Merge branch 'polishing' into 'development'
Polishing See merge request damask/DAMASK!401
This commit is contained in:
Sharan Roongta
commit
df5f9822f0
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@ -87,7 +87,6 @@ checkout:
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- git checkout $CI_COMMIT_SHA
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- git submodule update --init
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- source env/DAMASK.sh
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- ./installation/symlink_Processing.py
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except:
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- master
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- release
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|
|
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2
PRIVATE
2
PRIVATE
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@ -1 +1 @@
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Subproject commit 6363147d0a8bb45e681c5dc39041828a6b34664e
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Subproject commit 023f86ff9e603dcc8c7adc16545783653083ea83
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@ -16,8 +16,8 @@ phase:
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a_sl: 2.25
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atol_xi: 1.0
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||||
dot_gamma_0_sl: 0.001
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h_0_sl_sl: 75e6
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h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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h_0_sl-sl: 75e6
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h_sl-sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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n_sl: 20
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output: [xi_sl]
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xi_0_sl: [31e6]
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|
|
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@ -19,7 +19,7 @@ TWIP_Steel_FeMnC:
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D_0: 4.0e-5 # Vacancy diffusion prefactor / m^2/s
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D_a: 1.0 # minimum dipole distance / b
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Q_cl: 4.5e-19 # Activation energy for climb / J
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h_sl_sl: [0.122, 0.122, 0.625, 0.07, 0.137, 0.137, 0.122] # Interaction coefficients (Kubin et al. 2008)
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h_sl-sl: [0.122, 0.122, 0.625, 0.07, 0.137, 0.137, 0.122] # Interaction coefficients (Kubin et al. 2008)
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# shear band parameters
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xi_sb: 180.0e6
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Q_sb: 3.7e-19
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@ -35,7 +35,7 @@ TWIP_Steel_FeMnC:
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V_cs: 1.67e-29 # cross slip volume / m^3
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p_tw: [10.0] # r-exponent in twin formation probability
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i_tw: 1.0 # Adj. parameter controlling twin mean free path
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h_sl_tw: [0.0, 1.0, 1.0] # dislocation-twin interaction coefficients
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h_tw_tw: [0.0, 1.0] # twin-twin interaction coefficients
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h_sl-tw: [0.0, 1.0, 1.0] # dislocation-twin interaction coefficients
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h_tw-tw: [0.0, 1.0] # twin-twin interaction coefficients
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Gamma_sf_0K: -0.0396 # stacking fault energy / J/m^2 at zero K; TWIP steel: -0.0526; Cu: -0.0396
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dGamma_sf_dT: 0.0002 # temperature dependence / J/(m^2 K) of stacking fault energy
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@ -18,4 +18,4 @@ Tungsten:
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D_0: 4.0e-5 # Vacancy diffusion prefactor / m^2/s
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D_a: 1.0 # minimum dipole distance / b
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Q_cl: 4.5e-19 # Activation energy for climb / J
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h_sl_sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4]
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h_sl-sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4]
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@ -7,8 +7,8 @@ Aluminum:
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N_sl: [12]
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a_sl: 2.25
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dot_gamma_0_sl: 0.001
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h_0_sl_sl: 75e6
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h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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h_0_sl-sl: 75e6
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h_sl-sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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n_sl: 20
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output: [xi_sl, gamma_sl]
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type: phenopowerlaw
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@ -9,8 +9,8 @@ Ferrite:
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N_sl: [12, 12]
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a_sl: 2.0
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dot_gamma_0_sl: 0.001
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h_0_sl_sl: 1000.0e6
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h_sl_sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4]
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h_0_sl-sl: 1000.0e6
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h_sl-sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4]
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n_sl: 20
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type: phenopowerlaw
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xi_0_sl: [95.e6, 96.e6]
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@ -9,8 +9,8 @@ Martensite:
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N_sl: [12, 12]
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a_sl: 2.0
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dot_gamma_0_sl: 0.001
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h_0_sl_sl: 563.0e9
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h_sl_sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4]
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h_0_sl-sl: 563.0e9
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h_sl-sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4, 1.4]
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n_sl: 20
