consistent API
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@ -861,7 +861,7 @@ subroutine constitutive_collectDotState(S6, FeArray, Fi, FpArray, subdt, subfrac
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plasticityType: select case (phase_plasticity(material_phase(ipc,ip,el)))
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plasticityType: select case (phase_plasticity(material_phase(ipc,ip,el)))
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case (PLASTICITY_ISOTROPIC_ID) plasticityType
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case (PLASTICITY_ISOTROPIC_ID) plasticityType
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call plastic_isotropic_dotState (math_Mandel33to6(Mp),ipc,ip,el)
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call plastic_isotropic_dotState (Mp,ipc,ip,el)
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case (PLASTICITY_PHENOPOWERLAW_ID) plasticityType
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case (PLASTICITY_PHENOPOWERLAW_ID) plasticityType
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of = phasememberAt(ipc,ip,el)
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of = phasememberAt(ipc,ip,el)
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@ -300,8 +300,7 @@ subroutine plastic_isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ipc,ip,el)
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write(6,'(/,a,/,f12.5)') '<< CONST isotropic >> norm Tstar / MPa', norm_Mp_dev*1.0e-6_pReal
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write(6,'(/,a,/,f12.5)') '<< CONST isotropic >> norm Tstar / MPa', norm_Mp_dev*1.0e-6_pReal
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write(6,'(/,a,/,f12.5)') '<< CONST isotropic >> gdot', gamma_dot
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write(6,'(/,a,/,f12.5)') '<< CONST isotropic >> gdot', gamma_dot
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end if
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end if
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!--------------------------------------------------------------------------------------------------
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! Calculation of the tangent of Lp
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
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dLp_dMp(k,l,m,n) = (prm%n-1.0_pReal) * Mp_dev(k,l)*Mp_dev(m,n) / squarenorm_Mp_dev
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dLp_dMp(k,l,m,n) = (prm%n-1.0_pReal) * Mp_dev(k,l)*Mp_dev(m,n) / squarenorm_Mp_dev
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt) &
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt) &
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@ -312,6 +311,7 @@ subroutine plastic_isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ipc,ip,el)
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end if
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end if
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end associate
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end associate
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end subroutine plastic_isotropic_LpAndItsTangent
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end subroutine plastic_isotropic_LpAndItsTangent
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@ -331,7 +331,7 @@ subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dTstar,Tstar,instance,of)
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real(pReal), dimension(3,3), intent(in) :: &
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real(pReal), dimension(3,3), intent(in) :: &
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Tstar !< Mandel stress
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Tstar !< Mandel stress
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integer(pInt), intent(in) :: &
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integer(pInt), intent(in) :: &
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instance, &
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instance, &
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of
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of
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@ -350,14 +350,10 @@ subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dTstar,Tstar,instance,of)
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squarenorm_Tstar_sph = math_mul33xx33(Tstar_sph,Tstar_sph)
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squarenorm_Tstar_sph = math_mul33xx33(Tstar_sph,Tstar_sph)
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norm_Tstar_sph = sqrt(squarenorm_Tstar_sph)
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norm_Tstar_sph = sqrt(squarenorm_Tstar_sph)
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if (prm%dilatation .and. norm_Tstar_sph > 0.0_pReal) then ! Tstar == 0 or J2 plascitiy --> both Li and dLi_dTstar are zero
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if (prm%dilatation .and. norm_Tstar_sph > 0.0_pReal) then ! no stress or J2 plastitiy --> Li and its derivative are zero
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gamma_dot = prm%gdot0 &
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gamma_dot = prm%gdot0 * (sqrt(1.5_pReal) * norm_Tstar_sph /(prm%fTaylor*stt%flowstress(of))) **prm%n
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* (sqrt(1.5_pReal) * norm_Tstar_sph / prm%fTaylor / stt%flowstress(of) ) **prm%n
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Li = Tstar_sph/norm_Tstar_sph * gamma_dot/prm%fTaylor
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Li = Tstar_sph/norm_Tstar_sph * gamma_dot/prm%fTaylor
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!--------------------------------------------------------------------------------------------------
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! Calculation of the tangent of Li
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
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dLi_dTstar(k,l,m,n) = (prm%n-1.0_pReal) * Tstar_sph(k,l)*Tstar_sph(m,n) / squarenorm_Tstar_sph
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dLi_dTstar(k,l,m,n) = (prm%n-1.0_pReal) * Tstar_sph(k,l)*Tstar_sph(m,n) / squarenorm_Tstar_sph
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt) &
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt) &
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@ -365,8 +361,8 @@ subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dTstar,Tstar,instance,of)
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dLi_dTstar = gamma_dot / prm%fTaylor * dLi_dTstar / norm_Tstar_sph
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dLi_dTstar = gamma_dot / prm%fTaylor * dLi_dTstar / norm_Tstar_sph
