Add DENIM incomplete-physics closure dataset and evidence
Browse filesAdds the 128-trajectory three-memory-to-two-memory closure cohort, DENIM versus GRU/J2 metrics, time-step and structural deployment gates, figures, source and reproducibility documentation.
- DENIM_REPRODUCE.md +16 -0
- DENIM_START_HERE.md +29 -0
- README.md +35 -2
- SHA256SUMS +23 -120
- artifacts/t2_graybox_closure_v1/closure_summary.png +3 -0
- artifacts/t2_graybox_closure_v1/deployment_validation.json +43 -0
- artifacts/t2_graybox_closure_v1/model_metrics.json +938 -0
- artifacts/t2_graybox_closure_v1/structural_reaction_comparison.png +3 -0
- data/t2_graybox_closure_v1/cohort.h5 +3 -0
- data/t2_graybox_closure_v1/manifest.json +39 -0
- docs/T2_GRAYBOX_CLOSURE_RESULTS.md +147 -0
- docs/T2_GRAYBOX_RESEARCH_DESIGN.md +152 -0
- src/generate_t2_graybox_closure.py +178 -0
- src/generate_t2_graybox_cohort.py +183 -0
- src/plot_t2_graybox_closure.py +133 -0
- src/t2_graybox_discrete_energy.py +531 -0
- src/train_t2_graybox_closure.py +24 -0
- src/train_t2_graybox_discrete_energy.py +428 -0
- src/validate_t2_graybox.py +411 -0
- src/validate_t2_graybox_closure.py +46 -0
- tests/test_t2_graybox_closure.py +25 -0
- tests/test_t2_graybox_discrete_energy.py +110 -0
DENIM_REPRODUCE.md
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# Reproduce DENIM closure v1
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From the AgentFEM-Physics-Data project root with the configured `fenicsx-env`:
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```bash
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python -m src.generate_t2_graybox_closure --count-per-family 16 --force
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python -m src.train_t2_graybox_closure
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python -m src.validate_t2_graybox_closure
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python -m src.plot_t2_graybox_closure
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python -m pytest -q tests/test_t2_graybox_discrete_energy.py tests/test_t2_graybox_closure.py
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```
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The data were generated with AgentFEM commit
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`e76f2a96f58cc12f47fd6fae996c22fdca300ed1`. Reproducing generation therefore
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requires AgentFEM and its FEniCSx environment. Loading the published DENIM
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weights only requires PyTorch and the included core implementation.
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DENIM_START_HERE.md
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# DENIM incomplete-physics closure
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DENIM is the **Discrete-Energy Neural Internal-variable Model** developed in
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the AgentFEM material-loading-memory study.
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This increment contains 128 complete multiaxial trajectories, each with 241
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ordered states. Training uses five path families (80 trajectories), validation
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uses rotating-principal loading (16), and test fully withholds out-of-phase
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Lissajous and random-direction-block loading (32).
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The reference is intentionally richer than the learned model:
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- reference: three kinematic memories plus tabulated isotropic hardening;
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- DENIM: two tensor memories plus a learned monotone saturating hardening law;
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- known to DENIM: isotropic elasticity, J2 geometry and initial yield stress;
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- hidden: reference hardening table, recovery parameters and update equations.
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Start with:
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- `data/t2_graybox_closure_v1/manifest.json`
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- `artifacts/t2_graybox_closure_v1/model_metrics.json`
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- `artifacts/t2_graybox_closure_v1/deployment_validation.json`
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- `docs/T2_GRAYBOX_CLOSURE_RESULTS.md`
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The HDF5 groups store strain, stress, plastic strain, PEEQ, plastic increments,
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the three reference memories and the two-channel closure state. SI units and
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Voigt order `xx, yy, zz, xy, yz, xz` with tensor shear are used throughout.
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Data are CC BY 4.0. Included code uses the repository code license.
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README.md
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- **T2 multiaxial v2:** 1,024 independently generated J2 and Chaboche
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trajectories in the complete five-dimensional deviatoric strain space,
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with ID, path-OOD and parameter-OOD splits.
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Start with `
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for the
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## Multiaxial v2 at a glance
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- Manuscript roadmap: `docs/T2_MULTIAXIAL_RESEARCH_MEMO.md`
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- Literature map: `docs/T2_MULTIAXIAL_LITERATURE.md`
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- Commands: `T2_V2_REPRODUCE.md`
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The data were generated with AgentFEM commit
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`058faecc05aeda143d014fd229401003a9258bbb` (`0.3.7.dev0`). All quantities use
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- **T2 multiaxial v2:** 1,024 independently generated J2 and Chaboche
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trajectories in the complete five-dimensional deviatoric strain space,
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with ID, path-OOD and parameter-OOD splits.
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- **T2 DENIM closure v1:** 128 multiaxial trajectories from a deliberately
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richer three-memory, tabulated-hardening reference material. The published
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two-memory DENIM model must learn the missing internal-variable closure.
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Start with `DENIM_START_HERE.md` for the incomplete-physics study,
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`T2_V2_START_HERE.md` for the multiaxial benchmark, or `START_HERE.md` for the
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original v1 release.
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## DENIM incomplete-physics closure
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DENIM stands for **Discrete-Energy Neural Internal-variable Model**. The
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reference material contains three kinematic memory channels and a non-
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exponential tabulated isotropic-hardening curve. DENIM retains only two memory
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channels and receives none of the reference hardening equations or parameters.
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Held-out non-proportional path results:
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| Model | Test RMSE | Test R2 |
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|---|---:|---:|
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| Incomplete J2, no learned hardening | 59.541 MPa | 0.730208 |
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| GRU | 76.988 MPa | 0.548933 |
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| **DENIM** | **1.136 MPa** | **0.999902** |
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The 918-parameter DENIM also passed coarse/fine increment checks and three
