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DAMASK_EICMD
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in crystallite_integrateStress: pass full 2nd PK stress to LpAndItsTangent instead of only the deviatoric part; otherwise constitutive laws that depend on the hydrostatic pressure do not work; constitutive laws that require a deviatoric stress need to calculate it internally (as is e.g. already done in the J2 model)

This commit is contained in:
Christoph Kords 2014-01-16 10:36:40 +00:00
parent a011b0a4a2
commit 77cba87bf3
1 changed files with 2 additions and 5 deletions
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code/crystallite.f90
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@ -3131,8 +3131,6 @@ logical function crystallite_integrateStress(&
Fe = math_mul33x33(A,B) ! current elastic deformation tensor
call constitutive_TandItsTangent(Tstar, dT_dFe3333, Fe, g,i,e) ! call constitutive law to calculate 2nd Piola-Kirchhoff stress and its derivative
Tstar_v = math_Mandel33to6(Tstar)
p_hydro = sum(Tstar_v(1:3)) / 3.0_pReal
forall(n=1_pInt:3_pInt) Tstar_v(n) = Tstar_v(n) - p_hydro ! get deviatoric stress tensor
!* calculate plastic velocity gradient and its tangent from constitutive law
@ -3197,7 +3195,7 @@ logical function crystallite_integrateStress(&
if (mod(jacoCounter, iJacoLpresiduum) == 0_pInt) then
dFe_dLp3333 = 0.0_pReal
do o=1_pInt,3_pInt; do p=1_pInt,3_pInt
dFe_dLp3333(p,o,1:3,p) = A(o,1:3) ! dFe_dLp(i,j,k,l) = -dt * A(i,k) delta(j,l)
dFe_dLp3333(p,o,1:3,p) = A(o,1:3) ! dFe_dLp(i,j,k,l) = -dt * A(i,k) delta(l,j)
enddo; enddo
dFe_dLp3333 = -dt * dFe_dLp3333
dFe_dLp = math_Plain3333to99(dFe_dLp3333)
@ -3262,9 +3260,8 @@ logical function crystallite_integrateStress(&
Fe_new = math_mul33x33(Fg_new,invFp_new) ! calc resulting Fe
!* add volumetric component to 2nd Piola-Kirchhoff stress and calculate 1st Piola-Kirchhoff stress
!* calculate 1st Piola-Kirchhoff stress
forall (n=1_pInt:3_pInt) Tstar_v(n) = Tstar_v(n) + p_hydro
crystallite_P(1:3,1:3,g,i,e) = math_mul33x33(Fe_new, math_mul33x33(math_Mandel6to33(Tstar_v), &
math_transpose33(invFp_new)))