Merge remote-tracking branch 'origin/master' into generalize-configmaterial

This commit is contained in:
Martin Diehl 2021-02-24 00:46:16 +01:00
commit ec2fbdc882
21 changed files with 99 additions and 176 deletions

@ -1 +1 @@
Subproject commit e214896b6a5402bea8113cc89a7e86c9b59ed713
Subproject commit a8e76a140f3f08a4dcfd3858d4b722cacd2bb2fd

View File

@ -1 +1 @@
v3.0.0-alpha2-486-g23a3354ac
v3.0.0-alpha2-520-g5ee538a38

View File

@ -1,8 +0,0 @@
[SX]
type isostrain
Ngrains 1
{./Homogenization_Damage_NonLocal.config}
{./Homogenization_Thermal_Conduction.config}
{./Homogenization_VacancyFlux_CahnHilliard.config}
{./Homogenization_Porosity_PhaseField.config}
{./Homogenization_HydrogenFlux_CahnHilliard.config}

View File

@ -1,9 +1,9 @@
# Kuo, J. C., Mikrostrukturmechanik von Bikristallen mit Kippkorngrenzen. Shaker-Verlag 2004. http://edoc.mpg.de/204079
Aluminum:
lattice: aP
mechanics:
lattice: aP
elasticity: {C_11: 110.9e9, C_12: 58.34e9, type: hooke}
output: [F, P, Fe, Fp, Lp]
output: [F, P, F_e, F_p, L_p]
elasticity: {type: hooke, C_11: 110.9e9, C_12: 58.34e9}
plasticity:
type: isotropic
output: [xi]

View File

@ -1,9 +1,8 @@
# Maiti and Eisenlohr 2018 Scripta Materialia
Air:
lattice: aP
mechanics:
lattice: aP
elasticity: {C_11: 10e9, C_12: 0.0, type: hooke}
output: [F, P, Fe, Fp, Lp]
output: [F, P, F_e, F_p, L_p]
elasticity: {type: hooke, C_11: 1e8, C_12: 1e6}
plasticity:
type: isotropic
output: [xi]
@ -14,4 +13,4 @@ Air:
M: 3
h_0: 1e6
a: 2
dilatation: true
dilatation: True

View File

@ -1,21 +0,0 @@
[Aluminum]
elasticity hooke
plasticity phenopowerlaw
(output) resistance_slip
(output) accumulatedshear_slip
lattice_structure fcc
Nslip 12 # per family
c11 106.75e9
c12 60.41e9
c44 28.34e9
gdot0_slip 0.001
n_slip 20
tau0_slip 31e6 # per family
tausat_slip 63e6 # per family
a_slip 2.25
h0_slipslip 75e6
interaction_slipslip 1 1 1.4 1.4 1.4 1.4

View File

@ -0,0 +1,16 @@
Aluminum:
lattice: cF
mechanics:
output: [F, P, F_e, F_p, L_p, O]
elasticity: {C_11: 106.75e9, C_12: 60.41e9, C_44: 28.34e9, type: hooke}
plasticity:
N_sl: [12]
a_sl: 2.25
dot_gamma_0_sl: 0.001
h_0_sl_sl: 75e6
h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4]
n_sl: 20
output: [xi_sl, gamma_sl]
type: phenopowerlaw
xi_0_sl: [31e6]
xi_inf_sl: [63e6]

View File

@ -2,8 +2,8 @@
# Tasan et.al. 2015 International Journal of Plasticity
# Diehl et.al. 2015 Meccanica
Ferrite:
lattice: cI
mechanics:
lattice: cI
elasticity: {C_11: 233.3e9, C_12: 135.5e9, C_44: 118.0e9, type: hooke}
plasticity:
N_sl: [12, 12]

View File

@ -2,8 +2,8 @@
# Tasan et.al. 2015 International Journal of Plasticity
# Diehl et.al. 2015 Meccanica
Martensite:
lattice: cI
mechanics:
lattice: cI
elasticity: {C_11: 417.4e9, C_12: 242.4e9, C_44: 211.1e9, type: hooke}
plasticity:
N_sl: [12, 12]