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notched-bar deployment gates. Cyclic and monotonic reaction relative-L2 errors
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were 0.636% and 0.500%; the severe cyclic stress test required one global
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trust-region fallback. This remains a fixed synthetic material study with
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internal-state supervision, not an experimental calibration or a certified
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production material.
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The standalone weights and model card are published at
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[HaomingLuo/AgentFEM-DENIM](https://huggingface.co/HaomingLuo/AgentFEM-DENIM).
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## Multiaxial v2 at a glance
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- Manuscript roadmap: `docs/T2_MULTIAXIAL_RESEARCH_MEMO.md`
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- Literature map: `docs/T2_MULTIAXIAL_LITERATURE.md`
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- Commands: `T2_V2_REPRODUCE.md`
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- DENIM data and evidence: `DENIM_START_HERE.md`
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- DENIM reproduction: `DENIM_REPRODUCE.md`
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The data were generated with AgentFEM commit
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`058faecc05aeda143d014fd229401003a9258bbb` (`0.3.7.dev0`). All quantities use
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bcb156b8ecc18d5f222e9671dcf792a142fa7969b0eb9455591506a66ed21c36 environment-reproduce.yml
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56e443773f51c475d624041e169eb170a6552e357e905f56cfd84d727d881ebd models/t2_multiaxial_ood_v2/id_physics_state_gru_history.json
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0e14ef379256b97176cf73fd4c83754d8ef956de4ef51f3b3d096478096a8f7c models/t2_multiaxial_ood_v2/id_pointwise_mlp_history.json
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|
| 1 |
+
{
|
| 2 |
+
"scope": "out-of-template fixed material: three-memory tabulated reference; two-memory DENRM closure; reference equations and parameters hidden",
|
| 3 |
+
"training": {
|
| 4 |
+
"denrm": {
|
| 5 |
+
"training_seconds": 5.88968341704458,
|
| 6 |
+
"best_validation_loss": 0.001059024827554822,
|
| 7 |
+
"steps": 1600,
|
| 8 |
+
"history": [
|
| 9 |
+
{
|
| 10 |
+
"step": 0,
|
| 11 |
+
"training_loss": 0.38579270243644714,
|
| 12 |
+
"validation_loss": 0.3402066230773926,
|
| 13 |
+
"moduli_pa": [
|
| 14 |
+
36511551488.0,
|
| 15 |
+
4961107456.0
|
| 16 |
+
],
|
| 17 |
+
"recovery_mean": [
|
| 18 |
+
53.978187561035156,
|
| 19 |
+
53.607749938964844
|
| 20 |
+
]
|
| 21 |
+
},
|
| 22 |
+
{
|
| 23 |
+
"step": 25,
|
| 24 |
+
"training_loss": 0.362447053194046,
|
| 25 |
+
"validation_loss": 0.3224169611930847,
|
| 26 |
+
"moduli_pa": [
|
| 27 |
+
34367172608.0,
|
| 28 |
+
5155069952.0
|
| 29 |
+
],
|
| 30 |
+
"recovery_mean": [
|
| 31 |
+
66.52778625488281,
|
| 32 |
+
42.87104034423828
|
| 33 |
+
]
|
| 34 |
+
},
|
| 35 |
+
{
|
| 36 |
+
"step": 50,
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|
| 860 |
+
}
|
| 861 |
+
},
|
| 862 |
+
"models": {
|
| 863 |
+
"incomplete_j2": {
|
| 864 |
+
"train": {
|
| 865 |
+
"trajectory_count": 80,
|
| 866 |
+
"rmse_mpa": 51.314945220947266,
|
| 867 |
+
"mae_mpa": 27.921403884887695,
|
| 868 |
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"r2": 0.7595025300979614
|
| 869 |
+
},
|
| 870 |
+
"validation": {
|
| 871 |
+
"trajectory_count": 16,
|
| 872 |
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"rmse_mpa": 75.12889862060547,
|
| 873 |
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"mae_mpa": 43.42414855957031,
|
| 874 |
+
"r2": 0.7140845060348511
|
| 875 |
+
},
|
| 876 |
+
"test": {
|
| 877 |
+
"trajectory_count": 32,
|
| 878 |
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"rmse_mpa": 59.54129409790039,
|
| 879 |
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"mae_mpa": 41.032962799072266,
|
| 880 |
+
"r2": 0.7302080392837524
|
| 881 |
+
},
|
| 882 |
+
"inference_seconds_all_trajectories": 2.0804422500077635
|
| 883 |
+
},
|
| 884 |
+
"gru": {
|
| 885 |
+
"train": {
|
| 886 |
+
"trajectory_count": 80,
|
| 887 |
+
"rmse_mpa": 23.556150436401367,
|
| 888 |
+
"mae_mpa": 14.713386535644531,
|
| 889 |
+
"r2": 0.9493206143379211
|
| 890 |
+
},
|
| 891 |
+
"validation": {
|
| 892 |
+
"trajectory_count": 16,
|
| 893 |
+
"rmse_mpa": 85.85247039794922,
|
| 894 |
+
"mae_mpa": 57.07228088378906,
|
| 895 |
+
"r2": 0.6266387701034546
|
| 896 |
+
},
|
| 897 |
+
"test": {
|
| 898 |
+
"trajectory_count": 32,
|
| 899 |
+
"rmse_mpa": 76.98819732666016,
|
| 900 |
+
"mae_mpa": 52.02629089355469,
|
| 901 |
+
"r2": 0.5489333271980286
|
| 902 |
+
},
|
| 903 |
+
"inference_seconds_all_trajectories": 0.06955916690640152
|
| 904 |
+
},
|
| 905 |
+
"denrm": {
|
| 906 |
+
"train": {
|
| 907 |
+
"trajectory_count": 80,
|
| 908 |
+
"rmse_mpa": 0.8718719482421875,
|
| 909 |
+
"mae_mpa": 0.4504835605621338,
|
| 910 |
+
"r2": 0.9999305605888367
|
| 911 |
+
},
|
| 912 |
+
"validation": {
|
| 913 |
+
"trajectory_count": 16,
|
| 914 |
+
"rmse_mpa": 1.9618406295776367,
|
| 915 |
+
"mae_mpa": 1.0055958032608032,
|
| 916 |
+
"r2": 0.9998050332069397
|
| 917 |
+
},
|
| 918 |
+
"test": {
|
| 919 |
+
"trajectory_count": 32,
|
| 920 |
+
"rmse_mpa": 1.135945200920105,
|
| 921 |
+
"mae_mpa": 0.6864870190620422,
|
| 922 |
+
"r2": 0.9999017715454102
|
| 923 |
+
},
|
| 924 |
+
"inference_seconds_all_trajectories": 10.250110333086923,
|
| 925 |
+
"maximum_yield_residual_pa": 96.0,
|
| 926 |
+
"maximum_plastic_trace": 6.51925802230835e-09,
|
| 927 |
+
"minimum_peeq_increment": 0.0,
|
| 928 |
+
"learned_moduli_pa": [
|
| 929 |
+
28024965120.0,
|
| 930 |
+
12740021248.0
|
| 931 |
+
],
|
| 932 |
+
"minimum_reference_yield_dissipation": 0.0172310508787632,
|
| 933 |
+
"minimum_dynamic_recovery_dissipation": 4.376159267849289e-06,
|
| 934 |
+
"minimum_backward_euler_dissipation": -0.047634124755859375,
|
| 935 |
+
"maximum_energy_balance_relative_residual": 1.5819839518371737e-06
|
| 936 |
+
}
|
| 937 |
+
}
|
| 938 |
+
}
|
artifacts/t2_graybox_closure_v1/structural_reaction_comparison.png
ADDED
|
Git LFS Details
|
data/t2_graybox_closure_v1/cohort.h5
ADDED
|
@@ -0,0 +1,3 @@
|
|
|
|
|
|
|
|
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|
|
|
| 1 |
+
version https://git-lfs.github.com/spec/v1
|
| 2 |
+
oid sha256:1789c8070f012c57d02c106dfa4c9193d162d96d0124a02cb8ad48046632d86f
|
| 3 |
+
size 10093525
|
data/t2_graybox_closure_v1/manifest.json
ADDED
|
@@ -0,0 +1,39 @@
|
|
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|
|
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|
|
|
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|
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|
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|
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|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
{
|
| 2 |
+
"schema": "agentfem.physics-data.incomplete-physics-closure",
|
| 3 |
+
"schema_version": "1.0.0",
|
| 4 |
+
"sample_count": 128,
|
| 5 |
+
"count_per_family": 16,
|
| 6 |
+
"points_per_trajectory": 241,
|
| 7 |
+
"path_families": [
|
| 8 |
+
"proportional_axial_cycle",
|
| 9 |
+
"proportional_shear_cycle",
|
| 10 |
+
"sequential_axial_shear",
|
| 11 |
+
"orthogonal_cross",
|
| 12 |
+
"nonproportional_square",
|
| 13 |
+
"rotating_principal_cycle",
|
| 14 |
+
"out_of_phase_lissajous",
|
| 15 |
+
"random_direction_blocks"
|
| 16 |
+
],
|
| 17 |
+
"splits": {
|
| 18 |
+
"train": 80,
|
| 19 |
+
"validation": 16,
|
| 20 |
+
"test": 32
|
| 21 |
+
},
|
| 22 |
+
"known_to_model": [
|
| 23 |
+
"young_pa",
|
| 24 |
+
"poisson",
|
| 25 |
+
"yield_stress_pa",
|
| 26 |
+
"J2_geometry"
|
| 27 |
+
],
|
| 28 |
+
"hidden_from_model": [
|
| 29 |
+
"three_reference_memory_channels",
|
| 30 |
+
"all_reference_recovery_parameters",
|
| 31 |
+
"piecewise_linear_isotropic_hardening_table",
|
| 32 |
+
"reference_hardening_update_equations"
|
| 33 |
+
],
|
| 34 |
+
"intentional_model_mismatch": "reference has three memories; DENRM has two and must close the lumped medium/slow state",
|
| 35 |
+
"ground_truth": "AgentFEM three-memory Chaboche with tabulated isotropic hardening",
|
| 36 |
+
"scope": "Out-of-template synthetic closure cohort; fixed material.",
|
| 37 |
+
"elapsed_seconds": 21.372640792047605,
|
| 38 |
+
"bytes": 10093525
|
| 39 |
+
}
|
docs/T2_GRAYBOX_CLOSURE_RESULTS.md
ADDED
|
@@ -0,0 +1,147 @@
|
|
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|