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type: phenopowerlaw
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xi_0_sl: [405.8e6, 456.7e6]
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@ -8,13 +8,13 @@ Magnesium:
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plastic:
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N_sl: [3, 3, 0, 6, 0, 6]
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N_tw: [6, 0, 0, 6]
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h_0_tw_tw: 50.0e6
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h_0_sl_sl: 500.0e6
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h_0_tw_sl: 150.0e6
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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]
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h_tw_tw: [1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1]
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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]
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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]
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h_0_tw-tw: 50.0e6
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h_0_sl-sl: 500.0e6
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h_0_tw-sl: 150.0e6
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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]
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h_tw-tw: [1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1]
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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]
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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]
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output: [xi_sl, xi_tw]
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type: phenopowerlaw
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xi_0_sl: [10.0e6, 55.0e6, 0, 60.0e6, 0.0, 60.0e6]
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@ -25,4 +25,4 @@ Magnesium:
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dot_gamma_0_tw: 0.001
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n_sl: 20
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n_tw: 20
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f_sat_sl_tw: 10.0
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f_sat_sl-tw: 10.0
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@ -11,8 +11,8 @@ cpTi:
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N_sl: [3, 3, 0, 6, 12]
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a_sl: 2.0
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dot_gamma_0_sl: 0.001
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h_0_sl_sl: 200e6
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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]
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h_0_sl-sl: 200e6
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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]
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n_sl: 20
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output: [gamma_sl]
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type: phenopowerlaw
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@ -18,7 +18,7 @@ q_sl: [1.55, 1.55]
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i_sl: [23.3, 23.3]
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D_a: 7.4 # C_anni
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B: [0.001, 0.001]
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h_sl_sl: [0.1, 0.72, 0.1, 0.053, 0.053, 0.073, 0.137, 0.72, 0.72, 0.053, 0.053, 0.053, 0.053, 0.073, 0.073, 0.073, 0.073, 0.073, 0.073, 0.137, 0.073, 0.073, 0.137, 0.073]
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h_sl-sl: [0.1, 0.72, 0.1, 0.053, 0.053, 0.073, 0.137, 0.72, 0.72, 0.053, 0.053, 0.053, 0.053, 0.073, 0.073, 0.073, 0.073, 0.073, 0.073, 0.137, 0.073, 0.073, 0.137, 0.073]
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D_0: 4.000E-05
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Q_cl: 5.400E-19 # no recovery!
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D: 40e-6 # estimated
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@ -10,8 +10,8 @@ output: [xi_sl, gamma_sl]
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N_sl: [12]
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n_sl: 83.3
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dot_gamma_0_sl: 0.001
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h_0_sl_sl: 75.0e6
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h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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h_0_sl-sl: 75.0e6
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h_sl-sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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a_sl: 1.0
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xi_0_sl: [26.25e6]
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xi_inf_sl: [53.0e6]
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@ -16,8 +16,8 @@ phase:
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a_sl: 2.25
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atol_xi: 1.0
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dot_gamma_0_sl: 0.001
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h_0_sl_sl: 75e6
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h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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h_0_sl-sl: 75e6
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h_sl-sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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n_sl: 20
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output: [xi_sl]
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xi_0_sl: [31e6]
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|
|
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@ -15,8 +15,8 @@ phase:
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a_sl: 2.25
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atol_xi: 1.0
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dot_gamma_0_sl: 0.001
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h_0_sl_sl: 75e6
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h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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h_0_sl-sl: 75e6
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h_sl-sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
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n_sl: 20
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output: [xi_sl]
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xi_0_sl: [31e6]
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|
|
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@ -1,28 +0,0 @@
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#!/usr/bin/env python3
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# Makes postprocessing routines accessible from everywhere.
