modularizing
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@ -83,93 +83,6 @@ submodule(constitutive) constitutive_mech
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myPlasticity
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end function plastic_nonlocal_init
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module subroutine plastic_isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_isotropic_LpAndItsTangent
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pure module subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_phenopowerlaw_LpAndItsTangent
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pure module subroutine plastic_kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_kinehardening_LpAndItsTangent
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module subroutine plastic_dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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real(pReal), intent(in) :: &
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T
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_dislotwin_LpAndItsTangent
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pure module subroutine plastic_dislotungsten_LpAndItsTangent(Lp,dLp_dMp,Mp,T,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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real(pReal), intent(in) :: &
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T
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_dislotungsten_LpAndItsTangent
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module subroutine plastic_nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
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Mp,Temperature,instance,of,ip,el)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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real(pReal), intent(in) :: &
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Temperature
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integer, intent(in) :: &
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instance, &
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of, &
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ip, & !< current integration point
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el !< current element number
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end subroutine plastic_nonlocal_LpAndItsTangent
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module subroutine plastic_isotropic_dotState(Mp,instance,of)
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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@ -267,6 +180,22 @@ submodule(constitutive) constitutive_mech
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ip, &
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el
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end subroutine plastic_nonlocal_deltaState
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module subroutine constitutive_plastic_LpAndItsTangents(Lp, dLp_dS, dLp_dFi, &
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S, Fi, co, ip, el)
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integer, intent(in) :: &
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co, & !< component-ID of integration point
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ip, & !< integration point
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el !< element
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real(pReal), intent(in), dimension(3,3) :: &
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S, & !< 2nd Piola-Kirchhoff stress
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Fi !< intermediate deformation gradient
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real(pReal), intent(out), dimension(3,3) :: &
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Lp !< plastic velocity gradient
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real(pReal), intent(out), dimension(3,3,3,3) :: &
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dLp_dS, &
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dLp_dFi !< derivative of Lp with respect to Fi
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end subroutine constitutive_plastic_LpAndItsTangents
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module function kinematics_cleavage_opening_init(kinematics_length) result(myKinematics)
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integer, intent(in) :: kinematics_length
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@ -621,72 +550,6 @@ module subroutine constitutive_plastic_dependentState(co, ip, el)
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end subroutine constitutive_plastic_dependentState
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!--------------------------------------------------------------------------------------------------
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!> @brief contains the constitutive equation for calculating the velocity gradient
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! ToDo: Discuss whether it makes sense if crystallite handles the configuration conversion, i.e.
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! Mp in, dLp_dMp out
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!--------------------------------------------------------------------------------------------------
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subroutine constitutive_plastic_LpAndItsTangents(Lp, dLp_dS, dLp_dFi, &
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S, Fi, co, ip, el)
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integer, intent(in) :: &
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co, & !< component-ID of integration point
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ip, & !< integration point
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el !< element
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real(pReal), intent(in), dimension(3,3) :: &
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S, & !< 2nd Piola-Kirchhoff stress
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Fi !< intermediate deformation gradient
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real(pReal), intent(out), dimension(3,3) :: &
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Lp !< plastic velocity gradient
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real(pReal), intent(out), dimension(3,3,3,3) :: &
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dLp_dS, &
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dLp_dFi !< derivative of Lp with respect to Fi
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real(pReal), dimension(3,3,3,3) :: &
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dLp_dMp !< derivative of Lp with respect to Mandel stress
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real(pReal), dimension(3,3) :: &
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Mp !< Mandel stress work conjugate with Lp
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integer :: &
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i, j, instance, me, ph
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Mp = matmul(matmul(transpose(Fi),Fi),S)
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me = material_phasememberAt(co,ip,el)
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ph = material_phaseAt(co,el)
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instance = phase_plasticityInstance(ph)
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plasticityType: select case (phase_plasticity(material_phaseAt(co,el)))
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case (PLASTICITY_NONE_ID) plasticityType
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Lp = 0.0_pReal
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dLp_dMp = 0.0_pReal
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case (PLASTICITY_ISOTROPIC_ID) plasticityType
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call plastic_isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,me)
