constitutive law for j2 pasticity again corrected, dotState didn't need the factor of sqrt(1.5)
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@ -343,11 +343,11 @@ function constitutive_j2_dotState(Tstar_v,Temperature,state,ipc,ip,el)
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matID = phase_constitutionInstance(material_phase(ipc,ip,el))
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norm_Tstar = dsqrt(math_mul6x6(Tstar_v,Tstar_v))
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constitutive_j2_dotState = dsqrt(1.5_pReal)*constitutive_j2_gdot0(matID)/constitutive_j2_fTaylor(matID)* &
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constitutive_j2_dotState = constitutive_j2_h0(matID)*(1.0_pReal-state(ipc,ip,el)%p(1)/constitutive_j2_s_sat(matID))** &
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constitutive_j2_w0(matID) * &
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constitutive_j2_gdot0(matID)/constitutive_j2_fTaylor(matID)* &
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(dsqrt(1.5_pReal)/constitutive_j2_fTaylor(matID)*norm_Tstar/state(ipc,ip,el)%p(1))** &
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constitutive_j2_n(matID) * &
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constitutive_j2_h0(matID)*(1.0_pReal-state(ipc,ip,el)%p(1)/constitutive_j2_s_sat(matID))** &
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constitutive_j2_w0(matID)
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constitutive_j2_n(matID)
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return
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@ -392,7 +392,7 @@ pure function constitutive_j2_postResults(Tstar_v,Temperature,dt,state,ipc,ip,el
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constitutive_j2_postResults(c+1) = state(ipc,ip,el)%p(1)
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c = c + 1
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case ('strainrate')
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constitutive_j2_postResults(c+1) = dsqrt(1.5_pReal)*constitutive_j2_gdot0(matID)/constitutive_j2_fTaylor(matID)* &
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constitutive_j2_postResults(c+1) = constitutive_j2_gdot0(matID)/constitutive_j2_fTaylor(matID)* &
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(dsqrt(1.5_pReal)/constitutive_j2_fTaylor(matID)*norm_Tstar/state(ipc,ip,el)%p(1))** &
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constitutive_j2_n(matID)
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c = c + 1
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