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|
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|
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|
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|
|
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|
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|
|
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|
|
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|
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|
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|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
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|
|
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|
|
|
|
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|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
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|
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|
|
|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
# T2真正不完备物理灰盒闭环:阶段结果
|
| 2 |
+
|
| 3 |
+
## 结论
|
| 4 |
+
|
| 5 |
+
本阶段已完成一条可复现的灰盒神经本构闭环,而不是增加一组黑箱网络对比。
|
| 6 |
+
最终方法定名为 **DENIM(Discrete-Energy Neural Internal-variable Model,离散能量神经内变量模型)**。
|
| 7 |
+
|
| 8 |
+
参考材料使用AgentFEM生成,包含三条运动硬化记忆通道和非指数、分段线性的各向同性
|
| 9 |
+
硬化表;DENIM只保留两条记忆通道,且不知道参考硬化方程、表格和参数。第二、第三条
|
| 10 |
+
参考记忆被合并为一个不完备状态,网络必须学习被删去自由度产生的有效闭合规律。
|
| 11 |
+
|
| 12 |
+
在完整留出的两类非比例多轴路径上,DENIM应力RMSE为 **1.136 MPa**、
|
| 13 |
+
`R2=0.999902`;相同数据上的GRU为 **76.988 MPa**、`R2=0.548933`,
|
| 14 |
+
不含硬化学习的J2骨架为 **59.541 MPa**、`R2=0.730208`。这说明结果不依赖
|
| 15 |
+
提出模型与三通道参考模型同构。
|
| 16 |
+
|
| 17 |
+
## 架构选择
|
| 18 |
+
|
| 19 |
+
保留的物理:小应变各向同性弹性、J2屈服几何、关联流动、塑性不可压缩、非负塑性
|
| 20 |
+
乘子、PEEQ单调、弹性预测—隐式塑性校正和状态提交/回滚。
|
| 21 |
+
|
| 22 |
+
学习的未知物理:
|
| 23 |
+
|
| 24 |
+
- 零点锚定的各向同性硬化函数;采用正权重饱和指数混合和非负线性尾项,结构上保证
|
| 25 |
+
`R(0)=0`和`dR/dp>=0`,并能表达Voce型及表格型饱和硬化;
|
| 26 |
+
- 两条无迹张量记忆的正生产模量;
|
| 27 |
+
- 由客观张量不变量、流动方向投影、PEEQ和反向加载指标驱动的非负动态恢复率。
|
| 28 |
+
|
| 29 |
+
网络只表示硬化闭合项,弹性、屈服几何、流动方向和局部隐式积分不交给网络猜测。
|
| 30 |
+
最终DENIM仅 **918** 个可训练参数,GRU为 **49,254** 个参数。
|
| 31 |
+
|
| 32 |
+
## 数据与划分
|
| 33 |
+
|
| 34 |
+
- 128条独立多轴轨迹,每条241个状态点;
|
| 35 |
+
- 训练80条:比例轴向、比例剪切、顺序轴剪、正交交叉和非比例方形路径;
|
| 36 |
+
- 验证16条:旋转主方向路径;
|
| 37 |
+
- 测试32条:完整留出的异相Lissajous和随机方向块;
|
| 38 |
+
- 模型只知道`E`、`nu`、初始屈服应力和J2骨架;
|
| 39 |
+
- 参考模型的三通道参数、表格硬化数据和更新方程全部隐藏。
|
| 40 |
+
|
| 41 |
+
数据由AgentFEM提交`e76f2a96f58cc12f47fd6fae996c22fdca300ed1`生成。
|
| 42 |
+
|
| 43 |
+
## 核心结果
|
| 44 |
+
|
| 45 |
+
| 模型 | 训练RMSE / MPa | 验证RMSE / MPa | 未见路径测试RMSE / MPa | 测试R2 |
|
| 46 |
+
|---|---:|---:|---:|---:|
|
| 47 |
+
| 不完备J2,无硬化学习 | 51.315 | 75.129 | 59.541 | 0.730208 |
|
| 48 |
+
| GRU | 23.556 | 85.852 | 76.988 | 0.548933 |
|
| 49 |
+
| DENIM | **0.872** | **1.962** | **1.136** | **0.999902** |
|
| 50 |
+
|
| 51 |
+
DENIM相比GRU将未见路径RMSE降低 **98.52%**,相比不完备J2降低 **98.09%**。
|
| 52 |
+
训练用时5.89 s,GRU训练用时12.38 s。材料点推理方面,DENIM需要执行局部隐式
|
| 53 |
+
返回映射,128条轨迹用时10.25 s;GRU直接前向推理为0.070 s。该结果体现了可信
|
| 54 |
+
约束和速度之间的真实代价,后续应通过矢量化、隐式微分和编译优化缩小差距。
|
| 55 |
+
|
| 56 |
+
## 物理与数值门槛
|
| 57 |
+
|
| 58 |
+
- 最大屈服一致性残差:96 Pa;
|
| 59 |
+
- 最大塑性应变迹:`6.52e-9`;
|
| 60 |
+
- 最小PEEQ增量:0;
|
| 61 |
+
- 最小动态恢复耗散:`4.38e-6 J/m3`;
|
| 62 |
+
- 离散能量余额最大相对残差:`1.58e-6`;
|
| 63 |
+
- 后向欧拉耗散最小值为`-4.76e-2 J/m3`,属于单精度分账舍入量,正式论文应以
|
| 64 |
+
双精度重算并给出相对容差,不应直接宣称严格机器零负值。
|
| 65 |
+
|
| 66 |
+
初版返回映射曾在粗时间步的近90度正交换向中数值爆炸。根因是直接对包含大剪切
|
| 67 |
+
模量项的流动方向做固定点迭代,且根区间未闭合时仍接受状态。现已解析消去该大项,
|
| 68 |
+
使用单调的标量一致性方程并扩大根区间。修正后:
|
| 69 |
+
|
| 70 |
+
- 121点粗时间步RMSE:0.944 MPa;
|
| 71 |
+
- 481点细时间步RMSE:0.958 MPa;
|
| 72 |
+
- 两种离散下精度基本一致;最大屈服残差均小于0.25 Pa;
|
| 73 |
+
- 121点与481点终态相对变化约1.07%,其中包含参考积分自身的离散差异。
|
| 74 |
+
|
| 75 |
+
## 结构有限元部署
|
| 76 |
+
|
| 77 |
+
DENIM作为材料更新嵌入12单元变截面杆的全局平衡迭代,并与AgentFEM原生三通道
|
| 78 |
+
表格硬化材料对照:
|
| 79 |
+
|
| 80 |
+
| 结构门槛 | 反力相对L2误差 | 最大Newton迭代 | 回退 |
|
| 81 |
+
|---|---:|---:|---:|
|
| 82 |
+
| 轻缺口循环加载 | **0.636%** | 39 | 0 |
|
| 83 |
+
| 强缺口单调加载 | **0.500%** | 4 | 0 |
|
| 84 |
+
| 强缺口循环压力测试 | 通过 | 68 | 1次信赖域回退 |
|
| 85 |
+
|
| 86 |
+
强缺口循环工况通过,但一次回退说明当前有限差分方向切线在完全换向附近仍不够理想。
|
| 87 |
+
论文升级应实现由局部隐式残量Jacobian得到的一致算法切线,并与固定旧状态有限差分
|
| 88 |
+
逐点核验。
|
| 89 |
+
|
| 90 |
+
## 科研价值与文章定位
|
| 91 |
+
|
| 92 |
+
当前工作已经形成一篇论文的核心方法和主要数值证据:
|
| 93 |
+
|
| 94 |
+
1. 不是轨迹到应力的黑箱映射,而是只学习未知硬化闭合项;
|
| 95 |
+
2. 参考模型三条记忆、学习模型两条记忆,验证了不完备状态下的有效闭合;
|
| 96 |
+
3. 物理约束由架构保证,不依赖损失惩罚;
|
| 97 |
+
4. 粗细时间步、离散能量和结构Newton共同验证;
|
| 98 |
+
5. 过程中暴露并修正了非比例大转向下返回映射失稳,形成可讨论的数值贡献。
|
| 99 |
+
|
| 100 |
+
仅凭当前合成固定材料结果,适合形成高质量计算力学/工程AI论文初稿,尚不足以稳妥
|
| 101 |
+
宣称CMAME/IJNME级完成稿。提升到更高水平至少还需要:
|
| 102 |
+
|
| 103 |
+
- 一组公开实验多轴循环数据,或自有实验数据;
|
| 104 |
+
- 从当前内部状态监督推进到应力—应变主监督,内部状态仅用于诊断或教师蒸馏;
|
| 105 |
+
- 自动/隐式一致切线和二维或三维积分点部署;
|
| 106 |
+
- 多随机种子、噪声与数据稀缺性统计,不需要海选更多网络;
|
| 107 |
+
- 与经标定经典模型比较,而不只比较无硬化J2和GRU。
|
| 108 |
+
|
| 109 |
+
建议论文题目:
|
| 110 |
+
|
| 111 |
+
> **From trajectory fitting to deployable constitutive closure: a discrete-energy neural return map for path-dependent plasticity**
|
| 112 |
+
|
| 113 |
+
## 与文献的关系
|
| 114 |
+
|
| 115 |
+
- [Masi et al., TANN, JMPS 2021](https://doi.org/10.1016/j.jmps.2020.104277):
|
| 116 |
+
将热力学结构嵌入神经本构;
|
| 117 |
+
- [Vlassis and Sun, CMAME 2021](https://doi.org/10.1016/j.cma.2021.113695):
|
| 118 |
+
Sobolev/level-set方法学习可解释塑性硬化,并比较GRU等黑箱模型;
|
| 119 |
+
- [Meyer and Ekre, JMPS 2023](https://doi.org/10.1016/j.jmps.2023.105416):
|
| 120 |
+
神经网络只表示未知演化律,并从实验中发现可解释方程;
|
| 121 |
+
- [Bleyer, CMAME 2025](https://doi.org/10.1016/j.cma.2025.118145):
|
| 122 |
+
将塑性更新写成隐式优化层并使用隐式微分;
|
| 123 |
+
- [Masi, CMAME 2026](https://doi.org/10.1016/j.cma.2026.119260):
|
| 124 |
+
以凸自由能和半正定传输算子实施硬热力学约束。
|
| 125 |
+
|
| 126 |
+
DENIM不把“物理神经本构”本身视为新概念。可主张的组合创新是:面向不完备硬化
|
| 127 |
+
状态的紧凑闭合、可审计离散能量分账、非比例粗时间步稳定返回映射,以及从材料点到
|
| 128 |
+
结构Newton的统一部署证据。
|
| 129 |
+
|
| 130 |
+
## 可复现资产
|
| 131 |
+
|
| 132 |
+
- 数据:`data/t2_graybox_closure_v1/cohort.h5`
|
| 133 |
+
- 数据清单:`data/t2_graybox_closure_v1/manifest.json`
|
| 134 |
+
- DENIM权重:`models/t2_graybox_closure_v1/denrm.pt`(发布时文件名为`denim.pt`)
|
| 135 |
+
- GRU权重:`models/t2_graybox_closure_v1/gru.pt`
|
| 136 |
+
- 模型指标:`artifacts/t2_graybox_closure_v1/model_metrics.json`
|
| 137 |
+
- 部署指标:`artifacts/t2_graybox_closure_v1/deployment_validation.json`
|
| 138 |
+
- 总结图:`artifacts/t2_graybox_closure_v1/closure_summary.png`
|
| 139 |
+
- 结构反力图:`artifacts/t2_graybox_closure_v1/structural_reaction_comparison.png`
|
| 140 |
+
- 核心实现:`src/t2_graybox_discrete_energy.py`
|
| 141 |
+
- 数据生成:`src/generate_t2_graybox_closure.py`
|
| 142 |
+
- 训练:`src/train_t2_graybox_closure.py`
|
| 143 |
+
- 部署验证:`src/validate_t2_graybox_closure.py`
|
| 144 |
+
- 回归测试:`tests/test_t2_graybox_closure.py`及`tests/test_t2_graybox_discrete_energy.py`
|
| 145 |
+
|
| 146 |
+
复现顺序:生成数据、训练、部署验证、绘图。所有产物均写入本项目目录,未修改
|
| 147 |
+
AgentFEM核心代码。
|
docs/T2_GRAYBOX_RESEARCH_DESIGN.md
ADDED
|
@@ -0,0 +1,152 @@
|
|
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|
|
|
|
|
|
|
|
| 1 |
+
# T2灰盒神经本构主线:离散能量约束的神经硬化返回映射
|
| 2 |
+
|
| 3 |
+
## 研究问题
|
| 4 |
+
|
| 5 |
+
材料点随机留出精度不能回答未知加载路径、时间步变化和结构有限元收敛问题。
|
| 6 |
+
现有白盒物理积分网络直接使用J2/Chaboche硬化公式,适合作为算法积分上限,
|
| 7 |
+
不能证明神经网络能够学习未知本构演化。下一阶段只保留可靠的力学骨架,让
|
| 8 |
+
网络学习未知硬化记忆,并检验该模型能否从材料点进入结构Newton求解。
|
| 9 |
+
|
| 10 |
+
核心问题为:
|
| 11 |
+
|
| 12 |
+
> 在不提供Chaboche硬化演化公式的条件下,能否从有限的多轴应力—应变历程中
|
| 13 |
+
> 学得紧凑、客观、耗散可接受的硬化记忆,并在未见路径、改变时间步和非均匀
|
| 14 |
+
> 结构中保持精度与求解稳定性?
|
| 15 |
+
|
| 16 |
+
## 文献判断
|
| 17 |
+
|
| 18 |
+
现有重要路线包括:
|
| 19 |
+
|
| 20 |
+
1. TANN从自由能和耗散出发,将热力学关系嵌入网络;
|
| 21 |
+
2. Sobolev/level-set方法学习屈服面与硬化并控制函数导数;
|
| 22 |
+
3. Meyer—Ekre方法将神经网络嵌入标准耗散材料结构,学习并进一步识别未知演化律;
|
| 23 |
+
4. 隐式层方法把塑性更新写成可微凸优化层;
|
| 24 |
+
5. 2026年的hard-thermodynamic与thermodynamic-hierarchy工作进一步比较自由能、
|
| 25 |
+
耗散势、传输算子和神经ODE等框架。
|
| 26 |
+
|
| 27 |
+
因此,本项目不把“热力学神经网络”“神经返回映射”或“学习演化律”本身作为
|
| 28 |
+
新的概念。可形成差异的部分是:以一个明确不完备的J2骨架为起点,把未知硬化
|
| 29 |
+
学习、后向欧拉离散能量分账、时间步OOD、一致算法切线及结构Newton门统一在
|
| 30 |
+
同一条可复现的AgentFEM工作流中。
|
| 31 |
+
|
| 32 |
+
## 唯一主架构
|
| 33 |
+
|
| 34 |
+
定名为 **DENIM(Discrete-Energy Neural Internal-variable Model,离散能量神经内变量模型)**。
|
| 35 |
+
名称指向“离散能量+可学习内变量”的方法范式;当前实例限定为小应变J2循环塑性,不把名称扩张为所有材料模型的通用解。
|
| 36 |
+
|
| 37 |
+
### 保留的已知物理
|
| 38 |
+
|
| 39 |
+
- 小应变各向同性线弹性;
|
| 40 |
+
- J2屈服几何;
|
| 41 |
+
- 关联流动方向;
|
| 42 |
+
- 塑性不可压缩;
|
| 43 |
+
- 非负塑性乘子与PEEQ单调;
|
| 44 |
+
- 弹性预测—隐式塑性校正;
|
| 45 |
+
- 接受状态的commit/rollback语义。
|
| 46 |
+
|
| 47 |
+
### 故意移除的物理
|
| 48 |
+
|
| 49 |
+
- Voce指数型各向同性硬化公式;
|
| 50 |
+
- 固定Armstrong—Frederick动态恢复公式;
|
| 51 |
+
- 数据生成器中的Chaboche参数及其更新方程。
|
| 52 |
+
|
| 53 |
+
### 神经硬化状态
|
| 54 |
+
|
| 55 |
+
状态为塑性应变、PEEQ、标量各向同性硬化量和两个无迹二阶记忆张量。两个张量
|
| 56 |
+
表示快、慢两类方向记忆,但不向网络提供Chaboche的解析更新。
|
| 57 |
+
|
| 58 |
+
各向同性硬化使用零点锚定的单调神经函数
|
| 59 |
+
|
| 60 |
