to the Young's modulus for a linear material [NEO-HOOKIAN, MOONEY-RIVLIN].

Force/Length^2

(Real≥0)

2. D
Properties of a hyper elastic material
Use to set the incompressibility parameter to determine the penalty of a volume constraint. As this value becomes smaller, the volume constraint is tighter. When a flexible body with hyper elastic material is contacted with the other body, the Motion solver sometimes has a small step size. In this case, if this value is large, the step size can be increased [All Models].

N/A

(0<Real≤1)

3. Mu
Properties of a hyper elastic material

Use to set the elastic constant which corresponds to the shear modulus in a linear material [ARRUDA-BOYCE, OGDEN].

Note: Be careful not to confuse the material constant Properties of a hyper elastic material  with the initial shear modulus Properties of a hyper elastic material . The relationship between initial shear modulus Properties of a hyper elastic material , Properties of a hyper elastic material  and Properties of a hyper elastic material  is shown in the NEO-HOOKIAN and MOONEY-RIVLIN section of the Figure 8.86: Strain energy of a hyper elastic material.

Force/Length^2

(Real≥0)

4. Lambda
Properties of a hyper elastic material
Use to set the locking stretch [ARRUDA-BOYCE].

N/A

(Real)

5. ListN/AUse to show the material parameters. The maximum number of the parameter set is six [OGDEN].N/A
6. OperatorsN/AUse to add a parameter set, or modify or delete the selected set [OGDEN].N/A
7. Alpha
Properties of a hyper elastic material
Use to set the elastic constant [OGDEN].

N/A

(Real)

8. C01
Properties of a hyper elastic material
Use to set the 2nd elastic constant which corresponds to the Young's modulus in a linear material [MOONEY-RIVLIN].

Force/Length^2

(Real≥0)


As with Equation 8–74, the strain energy of a hyper elastic material can be expressed as shown in the table below with the parameters as described in the table above.

Figure 8.86: Strain energy of a hyper elastic material

ModelFormulations
NEO-HOOKIAN

Strain energy of a hyper elastic material

where Strain energy of a hyper elastic material  is the volume strain and Strain energy of a hyper elastic material  can be calculated with the invariant of the Cauchy-Green deformation tensor Strain energy of a hyper elastic material  as follows.

Strain energy of a hyper elastic material

The relationship between Initial Shear Modulus Strain energy of a hyper elastic material  and Strain energy of a hyper elastic material  is as follows.

Strain energy of a hyper elastic material

ARRUDA-BOYCE

Strain energy of a hyper elastic material

where Strain energy of a hyper elastic material  is defined in the formulation for NEO-HOOKIAN.

OGDEN

Strain energy of a hyper elastic material

where Strain energy of a hyper elastic material  can be calculated with the eigenvalue of the Cauchy-Green deformation tensor of Strain energy of a hyper elastic material  as follows.

Strain energy of a hyper elastic material

In the equation for strain energy shown above, the terms for Strain energy of a hyper elastic material  and Strain energy of a hyper elastic material  can be expressed as follows using Strain energy of a hyper elastic material  and Strain energy of a hyper elastic material.

Strain energy of a hyper elastic material

In the form of the above formula, the following relationship is established.

Strain energy of a hyper elastic material

MOONEY-RIVLIN

Strain energy of a hyper elastic material

where Strain energy of a hyper elastic material  is defined in the formulation for NEO-HOOKIAN.

The relationship between Initial Shear Modulus Strain energy of a hyper elastic material, Strain energy of a hyper elastic material. and Strain energy of a hyper elastic material is as follows.

Strain energy of a hyper elastic material