Abstract
In the representation theorem for the stored energy function of a hyperelastic material, it is necessary to determine a subgroup g*1 of the symmetry group g of the stress tensor. It is the purpose of this note to study the construction of g*1 and its relation to the other subgroups ot g, viz. the commutator subgroup gc and the orthogonal subgroup g0.
| Original language | English |
|---|---|
| Pages (from-to) | 677-681 |
| Number of pages | 5 |
| Journal | International Journal of Non-Linear Mechanics |
| Volume | 6 |
| Issue number | 6 |
| DOIs | |
| Publication status | Published - Dec 1971 |
| Externally published | Yes |