View File

@ -1,27 +0,0 @@
# parameters fitted by D. Ma to:
# I. Kovács, G. Vörös
# On the mathematical description of the tensile stress-strain curves of polycrystalline face centered cubic metals
# International Journal of Plasticity, Volume 12, Issue 1, 1996, Pages 3543
# DOI: 10.1016/S0749-6419(95)00043-7
[gold_phenopowerlaw]
elasticity hooke
plasticity phenopowerlaw
(output) resistance_slip
lattice_structure fcc
Nslip 12 # per family
c11 191.0e9
c12 162.0e9
c44 42.20e9
gdot0_slip 0.001
n_slip 83.3
tau0_slip 26.25e6 # per family
tausat_slip 53.00e6 # per family
a_slip 1.0
h0_slipslip 75e6
interaction_slipslip 1 1 1.4 1.4 1.4 1.4

View File

@ -0,0 +1,21 @@
# parameters fitted by D. Ma to:
# On the mathematical description of the tensile stress-strain curves of polycrystalline face centered cubic metals
# International Journal of Plasticity, Volume 12, Issue 1, 1996, Pages 35-43
# DOI: 10.1016/S0749-6419(95)00043-7
Gold:
lattice: cF
mechanics:
output: [F, P, F_e, F_p, L_p, O]
elasticity: {type: hooke, C_11: 191e9, C_12: 162e9, C_44: 42.2e9}
plasticity:
type: phenopowerlaw
output: [xi_sl]
N_sl: [12]
n_sl: 83
dot_gamma_0_sl: 0.001
h_0_sl_sl: 75e6
h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4]
a_sl: 1.0
xi_0_sl: [26e6]
xi_inf_sl: [53e6]

View File

@ -1,56 +0,0 @@
#-------------------#
<phase>
#-------------------#
/echo/
[Mg]
plasticity phenopowerlaw
elasticity hooke
(output) resistance_slip
(output) resistance_twin
lattice_structure hex
c/a 1.62350 # from Tromans 2011, Elastic Anisotropy of HCP Metal Crystals and Polycrystals
c11 59.3e9 # - " -
c33 61.5e9 # - " -
c44 16.4e9 # - " -
c12 25.7e9 # - " -
c13 21.4e9 # - " -
# basal prism prism pyr(a) pyr(c+a) pyr(c+a)
Nslip 3 3 0 6 0 6 # from Agnew et al 2006, Validating a polycrystal model for the elastoplastic response of mg alloy AZ32 using in situ neutron diffraction
# T1 C1 T2 C2
Ntwin 6 0 0 6 # - " -
# basal prism prism pyr(a) pyr(c+a) pyr(c+a)
tau0_slip 10.0e6 55.0e6 0 60.0e6 0.0 60.0e6 # - " - table 1, pyr(a) set to pyr(c+a)
tausat_slip 40.0e6 135.0e6 0 150.0e6 0.0 150.0e6 # - " - table 1, pyr(a) set to pyr(c+a)
# T1 C1 T2 C2
tau0_twin 40e6 0.0 0.0 60.0e6 # - " - table 1, compressive twin guessed by Steffi, tensile twin modified to match experimental results
h0_twintwin 50.0e6 # - " - table 1, same range as theta_0
h0_slipslip 500.0e6 # - " - table 1, same range as theta_0
h0_twinslip 150.0e6 # guessing
interaction_slipslip 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 # just guessing
interaction_twintwin 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 # - " -
interaction_sliptwin 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 # - " -
interaction_twinslip 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 # - " -
####################################################
# open for discussion
####################################################
n_twin 20
n_slip 20
gdot0_twin 0.001
gdot0_slip 0.001
twin_b 0
twin_c 0
twin_d 20
twin_e 20
a_slip 2.25
s_pr 10.0 # push-up factor for slip saturation due to twinning

View File

@ -0,0 +1,31 @@
# Tromans 2011, Elastic Anisotropy of HCP Metal Crystals and Polycrystals
Magnesium:
lattice: hP
c/a: 1.62350
mechanics:
output: [F, P, F_e, F_p, L_p, O]
elasticity: {C_11: 59.3e9, C_12: 25.7e9, C_13: 21.4e9, C_33: 61.5e9, C_44: 16.4e9, type: hooke}
plasticity:
N_sl: [3, 3, 0, 6, 0, 6]
N_tw: [6, 0, 0, 6]
h_0_tw_tw: 50.0e6
h_0_sl_sl: 500.0e6
h_0_tw_sl: 150.0e6
h_sl_sl: [1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1]
h_tw_tw: [1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1]
h_sl_tw: [1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1]
h_tw_sl: [1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1]
output: [xi_sl, xi_tw]
type: phenopowerlaw
xi_0_sl: [10.0e6, 55.0e6, 0, 60.0e6, 0.0, 60.0e6]
xi_inf_sl: [40.0e6, 135.0e6, 0, 150.0e6, 0.0, 150.0e6]
xi_0_tw: [40e6, 0.0, 0.0, 60.0e6]
####################################################
# open for discussion
####################################################
a_sl: 2.25
dot_gamma_0_sl: 0.001
dot_gamma_0_tw: 0.001
n_sl: 20
n_tw: 20
f_sl_sat_tw: 10.0