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case (PLASTICITY_PHENOPOWERLAW_ID) plasticityType
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call plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,me)
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case (PLASTICITY_KINEHARDENING_ID) plasticityType
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call plastic_kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,me)
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case (PLASTICITY_NONLOCAL_ID) plasticityType
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call plastic_nonlocal_LpAndItsTangent(Lp,dLp_dMp,Mp, thermal_T(ph,me),instance,me,ip,el)
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case (PLASTICITY_DISLOTWIN_ID) plasticityType
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call plastic_dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp, thermal_T(ph,me),instance,me)
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case (PLASTICITY_DISLOTUNGSTEN_ID) plasticityType
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call plastic_dislotungsten_LpAndItsTangent(Lp,dLp_dMp,Mp, thermal_T(ph,me),instance,me)
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end select plasticityType
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do i=1,3; do j=1,3
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dLp_dFi(i,j,1:3,1:3) = matmul(matmul(Fi,S),transpose(dLp_dMp(i,j,1:3,1:3))) + &
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matmul(matmul(Fi,dLp_dMp(i,j,1:3,1:3)),S)
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dLp_dS(i,j,1:3,1:3) = matmul(matmul(transpose(Fi),Fi),dLp_dMp(i,j,1:3,1:3)) ! ToDo: @PS: why not: dLp_dMp:(FiT Fi)
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enddo; enddo
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end subroutine constitutive_plastic_LpAndItsTangents
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!--------------------------------------------------------------------------------------------------
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@ -0,0 +1,162 @@
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submodule(constitutive:constitutive_mech) plastic
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interface
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module subroutine plastic_isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_isotropic_LpAndItsTangent
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pure module subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_phenopowerlaw_LpAndItsTangent
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pure module subroutine plastic_kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_kinehardening_LpAndItsTangent
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module subroutine plastic_dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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real(pReal), intent(in) :: &
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T
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_dislotwin_LpAndItsTangent
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pure module subroutine plastic_dislotungsten_LpAndItsTangent(Lp,dLp_dMp,Mp,T,instance,of)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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real(pReal), intent(in) :: &
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T
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integer, intent(in) :: &
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instance, &
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of
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end subroutine plastic_dislotungsten_LpAndItsTangent
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module subroutine plastic_nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
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Mp,Temperature,instance,of,ip,el)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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real(pReal), intent(in) :: &
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Temperature
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integer, intent(in) :: &
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instance, &
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of, &
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ip, & !< current integration point
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el !< current element number
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end subroutine plastic_nonlocal_LpAndItsTangent
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end interface
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contains
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!--------------------------------------------------------------------------------------------------
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!> @brief contains the constitutive equation for calculating the velocity gradient
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! ToDo: Discuss whether it makes sense if crystallite handles the configuration conversion, i.e.
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! Mp in, dLp_dMp out
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!--------------------------------------------------------------------------------------------------
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module subroutine constitutive_plastic_LpAndItsTangents(Lp, dLp_dS, dLp_dFi, &
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S, Fi, co, ip, el)
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integer, intent(in) :: &
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co, & !< component-ID of integration point
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ip, & !< integration point
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el !< element
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real(pReal), intent(in), dimension(3,3) :: &
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S, & !< 2nd Piola-Kirchhoff stress
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Fi !< intermediate deformation gradient
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real(pReal), intent(out), dimension(3,3) :: &
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Lp !< plastic velocity gradient
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real(pReal), intent(out), dimension(3,3,3,3) :: &
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dLp_dS, &
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dLp_dFi !< derivative of Lp with respect to Fi
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real(pReal), dimension(3,3,3,3) :: &
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dLp_dMp !< derivative of Lp with respect to Mandel stress
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real(pReal), dimension(3,3) :: &
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Mp !< Mandel stress work conjugate with Lp
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integer :: &
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i, j, instance, me, ph
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Mp = matmul(matmul(transpose(Fi),Fi),S)
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me = material_phasememberAt(co,ip,el)
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ph = material_phaseAt(co,el)
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instance = phase_plasticityInstance(ph)
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plasticityType: select case (phase_plasticity(material_phaseAt(co,el)))
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case (PLASTICITY_NONE_ID) plasticityType
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Lp = 0.0_pReal
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dLp_dMp = 0.0_pReal
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case (PLASTICITY_ISOTROPIC_ID) plasticityType