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else
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else
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Li = 0.0_pReal
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Li = 0.0_pReal
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dLi_dTstar = 0.0_pReal
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dLi_dTstar = 0.0_pReal
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endif
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endif
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end associate
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end associate
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@ -377,52 +373,46 @@ subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dTstar,Tstar,instance,of)
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!--------------------------------------------------------------------------------------------------
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!--------------------------------------------------------------------------------------------------
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!> @brief calculates the rate of change of microstructure
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!> @brief calculates the rate of change of microstructure
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!--------------------------------------------------------------------------------------------------
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!--------------------------------------------------------------------------------------------------
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subroutine plastic_isotropic_dotState(Tstar_v,ipc,ip,el)
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subroutine plastic_isotropic_dotState(Mp,ipc,ip,el)
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use prec, only: &
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use prec, only: &
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dEq0
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dEq0
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use math, only: &
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use math, only: &
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math_mul6x6
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math_mul33xx33, &
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math_deviatoric33
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use material, only: &
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use material, only: &
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phasememberAt, &
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phasememberAt, &
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material_phase, &
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material_phase, &
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phase_plasticityInstance
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phase_plasticityInstance
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implicit none
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implicit none
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real(pReal), dimension(6), intent(in):: &
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real(pReal), dimension(3,3), intent(in) :: &
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Tstar_v !< 2nd Piola Kirchhoff stress tensor in Mandel notation
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Mp !< Mandel stress
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integer(pInt), intent(in) :: &
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integer(pInt), intent(in) :: &
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ipc, & !< component-ID of integration point
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ipc, & !< component-ID of integration point
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ip, & !< integration point
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ip, & !< integration point
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el !< element
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el !< element
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real(pReal), dimension(6) :: &
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Tstar_dev_v !< deviatoric 2nd Piola Kirchhoff stress tensor in Mandel notation
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real(pReal) :: &
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real(pReal) :: &
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gamma_dot, & !< strainrate
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gamma_dot, & !< strainrate
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hardening, & !< hardening coefficient
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hardening, & !< hardening coefficient
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saturation, & !< saturation flowstress
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saturation, & !< saturation flowstress
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norm_Tstar_v !< euclidean norm of Tstar_dev
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norm_Mp !< norm of the Mandel stress
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integer(pInt) :: &
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integer(pInt) :: &
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instance, & !< instance of my instance (unique number of my constitutive model)
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instance, &
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of !< shortcut notation for offset position in state array
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of !< shortcut notation for offset position in state array
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of = phasememberAt(ipc,ip,el) ! phasememberAt should be tackled by material and be renamed to material_phasemember
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of = phasememberAt(ipc,ip,el) ! phasememberAt should be tackled by material and be renamed to material_phasemember
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instance = phase_plasticityInstance(material_phase(ipc,ip,el))
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instance = phase_plasticityInstance(material_phase(ipc,ip,el))
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associate(prm => param(instance))
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associate(prm => param(instance), stt => state(instance), dot => dotState(instance))
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!--------------------------------------------------------------------------------------------------