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import sys
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from pathlib import Path
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import os
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bin_dir = Path(os.environ['DAMASK_ROOT'])/'bin'
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if not bin_dir.exists():
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bin_dir.mkdir()
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sys.stdout.write('\nsymbolic linking...\n')
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||||
for sub_dir in ['pre','post']:
|
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the_dir = Path(os.environ['DAMASK_ROOT'])/'processing'/sub_dir
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for the_file in the_dir.glob('*.py'):
|
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src = the_dir/the_file
|
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dst = bin_dir/Path(the_file.with_suffix('').name)
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if dst.is_file(): dst.unlink() # dst.unlink(True) for Python >3.8
|
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dst.symlink_to(src)
|
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|
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|
||||
sys.stdout.write('\npruning broken links...\n')
|
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for filename in bin_dir.glob('*'):
|
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if not filename.is_file():
|
||||
filename.unlink()
|
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|
|
@ -108,6 +108,10 @@ class ConfigMaterial(Config):
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and grain- or cell-wise data. Defaults to None, in which case
|
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it is set as the path that contains _SIMPL_GEOMETRY/SPACING.
|
||||
|
||||
Notes
|
||||
-----
|
||||
Homogenization and phase entries are emtpy and need to be defined separately.
|
||||
|
||||
Returns
|
||||
-------
|
||||
loaded : damask.ConfigMaterial
|
||||
|
|
|
|||
|
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@ -31,14 +31,15 @@ class Grid:
|
|||
|
||||
Parameters
|
||||
----------
|
||||
material : numpy.ndarray
|
||||
Material index array (3D).
|
||||
size : list or numpy.ndarray
|
||||
Physical size of the grid in meter.
|
||||
origin : list or numpy.ndarray, optional
|
||||
Physical origin of the grid in meter.
|
||||
material : numpy.ndarray of shape (:,:,:)
|
||||
Material indices. The shape of the material array defines
|
||||
the number of cells.
|
||||
size : list or numpy.ndarray of shape (3)
|
||||
Physical size of grid in meter.
|
||||
origin : list or numpy.ndarray of shape (3), optional
|
||||
Coordinates of grid origin in meter.
|
||||
comments : list of str, optional
|
||||
Comment lines.
|
||||
Comments, e.g. history of operations.
|
||||
|
||||
"""
|
||||
self.material = material
|
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|
|
|
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|
|
@ -78,7 +78,7 @@ class Result:
|
|||
>>> r = damask.Result('my_file.hdf5')
|
||||
>>> r.add_Cauchy()
|
||||
>>> r.add_equivalent_Mises('sigma')
|
||||
>>> r.save_VTK()
|
||||
>>> r.export_VTK()
|
||||
>>> r_last = r.view('increments',-1)
|
||||
>>> sigma_vM_last = r_last.get('sigma_vM')
|
||||
|
||||
|
|
@ -1377,13 +1377,13 @@ class Result:
|
|||
pool.join()
|
||||
|
||||
|
||||
def save_XDMF(self,output='*'):
|
||||
def export_XDMF(self,output='*'):
|
||||
"""
|
||||
Write XDMF file to directly visualize data in DADF5 file.
|
||||
|
||||
The XDMF format is only supported for structured grids
|
||||
with single phase and single constituent.
|
||||
For other cases use `save_VTK`.
|
||||
For other cases use `export_VTK`.
|
||||
|
||||
Parameters
|
||||
----------
|
||||
|
|
@ -1511,7 +1511,7 @@ class Result:
|
|||
return at_cell_ph,in_data_ph,at_cell_ho,in_data_ho
|
||||
|
||||
|
||||
def save_VTK(self,output='*',mode='cell',constituents=None,fill_float=np.nan,fill_int=0,parallel=True):
|
||||
def export_VTK(self,output='*',mode='cell',constituents=None,fill_float=np.nan,fill_int=0,parallel=True):
|
||||
"""
|
||||
Export to VTK cell/point data.
