preparing for vectorization
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@ -657,11 +657,13 @@ math_mul33xx33
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integer(pInt) :: &
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j
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real(pReal) :: StressRatio_p,StressRatio_pminus1,&
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BoltzmannRatio,DotGamma0,stressRatio,&
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dvel_slip, vel_slip
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real(pReal) :: dvel_slip, vel_slip
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real(pReal), intent(out), dimension(prm%totalNslip) :: &
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gdot_slip_pos,dgdot_dtauslip_pos,tau_slip_pos,gdot_slip_neg,dgdot_dtauslip_neg,tau_slip_neg
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real(pReal), dimension(prm%totalNslip) :: &
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StressRatio, BoltzmannRatio, &
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StressRatio_p,StressRatio_pminus1, &
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DotGamma0
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gdot_slip_pos = 0.0_pReal
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gdot_slip_neg = 0.0_pReal
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@ -673,56 +675,57 @@ math_mul33xx33
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tau_slip_neg(j) = math_mul33xx33(Mp,prm%nonSchmid_neg(1:3,1:3,j))
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enddo
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BoltzmannRatio = prm%H0kp/(kB*Temperature)
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DotGamma0 = stt%rhoEdge(:,of)*prm%burgers*prm%v0
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do j = 1_pInt, prm%totalNslip
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BoltzmannRatio = prm%H0kp(j)/(kB*Temperature)
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DotGamma0 = stt%rhoEdge(j,of)*prm%burgers(j)*prm%v0(j)
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significantPositiveTau: if((abs(tau_slip_pos(j))-dst%threshold_stress(j, of)) > tol_math_check) then
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stressRatio = ((abs(tau_slip_pos(j))-dst%threshold_stress(j, of)) &
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StressRatio(j) = ((abs(tau_slip_pos(j))-dst%threshold_stress(j, of)) &
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/ (prm%solidSolutionStrength+prm%tau_Peierls(j)))
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stressRatio_p = stressRatio** prm%p(j)
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stressRatio_pminus1 = stressRatio**(prm%p(j)-1.0_pReal)
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StressRatio_p(j) = StressRatio(j)** prm%p(j)
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StressRatio_pminus1(j) = StressRatio(j)**(prm%p(j)-1.0_pReal)
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vel_slip = 2.0_pReal*prm%burgers(j) * prm%kink_height(j) * prm%omega(j) &
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* ( dst%mfp(j,of) - prm%kink_width(j) ) &
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* (tau_slip_pos(j) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) ) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) ) &
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/ ( &
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2.0_pReal*(prm%burgers(j)**2.0_pReal)*tau_slip_pos(j) &
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+ prm%omega(j) * prm%B(j) &
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*(( dst%mfp(j,of) - prm%kink_width(j) )**2.0_pReal) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) &
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)
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gdot_slip_pos(j) = DotGamma0 * sign(vel_slip,tau_slip_pos(j))
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gdot_slip_pos(j) = DotGamma0(j) * sign(vel_slip,tau_slip_pos(j))
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dvel_slip = 2.0_pReal*prm%burgers(j) * prm%kink_height(j) * prm%omega(j) &
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* ( dst%mfp(j,of) - prm%kink_width(j) ) &
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* ( &
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(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) &
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(exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) &
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+ tau_slip_pos(j) &
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* (abs(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)))&
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*BoltzmannRatio*prm%p(j)&
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* (abs(exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)))&
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*BoltzmannRatio(j)*prm%p(j)&
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*prm%q(j)/&
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(prm%solidSolutionStrength+prm%tau_Peierls(j))*&
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StressRatio_pminus1*(1-StressRatio_p)**(prm%q(j)-1.0_pReal) ) &
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StressRatio_pminus1(j)*(1-StressRatio_p(j))**(prm%q(j)-1.0_pReal) ) &
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) &
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* (2.0_pReal*(prm%burgers(j)**2.0_pReal)*tau_slip_pos(j) &
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+ prm%omega(j) * prm%B(j) &
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*(( dst%mfp(j,of) - prm%kink_width(j) )**2.0_pReal) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) &
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) &
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- (tau_slip_pos(j) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) ) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) ) &
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* (2.0_pReal*(prm%burgers(j)**2.0_pReal) &
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+ prm%omega(j) * prm%B(j) &
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*(( dst%mfp(j,of) - prm%kink_width(j) )**2.0_pReal) &
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* (abs(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)))&
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*BoltzmannRatio*prm%p(j)&
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* (abs(exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)))&
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*BoltzmannRatio(j)*prm%p(j)&
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*prm%q(j)/&
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(prm%solidSolutionStrength+prm%tau_Peierls(j))*&
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StressRatio_pminus1*(1-StressRatio_p)**(prm%q(j)-1.0_pReal) )&
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StressRatio_pminus1(j)*(1-StressRatio_p(j))**(prm%q(j)-1.0_pReal) )&
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) &
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) &