+
`R_theta(p) >= 0, dR_theta/dp >= 0, R_theta(0)=0`。
|
| 61 |
+
|
| 62 |
+
张量记忆采用客观的后向欧拉更新。网络只读取张量不变量、与当前流动方向的
|
| 63 |
+
投影、PEEQ和反向加载指标,输出非负动态恢复率;生产模量保持为正的可学习
|
| 64 |
+
材料常数。经典双背应力Chaboche是该模型的一个特例,但网络也可表达随状态和
|
| 65 |
+
方向历史变化的恢复规律。
|
| 66 |
+
|
| 67 |
+
### 离散能量
|
| 68 |
+
|
| 69 |
+
每个接受增量显式记录:
|
| 70 |
+
|
| 71 |
+
- 塑性功;
|
| 72 |
+
- 各向同性硬化储能变化;
|
| 73 |
+
- 运动硬化储能变化;
|
| 74 |
+
- 初始屈服耗散;
|
| 75 |
+
- 动态恢复耗散;
|
| 76 |
+
- 后向欧拉数值耗散;
|
| 77 |
+
- 离散能量余额。
|
| 78 |
+
|
| 79 |
+
正参数化和单调硬化保证关键耗散通道非负;训练、验证和结构部署均使用同一
|
| 80 |
+
分账定义。连续热力学正确但离散积分失真的模型不能通过时间步门。
|
| 81 |
+
|
| 82 |
+
### 一致切线
|
| 83 |
+
|
| 84 |
+
局部塑性校正写成隐式残量。训练阶段可使用可微固定点/隐式微分,部署阶段由
|
| 85 |
+
局部残量的Jacobian得到算法切线,并以固定旧状态的有限差分独立核验。结构门
|
| 86 |
+
同时报告反力误差、Newton迭代、cutback和回退,不以材料点RMSE替代稳定性。
|
| 87 |
+
|
| 88 |
+
## 数据设计
|
| 89 |
+
|
| 90 |
+
不重新海选网络,只增加一组面向演化发现的固定材料队列:
|
| 91 |
+
|
| 92 |
+
1. 已知`E, nu, sigma_y`,隐藏所有硬化公式与硬化参数;
|
| 93 |
+
2. 训练路径使用比例、剪切、顺序轴剪、正交和方形非比例加载;
|
| 94 |
+
3. 验证留出旋转主方向;
|
| 95 |
+
4. 测试完整留出Lissajous和随机五维方向块;
|
| 96 |
+
5. 对同一连续路径随机改变离散步长,形成时间步OOD;
|
| 97 |
+
6. 第一真值为AgentFEM组合硬化,用于验证能否恢复已知规律;
|
| 98 |
+
7. 第二真值使用非指数表格硬化和多时间尺度记忆,避免提出模型与生成器同构;
|
| 99 |
+
8. 最后增加公开OFHC铜/316钢路径或实验数据,不把合成结果冒充实验发现。
|
| 100 |
+
|
| 101 |
+
## 最小对照组
|
| 102 |
+
|
| 103 |
+
只保留三个必要对照,不重新训练一排相似网络:
|
| 104 |
+
|
| 105 |
+
1. 现有GRU:代表黑箱历史模型;
|
| 106 |
+
2. 不含硬化的J2骨架:代表物理不完备但没有学习;
|
| 107 |
+
3. DENIM:本文方法。
|
| 108 |
+
|
| 109 |
+
现有白盒物理积分网络只作为不可超越的“知道真公式”参考上限,不参与公平的
|
| 110 |
+
未知物理排名。
|
| 111 |
+
|
| 112 |
+
## 成功门槛
|
| 113 |
+
|
| 114 |
+
DENIM必须同时满足:
|
| 115 |
+
|
| 116 |
+
- 路径OOD应力RMSE显著低于GRU;
|
| 117 |
+
- PEEQ、塑性不可压缩和客观性零违例;
|
| 118 |
+
- 离散能量余额达到数值积分容差,耗散通道无负值;
|
| 119 |
+
- 241、121及非均匀时间步下终态和历程保持自洽;
|
| 120 |
+
- 算法切线与固定旧状态有限差分一致;
|
| 121 |
+
- 二维或三维非均匀结构中达到可接受反力误差,并稳定完成全局Newton;
|
| 122 |
+
- 公开路径/实验对照不劣于经标定的经典基线。
|
| 123 |
+
|
| 124 |
+
若DENIM不能超过GRU,应保留失败结果并检查信息不足、状态维数、离散更新和
|
| 125 |
+
训练路径覆盖,不通过增删测试集制造胜出。
|
| 126 |
+
|
| 127 |
+
## 论文主线
|
| 128 |
+
|
| 129 |
+
建议题目方向:
|
| 130 |
+
|
| 131 |
+
**From trajectory fitting to deployable constitutive discovery: a discrete-energy neural return map for path-dependent plasticity**
|
| 132 |
+
|
| 133 |
+
文章的核心贡献不是新网络名称,而是证明:未知硬化可以在保留少量可靠物理的
|
| 134 |
+
条件下学习;连续层面的物理约束仍不够,离散能量、时间步一致性、算法切线和
|
| 135 |
+
结构平衡必须共同构成神经本构的可信验证链。
|
| 136 |
+
|
| 137 |
+
## 主要文献入口
|
| 138 |
+
|
| 139 |
+
- Masi et al., Thermodynamics-based Artificial Neural Networks, JMPS 2021,
|
| 140 |
+
https://doi.org/10.1016/j.jmps.2020.104277
|
| 141 |
+
- Vlassis and Sun, Sobolev training of thermodynamic-informed neural networks,
|
| 142 |
+
CMAME 2021, https://doi.org/10.1016/j.cma.2021.113695
|
| 143 |
+
- Meyer and Ekre, Thermodynamically consistent neural network plasticity
|
| 144 |
+
modeling and discovery of evolution laws, JMPS 2023,
|
| 145 |
+
https://doi.org/10.1016/j.jmps.2023.105416
|
| 146 |
+
- Bleyer, Learning elastoplasticity with implicit layers, CMAME 2025,
|
| 147 |
+
https://doi.org/10.1016/j.cma.2025.118145
|
| 148 |
+
- Masi, Learning inelastic constitutive models from stress-strain data under
|
| 149 |
+
hard thermodynamic constraints, CMAME 2026,
|
| 150 |
+
https://doi.org/10.1016/j.cma.2026.119260
|
| 151 |
+
- Jones and Fuhg, A hierarchy of thermodynamics learning frameworks for
|
| 152 |
+
inelastic constitutive modeling, arXiv:2603.02645
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src/generate_t2_graybox_closure.py
ADDED
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| 1 |
+
"""Generate the out-of-template cohort for incomplete-physics closure.
|
| 2 |
+
|
| 3 |
+
The reference material has three kinematic time scales and a piecewise-linear
|
| 4 |
+
isotropic hardening curve. DENRM is deliberately restricted to two memory
|
| 5 |
+
channels and is not given either reference evolution law.
|
| 6 |
+
"""
|
| 7 |
+
|
| 8 |
+
from __future__ import annotations
|
| 9 |
+
|
| 10 |
+
import argparse
|
| 11 |
+
import json
|
| 12 |
+
import time
|
| 13 |
+
from pathlib import Path
|
| 14 |
+
|
| 15 |
+
import h5py
|
| 16 |
+
import numpy as np
|
| 17 |
+
|
| 18 |
+
from agentfem import constitutive
|
| 19 |
+
|
| 20 |
+
from src.generate_t2_graybox_cohort import design, split_for_family
|
| 21 |
+
from src.t2_multiaxial_ood_v2 import PATH_FAMILIES, strain_history, tensor_to_voigt
|
| 22 |
+
|
| 23 |
+
|
| 24 |
+
ROOT = Path(__file__).resolve().parents[1]
|
| 25 |
+
DATA_DIR = ROOT / "data" / "t2_graybox_closure_v1"
|
| 26 |
+
DATA_PATH = DATA_DIR / "cohort.h5"
|
| 27 |
+
MANIFEST_PATH = DATA_DIR / "manifest.json"
|
| 28 |
+
|
| 29 |
+
MATERIAL = {
|
| 30 |
+
"young_pa": 190.0e9,
|
| 31 |
+
"poisson": 0.30,
|
| 32 |
+
"yield_stress_pa": 280.0e6,
|
| 33 |
+
"backstress_c1_pa": 28.0e9,
|
| 34 |
+
"backstress_gamma1": 80.0,
|
| 35 |
+
"backstress_c2_pa": 10.0e9,
|
| 36 |
+
"backstress_gamma2": 12.0,
|
| 37 |
+
"backstress_c3_pa": 3.0e9,
|
| 38 |
+
"backstress_gamma3": 1.5,
|
| 39 |
+
"hardening_peeq": (0.0, 0.002, 0.006, 0.015, 0.030, 0.060, 0.100),
|
| 40 |
+
"hardening_stress_pa": (
|
| 41 |
+
280.0e6,
|
| 42 |
+
301.0e6,
|
| 43 |
+
324.0e6,
|
| 44 |
+
345.0e6,
|
| 45 |
+
358.0e6,
|
| 46 |
+
370.0e6,
|
| 47 |
+
378.0e6,
|
| 48 |
+
),
|
| 49 |
+
}
|
| 50 |
+
|
| 51 |
+
|
| 52 |
+
def closure_design(count_per_family: int = 16) -> list[dict[str, object]]:
|
| 53 |
+
rows = design(count_per_family)
|
| 54 |
+
for row in rows:
|
| 55 |
+
row.update(MATERIAL)
|
| 56 |
+
row["material_model"] = "hidden_three_memory_tabulated_hardening"
|
| 57 |
+
return rows
|
| 58 |
+
|
| 59 |
+
|
| 60 |
+
def material() -> constitutive.ChabocheCombinedHardening:
|
| 61 |
+
hardening = constitutive.TabulatedIsotropicHardening(
|
| 62 |
+
equivalent_plastic_strain=tuple(MATERIAL["hardening_peeq"]),
|
| 63 |
+
yield_stress=tuple(MATERIAL["hardening_stress_pa"]),
|
| 64 |
+
extrapolation="constant",
|
| 65 |
+
)
|
| 66 |
+
return constitutive.chaboche(
|
| 67 |
+
young=float(MATERIAL["young_pa"]),
|
| 68 |
+
poisson=float(MATERIAL["poisson"]),
|
| 69 |
+
yield_stress=float(MATERIAL["yield_stress_pa"]),
|
| 70 |
+
backstresses=(
|
| 71 |
+
(float(MATERIAL["backstress_c1_pa"]), float(MATERIAL["backstress_gamma1"])),
|
| 72 |
+
(float(MATERIAL["backstress_c2_pa"]), float(MATERIAL["backstress_gamma2"])),
|
| 73 |
+
(float(MATERIAL["backstress_c3_pa"]), float(MATERIAL["backstress_gamma3"])),
|
| 74 |
+
),
|
| 75 |
+
isotropic_hardening=hardening,
|
| 76 |
+
name="hidden three-memory tabulated reference",
|
| 77 |
+
)
|
| 78 |
+
|
| 79 |
+
|
| 80 |
+
def solve(parameters: dict[str, object], *, points: int | None = None) -> dict[str, np.ndarray]:
|
| 81 |
+
law = material()
|
| 82 |
+
coordinates, strains = strain_history(parameters, points=points)
|
| 83 |
+
count = len(strains)
|
| 84 |
+
stress = np.empty_like(strains)
|
| 85 |
+
plastic = np.empty_like(strains)
|
| 86 |
+
peeq = np.empty(count)
|
| 87 |
+
increment = np.empty(count)
|
| 88 |
+
truth_memories = np.empty((count, 3, 3, 3))
|
| 89 |
+
latent_memories = np.empty((count, 2, 3, 3))
|
| 90 |
+
radius = np.empty(count)
|
| 91 |
+
state = None
|
| 92 |
+
for index, strain in enumerate(strains):
|
| 93 |
+
update = law.update(strain, state, linearization="none")
|
| 94 |
+
state = update.state
|
| 95 |
+
stress[index] = update.stress
|
| 96 |
+
plastic[index] = state.plastic_strain
|
| 97 |
+
peeq[index] = state.equivalent_plastic_strain
|
| 98 |
+
increment[index] = update.plastic_multiplier_increment
|
| 99 |
+
truth_memories[index] = state.backstresses
|
| 100 |
+
# The two-channel closure sees one fast state and one deliberately
|
| 101 |
+
# unresolved aggregate of the medium and slow reference mechanisms.
|
| 102 |
+
latent_memories[index, 0] = state.backstresses[0]
|
| 103 |
+
latent_memories[index, 1] = state.backstresses[1] + state.backstresses[2]
|
| 104 |
+
radius[index] = law.current_yield_stress(peeq[index]) - law.yield_stress
|
| 105 |
+
return {
|
| 106 |
+
"strain": tensor_to_voigt(strains),
|
| 107 |
+
"stress_pa": tensor_to_voigt(stress),
|
| 108 |
+
"plastic_strain": tensor_to_voigt(plastic),
|
| 109 |
+
"peeq": peeq,
|
| 110 |
+
"plastic_increment": increment,
|
| 111 |
+
"memories_pa": tensor_to_voigt(latent_memories),
|
| 112 |
+
"truth_memories_pa": tensor_to_voigt(truth_memories),
|
| 113 |
+
"isotropic_radius_pa": radius,
|
| 114 |
+
"path_coordinates": coordinates,
|
| 115 |
+
}
|
| 116 |
+
|
| 117 |
+
|
| 118 |
+
def generate(count_per_family: int = 16, *, force: bool = False) -> dict[str, object]:
|
| 119 |
+
rows = closure_design(count_per_family)
|
| 120 |
+
DATA_DIR.mkdir(parents=True, exist_ok=True)
|
| 121 |
+
if DATA_PATH.exists() and not force:
|
| 122 |
+
raise FileExistsError(f"{DATA_PATH} already exists; pass --force to replace it.")
