mean velocity of dislocation corrected for higher temperatures
- v_wait: obstacle spacing over waiting time (effective velocity) - v_run: 'true' velocity of a dislocation moving between obstacles for higher temperatures v_run becomes important and bounds the velocity
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@ -1404,20 +1404,27 @@ pure subroutine kinetics_slip(prm,stt,mse,of,Mp,temperature,gdot_slip,dgdot_dtau
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tau, &
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stressRatio, &
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StressRatio_p, &
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BoltzmannRatio
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BoltzmannRatio, &
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v_wait_inverse, & !< inverse of the effective velocity of a dislocation waiting at obstacles
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v_run_inverse, & !< inverse of the velocity of a free moving dislocation
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tau_eff !< effective resolved stress
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integer(pInt) :: i
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do i = 1_pInt, prm%totalNslip
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tau(i) = math_mul33xx33(Mp,prm%Schmid_slip(1:3,1:3,i))
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enddo
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significantStress: where((abs(tau)-mse%threshold_stress_slip(:,of)) > tol_math_check)
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stressRatio = ((abs(tau)- mse%threshold_stress_slip(:,of))/&
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(prm%SolidSolutionStrength+prm%tau_peierls(:)))
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tau_eff = abs(tau)-mse%threshold_stress_slip(:,of)
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significantStress: where(tau_eff > tol_math_check)
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stressRatio = tau_eff/(prm%SolidSolutionStrength+prm%tau_peierls)
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StressRatio_p = stressRatio** prm%p
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BoltzmannRatio = prm%Qedge/(kB*Temperature)
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gdot_slip = stt%rhoEdge(:,of)*prm%burgers_slip* prm%v0 &
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* sign(exp(-BoltzmannRatio*(1.0_pReal-StressRatio_p)** prm%q), tau)
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v_wait_inverse = prm%v0**(-1.0_pReal) * exp(BoltzmannRatio*(1.0_pReal-StressRatio_p)** prm%q)
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v_run_inverse = prm%B/(tau_eff*prm%burgers_slip)
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gdot_slip = sign(stt%rhoEdge(:,of)*prm%burgers_slip/(v_wait_inverse+v_run_inverse),tau)
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dgdot_dtau = abs(gdot_slip)*BoltzmannRatio*prm%p * prm%q &
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/ (prm%SolidSolutionStrength+prm%tau_peierls) &
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* stressRatio**(prm%p-1.0_pReal)*(1.0_pReal-StressRatio_p)**(prm%q-1.0_pReal)
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@ -1428,11 +1435,11 @@ pure subroutine kinetics_slip(prm,stt,mse,of,Mp,temperature,gdot_slip,dgdot_dtau
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if(present(dgdot_dtau_slip)) dgdot_dtau_slip = dgdot_dtau
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end subroutine
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end subroutine kinetics_slip
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!--------------------------------------------------------------------------------------------------
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!> @brief calculates shear rates on slip systems
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!> @brief calculates shear rates on twin systems
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!--------------------------------------------------------------------------------------------------
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pure subroutine kinetics_twin(prm,stt,mse,of,Mp,temperature,gdot_slip,gdot_twin,dgdot_dtau_twin)
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use prec, only: &
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@ -1475,7 +1482,7 @@ pure subroutine kinetics_twin(prm,stt,mse,of,Mp,temperature,gdot_slip,gdot_twin,
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s1=prm%fcc_twinNucleationSlipPair(1,i)
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s2=prm%fcc_twinNucleationSlipPair(2,i)
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if (tau(i) < mse%tau_r_twin(i,of)) then
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Ndot0_twin=(abs(gdot_slip(s1))*(stt%rhoEdge(s2,of)+stt%rhoEdgeDip(s2,of))+& !!!!! correct?
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Ndot0_twin=(abs(gdot_slip(s1))*(stt%rhoEdge(s2,of)+stt%rhoEdgeDip(s2,of))+&
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abs(gdot_slip(s2))*(stt%rhoEdge(s1,of)+stt%rhoEdgeDip(s1,of)))/&
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(prm%L0_twin*prm%burgers_slip(i))*&
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(1.0_pReal-exp(-prm%VcrossSlip/(kB*Temperature)*&
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@ -1500,7 +1507,7 @@ pure subroutine kinetics_twin(prm,stt,mse,of,Mp,temperature,gdot_slip,gdot_twin,
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if(present(dgdot_dtau_twin)) dgdot_dtau_twin = dgdot_dtau
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end subroutine
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end subroutine kinetics_twin
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!--------------------------------------------------------------------------------------------------
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@ -1547,7 +1554,7 @@ pure subroutine kinetics_trans(prm,stt,mse,of,Mp,temperature,gdot_slip,gdot_tran
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s1=prm%fcc_twinNucleationSlipPair(1,i)
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s2=prm%fcc_twinNucleationSlipPair(2,i)
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if (tau(i) < mse%tau_r_trans(i,of)) then
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Ndot0_trans=(abs(gdot_slip(s1))*(stt%rhoEdge(s2,of)+stt%rhoEdgeDip(s2,of))+& ! s1/s2 mixing correct?
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Ndot0_trans=(abs(gdot_slip(s1))*(stt%rhoEdge(s2,of)+stt%rhoEdgeDip(s2,of))+&
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abs(gdot_slip(s2))*(stt%rhoEdge(s1,of)+stt%rhoEdgeDip(s1,of)))/&
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(prm%L0_trans*prm%burgers_slip(i))*& ! burgers_slip correct?
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(1.0_pReal-exp(-prm%VcrossSlip/(kB*Temperature)*&
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@ -1583,7 +1590,7 @@ pure subroutine kinetics_trans(prm,stt,mse,of,Mp,temperature,gdot_slip,gdot_tran
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!
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! if(present(dgdot_dtau_twin)) dgdot_dtau_twin = dgdot_dtau
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!
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end subroutine
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end subroutine kinetics_trans
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!--------------------------------------------------------------------------------------------------
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!> @brief return array of constitutive results
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