|
||||
|
||||
|
|
@ -1549,7 +1549,7 @@ class Result:
|
|||
else:
|
||||
raise ValueError(f'invalid mode {mode}')
|
||||
|
||||
v.set_comments(util.execution_stamp('Result','save_VTK'))
|
||||
v.set_comments(util.execution_stamp('Result','export_VTK'))
|
||||
|
||||
N_digits = int(np.floor(np.log10(max(1,int(self.increments[-1][10:])))))+1
|
||||
|
||||
|
|
@ -1732,3 +1732,6 @@ class Result:
|
|||
if flatten: r = util.dict_flatten(r)
|
||||
|
||||
return None if (type(r) == dict and r == {}) else r
|
||||
|
||||
save_VTK = export_VTK
|
||||
save_XDMF = export_XDMF
|
||||
|
|
|
|||
|
|
@ -588,9 +588,11 @@ class _ProgressBar:
|
|||
fraction = (iteration+1) / self.total
|
||||
filled_length = int(self.bar_length * fraction)
|
||||
|
||||
if filled_length > int(self.bar_length * self.last_fraction):
|
||||
delta_time = datetime.datetime.now() - self.start_time
|
||||
|
||||
if filled_length > int(self.bar_length * self.last_fraction) or \
|
||||
delta_time > datetime.timedelta(minutes=1):
|
||||
bar = '█' * filled_length + '░' * (self.bar_length - filled_length)
|
||||
delta_time = datetime.datetime.now() - self.start_time
|
||||
remaining_time = (self.total - (iteration+1)) * delta_time / (iteration+1)
|
||||
remaining_time -= datetime.timedelta(microseconds=remaining_time.microseconds) # remove μs
|
||||
sys.stderr.write(f'\r{self.prefix} {bar} {fraction:>4.0%} ETA {remaining_time}')
|
||||
|
|
|
|||
|
|
@ -15,8 +15,8 @@ phase:
|
|||
a_sl: 2.25
|
||||
atol_xi: 1.0
|
||||
dot_gamma_0_sl: 0.001
|
||||
h_0_sl_sl: 75e6
|
||||
h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
|
||||
h_0_sl-sl: 75e6
|
||||
h_sl-sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
|
||||
n_sl: 20
|
||||
output: [xi_sl]
|
||||
type: phenopowerlaw
|
||||
|
|
@ -32,8 +32,8 @@ phase:
|
|||
a_sl: 2.25
|
||||
atol_xi: 1.0
|
||||
dot_gamma_0_sl: 0.001
|
||||
h_0_sl_sl: 75e6
|
||||
h_sl_sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4]
|
||||
h_0_sl-sl: 75e6
|
||||
h_sl-sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4]
|
||||
n_sl: 20
|
||||
output: [xi_sl]
|
||||
type: phenopowerlaw
|
||||
|
|
|
|||
|
|
@ -647,8 +647,8 @@ phase:
|
|||
a_sl: 2.25
|
||||
atol_xi: 1.0
|
||||
dot_gamma_0_sl: 0.001
|
||||
h_0_sl_sl: 75e6
|
||||
h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4]
|
||||
h_0_sl-sl: 75e6
|
||||
h_sl-sl: [1, 1, 1.4, 1.4, 1.4, 1.4]
|
||||
n_sl: 20
|
||||
output: [xi_sl]
|
||||
type: phenopowerlaw
|
||||
|
|
@ -664,8 +664,8 @@ phase:
|
|||
a_sl: 2.25
|
||||
atol_xi: 1.0
|
||||
dot_gamma_0_sl: 0.001
|
||||
h_0_sl_sl: 75e6
|
||||
h_sl_sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4]
|
||||
h_0_sl-sl: 75e6
|
||||
h_sl-sl: [1, 1.4, 1, 1.4, 1.4, 1.4, 1.4]
|
||||
n_sl: 20
|
||||
output: [xi_sl]
|
||||
type: phenopowerlaw
|
||||
|
|
|
|||
|
|
@ -15,8 +15,8 @@ phase:
|
|||
a_sl: 2.25
|
||||
atol_xi: 1.0
|
||||
dot_gamma_0_sl: 0.001
|
||||
h_0_sl_sl: 75e6
|
||||
h_sl_sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
|
||||
h_0_sl-sl: 75e6
|
||||
h_sl-sl: [1, 1, 1.4, 1.4, 1.4, 1.4, 1.4]
|
