Abstract
We consider \(N\times N\) tensors for \(N= 3,4,5,6\). In the case \(N=3\), it is desired to find the three principal invariants \(i_{1}, i_{2}, i_{3}\) of \({\mathbf{U}}\) in terms of the three principal invariants \(I_{1}, I_{2}, I_{3}\) of \({\mathbf{C}}={\mathbf{U}}^{2}\). Equations connecting the \(i_{\alpha }\) and \(I_{\alpha }\) are obtained by taking determinants of the factorisation
and comparing coefficients. On eliminating \(i_{2}\) we obtain a quartic equation with coefficients depending solely on the \(I_{\alpha }\) whose largest root is \(i_{1}\). Similarly, we may obtain a quartic equation whose largest root is \(i_{2}\). For \(N=4\) we find that \(i_{2}\) is once again the largest root of a quartic equation and so all the \(i_{\alpha }\) are expressed in terms of the \(I_{\alpha }\). Then \({\mathbf{U}}\) and \({\mathbf{U}}^{-1}\) are expressed solely in terms of \({\mathbf{C}}\), as for \(N=3\). For \(N= 5\) we find, but do not exhibit, a twentieth degree polynomial of which \(i_{1}\) is the largest root and which has four spurious zeros. We are unable to express the \(i_{\alpha }\) in terms of the \(I_{\alpha }\) for \(N=5\). Nevertheless, \({\mathbf{U}}\) and \({\mathbf{U}}^{-1}\) are expressed in terms of powers of \({\mathbf{C}}\) with coefficients now depending on the \(i_{\alpha }\). For \(N=6\) we find, but do not exhibit, a 32 degree polynomial which has largest root \(i_{1}^{2}\). Sixteen of these roots are relevant, which we exhibit, but the other 16 are spurious. \({\mathbf{U}}\) and \({\mathbf{U}}^{-1}\) are expressed in terms of powers of \({\mathbf{C}}\). The cases \(N>6\) are discussed.
References
Bouby, C., Fortune, D., Pietraszkiewicz, W., Vallée, C.: Direct determination of the rotation in the polar decomposition of the deformation gradient by maximizing a Rayleigh quotient. Z. Angew. Math. Mech. 85, 155–162 (2005)
Carroll, M.M.: Derivatives of the rotation and stretch tensors. Math. Mech. Solids 9, 543–553 (2004)
Fitzgerald, T.: Nonlinear fluid-structure interactions in flapping wing systems. PhD Thesis, University of Maryland, College Park, USA (2013)
Franca, L.P.: An algorithm to compute the square root of a \(3\times 3\) positive definite matrix. Comput. Math. Appl. 18, 459–466 (1989)
Hoger, A., Carlson, D.E.: Determination of the stretch and rotation in the polar decomposition of the deformation gradient. Q. Appl. Math. XLII, 113–117 (1984)
Jog, C.S.: On the explicit determination of the polar decomposition in \(n\)-dimensional vector spaces. J. Elast. 66, 159–169 (2002)
Luehr, C.P., Rubin, M.B.: The significance of projection operators in the spectral representation of symmetric second order tensors. Comput. Methods Appl. Mech. Eng. 84, 243–246 (1990)
Norris, A.N.: Invariants of \({\mathbf{C}}^{1/2}\) in terms of the invariants of \({\mathbf{C}}\). J. Mech. Mater. Struct. 2, 1805–1812 (2007)
Sawyers, K.: Comments on the paper determination of the stretch and rotation in the polar decomposition of the deformation gradient by A. Hoger and D.E. Carlson. Q. Appl. Math. XLIV, 309–311 (1986)
Ting, T.C.T.: Determination of \({\mathbf{C}}^{1/2}\), \({\mathbf{C}}^{-1/2}\) and more general isotropic tensor functions of \({\mathbf{C}}\). J. Elast. 15, 319–323 (1985)
Author information
Authors and Affiliations
Corresponding author
Additional information
Publisher’s Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Rights and permissions
About this article
Cite this article
Scott, N.H. \({\mathbf{U}} = \mathbf{C}^{1/2}\) and Its Invariants in Terms of \(\mathbf{C}\) and Its Invariants. J Elast 141, 363–379 (2020). https://doi.org/10.1007/s10659-020-09780-x
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s10659-020-09780-x
Keywords
- Continuum mechanics
- Polar decomposition
- Tensor square roots
- Principal invariants
- Cubic equations
- Quartic equations
- Equations of degree 16