|
| 123 |
+
temporary = DATA_PATH.with_suffix(".h5.tmp")
|
| 124 |
+
started = time.perf_counter()
|
| 125 |
+
with h5py.File(temporary, "w") as h5:
|
| 126 |
+
h5.attrs["schema"] = "agentfem.physics-data.incomplete-physics-closure"
|
| 127 |
+
h5.attrs["schema_version"] = "1.0.0"
|
| 128 |
+
h5.attrs["material_json"] = json.dumps(MATERIAL, sort_keys=True)
|
| 129 |
+
for index, row in enumerate(rows):
|
| 130 |
+
group = h5.create_group(f"{index:05d}")
|
| 131 |
+
group.attrs["path_family"] = str(row["path_family"])
|
| 132 |
+
group.attrs["split"] = split_for_family(str(row["path_family"]))
|
| 133 |
+
group.attrs["parameters_json"] = json.dumps(row, sort_keys=True)
|
| 134 |
+
for name, value in solve(row).items():
|
| 135 |
+
group.create_dataset(name, data=value, compression="gzip", shuffle=True)
|
| 136 |
+
temporary.replace(DATA_PATH)
|
| 137 |
+
manifest = {
|
| 138 |
+
"schema": "agentfem.physics-data.incomplete-physics-closure",
|
| 139 |
+
"schema_version": "1.0.0",
|
| 140 |
+
"sample_count": len(rows),
|
| 141 |
+
"count_per_family": count_per_family,
|
| 142 |
+
"points_per_trajectory": 241,
|
| 143 |
+
"path_families": list(PATH_FAMILIES),
|
| 144 |
+
"splits": {
|
| 145 |
+
"train": 5 * count_per_family,
|
| 146 |
+
"validation": count_per_family,
|
| 147 |
+
"test": 2 * count_per_family,
|
| 148 |
+
},
|
| 149 |
+
"known_to_model": ["young_pa", "poisson", "yield_stress_pa", "J2_geometry"],
|
| 150 |
+
"hidden_from_model": [
|
| 151 |
+
"three_reference_memory_channels",
|
| 152 |
+
"all_reference_recovery_parameters",
|
| 153 |
+
"piecewise_linear_isotropic_hardening_table",
|
| 154 |
+
"reference_hardening_update_equations",
|
| 155 |
+
],
|
| 156 |
+
"intentional_model_mismatch": (
|
| 157 |
+
"reference has three memories; DENRM has two and must close the lumped medium/slow state"
|
| 158 |
+
),
|
| 159 |
+
"ground_truth": "AgentFEM three-memory Chaboche with tabulated isotropic hardening",
|
| 160 |
+
"scope": "Out-of-template synthetic closure cohort; fixed material.",
|
| 161 |
+
"elapsed_seconds": time.perf_counter() - started,
|
| 162 |
+
"bytes": DATA_PATH.stat().st_size,
|
| 163 |
+
}
|
| 164 |
+
MANIFEST_PATH.write_text(json.dumps(manifest, indent=2) + "\n", encoding="utf-8")
|
| 165 |
+
print(json.dumps(manifest, indent=2))
|
| 166 |
+
return manifest
|
| 167 |
+
|
| 168 |
+
|
| 169 |
+
def main() -> None:
|
| 170 |
+
parser = argparse.ArgumentParser()
|
| 171 |
+
parser.add_argument("--count-per-family", type=int, default=16)
|
| 172 |
+
parser.add_argument("--force", action="store_true")
|
| 173 |
+
args = parser.parse_args()
|
| 174 |
+
generate(args.count_per_family, force=args.force)
|
| 175 |
+
|
| 176 |
+
|
| 177 |
+
if __name__ == "__main__":
|
| 178 |
+
main()
|
src/generate_t2_graybox_cohort.py
ADDED
|
@@ -0,0 +1,183 @@
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|
| 1 |
+
"""Generate the fixed-material cohort for T2 gray-box hardening discovery."""
|
| 2 |
+
|
| 3 |
+
from __future__ import annotations
|
| 4 |
+
|
| 5 |
+
import argparse
|
| 6 |
+
import json
|
| 7 |
+
import time
|
| 8 |
+
from pathlib import Path
|
| 9 |
+
|
| 10 |
+
import h5py
|
| 11 |
+
import numpy as np
|
| 12 |
+
|
| 13 |
+
from agentfem import constitutive
|
| 14 |
+
|
| 15 |
+
from src.t2_multiaxial_ood_v2 import (
|
| 16 |
+
PATH_FAMILIES,
|
| 17 |
+
design_parameters,
|
| 18 |
+
strain_history,
|
| 19 |
+
tensor_to_voigt,
|
| 20 |
+
)
|
| 21 |
+
|
| 22 |
+
|
| 23 |
+
ROOT = Path(__file__).resolve().parents[1]
|
| 24 |
+
DATA_DIR = ROOT / "data" / "t2_graybox_hardening_v1"
|
| 25 |
+
DATA_PATH = DATA_DIR / "cohort.h5"
|
| 26 |
+
MANIFEST_PATH = DATA_DIR / "manifest.json"
|
| 27 |
+
|
| 28 |
+
MATERIAL = {
|
| 29 |
+
"young_pa": 190.0e9,
|
| 30 |
+
"poisson": 0.30,
|
| 31 |
+
"yield_stress_pa": 280.0e6,
|
| 32 |
+
"backstress_c1_pa": 35.0e9,
|
| 33 |
+
"backstress_gamma1": 60.0,
|
| 34 |
+
"backstress_c2_pa": 8.0e9,
|
| 35 |
+
"backstress_gamma2": 8.0,
|
| 36 |
+
"isotropic_saturation_pa": 70.0e6,
|
| 37 |
+
"isotropic_rate": 8.0,
|
| 38 |
+
}
|
| 39 |
+
|
| 40 |
+
|
| 41 |
+
def design(count_per_family: int = 32) -> list[dict[str, object]]:
|
| 42 |
+
if count_per_family < 4 or count_per_family > 64:
|
| 43 |
+
raise ValueError("count_per_family must be between 4 and 64.")
|
| 44 |
+
source = design_parameters()
|
| 45 |
+
rows: list[dict[str, object]] = []
|
| 46 |
+
for family_index, family in enumerate(PATH_FAMILIES):
|
| 47 |
+
start = 512 + family_index * 64
|
| 48 |
+
for replicate in range(count_per_family):
|
| 49 |
+
row = dict(source[start + replicate])
|
| 50 |
+
row.update(MATERIAL)
|
| 51 |
+
row["material_model"] = "hidden_combined_hardening"
|
| 52 |
+
row["path_family"] = family
|
| 53 |
+
row["replicate"] = replicate
|
| 54 |
+
row["hardening_modulus_pa"] = 0.0
|
| 55 |
+
rows.append(row)
|
| 56 |
+
return rows
|
| 57 |
+
|
| 58 |
+
|
| 59 |
+
def split_for_family(family: str) -> str:
|
| 60 |
+
if family in {
|
| 61 |
+
"proportional_axial_cycle",
|
| 62 |
+
"proportional_shear_cycle",
|
| 63 |
+
"sequential_axial_shear",
|
| 64 |
+
"orthogonal_cross",
|
| 65 |
+
"nonproportional_square",
|
| 66 |
+
}:
|
| 67 |
+
return "train"
|
| 68 |
+
if family == "rotating_principal_cycle":
|
| 69 |
+
return "validation"
|
| 70 |
+
return "test"
|
| 71 |
+
|
| 72 |
+
|
| 73 |
+
def solve(
|
| 74 |
+
parameters: dict[str, object], *, points: int | None = None
|
| 75 |
+
) -> dict[str, np.ndarray]:
|
| 76 |
+
law = constitutive.chaboche(
|
| 77 |
+
young=float(parameters["young_pa"]),
|
| 78 |
+
poisson=float(parameters["poisson"]),
|
| 79 |
+
yield_stress=float(parameters["yield_stress_pa"]),
|
| 80 |
+
backstresses=(
|
| 81 |
+
(
|
| 82 |
+
float(parameters["backstress_c1_pa"]),
|
| 83 |
+
float(parameters["backstress_gamma1"]),
|
| 84 |
+
),
|
| 85 |
+
(
|
| 86 |
+
float(parameters["backstress_c2_pa"]),
|
| 87 |
+
float(parameters["backstress_gamma2"]),
|
| 88 |
+
),
|
| 89 |
+
),
|
| 90 |
+
isotropic_saturation=float(parameters["isotropic_saturation_pa"]),
|
| 91 |
+
isotropic_rate=float(parameters["isotropic_rate"]),
|
| 92 |
+
)
|
| 93 |
+
coordinates, strains = strain_history(parameters, points=points)
|
| 94 |
+
count = len(strains)
|
| 95 |
+
stress = np.empty_like(strains)
|
| 96 |
+
plastic = np.empty_like(strains)
|
| 97 |
+
peeq = np.empty(count)
|
| 98 |
+
increment = np.empty(count)
|
| 99 |
+
memories = np.empty((count, 2, 3, 3))
|
| 100 |
+
radius = np.empty(count)
|
| 101 |
+
state = None
|
| 102 |
+
for index, strain in enumerate(strains):
|
| 103 |
+
update = law.update(strain, state, linearization="none")
|
| 104 |
+
state = update.state
|
| 105 |
+
stress[index] = update.stress
|
| 106 |
+
plastic[index] = state.plastic_strain
|
| 107 |
+
peeq[index] = state.equivalent_plastic_strain
|
| 108 |
+
increment[index] = update.plastic_multiplier_increment
|
| 109 |
+
memories[index] = state.backstresses
|
| 110 |
+
radius[index] = law.current_yield_stress(peeq[index]) - law.yield_stress
|
| 111 |
+
return {
|
| 112 |
+
"strain": tensor_to_voigt(strains),
|
| 113 |
+
"stress_pa": tensor_to_voigt(stress),
|
| 114 |
+
"plastic_strain": tensor_to_voigt(plastic),
|
| 115 |
+
"peeq": peeq,
|
| 116 |
+
"plastic_increment": increment,
|
| 117 |
+
"memories_pa": tensor_to_voigt(memories),
|
| 118 |
+
"isotropic_radius_pa": radius,
|
| 119 |
+
"path_coordinates": coordinates,
|
| 120 |
+
}
|
| 121 |
+
|
| 122 |
+
|
| 123 |
+
def generate(count_per_family: int = 32, *, force: bool = False) -> dict[str, object]:
|
| 124 |
+
rows = design(count_per_family)
|
| 125 |
+
DATA_DIR.mkdir(parents=True, exist_ok=True)
|
| 126 |
+
if DATA_PATH.exists() and not force:
|
| 127 |
+
raise FileExistsError(f"{DATA_PATH} already exists; pass --force to replace it.")