||||
n_sl: 20
|
||||
output: [xi_sl]
|
||||
type: phenopowerlaw
|
||||
|
|
|
|||
|
|
@ -0,0 +1 @@
|
|||
d5db0be324a959f00245e42704ea2d6f
|
||||
|
|
@ -0,0 +1 @@
|
|||
fe9ddaf54ac1fb785094251d29fcdc9c
|
||||
|
|
@ -0,0 +1 @@
|
|||
9c8ac0bb1eb4a7b9ebc3e5fd5840b0a4
|
||||
|
|
@ -0,0 +1 @@
|
|||
1b9ebd17c5257e2edba48d006f25d4e6
|
||||
|
|
@ -0,0 +1 @@
|
|||
8967bb1a6c329a072baaa83da534ae56
|
||||
|
|
@ -0,0 +1 @@
|
|||
752e8b6186ad2b6b1b5c781940669cb1
|
||||
|
|
@ -1 +0,0 @@
|
|||
6d4da1188f1de0a80142692e9e135aed
|
||||
|
|
@ -1 +0,0 @@
|
|||
5926c1f393871ee942750069545798a7
|
||||
|
|
@ -1 +0,0 @@
|
|||
743c9a868d54b78ee0648613249a0bdc
|
||||
|
|
@ -1 +0,0 @@
|
|||
09f5a7a6dd7a8e7d30e47aec07f7f616
|
||||
|
|
@ -1 +0,0 @@
|
|||
5715cfc5fc21c6d04590354f0941cf7b
|
||||
|
|
@ -1 +0,0 @@
|
|||
2f7b43ea8fe65173f47acb8281f0a919
|
||||
|
|
@ -369,7 +369,7 @@ class TestResult:
|
|||
def test_vtk(self,request,tmp_path,ref_path,update,patch_execution_stamp,patch_datetime_now,output,fname,inc):
|
||||
result = Result(ref_path/fname).view('increments',inc)
|
||||
os.chdir(tmp_path)
|
||||
result.save_VTK(output)
|
||||
result.export_VTK(output)
|
||||
fname = fname.split('.')[0]+f'_inc{(inc if type(inc) == int else inc[0]):0>2}.vti'
|
||||
last = ''
|
||||
for i in range(10):
|
||||
|
|
@ -382,9 +382,9 @@ class TestResult:
|
|||
last = cur
|
||||
time.sleep(.5)
|
||||
if update:
|
||||
with open((ref_path/'save_VTK'/request.node.name).with_suffix('.md5'),'w') as f:
|
||||
with open((ref_path/'export_VTK'/request.node.name).with_suffix('.md5'),'w') as f:
|
||||
f.write(cur)
|
||||
with open((ref_path/'save_VTK'/request.node.name).with_suffix('.md5')) as f:
|
||||
with open((ref_path/'export_VTK'/request.node.name).with_suffix('.md5')) as f:
|
||||
assert cur == f.read()
|
||||
|
||||
@pytest.mark.parametrize('mode',['point','cell'])
|
||||
|
|
@ -392,7 +392,7 @@ class TestResult:
|
|||
def test_vtk_marc(self,tmp_path,ref_path,mode,output):
|
||||
os.chdir(tmp_path)
|
||||
result = Result(ref_path/'check_compile_job1.hdf5')
|
||||
result.save_VTK(output,mode)
|
||||
result.export_VTK(output,mode)
|
||||
|
||||
def test_marc_coordinates(self,ref_path):
|
||||
result = Result(ref_path/'check_compile_job1.hdf5').view('increments',-1)
|
||||
|
|
@ -403,7 +403,7 @@ class TestResult:
|
|||
@pytest.mark.parametrize('mode',['point','cell'])
|
||||
def test_vtk_mode(self,tmp_path,single_phase,mode):
|
||||
os.chdir(tmp_path)
|
||||
single_phase.save_VTK(mode=mode)
|
||||
single_phase.export_VTK(mode=mode)
|
||||
|
||||
def test_XDMF_datatypes(self,tmp_path,single_phase,update,ref_path):
|
||||
for shape in [('scalar',()),('vector',(3,)),('tensor',(3,3)),('matrix',(12,))]:
|
||||
|
|
@ -411,9 +411,7 @@ class TestResult:
|
|||
single_phase.add_calculation(f"np.ones(np.shape(#F#)[0:1]+{shape[1]},'{dtype}')",f'{shape[0]}_{dtype}')
|
||||
fname = os.path.splitext(os.path.basename(single_phase.fname))[0]+'.xdmf'
|
||||
os.chdir(tmp_path)
|
||||
|
||||
single_phase.save_XDMF()
|
||||
|
||||
single_phase.export_XDMF()
|
||||