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/ ( &
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@ -730,61 +733,61 @@ math_mul33xx33
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2.0_pReal*(prm%burgers(j)**2.0_pReal)*tau_slip_pos(j) &
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+ prm%omega(j) * prm%B(j) &
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*(( dst%mfp(j,of) - prm%kink_width(j) )**2.0_pReal) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) &
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)**2.0_pReal &
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)
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dgdot_dtauslip_pos(j) = DotGamma0 * dvel_slip
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dgdot_dtauslip_pos(j) = DotGamma0(j) * dvel_slip
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endif significantPositiveTau
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significantNegativeTau: if((abs(tau_slip_neg(j))-dst%threshold_stress(j, of)) > tol_math_check) then
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stressRatio = ((abs(tau_slip_neg(j))-dst%threshold_stress(j, of)) &
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StressRatio(j) = ((abs(tau_slip_neg(j))-dst%threshold_stress(j, of)) &
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/ (prm%solidSolutionStrength+prm%tau_Peierls(j)))
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stressRatio_p = stressRatio** prm%p(j)
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stressRatio_pminus1 = stressRatio**(prm%p(j)-1.0_pReal)
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StressRatio_p(j) = StressRatio(j)** prm%p(j)
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StressRatio_pminus1(j) = StressRatio(j)**(prm%p(j)-1.0_pReal)
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vel_slip = 2.0_pReal*prm%burgers(j) * prm%kink_height(j) * prm%omega(j) &
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* ( dst%mfp(j,of) - prm%kink_width(j) ) &
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* (tau_slip_neg(j) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) ) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) ) &
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/ ( &
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2.0_pReal*(prm%burgers(j)**2.0_pReal)*tau_slip_neg(j) &
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+ prm%omega(j) * prm%B(j) &
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*(( dst%mfp(j,of) - prm%kink_width(j) )**2.0_pReal) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) &
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)
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gdot_slip_neg(j) = DotGamma0 * sign(vel_slip,tau_slip_neg(j))
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gdot_slip_neg(j) = DotGamma0(j) * sign(vel_slip,tau_slip_neg(j))
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dvel_slip = 2.0_pReal*prm%burgers(j) * prm%kink_height(j) * prm%omega(j) &
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* ( dst%mfp(j,of) - prm%kink_width(j) ) &
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* ( &
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(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) &
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(exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) &
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+ tau_slip_neg(j) &
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* (abs(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)))&
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*BoltzmannRatio*prm%p(j)&
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* (abs(exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)))&
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*BoltzmannRatio(j)*prm%p(j)&
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*prm%q(j)/&
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(prm%solidSolutionStrength+prm%tau_Peierls(j))*&
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StressRatio_pminus1*(1-StressRatio_p)**(prm%q(j)-1.0_pReal) ) &
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StressRatio_pminus1(j)*(1-StressRatio_p(j))**(prm%q(j)-1.0_pReal) ) &
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) &
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* (2.0_pReal*(prm%burgers(j)**2.0_pReal)*tau_slip_neg(j) &
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+ prm%omega(j) * prm%B(j) &
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*(( dst%mfp(j,of) - prm%kink_width(j) )**2.0_pReal) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) &
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) &
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- (tau_slip_neg(j) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) ) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) ) &
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* (2.0_pReal*(prm%burgers(j)**2.0_pReal) &
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+ prm%omega(j) * prm%B(j) &
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*(( dst%mfp(j,of) - prm%kink_width(j) )**2.0_pReal) &
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* (abs(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)))&
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*BoltzmannRatio*prm%p(j)&
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* (abs(exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)))&
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*BoltzmannRatio(j)*prm%p(j)&
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*prm%q(j)/&
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(prm%solidSolutionStrength+prm%tau_Peierls(j))*&
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StressRatio_pminus1*(1-StressRatio_p)**(prm%q(j)-1.0_pReal) )&
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StressRatio_pminus1(j)*(1-StressRatio_p(j))**(prm%q(j)-1.0_pReal) )&
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) &
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) &
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/ ( &
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@ -792,12 +795,12 @@ math_mul33xx33
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2.0_pReal*(prm%burgers(j)**2.0_pReal)*tau_slip_neg(j) &
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+ prm%omega(j) * prm%B(j) &
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*(( dst%mfp(j,of) - prm%kink_width(j) )**2.0_pReal) &
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* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q(j)) &
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* exp(-BoltzmannRatio(j)*(1-StressRatio_p(j)) ** prm%q(j)) &
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)**2.0_pReal &
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)
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dgdot_dtauslip_neg(j) = DotGamma0 * dvel_slip
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dgdot_dtauslip_neg(j) = DotGamma0(j) * dvel_slip
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endif significantNegativeTau
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enddo
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