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 |
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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 |