if update:
|
||||
shutil.copy(tmp_path/fname,ref_path/fname)
|
||||
|
||||
|
|
@ -423,7 +421,7 @@ class TestResult:
|
|||
def test_XDMF_shape(self,tmp_path,single_phase):
|
||||
os.chdir(tmp_path)
|
||||
|
||||
single_phase.save_XDMF()
|
||||
single_phase.export_XDMF()
|
||||
fname = os.path.splitext(os.path.basename(single_phase.fname))[0]+'.xdmf'
|
||||
reader_xdmf = vtk.vtkXdmfReader()
|
||||
reader_xdmf.SetFileName(fname)
|
||||
|
|
@ -431,7 +429,7 @@ class TestResult:
|
|||
dim_xdmf = reader_xdmf.GetOutput().GetDimensions()
|
||||
bounds_xdmf = reader_xdmf.GetOutput().GetBounds()
|
||||
|
||||
single_phase.view('increments',0).save_VTK()
|
||||
single_phase.view('increments',0).export_VTK()
|
||||
fname = os.path.splitext(os.path.basename(single_phase.fname))[0]+'_inc00.vti'
|
||||
for i in range(10): # waiting for parallel IO
|
||||
reader_vti = vtk.vtkXMLImageDataReader()
|
||||
|
|
@ -447,7 +445,7 @@ class TestResult:
|
|||
|
||||
def test_XDMF_invalid(self,default):
|
||||
with pytest.raises(TypeError):
|
||||
default.save_XDMF()
|
||||
default.export_XDMF()
|
||||
|
||||
@pytest.mark.parametrize('view,output,flatten,prune',
|
||||
[({},['F','P','F','L_p','F_e','F_p'],True,True),
|
||||
|
|
|
|||
|
|
@ -149,7 +149,7 @@ module function plastic_dislotungsten_init() result(myPlasticity)
|
|||
prm%nonSchmid_neg = prm%P_sl
|
||||
endif
|
||||
|
||||
prm%h_sl_sl = lattice_interaction_SlipBySlip(N_sl,pl%get_as1dFloat('h_sl_sl'), &
|
||||
prm%h_sl_sl = lattice_interaction_SlipBySlip(N_sl,pl%get_as1dFloat('h_sl-sl'), &
|
||||
phase%get_asString('lattice'))
|
||||
prm%forestProjection = lattice_forestProjection_edge(N_sl,phase%get_asString('lattice'),&
|
||||
phase%get_asFloat('c/a',defaultVal=0.0_pReal))
|
||||
|
|
|
|||
|
|
@ -194,7 +194,7 @@ module function plastic_dislotwin_init() result(myPlasticity)
|
|||
slipActive: if (prm%sum_N_sl > 0) then
|
||||
prm%P_sl = lattice_SchmidMatrix_slip(N_sl,phase%get_asString('lattice'),&
|
||||
phase%get_asFloat('c/a',defaultVal=0.0_pReal))
|
||||
prm%h_sl_sl = lattice_interaction_SlipBySlip(N_sl,pl%get_as1dFloat('h_sl_sl'), &
|
||||
prm%h_sl_sl = lattice_interaction_SlipBySlip(N_sl,pl%get_as1dFloat('h_sl-sl'), &
|
||||
phase%get_asString('lattice'))
|
||||
prm%forestProjection = lattice_forestProjection_edge(N_sl,phase%get_asString('lattice'),&
|
||||
phase%get_asFloat('c/a',defaultVal=0.0_pReal))
|
||||
|
|
@ -271,7 +271,7 @@ module function plastic_dislotwin_init() result(myPlasticity)
|
|||
prm%P_tw = lattice_SchmidMatrix_twin(N_tw,phase%get_asString('lattice'),&
|
||||
phase%get_asFloat('c/a',defaultVal=0.0_pReal))
|
||||
prm%h_tw_tw = lattice_interaction_TwinByTwin(N_tw,&
|
||||
pl%get_as1dFloat('h_tw_tw'), &
|
||||
pl%get_as1dFloat('h_tw-tw'), &
|
||||
phase%get_asString('lattice'))
|
||||
|
||||
prm%b_tw = pl%get_as1dFloat('b_tw', requiredSize=size(N_tw))
|
||||
|
|
@ -327,7 +327,7 @@ module function plastic_dislotwin_init() result(myPlasticity)
|
|||
prm%x_c_tr = pl%get_asFloat('x_c_tr', defaultVal=0.0_pReal) ! ToDo: How to handle that???