|
| 128 |
+
temporary = DATA_PATH.with_suffix(".h5.tmp")
|
| 129 |
+
started = time.perf_counter()
|
| 130 |
+
with h5py.File(temporary, "w") as h5:
|
| 131 |
+
h5.attrs["schema"] = "agentfem.physics-data.graybox-hardening"
|
| 132 |
+
h5.attrs["schema_version"] = "1.0.0-pilot"
|
| 133 |
+
h5.attrs["material_json"] = json.dumps(MATERIAL, sort_keys=True)
|
| 134 |
+
for index, row in enumerate(rows):
|
| 135 |
+
group = h5.create_group(f"{index:05d}")
|
| 136 |
+
group.attrs["path_family"] = str(row["path_family"])
|
| 137 |
+
group.attrs["split"] = split_for_family(str(row["path_family"]))
|
| 138 |
+
group.attrs["parameters_json"] = json.dumps(row, sort_keys=True)
|
| 139 |
+
for name, value in solve(row).items():
|
| 140 |
+
group.create_dataset(name, data=value, compression="gzip", shuffle=True)
|
| 141 |
+
temporary.replace(DATA_PATH)
|
| 142 |
+
manifest = {
|
| 143 |
+
"schema": "agentfem.physics-data.graybox-hardening",
|
| 144 |
+
"schema_version": "1.0.0-pilot",
|
| 145 |
+
"sample_count": len(rows),
|
| 146 |
+
"count_per_family": count_per_family,
|
| 147 |
+
"points_per_trajectory": 241,
|
| 148 |
+
"path_families": list(PATH_FAMILIES),
|
| 149 |
+
"splits": {
|
| 150 |
+
"train": 5 * count_per_family,
|
| 151 |
+
"validation": count_per_family,
|
| 152 |
+
"test": 2 * count_per_family,
|
| 153 |
+
},
|
| 154 |
+
"known_to_model": ["young_pa", "poisson", "yield_stress_pa"],
|
| 155 |
+
"hidden_from_model": [
|
| 156 |
+
"backstress_c1_pa",
|
| 157 |
+
"backstress_gamma1",
|
| 158 |
+
"backstress_c2_pa",
|
| 159 |
+
"backstress_gamma2",
|
| 160 |
+
"isotropic_saturation_pa",
|
| 161 |
+
"isotropic_rate",
|
| 162 |
+
"hardening_update_equations",
|
| 163 |
+
],
|
| 164 |
+
"ground_truth": "AgentFEM Chaboche combined hardening",
|
| 165 |
+
"scope": "Fixed synthetic material; controlled recovery-of-known-law cohort.",
|
| 166 |
+
"elapsed_seconds": time.perf_counter() - started,
|
| 167 |
+
"bytes": DATA_PATH.stat().st_size,
|
| 168 |
+
}
|
| 169 |
+
MANIFEST_PATH.write_text(json.dumps(manifest, indent=2) + "\n", encoding="utf-8")
|
| 170 |
+
print(json.dumps(manifest, indent=2))
|
| 171 |
+
return manifest
|
| 172 |
+
|
| 173 |
+
|
| 174 |
+
def main() -> None:
|
| 175 |
+
parser = argparse.ArgumentParser()
|
| 176 |
+
parser.add_argument("--count-per-family", type=int, default=32)
|
| 177 |
+
parser.add_argument("--force", action="store_true")
|
| 178 |
+
args = parser.parse_args()
|
| 179 |
+
generate(args.count_per_family, force=args.force)
|
| 180 |
+
|
| 181 |
+
|
| 182 |
+
if __name__ == "__main__":
|
| 183 |
+
main()
|
src/plot_t2_graybox_closure.py
ADDED
|
@@ -0,0 +1,133 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
"""Create compact paper-ready figures for the incomplete-physics closure."""
|
| 2 |
+
|
| 3 |
+
from __future__ import annotations
|
| 4 |
+
|
| 5 |
+
import json
|
| 6 |
+
from pathlib import Path
|
| 7 |
+
|
| 8 |
+
import matplotlib
|
| 9 |
+
|
| 10 |
+
matplotlib.use("Agg")
|
| 11 |
+
import matplotlib.pyplot as plt
|
| 12 |
+
import numpy as np
|
| 13 |
+
import torch
|
| 14 |
+
|
| 15 |
+
from src import t2_graybox_discrete_energy as graybox
|
| 16 |
+
from src.generate_t2_graybox_closure import MATERIAL
|
| 17 |
+
from src.train_t2_graybox_discrete_energy import load_cohort
|
| 18 |
+
from src.train_t2_multiaxial_models import RecurrentStress
|
| 19 |
+
|
| 20 |
+
|
| 21 |
+
ROOT = Path(__file__).resolve().parents[1]
|
| 22 |
+
DATA = ROOT / "data" / "t2_graybox_closure_v1" / "cohort.h5"
|
| 23 |
+
MODELS = ROOT / "models" / "t2_graybox_closure_v1"
|
| 24 |
+
ARTIFACTS = ROOT / "artifacts" / "t2_graybox_closure_v1"
|
| 25 |
+
|
| 26 |
+
|
| 27 |
+
def main() -> None:
|
| 28 |
+
cohort = load_cohort(DATA)
|
| 29 |
+
denrm_checkpoint = torch.load(MODELS / "denrm.pt", map_location="cpu", weights_only=False)
|
| 30 |
+
denrm = graybox.NeuralHardeningLaw(channels=2)
|
| 31 |
+
denrm.load_state_dict(denrm_checkpoint["state_dict"])
|
| 32 |
+
denrm.eval()
|
| 33 |
+
gru_checkpoint = torch.load(MODELS / "gru.pt", map_location="cpu", weights_only=False)
|
| 34 |
+
gru = RecurrentStress(6, cell="gru", hidden=72)
|
| 35 |
+
gru.load_state_dict(gru_checkpoint["state_dict"])
|
| 36 |
+
gru.eval()
|
| 37 |
+
norm = gru_checkpoint["normalization"]
|
| 38 |
+
with torch.no_grad():
|
| 39 |
+
denrm_stress = graybox.rollout(
|
| 40 |
+
cohort.strain,
|
| 41 |
+
torch.full((len(cohort.strain),), float(MATERIAL["young_pa"])),
|
| 42 |
+
torch.full((len(cohort.strain),), float(MATERIAL["poisson"])),
|
| 43 |
+
torch.full((len(cohort.strain),), float(MATERIAL["yield_stress_pa"])),
|
| 44 |
+
denrm,
|
| 45 |
+
bisection_iterations=24,
|
| 46 |
+
)["stress"]
|
| 47 |
+
gru_stress = (
|
| 48 |
+
gru((cohort.strain - norm["strain_mean"]) / norm["strain_std"])
|
| 49 |
+
* norm["stress_std"]
|
| 50 |
+
+ norm["stress_mean"]
|
| 51 |
+
)
|
| 52 |
+
|
| 53 |
+
metrics = json.loads((ARTIFACTS / "model_metrics.json").read_text())
|
| 54 |
+
figure, axes = plt.subplots(2, 2, figsize=(11.0, 7.8), constrained_layout=True)
|
| 55 |
+
colors = {"truth": "#1f2937", "denrm": "#e11d48", "gru": "#2563eb"}
|
| 56 |
+
component_labels = ("xx", "yy", "zz", "xy", "yz", "xz")
|
| 57 |
+
for axis, family in zip(
|
| 58 |
+
axes[0], ("out_of_phase_lissajous", "random_direction_blocks"), strict=True
|
| 59 |
+
):
|
| 60 |
+
index = next(i for i, value in enumerate(cohort.families) if value == family)
|
| 61 |
+
strain = cohort.strain[index].numpy()
|
| 62 |
+
component = int(np.argmax(np.ptp(strain, axis=0)))
|
| 63 |
+
x = 100.0 * strain[:, component]
|
| 64 |
+
axis.plot(
|
| 65 |
+
x,
|
| 66 |
+
cohort.stress[index, :, component].numpy() / 1.0e6,
|
| 67 |
+
color=colors["truth"],
|
| 68 |
+
linewidth=2.1,
|
| 69 |
+
label="AgentFEM reference",
|
| 70 |
+
)
|
| 71 |
+
axis.plot(
|
| 72 |
+
x,
|
| 73 |
+
denrm_stress[index, :, component].numpy() / 1.0e6,
|
| 74 |
+
"--",
|
| 75 |
+
color=colors["denrm"],
|
| 76 |
+
linewidth=1.8,
|
| 77 |
+
label="DENIM (2-state closure)",
|
| 78 |
+
)
|
| 79 |
+
axis.plot(
|
| 80 |
+
x,
|
| 81 |
+
gru_stress[index, :, component].numpy() / 1.0e6,
|
| 82 |
+
color=colors["gru"],
|
| 83 |
+
linewidth=1.1,
|
| 84 |
+
alpha=0.85,
|
| 85 |
+
label="GRU",
|
| 86 |
+
)
|
| 87 |
+
axis.set_title(family.replace("_", " "))
|
| 88 |
+
axis.set_xlabel(f"strain {component_labels[component]} (%)")
|
| 89 |
+
axis.set_ylabel(f"stress {component_labels[component]} (MPa)")
|
| 90 |
+
axis.grid(alpha=0.22)
|
| 91 |
+
axes[0, 0].legend(frameon=False, fontsize=8)
|
| 92 |
+
|
| 93 |
+
names = ("Incomplete J2", "GRU", "DENIM")
|
| 94 |
+
keys = ("incomplete_j2", "gru", "denrm")
|
| 95 |
+
rmse = [metrics["models"][key]["test"]["rmse_mpa"] for key in keys]
|
| 96 |
+
bars = axes[1, 0].bar(
|
| 97 |
+
names, rmse, color=("#9ca3af", colors["gru"], colors["denrm"])
|
| 98 |
+
)
|
| 99 |
+
axes[1, 0].bar_label(bars, fmt="%.2f")
|
| 100 |
+
axes[1, 0].set_ylabel("held-out path RMSE (MPa)")
|
| 101 |
+
axes[1, 0].set_title("unseen loading-path accuracy")
|
| 102 |
+
axes[1, 0].grid(axis="y", alpha=0.22)
|
| 103 |
+
|
| 104 |
+
peeq = np.linspace(0.0, 0.10, 250)
|
| 105 |
+
with torch.no_grad():
|
| 106 |
+
learned = denrm.isotropic(
|
| 107 |
+
torch.tensor(peeq, dtype=torch.float32),
|
| 108 |
+
torch.full((len(peeq),), float(MATERIAL["yield_stress_pa"])),
|
| 109 |
+
).numpy()
|
| 110 |
+
reference = np.interp(
|
| 111 |
+
peeq,
|
| 112 |
+
np.asarray(MATERIAL["hardening_peeq"]),
|
| 113 |
+
np.asarray(MATERIAL["hardening_stress_pa"]),
|
| 114 |
+
) - float(MATERIAL["yield_stress_pa"])
|
| 115 |
+
axes[1, 1].plot(peeq, reference / 1.0e6, color=colors["truth"], linewidth=2.1, label="hidden table")
|
| 116 |
+
axes[1, 1].plot(peeq, learned / 1.0e6, "--", color=colors["denrm"], linewidth=1.8, label="learned monotone law")
|
| 117 |
+
axes[1, 1].set_xlabel("equivalent plastic strain")
|
| 118 |
+
axes[1, 1].set_ylabel("isotropic hardening radius (MPa)")
|
| 119 |
+
axes[1, 1].set_title("unknown hardening-law recovery")
|
| 120 |
+
axes[1, 1].grid(alpha=0.22)
|
| 121 |
+
axes[1, 1].legend(frameon=False, fontsize=8)
|
| 122 |
+
|
| 123 |
+
figure.suptitle(
|
| 124 |
+
"Incomplete-physics closure: 3-state tabulated reference → 2-state DENIM",
|
| 125 |
+
fontsize=13,
|
| 126 |
+
)
|
| 127 |
+
ARTIFACTS.mkdir(parents=True, exist_ok=True)
|
| 128 |
+
figure.savefig(ARTIFACTS / "closure_summary.png", dpi=220)
|
| 129 |
+
plt.close(figure)
|
| 130 |
+
|
| 131 |
+
|
| 132 |
+
if __name__ == "__main__":
|
| 133 |
+
main()
|
src/t2_graybox_discrete_energy.py
ADDED
|
@@ -0,0 +1,531 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
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|
| 1 |
+
"""Core assets for a discrete-energy neural hardening return map.