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!--------------------------------------------------------------------------------------------------
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! norm of (deviatoric) 2nd Piola-Kirchhoff stress
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! norm of (deviatoric) Mandel stress
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if (prm%dilatation) then
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if (prm%dilatation) then
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norm_Tstar_v = sqrt(math_mul6x6(Tstar_v,Tstar_v))
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norm_Mp = sqrt(math_mul33xx33(Mp,Mp))
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else
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else
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Tstar_dev_v(1:3) = Tstar_v(1:3) - sum(Tstar_v(1:3))/3.0_pReal
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norm_Mp = sqrt(math_mul33xx33(math_deviatoric33(Mp),math_deviatoric33(Mp)))
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Tstar_dev_v(4:6) = Tstar_v(4:6)
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endif
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norm_Tstar_v = sqrt(math_mul6x6(Tstar_dev_v,Tstar_dev_v))
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end if
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gamma_dot = prm%gdot0 * (sqrt(1.5_pReal) * norm_Mp /(prm%fTaylor*stt%flowstress(of))) **prm%n
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!--------------------------------------------------------------------------------------------------
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! strain rate
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gamma_dot = prm%gdot0 * ( sqrt(1.5_pReal) * norm_Tstar_v &
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/ &!-----------------------------------------------------------------------------------
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(prm%fTaylor*state(instance)%flowstress(of) ))**prm%n
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!--------------------------------------------------------------------------------------------------
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!--------------------------------------------------------------------------------------------------
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! hardening coefficient
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! hardening coefficient
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@ -431,27 +421,25 @@ subroutine plastic_isotropic_dotState(Tstar_v,ipc,ip,el)
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saturation = prm%tausat
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saturation = prm%tausat
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else
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else
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saturation = prm%tausat &
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saturation = prm%tausat &
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+ asinh( (gamma_dot / prm%tausat_SinhFitA&
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+ asinh( (gamma_dot / prm%tausat_SinhFitA)**(1.0_pReal / prm%tausat_SinhFitD) &
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)**(1.0_pReal / prm%tausat_SinhFitD)&
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)**(1.0_pReal / prm%tausat_SinhFitC) &
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)**(1.0_pReal / prm%tausat_SinhFitC) &
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/ ( prm%tausat_SinhFitB &
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/ prm%tausat_SinhFitB * (gamma_dot / prm%gdot0)**(1.0_pReal / prm%n)
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* (gamma_dot / prm%gdot0)**(1.0_pReal / prm%n) &
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)
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endif
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endif
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hardening = ( prm%h0 + prm%h0_slopeLnRate * log(gamma_dot) ) &
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hardening = ( prm%h0 + prm%h0_slopeLnRate * log(gamma_dot) ) &
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* abs( 1.0_pReal - state(instance)%flowstress(of)/saturation )**prm%a &
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* abs( 1.0_pReal - stt%flowstress(of)/saturation )**prm%a &
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* sign(1.0_pReal, 1.0_pReal - state(instance)%flowstress(of)/saturation)
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* sign(1.0_pReal, 1.0_pReal - stt%flowstress(of)/saturation)
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else
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else
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hardening = 0.0_pReal
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hardening = 0.0_pReal
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endif
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endif
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dotState(instance)%flowstress (of) = hardening * gamma_dot
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dot%flowstress (of) = hardening * gamma_dot
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dotState(instance)%accumulatedShear(of) = gamma_dot
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dot%accumulatedShear(of) = gamma_dot
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end associate
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end associate
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end subroutine plastic_isotropic_dotState
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end subroutine plastic_isotropic_dotState
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!--------------------------------------------------------------------------------------------------
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!--------------------------------------------------------------------------------------------------
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!> @brief return array of constitutive results
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!> @brief return array of constitutive results
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!--------------------------------------------------------------------------------------------------
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!--------------------------------------------------------------------------------------------------
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