|
||||
prm%L_tr = pl%get_asFloat('L_tr')
|
||||
|
||||
prm%h_tr_tr = lattice_interaction_TransByTrans(N_tr,pl%get_as1dFloat('h_tr_tr'), &
|
||||
prm%h_tr_tr = lattice_interaction_TransByTrans(N_tr,pl%get_as1dFloat('h_tr-tr'), &
|
||||
phase%get_asString('lattice'))
|
||||
|
||||
prm%C66_tr = lattice_C66_trans(N_tr,prm%C66,pl%get_asString('lattice_tr'), &
|
||||
|
|
@ -392,14 +392,14 @@ module function plastic_dislotwin_init() result(myPlasticity)
|
|||
|
||||
slipAndTwinActive: if (prm%sum_N_sl * prm%sum_N_tw > 0) then
|
||||
prm%h_sl_tw = lattice_interaction_SlipByTwin(N_sl,N_tw,&
|
||||
pl%get_as1dFloat('h_sl_tw'), &
|
||||
pl%get_as1dFloat('h_sl-tw'), &
|
||||
phase%get_asString('lattice'))
|
||||
if (prm%fccTwinTransNucleation .and. size(N_tw) /= 1) extmsg = trim(extmsg)//' interaction_sliptwin'
|
||||
endif slipAndTwinActive
|
||||
|
||||
slipAndTransActive: if (prm%sum_N_sl * prm%sum_N_tr > 0) then
|
||||
prm%h_sl_tr = lattice_interaction_SlipByTrans(N_sl,N_tr,&
|
||||
pl%get_as1dFloat('h_sl_tr'), &
|
||||
pl%get_as1dFloat('h_sl-tr'), &
|
||||
phase%get_asString('lattice'))
|
||||
if (prm%fccTwinTransNucleation .and. size(N_tr) /= 1) extmsg = trim(extmsg)//' interaction_sliptrans'
|
||||
endif slipAndTransActive
|
||||
|
|
|
|||
|
|
@ -125,7 +125,7 @@ module function plastic_kinehardening_init() result(myPlasticity)
|
|||
prm%nonSchmid_neg = prm%P
|
||||
endif
|
||||
prm%interaction_SlipSlip = lattice_interaction_SlipBySlip(N_sl, &
|
||||
pl%get_as1dFloat('h_sl_sl'), &
|
||||
pl%get_as1dFloat('h_sl-sl'), &
|
||||
phase%get_asString('lattice'))
|
||||
|
||||
xi_0 = pl%get_as1dFloat('xi_0', requiredSize=size(N_sl))
|
||||
|
|
|
|||
|
|
@ -261,7 +261,7 @@ module function plastic_nonlocal_init() result(myPlasticity)
|
|||
endif
|
||||
|
||||
prm%h_sl_sl = lattice_interaction_SlipBySlip(ini%N_sl, &
|
||||
pl%get_as1dFloat('h_sl_sl'), &
|
||||
pl%get_as1dFloat('h_sl-sl'), &
|
||||
phase%get_asString('lattice'))
|
||||
|
||||
prm%forestProjection_edge = lattice_forestProjection_edge (ini%N_sl,phase%get_asString('lattice'),&
|
||||
|
|
|
|||
|
|
@ -128,7 +128,7 @@ module function plastic_phenopowerlaw_init() result(myPlasticity)
|
|||
prm%nonSchmid_neg = prm%P_sl
|
||||
endif
|
||||
prm%h_sl_sl = lattice_interaction_SlipBySlip(N_sl, &
|
||||
pl%get_as1dFloat('h_sl_sl'), &
|
||||
pl%get_as1dFloat('h_sl-sl'), &
|
||||
phase%get_asString('lattice'))
|
||||
|
||||
xi_0_sl = pl%get_as1dFloat('xi_0_sl', requiredSize=size(N_sl))
|