|
| 2 |
+
|
| 3 |
+
This module deliberately keeps elasticity and J2 kinematics explicit while
|
| 4 |
+
leaving the isotropic hardening curve and state-dependent dynamic recovery to
|
| 5 |
+
small neural functions. It is the constitutive core of the T2 gray-box study,
|
| 6 |
+
not yet an AgentFEM material provider.
|
| 7 |
+
"""
|
| 8 |
+
|
| 9 |
+
from __future__ import annotations
|
| 10 |
+
|
| 11 |
+
from dataclasses import dataclass
|
| 12 |
+
|
| 13 |
+
import torch
|
| 14 |
+
from torch import nn
|
| 15 |
+
from torch.nn import functional as F
|
| 16 |
+
|
| 17 |
+
|
| 18 |
+
VOIGT_WEIGHTS = torch.tensor((1.0, 1.0, 1.0, 2.0, 2.0, 2.0))
|
| 19 |
+
|
| 20 |
+
|
| 21 |
+
def double_contract(left: torch.Tensor, right: torch.Tensor) -> torch.Tensor:
|
| 22 |
+
weights = VOIGT_WEIGHTS.to(dtype=left.dtype, device=left.device)
|
| 23 |
+
return (left * right * weights).sum(dim=-1)
|
| 24 |
+
|
| 25 |
+
|
| 26 |
+
def deviatoric(value: torch.Tensor) -> torch.Tensor:
|
| 27 |
+
mean = value[..., :3].mean(dim=-1, keepdim=True)
|
| 28 |
+
return torch.cat((value[..., :3] - mean, value[..., 3:]), dim=-1)
|
| 29 |
+
|
| 30 |
+
|
| 31 |
+
def von_mises(value: torch.Tensor) -> torch.Tensor:
|
| 32 |
+
selected = deviatoric(value)
|
| 33 |
+
return torch.sqrt(torch.clamp(1.5 * double_contract(selected, selected), min=0.0))
|
| 34 |
+
|
| 35 |
+
|
| 36 |
+
def elastic_stress(
|
| 37 |
+
strain: torch.Tensor,
|
| 38 |
+
plastic_strain: torch.Tensor,
|
| 39 |
+
young: torch.Tensor,
|
| 40 |
+
poisson: torch.Tensor,
|
| 41 |
+
) -> torch.Tensor:
|
| 42 |
+
elastic = strain - plastic_strain
|
| 43 |
+
shear = young / (2.0 * (1.0 + poisson))
|
| 44 |
+
bulk = young / (3.0 * (1.0 - 2.0 * poisson))
|
| 45 |
+
trace = elastic[..., :3].sum(dim=-1)
|
| 46 |
+
mean = trace / 3.0
|
| 47 |
+
normal = (
|
| 48 |
+
2.0 * shear[..., None] * (elastic[..., :3] - mean[..., None])
|
| 49 |
+
+ bulk[..., None] * trace[..., None]
|
| 50 |
+
)
|
| 51 |
+
return torch.cat((normal, 2.0 * shear[..., None] * elastic[..., 3:]), dim=-1)
|
| 52 |
+
|
| 53 |
+
|
| 54 |
+
class MonotoneIsotropicHardening(nn.Module):
|
| 55 |
+
"""Zero-anchored monotone saturating hardening curve.
|
| 56 |
+
|
| 57 |
+
A positive mixture of exponential saturation modes represents Voce-like
|
| 58 |
+
and tabulated concave hardening while a nonnegative linear tail permits
|
| 59 |
+
continued hardening. Positivity makes monotonicity structural rather than
|
| 60 |
+
a soft training penalty.
|
| 61 |
+
"""
|
| 62 |
+
|
| 63 |
+
def __init__(self, neurons: int = 12, plastic_scale: float = 0.01):
|
| 64 |
+
super().__init__()
|
| 65 |
+
self.plastic_scale = float(plastic_scale)
|
| 66 |
+
self.raw_weight = nn.Parameter(torch.full((neurons,), -5.0))
|
| 67 |
+
self.raw_slope = nn.Parameter(torch.linspace(-1.5, 1.5, neurons))
|
| 68 |
+
self.raw_linear = nn.Parameter(torch.tensor(-5.0))
|
| 69 |
+
|
| 70 |
+
def _positive_parameters(self) -> tuple[torch.Tensor, torch.Tensor, torch.Tensor]:
|
| 71 |
+
weight = F.softplus(self.raw_weight)
|
| 72 |
+
slope = F.softplus(self.raw_slope) + 1.0e-6
|
| 73 |
+
linear = F.softplus(self.raw_linear)
|
| 74 |
+
return weight, slope, linear
|
| 75 |
+
|
| 76 |
+
def forward(self, peeq: torch.Tensor, stress_scale: torch.Tensor) -> torch.Tensor:
|
| 77 |
+
weight, slope, linear = self._positive_parameters()
|
| 78 |
+
coordinate = peeq[..., None] / self.plastic_scale
|
| 79 |
+
saturation = -torch.expm1(-slope * coordinate)
|
| 80 |
+
dimensionless = linear * coordinate.squeeze(-1) + (
|
| 81 |
+
weight * saturation
|
| 82 |
+
).sum(dim=-1)
|
| 83 |
+
return stress_scale * dimensionless
|
| 84 |
+
|
| 85 |
+
def derivative(self, peeq: torch.Tensor, stress_scale: torch.Tensor) -> torch.Tensor:
|
| 86 |
+
weight, slope, linear = self._positive_parameters()
|
| 87 |
+
coordinate = peeq[..., None] / self.plastic_scale
|
| 88 |
+
value = linear + (
|
| 89 |
+
weight * slope * torch.exp(-slope * coordinate)
|
| 90 |
+
).sum(dim=-1)
|
| 91 |
+
return stress_scale * value / self.plastic_scale
|
| 92 |
+
|
| 93 |
+
def stored_energy(self, peeq: torch.Tensor, stress_scale: torch.Tensor) -> torch.Tensor:
|
| 94 |
+
coordinate = torch.linspace(
|
| 95 |
+
0.0, 1.0, 65, dtype=peeq.dtype, device=peeq.device
|
| 96 |
+
)
|
| 97 |
+
points = peeq[..., None] * coordinate
|
| 98 |
+
values = self.forward(points, stress_scale[..., None])
|
| 99 |
+
return torch.trapezoid(values, points, dim=-1)
|
| 100 |
+
|
| 101 |
+
|
| 102 |
+
class ObjectiveRecoveryNetwork(nn.Module):
|
| 103 |
+
"""Positive recovery rates from objective scalar state descriptors."""
|
| 104 |
+
|
| 105 |
+
def __init__(self, channels: int = 2, hidden: int = 24):
|
| 106 |
+
super().__init__()
|
| 107 |
+
self.channels = int(channels)
|
| 108 |
+
input_size = 3 + 3 * self.channels
|
| 109 |
+
self.network = nn.Sequential(
|
| 110 |
+
nn.Linear(input_size, hidden),
|
| 111 |
+
nn.SiLU(),
|
| 112 |
+
nn.Linear(hidden, hidden),
|
| 113 |
+
nn.SiLU(),
|
| 114 |
+
nn.Linear(hidden, self.channels),
|
| 115 |
+
)
|
| 116 |
+
nn.init.zeros_(self.network[-1].weight)
|
| 117 |
+
nn.init.constant_(self.network[-1].bias, -1.0)
|
| 118 |
+
|
| 119 |
+
def features(
|
| 120 |
+
self,
|
| 121 |
+
peeq: torch.Tensor,
|
| 122 |
+
isotropic_radius: torch.Tensor,
|
| 123 |
+
flow_direction: torch.Tensor,
|
| 124 |
+
memories: torch.Tensor,
|
| 125 |
+
stress_scale: torch.Tensor,
|
| 126 |
+
reversal: torch.Tensor,
|
| 127 |
+
) -> torch.Tensor:
|
| 128 |
+
scale = stress_scale.clamp_min(1.0)
|
| 129 |
+
norms = torch.sqrt(
|
| 130 |
+
torch.clamp(double_contract(memories, memories), min=0.0)
|
| 131 |
+
) / scale[..., None]
|
| 132 |
+
projections = double_contract(memories, flow_direction[..., None, :]) / scale[..., None]
|
| 133 |
+
cross = torch.zeros_like(norms)
|
| 134 |
+
if self.channels > 1:
|
| 135 |
+
for index in range(self.channels):
|
| 136 |
+
other = (index + 1) % self.channels
|
| 137 |
+
cross[..., index] = double_contract(
|
| 138 |
+
memories[..., index, :], memories[..., other, :]
|
| 139 |
+
) / scale.square()
|
| 140 |
+
scalars = torch.stack(
|
| 141 |
+
(peeq / 0.02, isotropic_radius / scale, reversal), dim=-1
|
| 142 |
+
)
|
| 143 |
+
return torch.cat((scalars, norms, projections, cross), dim=-1)
|
| 144 |
+
|
| 145 |
+
def forward(
|
| 146 |
+
self,
|
| 147 |
+
peeq: torch.Tensor,
|
| 148 |
+
isotropic_radius: torch.Tensor,
|
| 149 |
+
flow_direction: torch.Tensor,
|
| 150 |
+
memories: torch.Tensor,
|
| 151 |
+
stress_scale: torch.Tensor,
|
| 152 |
+
reversal: torch.Tensor,
|
| 153 |
+
) -> torch.Tensor:
|
| 154 |
+
values = self.features(
|
| 155 |
+
peeq,
|
| 156 |
+
isotropic_radius,
|
| 157 |
+
flow_direction,
|
| 158 |
+
memories,
|
| 159 |
+
stress_scale,
|
| 160 |
+
reversal,
|
| 161 |
+
)
|
| 162 |
+
return 200.0 * torch.sigmoid(self.network(values)) + 1.0e-6
|
| 163 |
+
|
| 164 |
+
|
| 165 |
+
@dataclass
|
| 166 |
+
class GrayboxState:
|
| 167 |
+
plastic_strain: torch.Tensor
|
| 168 |
+
peeq: torch.Tensor
|
| 169 |
+
memories: torch.Tensor
|
| 170 |
+
previous_flow: torch.Tensor
|
| 171 |
+
|
| 172 |
+
@property
|
| 173 |
+
def backstress(self) -> torch.Tensor:
|
| 174 |
+
return self.memories.sum(dim=-2)
|
| 175 |
+
|
| 176 |
+
|
| 177 |
+
def initial_state(
|
| 178 |
+
batch: int,
|
| 179 |
+
*,
|
| 180 |
+
channels: int = 2,
|
| 181 |
+
dtype: torch.dtype = torch.float32,
|
| 182 |
+
device: torch.device | str = "cpu",
|
| 183 |
+
) -> GrayboxState:
|
| 184 |
+
tensor = torch.zeros((batch, 6), dtype=dtype, device=device)
|
| 185 |
+
memories = torch.zeros((batch, channels, 6), dtype=dtype, device=device)
|
| 186 |
+
return GrayboxState(
|
| 187 |
+
plastic_strain=tensor,
|
| 188 |
+
peeq=torch.zeros(batch, dtype=dtype, device=device),
|
| 189 |
+
memories=memories,
|
| 190 |
+
previous_flow=tensor.clone(),
|
| 191 |
+
)
|
| 192 |
+
|
| 193 |
+
|
| 194 |
+
class NeuralHardeningLaw(nn.Module):
|
| 195 |
+
"""Unknown hardening law embedded in a known J2 state representation."""