View File

@ -1,23 +0,0 @@
[cpTi-alpha]
plasticity phenopowerlaw
elasticity hooke
lattice_structure hex
covera_ratio 1.587
# M. Levy, Handbook of Elastic Properties of Solids, Liquids, and Gases (2001)
c11 160.0e9
c12 90.0e9
c13 66.0e9
c33 181.7e9
c44 46.5e9
# C. Zambaldi, "Orientation informed nanoindentation of a-titanium: Indentation pileup in hexagonal metals deforming by prismatic slip", J. Mater. Res., Vol. 27, No. 1, Jan 14, 2012
gdot0_slip 0.001
n_slip 20
nslip 3 3 0 6
tau0_slip 349.3e6 150e6 0 1107.9e6
tausat_slip 568.6e6 1502.2e6 0 3420.1e6
a_slip 2
h0_slipslip 15e6
interaction_slipslip 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1

View File

@ -0,0 +1,19 @@
# M. Levy, Handbook of Elastic Properties of Solids, Liquids, and Gases (2001)
# C. Zambaldi, "Orientation informed nanoindentation of a-titanium: Indentation pileup in hexagonal metals deforming by prismatic slip", J. Mater. Res., Vol. 27, No. 1, Jan 14, 2012
Ti-alpha:
lattice: hP
c/a: 1.587
mechanics:
output: [F, P, F_e, F_p, L_p, O]
elasticity: {C_11: 160.0e9, C_12: 90.0e9, C_13: 66.0e9, C_33: 181.7e9, C_44: 46.5e9, type: hooke}
plasticity:
N_sl: [3, 3, 0, 0, 12]
a_sl: 2.0
dot_gamma_0_sl: 0.001
h_0_sl_sl: 200e6
h_sl_sl: [1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1]
n_sl: 20
output: [gamma_sl]
type: phenopowerlaw
xi_0_sl: [349e6, 150e6, 0, 0, 1107e6]
xi_inf_sl: [568e6, 1502e6, 0, 0, 3420e6]

View File

@ -1,2 +0,0 @@
[001]
(gauss) phi1 0.000 Phi 0.000 phi2 0.000

View File

@ -1,2 +0,0 @@
[101]
(gauss) phi1 0.000 Phi 45.000 phi2 90.000

View File

@ -1,2 +0,0 @@
[111]
(gauss) phi1 0.000 Phi 54.7356 phi2 45.000

View File

@ -1,2 +0,0 @@
[123]
(gauss) phi1 209.805 Phi 29.206 phi2 63.435

View File

@ -1,20 +0,0 @@
# The material.config file needs to specify five parts:
# homogenization, microstructure, crystallite, phase, and texture.
# You can either put the full text in here or include suited separate files
<homogenization>
{./Homogenization_Isostrain_SX.config}
<microstructure>
[one_only]
crystallite 1
(constituent) phase 1 texture 1 fraction 1.0
<crystallite>
{./Crystallite_All.config}
<phase>
{./Phase_Phenopowerlaw_Aluminum.config}
<texture>
{./Texture_Gauss_001.config}

View File

@ -225,8 +225,8 @@ program DAMASK_grid
loadCases(l)%t = step_discretization%get_asFloat('t')
loadCases(l)%N = step_discretization%get_asInt ('N')
loadCases(l)%r = step_discretization%get_asFloat('r', defaultVal= 1.0_pReal)
loadCases(l)%f_restart = step_discretization%get_asInt ('f_restart', defaultVal=huge(0))
loadCases(l)%f_restart = load_step%get_asInt('f_restart', defaultVal=huge(0))
loadCases(l)%f_out = load_step%get_asInt('f_out', defaultVal=1)
loadCases(l)%estimate_rate = (load_step%get_asBool('estimate_rate',defaultVal=.true.) .and. &
merge(.true.,.false.,l > 1))