The stress-strain relationship for an optimally elastic material that emerges from a strain energy density function is known as a hyperelastic or Green elastic material. A specific instance of a Cauchy elastic material is the hyperelastic material. For many materials, linear elastic models do not adequately capture the actual behaviour of the materials. Rubber, which has a non-linearly elastic, isotropic, and incompressible stress-strain relationship, is the most prevalent example of this type of material. It is possible to simulate the stress-strain behaviour of such materials using hyperelasticity. Unfilled, vulcanised elastomers frequently behave in a way that nearly resembles the hyperelastic ideal. The hyperelastic idealisation is also frequently used to simulate filled elastomers and biological tissues. The Neo-Hookean and Mooney-Rivlin solids, the first hyperelastic models, were created by Ronald Rivlin and Melvin Mooney. Since then, several more hyperelastic models have been created. The Arruda-Boyce model and the Ogden model are two more popular hyperelastic material models.
Ephraim Suhir
Portland State University, United States
Thomas J Webster
Interstellar Therapeutics, United States
Robert Buenker
University of Wuppertal, Germany
Will Skene
Montreal University, Canada
Valeriy A Buryachenko
Micromechanics & Composites LLC, United States
Anis Rahman
Applied Research & Photonics, Inc, United States
Will Skene
Montreal University, Canada
Robert Guidoin
Laval University, Canada
Robert Buenker
University of Wuppertal, Germany
Martin Krus
Fraunhofer Institute for Building Physics, GermanySubmit your abstract Today
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