paper

and its invariants in terms of and its invariants

arXiv:2004.10496 · doi:10.1007/s10659-020-09780-x

Abstract

We consider tensors for . In the case , it is desired to find the three principal invariants of in terms of the three principal invariants of . Equations connecting the and are obtained by taking determinants of the factorisation \[λ^2{\bf I}- {\bf C} = (λ{\bf I}- {\bf U}) (λ{\bf I}+ {\bf U})\] and comparing coefficients. On eliminating we obtain a quartic equation with coefficients depending solely on the whose largest root is . Similarly, we may obtain a quartic equation whose largest root is . For we find that is once again the largest root of a quartic equation and so all the are expressed in terms of the . Then and are expressed solely in terms of , as for . For we find, but do not exhibit, a twentieth degree polynomial of which is the largest root and which has four spurious zeros. We are unable to express the in terms of the for . Nevertheless, and are expressed in terms of powers of with coefficients now depending on the . For we find, but do not exhibit, a 32 degree polynomial which has largest root . Sixteen of these roots are relevant but the other 16, which we exhibit, are spurious. and are expressed in terms of powers of . The cases are discussed. Keywords: Continuum mechanics, polar decomposition, tensor square roots, principal invariants, cubic equations, quartic equations, equations of degree 16

19 pages, 0 figures. Journal of Elasticity (2020)

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