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/MAT/LAW79 - Johnson-Holmquist Model [1][]
Description
This material law describes the behavior of brittle materials, such as ceramics and glass. The implementation is the second Johnson Holmquist model: JH-2
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#RADIOSS STARTER #---1----|----2----|----3----|----4----|----5----|----6----|----7----|----8----|----9----|---10----| /UNIT/1 unit for mat g mm ms #---1----|----2----|----3----|----4----|----5----|----6----|----7----|----8----|----9----|---10----| #- 2. MATERIALS: #---1----|----2----|----3----|----4----|----5----|----6----|----7----|----8----|----9----|---10----| /MAT/LAW79/1/1 concrete # RHO_I RHO_0 .0037 0 # G 90160 # a b m n .93 0 0 .6 # c EPS0 SIGMA_FMAX 0 .001 1E-30 # T HEL PHEL 200 2790 1460 # D1 D2 0 0 # K1 K2 K3 BETA 130950 0 0 1 #---1----|----2----|----3----|----4----|----5----|----6----|----7----|----8----|----9----|---10----| #ENDDATA /END #---1----|----2----|----3----|----4----|----5----|----6----|----7----|----8----|----9----|---10----| |
with the equivalent stress of the intact material: and the equivalent stress of the failed material: Stress are normalized to the stress at the Hugoniot elastic limit: and pressure are normalized to PHEL: where, the plastic strain to failure is: where, the bulking pressure is computed as a function of the elastic energy loss converted into potential hydrostatic energy:
USR3: Damage D USR4: Bulking Pressure USR5: Yield Stress |