OOF2: The Manual

Name

IsotropicRank4Tensor — Representations of an isotropic 4th rank tensor.

Subclasses

Subclasses are listed as they appear in the GUI and (in parentheses) as they appear in scripts.

Description

The IsotropicRank4Tensor represents rank 4 tensor properties which are rotationally invariant, such as isotropic elasticity. The isotropic rank 4 tensor has two independent components, as shown in Figure 6.62. Because the elasticity literature uses many different representations of these two components, OOF2 allows you to enter the tensor in a variety of formats. The OOF2 GUI allows you to easily convert from one tensor format to another, as shown in Figure 6.64

[Note] Note

The word rank has different meanings in different fields. Here it means the number of indices on a tensor. Cijkl is a rank 4 tensor.

Figure 6.62. Structure of an Isotropic Fourth Rank Tensor

Isotropic rank 4 tensor diagram

Structure of an isotropic rank 4 tensor. For an explanation of the symbols, see Figure 6.63.


Figure 6.63. Key to the Tensor Diagrams

Key to the Tensor Diagrams

Symbols used in the tensor diagrams. The symmetries of symmetric fourth rank tensors, Cijkl , allow them to be displayed as second rank tensors, CIK , where I is the Voigt notation for ij and K is the Voigt notation for kl . To keep things simple(?), the diagrams use Voigt notation for the columns and ij notation for the rows.


Figure 6.64. Converting Between Isotropic Tensor Representations

Converting Between Isotropic Tensor Representations

(a) The dialog box for setting the elastic modulus of a material with isotropic elasticity. The menu at the top of the box shows that the Cij representation is being used.

(b) After selecting Lame in the pull-down menu …

(c) … the same modulus is now given in Lamé coefficients. The values can be edited in either representation, or any of the others.