Within the framework of hyperelastic materials, the polar decomposition theorem of Trusdell and Noll* occupies a position of primary importance. The polar decomposition theorem states that any deformation gradient tensor can be multiplicatively decomposed into the product of an orthogonal tensor, known as the rotation tensor, and a symmetric tensor called the right stretch tensor, or into the product of a symmetric tensor called the left stretch tensor and the same rotation tensor. The rotation tensor is a two-point Eulerian-Lagrangian second-order tensor, the right stretch tensor is a Lagrangian single-based second-order tensor and the left stretch tensor is single-order and Eulerian based. The relationship between right and left stretch tensors is derived through eigenvalue extraction. The polar decomposition theorem is the principal tool for studying finite deformations and the corresponding strains. The detailed formulation of the polar decomposition theorem is presented in terms of the right Cauchy-Green deformation tensor. A detailed numerical example is presented to demonstrate the polar decomposition theorem.
KeywordsPolar decomposition Deformation gradient Stretch tensors Rotation tensor Multiplicative decomposition Eigenvalue Numerical example
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