vectorized
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@ -504,9 +504,8 @@ subroutine plastic_kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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do j = 1_pInt, prm%totalNslip
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Lp = Lp + (gdot_pos(j)+gdot_neg(j))*prm%Schmid_slip(1:3,1:3,j) ! sum of all gdot*SchmidTensor gives Lp
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Lp = Lp + (gdot_pos(j)+gdot_neg(j))*prm%Schmid_slip(1:3,1:3,j)
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! Calculation of the tangent of Lp ! sensitivity of Lp
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if (dNeq0(gdot_pos(j))) then
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dgdot_dtau_pos = gdot_pos(j)*prm%n_slip/tau_pos(j)
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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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@ -616,24 +615,22 @@ subroutine plastic_kinehardening_dotState(Mp,instance,of)
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sumGamma = sum(stt%accshear(:,of))
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do j = 1_pInt, prm%totalNslip
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dot%crss(j,of) = & ! evolution of slip resistance j
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dot_product(prm%interaction_SlipSlip(j,:),abs(gdot_pos+gdot_neg)) * &
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( prm%theta1(j) + &
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(prm%theta0(j) - prm%theta1(j) &
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dot%crss(j,of) = &
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dot_product(prm%interaction_SlipSlip(j,:),dot%accshear(:,of)) * &
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( prm%theta1(j) + (prm%theta0(j) - prm%theta1(j) &
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+ prm%theta0(j)*prm%theta1(j)*sumGamma/prm%tau1(j)) &
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*exp(-sumGamma*prm%theta0(j)/prm%tau1(j)) & ! V term depending on the harding law
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)
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dot%crss_back(j,of) = & ! evolution of back stress resistance j
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stt%sense(j,of)*abs(gdot_pos(j)+gdot_neg(j)) * &
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( prm%theta1_b(j) + &
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(prm%theta0_b(j) - prm%theta1_b(j) &
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+ prm%theta0_b(j)*prm%theta1_b(j)/(prm%tau1_b(j)+stt%chi0(j,of)) &
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*(stt%accshear(j,of)-state(instance)%gamma0(j,of))) &
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*exp(-(state(instance)%accshear(j,of)-state(instance)%gamma0(j,of)) &
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*prm%theta0_b(j)/(prm%tau1_b(j)+state(instance)%chi0(j,of))) &
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) ! V term depending on the harding law for back stress
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enddo
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dot%crss_back(:,of) = &
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stt%sense(:,of)*dot%accshear(:,of) * &
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( prm%theta1_b + &
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(prm%theta0_b - prm%theta1_b &
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+ prm%theta0_b*prm%theta1_b/(prm%tau1_b+stt%chi0(:,of))*(stt%accshear(:,of)-stt%gamma0(:,of))&
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) &
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*exp(-(stt%accshear(:,of)-stt%gamma0(:,of)) *prm%theta0_b/(prm%tau1_b+stt%chi0(:,of))) &
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) ! V term depending on the harding law for back stress
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enddo
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end associate
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end subroutine plastic_kinehardening_dotState
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