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Hyperelastic bodies

The same modification is necessary when dealing in general with incompressible hyperelastic bodies. Introducing the additional term in Finger s constitutive equation, Eq. (7.63), and regarding the absence of Ills we obtain... [Pg.318]

In the following we analyze some elementary problems in which the deformation is homogeneous, i.e. the deformation gradient F is constant in whole body. Homogeneous deformations are equilibrium solution for all the class of hyperelastic materials for this reason they are called universal solutions [116]. [Pg.235]

See other pages where Hyperelastic bodies is mentioned: [Pg.242]    [Pg.315]    [Pg.332]    [Pg.332]    [Pg.376]    [Pg.398]    [Pg.398]    [Pg.242]    [Pg.315]    [Pg.332]    [Pg.332]    [Pg.376]    [Pg.398]    [Pg.398]    [Pg.45]    [Pg.174]    [Pg.107]    [Pg.228]    [Pg.716]    [Pg.720]   
See also in sourсe #XX -- [ Pg.315 ]

See also in sourсe #XX -- [ Pg.376 ]



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Hyperelasticity

Incompressible hyperelastic bodies

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