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call plastic_isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,me)
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case (PLASTICITY_PHENOPOWERLAW_ID) plasticityType
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call plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,me)
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case (PLASTICITY_KINEHARDENING_ID) plasticityType
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call plastic_kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,me)
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case (PLASTICITY_NONLOCAL_ID) plasticityType
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call plastic_nonlocal_LpAndItsTangent(Lp,dLp_dMp,Mp, thermal_T(ph,me),instance,me,ip,el)
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case (PLASTICITY_DISLOTWIN_ID) plasticityType
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call plastic_dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp, thermal_T(ph,me),instance,me)
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case (PLASTICITY_DISLOTUNGSTEN_ID) plasticityType
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call plastic_dislotungsten_LpAndItsTangent(Lp,dLp_dMp,Mp, thermal_T(ph,me),instance,me)
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end select plasticityType
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do i=1,3; do j=1,3
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dLp_dFi(i,j,1:3,1:3) = matmul(matmul(Fi,S),transpose(dLp_dMp(i,j,1:3,1:3))) + &
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matmul(matmul(Fi,dLp_dMp(i,j,1:3,1:3)),S)
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dLp_dS(i,j,1:3,1:3) = matmul(matmul(transpose(Fi),Fi),dLp_dMp(i,j,1:3,1:3)) ! ToDo: @PS: why not: dLp_dMp:(FiT Fi)
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enddo; enddo
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end subroutine constitutive_plastic_LpAndItsTangents
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end submodule plastic
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!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
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!> @brief crystal plasticity model for bcc metals, especially Tungsten
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!--------------------------------------------------------------------------------------------------
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submodule(constitutive:constitutive_mech) plastic_dislotungsten
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submodule(constitutive:plastic) dislotungsten
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real(pReal), parameter :: &
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kB = 1.38e-23_pReal !< Boltzmann constant in J/Kelvin
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@ -547,4 +547,4 @@ pure subroutine kinetics(Mp,T,instance,of, &
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end subroutine kinetics
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end submodule plastic_dislotungsten
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end submodule dislotungsten
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@ -7,7 +7,7 @@
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!> @brief material subroutine incoprorating dislocation and twinning physics
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!> @details to be done
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!--------------------------------------------------------------------------------------------------
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submodule(constitutive:constitutive_mech) plastic_dislotwin
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submodule(constitutive:plastic) dislotwin
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real(pReal), parameter :: &
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kB = 1.38e-23_pReal !< Boltzmann constant in J/Kelvin
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@ -1088,4 +1088,4 @@ pure subroutine kinetics_trans(Mp,T,dot_gamma_sl,instance,of,&
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end subroutine kinetics_trans
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end submodule plastic_dislotwin
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end submodule dislotwin
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!! resolving the stress on the slip systems. Will give the response of phenopowerlaw for an
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!! untextured polycrystal
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!--------------------------------------------------------------------------------------------------
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submodule(constitutive:constitutive_mech) plastic_isotropic
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submodule(constitutive:plastic) isotropic
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type :: tParameters
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real(pReal) :: &
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@ -348,4 +348,4 @@ module subroutine plastic_isotropic_results(instance,group)
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end subroutine plastic_isotropic_results
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end submodule plastic_isotropic
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end submodule isotropic
|
||||
|
|
|
@ -5,7 +5,7 @@
|
|||
!> @brief Phenomenological crystal plasticity using a power law formulation for the shear rates
|
||||
!! and a Voce-type kinematic hardening rule
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
submodule(constitutive:constitutive_mech) plastic_kinehardening
|
||||
submodule(constitutive:plastic) kinehardening
|
||||
|
||||
type :: tParameters
|
||||
real(pReal) :: &
|
||||
|
@ -474,4 +474,4 @@ pure subroutine kinetics(Mp,instance,of, &
|
|||
|
||||
end subroutine kinetics
|
||||
|
||||
end submodule plastic_kinehardening
|
||||
end submodule kinehardening
|
||||
|
|
|
@ -4,7 +4,7 @@
|
|||
!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
|
||||
!> @brief Dummy plasticity for purely elastic material
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
submodule(constitutive:constitutive_mech) plastic_none
|
||||
submodule(constitutive:plastic) none
|
||||
|
||||
contains
|
||||
|
||||
|
@ -50,4 +50,4 @@ module function plastic_none_init() result(myPlasticity)
|
|||
end function plastic_none_init
|
||||
|
||||
|
||||
end submodule plastic_none
|
||||
end submodule none
|
||||
|
|
|
@ -4,7 +4,7 @@
|
|||
!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
|
||||
!> @brief material subroutine for plasticity including dislocation flux
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
submodule(constitutive:constitutive_mech) plastic_nonlocal
|
||||
submodule(constitutive:plastic) nonlocal
|
||||
use geometry_plastic_nonlocal, only: &
|
||||
nIPneighbors => geometry_plastic_nonlocal_nIPneighbors, &
|
||||
IPneighborhood => geometry_plastic_nonlocal_IPneighborhood, &
|
||||
|
@ -1834,4 +1834,4 @@ pure function getRho0(instance,of,ip,el)
|
|||
|
||||
end function getRho0
|
||||
|
||||
end submodule plastic_nonlocal
|
||||
end submodule nonlocal
|
||||
|
|
|
@ -4,7 +4,7 @@
|
|||
!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
|
||||
!> @brief phenomenological crystal plasticity formulation using a powerlaw fitting
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
submodule(constitutive:constitutive_mech) plastic_phenopowerlaw
|
||||
submodule(constitutive:plastic) phenopowerlaw
|
||||
|
||||
type :: tParameters
|
||||
real(pReal) :: &
|
||||
|
@ -543,4 +543,4 @@ pure subroutine kinetics_twin(Mp,instance,of,&
|
|||
|
||||
end subroutine kinetics_twin
|
||||
|
||||
end submodule plastic_phenopowerlaw
|
||||
end submodule phenopowerlaw
|
||||
|
|
Loading…
Reference in New Issue