The material is assumed to have three orthogonal planes of symmetry. Assuming the material coordinate system is perpendicular to these planes of symmetry, the Hill yield criterion reads [Hill, 1983]
(3–59) |
where is the equivalent (also called effective) stress
(3–60) |
and is the yield stress that can, in general, evolve as a function of some material internal variables. (See Isotropic Hardening below.)
The equivalent stress can likewise be expressed in matrix form as
(3–61) |
where the plastic compliance matrix is given by
(3–62) |
The coefficients in this yield criterion are defined as
(3–63) |
The directional yield ratios are related to the isotropic yield stress parameter by
(3–64) |