||||
|
|
@ -139,7 +139,7 @@ module function plastic_phenopowerlaw_init() result(myPlasticity)
|
|||
prm%dot_gamma_0_sl = pl%get_asFloat('dot_gamma_0_sl')
|
||||
prm%n_sl = pl%get_asFloat('n_sl')
|
||||
prm%a_sl = pl%get_asFloat('a_sl')
|
||||
prm%h_0_sl_sl = pl%get_asFloat('h_0_sl_sl')
|
||||
prm%h_0_sl_sl = pl%get_asFloat('h_0_sl-sl')
|
||||
|
||||
! expand: family => system
|
||||
xi_0_sl = math_expand(xi_0_sl, N_sl)
|
||||
|
|
@ -167,7 +167,7 @@ module function plastic_phenopowerlaw_init() result(myPlasticity)
|
|||
prm%P_tw = lattice_SchmidMatrix_twin(N_tw,phase%get_asString('lattice'),&
|
||||
phase%get_asFloat('c/a',defaultVal=0.0_pReal))
|
||||
prm%h_tw_tw = lattice_interaction_TwinByTwin(N_tw,&
|
||||
pl%get_as1dFloat('h_tw_tw'), &
|
||||
pl%get_as1dFloat('h_tw-tw'), &
|
||||
phase%get_asString('lattice'))
|
||||
prm%gamma_char = lattice_characteristicShear_twin(N_tw,phase%get_asString('lattice'),&
|
||||
phase%get_asFloat('c/a',defaultVal=0.0_pReal))
|
||||
|
|
@ -180,8 +180,8 @@ module function plastic_phenopowerlaw_init() result(myPlasticity)
|
|||
prm%c_4 = pl%get_asFloat('c_4',defaultVal=0.0_pReal)
|
||||
prm%dot_gamma_0_tw = pl%get_asFloat('dot_gamma_0_tw')
|
||||
prm%n_tw = pl%get_asFloat('n_tw')
|
||||
prm%f_sat_sl_tw = pl%get_asFloat('f_sat_sl_tw')
|
||||
prm%h_0_tw_tw = pl%get_asFloat('h_0_tw_tw')
|
||||
prm%f_sat_sl_tw = pl%get_asFloat('f_sat_sl-tw')
|
||||
prm%h_0_tw_tw = pl%get_asFloat('h_0_tw-tw')
|
||||
|
||||
! expand: family => system
|
||||
xi_0_tw = math_expand(xi_0_tw,N_tw)
|
||||
|
|
@ -199,12 +199,12 @@ module function plastic_phenopowerlaw_init() result(myPlasticity)
|
|||
!--------------------------------------------------------------------------------------------------
|
||||
! slip-twin related parameters
|
||||
slipAndTwinActive: if (prm%sum_N_sl > 0 .and. prm%sum_N_tw > 0) then
|
||||
prm%h_0_tw_sl = pl%get_asFloat('h_0_tw_sl')
|
||||
prm%h_0_tw_sl = pl%get_asFloat('h_0_tw-sl')
|
||||
prm%h_sl_tw = lattice_interaction_SlipByTwin(N_sl,N_tw,&
|
||||
pl%get_as1dFloat('h_sl_tw'), &
|
||||
pl%get_as1dFloat('h_sl-tw'), &
|
||||
phase%get_asString('lattice'))
|
||||
prm%h_tw_sl = lattice_interaction_TwinBySlip(N_tw,N_sl,&
|
||||
pl%get_as1dFloat('h_tw_sl'), &
|
||||
pl%get_as1dFloat('h_tw-sl'), &
|
||||
phase%get_asString('lattice'))
|
||||
else slipAndTwinActive
|
||||
allocate(prm%h_sl_tw(prm%sum_N_sl,prm%sum_N_tw)) ! at least one dimension is 0
|
||||
|
|
|
|||
Loading…
Reference in New Issue