Explicit representation for the \(\mathrm{SO}(3)\) rotation tensor of deformable bodies
From MaRDI portal
Publication:2006310
DOI10.1016/j.aml.2020.106606OpenAlexW3037299446MaRDI QIDQ2006310
Publication date: 8 October 2020
Published in: Applied Mathematics Letters (Search for Journal in Brave)
Full work available at URL: https://doi.org/10.1016/j.aml.2020.106606
Vector and tensor algebra, theory of invariants (15A72) Nonlinear elasticity (74B20) Kinematics of deformation (74A05) Theory of constitutive functions in solid mechanics (74A20) Generalities, axiomatics, foundations of continuum mechanics of solids (74A99)
Related Items (1)
Uses Software
Cites Work
- Unnamed Item
- Unnamed Item
- Determination of \(C^{1/2}\), \(C^{-1/2}\) and more general isotropic tensor functions of C
- Determination of the rotation tensor in the polar decomposition
- Determination of the stretch and rotation in the polar decomposition of the deformation gradient
- On the Direct Determination of the Rotation Tensor from the Deformation Gradient
- Direct determination of the rotation in the polar decomposition of the deformation gradient by maximizing a Rayleigh quotient
- Elasticity with MATHEMATICA®
This page was built for publication: Explicit representation for the \(\mathrm{SO}(3)\) rotation tensor of deformable bodies