In continuum mechanics, a Mooney–Rivlin solid is a hyperelastic material model where the strain energy density function W {\displaystyle W\,} is a linear combination of two invariants of the left Cauchy–Green deformation tensor B {\displaystyle {\boldsymbol {B}}} . The model was proposed by Melvin Mooney in 1940 and expressed in terms of invariants by Ronald Rivlin in 1948.
In continuum mechanics, a Mooney–Rivlin solid is a hyperelastic material model where the strain energy density function W {\displaystyle W\,} is a linear combination of two invariants of the left Cauchy–Green deformation tensor B {\displaystyle {\boldsymbol {B}}} . The model was proposed by Melvin Mooney in 1940 and expressed in terms of invariants by Ronald Rivlin in 1948.
Source: Wikipedia "Mooney–Rivlin solid" · CC BY-SA 4.0
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