Corrected HomogenisedC:
1- No dependence on material volume fractions!!! 2- Can now depend on state of microstructure changed some loops from Nstatevars to Nslip
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@ -735,10 +735,11 @@ enddo
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end subroutine
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function constitutive_HomogenizedC(ipc,ip,el)
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function constitutive_HomogenizedC(state,ipc,ip,el)
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!*********************************************************************
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!* This function returns the homogenized elacticity matrix *
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!* INPUT: *
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!* - state : state variables *
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!* - ipc : component-ID of current integration point *
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!* - ip : current integration point *
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!* - el : current element *
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@ -751,7 +752,7 @@ integer(pInt) ipc,ip,el
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real(pReal), dimension(6,6) :: constitutive_homogenizedC
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!* Homogenization scheme
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constitutive_homogenizedC=constitutive_MatVolFrac(ipc,ip,el)*material_Cslip_66(:,:,constitutive_matID(ipc,ip,el))
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constitutive_homogenizedC=material_Cslip_66(:,:,constitutive_matID(ipc,ip,el))
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return
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end function
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@ -837,6 +838,8 @@ do i=1,material_Nslip(matID)
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Lp=Lp+gdot_slip(i)*crystal_Sslip(:,:,i,material_CrystalStructure(matID))
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enddo
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!* Lp twin
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!* Calculation of the tangent of Lp
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dLp_dTstar=0.0_pReal
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do i=1,material_Nslip(matID)
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@ -857,7 +860,7 @@ end subroutine
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function constitutive_dotState(Tstar_v,state,Tp,ipc,ip,el)
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!*********************************************************************
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!* This subroutine contains the constitutive equation for *
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!* calculating the velocity gradient *
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!* calculating rate of change of microstructure *
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!* INPUT: *
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!* - Tstar_v : 2nd Piola Kirchhoff stress tensor (Mandel) *
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!* - state : current microstructure *
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@ -875,21 +878,21 @@ implicit none
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!* Definition of variables
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integer(pInt) ipc,ip,el
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integer(pInt) matID,i
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real(pReal) Tp,tau_slip,gdot_slip
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real(pReal) Tp,tau_slip,gdot_slip,lock,recovery
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real(pReal), dimension(6) :: Tstar_v
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real(pReal), dimension(constitutive_Nstatevars(ipc,ip,el)) :: constitutive_dotState,state,lock,recovery
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real(pReal), dimension(constitutive_Nstatevars(ipc,ip,el)) :: constitutive_dotState,state
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!* Get the material-ID from the triplet(ipc,ip,el)
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matID = constitutive_matID(ipc,ip,el)
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!* Hardening of each system
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do i=1,constitutive_Nstatevars(ipc,ip,el)
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do i=1,material_Nslip(matID)
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tau_slip = dot_product(Tstar_v,crystal_Sslip_v(:,i,material_CrystalStructure(matID)))
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gdot_slip = constitutive_g0_slip(i)*sinh((abs(tau_slip)*constitutive_activation_volume(i))/(Kb*Tp))*&
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sign(1.0_pReal,tau_slip)
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lock(i)=(material_c4(matID)*sqrt(constitutive_rho_f(i))*abs(gdot_slip))/material_bg(matID)
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recovery(i)=material_c5(matID)*state(i)*abs(gdot_slip)
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constitutive_dotState(i)=lock(i)-recovery(i)
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lock=(material_c4(matID)*sqrt(constitutive_rho_f(i))*abs(gdot_slip))/material_bg(matID)
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recovery=material_c5(matID)*state(i)*abs(gdot_slip)
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constitutive_dotState(i)=lock-recovery
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enddo
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return
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