|
| 196 |
+
|
| 197 |
+
def __init__(self, channels: int = 2):
|
| 198 |
+
super().__init__()
|
| 199 |
+
self.channels = int(channels)
|
| 200 |
+
self.raw_moduli = nn.Parameter(torch.linspace(2.0, 0.0, channels))
|
| 201 |
+
self.log_total_modulus_ratio = nn.Parameter(torch.tensor(5.0))
|
| 202 |
+
self.isotropic = MonotoneIsotropicHardening()
|
| 203 |
+
self.recovery = ObjectiveRecoveryNetwork(channels=channels)
|
| 204 |
+
|
| 205 |
+
def moduli(self, stress_scale: torch.Tensor) -> torch.Tensor:
|
| 206 |
+
fractions = torch.softmax(self.raw_moduli, dim=0)
|
| 207 |
+
total = torch.exp(self.log_total_modulus_ratio).clamp(max=500.0)
|
| 208 |
+
return total * stress_scale[..., None] * fractions
|
| 209 |
+
|
| 210 |
+
def update_memories(
|
| 211 |
+
self,
|
| 212 |
+
state: GrayboxState,
|
| 213 |
+
flow_direction: torch.Tensor,
|
| 214 |
+
increment: torch.Tensor,
|
| 215 |
+
stress_scale: torch.Tensor,
|
| 216 |
+
) -> tuple[torch.Tensor, torch.Tensor, torch.Tensor]:
|
| 217 |
+
isotropic = self.isotropic(state.peeq, stress_scale)
|
| 218 |
+
old_norm = torch.sqrt(
|
| 219 |
+
torch.clamp(double_contract(state.previous_flow, state.previous_flow), min=0.0)
|
| 220 |
+
)
|
| 221 |
+
current_norm = torch.sqrt(
|
| 222 |
+
torch.clamp(double_contract(flow_direction, flow_direction), min=0.0)
|
| 223 |
+
)
|
| 224 |
+
reversal = double_contract(state.previous_flow, flow_direction) / (
|
| 225 |
+
old_norm * current_norm
|
| 226 |
+
).clamp_min(1.0e-12)
|
| 227 |
+
recovery = self.recovery(
|
| 228 |
+
state.peeq,
|
| 229 |
+
isotropic,
|
| 230 |
+
flow_direction,
|
| 231 |
+
state.memories,
|
| 232 |
+
stress_scale,
|
| 233 |
+
reversal,
|
| 234 |
+
)
|
| 235 |
+
moduli = self.moduli(stress_scale)
|
| 236 |
+
numerator = state.memories + (
|
| 237 |
+
(2.0 / 3.0)
|
| 238 |
+
* moduli[..., :, None]
|
| 239 |
+
* increment[..., None, None]
|
| 240 |
+
* flow_direction[..., None, :]
|
| 241 |
+
)
|
| 242 |
+
denominator = 1.0 + recovery * increment[..., None]
|
| 243 |
+
updated = numerator / denominator[..., None]
|
| 244 |
+
return updated, recovery, moduli
|
| 245 |
+
|
| 246 |
+
|
| 247 |
+
def _candidate_update(
|
| 248 |
+
trial_deviatoric: torch.Tensor,
|
| 249 |
+
state: GrayboxState,
|
| 250 |
+
increment: torch.Tensor,
|
| 251 |
+
shear: torch.Tensor,
|
| 252 |
+
yield_stress: torch.Tensor,
|
| 253 |
+
law: NeuralHardeningLaw,
|
| 254 |
+
*,
|
| 255 |
+
direction_iterations: int = 6,
|
| 256 |
+
) -> tuple[torch.Tensor, torch.Tensor, torch.Tensor, torch.Tensor, torch.Tensor]:
|
| 257 |
+
shifted_trial = trial_deviatoric - state.backstress
|
| 258 |
+
direction = 1.5 * shifted_trial / von_mises(shifted_trial).clamp_min(1.0)[..., None]
|
| 259 |
+
recovery = moduli = None
|
| 260 |
+
memories = state.memories
|
| 261 |
+
# For a fixed plastic increment the Armstrong--Frederick-type backward
|
| 262 |
+
# Euler update can be rearranged before finding the direction. Removing
|
| 263 |
+
# the large term proportional to G*increment avoids the oscillatory vector
|
| 264 |
+
# fixed point that occurs when a coarse increment rotates the loading path
|
| 265 |
+
# by nearly 90 degrees.
|
| 266 |
+
for _ in range(direction_iterations):
|
| 267 |
+
memories, recovery, moduli = law.update_memories(
|
| 268 |
+
state, direction, increment, yield_stress
|
| 269 |
+
)
|
| 270 |
+
denominator = 1.0 + recovery * increment[..., None]
|
| 271 |
+
effective_trial = trial_deviatoric - (
|
| 272 |
+
state.memories / denominator[..., None]
|
| 273 |
+
).sum(dim=-2)
|
| 274 |
+
direction = (
|
| 275 |
+
1.5
|
| 276 |
+
* effective_trial
|
| 277 |
+
/ von_mises(effective_trial).clamp_min(1.0)[..., None]
|
| 278 |
+
)
|
| 279 |
+
memories, recovery, moduli = law.update_memories(
|
| 280 |
+
state, direction, increment, yield_stress
|
| 281 |
+
)
|
| 282 |
+
denominator = 1.0 + recovery * increment[..., None]
|
| 283 |
+
effective_trial = trial_deviatoric - (
|
| 284 |
+
state.memories / denominator[..., None]
|
| 285 |
+
).sum(dim=-2)
|
| 286 |
+
radius = yield_stress + law.isotropic(state.peeq + increment, yield_stress)
|
| 287 |
+
effective_plastic_modulus = 3.0 * shear + (moduli / denominator).sum(dim=-1)
|
| 288 |
+
# Signed consistency equation. Unlike taking von Mises of an overshot
|
| 289 |
+
# trial state, this remains monotone after the root and therefore supplies
|
| 290 |
+
# a valid bracket for bisection.
|
| 291 |
+
residual = (
|
| 292 |
+
von_mises(effective_trial)
|
| 293 |
+
- effective_plastic_modulus * increment
|
| 294 |
+
- radius
|
| 295 |
+
)
|
| 296 |
+
return residual, direction, memories, recovery, moduli
|
| 297 |
+
|
| 298 |
+
|
| 299 |
+
def advance(
|
| 300 |
+
strain: torch.Tensor,
|
| 301 |
+
state: GrayboxState,
|
| 302 |
+
young: torch.Tensor,
|
| 303 |
+
poisson: torch.Tensor,
|
| 304 |
+
yield_stress: torch.Tensor,
|
| 305 |
+
law: NeuralHardeningLaw,
|
| 306 |
+
*,
|
| 307 |
+
bisection_iterations: int = 28,
|
| 308 |
+
direction_iterations: int = 6,
|
| 309 |
+
) -> tuple[torch.Tensor, GrayboxState, dict[str, torch.Tensor]]:
|
| 310 |
+
"""Accept one strain-driven increment using a bracketed neural return map."""
|
| 311 |
+
|
| 312 |
+
trial = elastic_stress(strain, state.plastic_strain, young, poisson)
|
| 313 |
+
trial_deviatoric = deviatoric(trial)
|
| 314 |
+
shifted_trial = trial_deviatoric - state.backstress
|
| 315 |
+
old_radius = yield_stress + law.isotropic(state.peeq, yield_stress)
|
| 316 |
+
trial_function = von_mises(shifted_trial) - old_radius
|
| 317 |
+
plastic = trial_function > yield_stress.clamp_min(1.0) * 1.0e-12
|
| 318 |
+
shear = young / (2.0 * (1.0 + poisson))
|
| 319 |
+
lower = torch.zeros_like(trial_function)
|
| 320 |
+
upper = 2.0 * F.relu(trial_function) / (3.0 * shear).clamp_min(1.0) + 1.0e-14
|
| 321 |
+
# Large non-proportional increments can rotate the flow direction almost
|
| 322 |
+
# orthogonally. A fixed four-doubling bracket silently failed in that
|
| 323 |
+
# regime and accepted a positive consistency residual. Expand until the
|
| 324 |
+
# monotone hardening return is safely bracketed over a much wider range.
|
| 325 |
+
for _ in range(16):
|
| 326 |
+
residual, *_ = _candidate_update(
|
| 327 |
+
trial_deviatoric,
|
| 328 |
+
state,
|
| 329 |
+
upper,
|
| 330 |
+
shear,
|
| 331 |
+
yield_stress,
|
| 332 |
+
law,
|
| 333 |
+
direction_iterations=direction_iterations,
|
| 334 |
+
)
|
| 335 |
+
upper = torch.where(plastic & (residual > 0.0), 2.0 * upper, upper)
|
| 336 |
+
for _ in range(bisection_iterations):
|
| 337 |
+
middle = 0.5 * (lower + upper)
|
| 338 |
+
residual, *_ = _candidate_update(
|
| 339 |
+
trial_deviatoric,
|
| 340 |
+
state,
|
| 341 |
+
middle,
|
| 342 |
+
shear,
|
| 343 |
+
yield_stress,
|
| 344 |
+
law,
|
| 345 |
+
direction_iterations=direction_iterations,
|
| 346 |
+
)
|
| 347 |
+
lower = torch.where(plastic & (residual > 0.0), middle, lower)
|
| 348 |
+
upper = torch.where(plastic & (residual <= 0.0), middle, upper)
|
| 349 |
+
increment = torch.where(plastic, 0.5 * (lower + upper), torch.zeros_like(lower))
|
| 350 |
+
residual, direction, memories, recovery, moduli = _candidate_update(
|
| 351 |
+
trial_deviatoric,
|
| 352 |
+
state,
|
| 353 |
+
increment,
|
| 354 |
+
shear,
|
| 355 |
+
yield_stress,
|
| 356 |
+
law,
|
| 357 |
+
direction_iterations=direction_iterations,
|
| 358 |
+
)
|
| 359 |
+
direction = torch.where(plastic[..., None], direction, torch.zeros_like(direction))
|
| 360 |
+
memories = torch.where(
|
| 361 |
+
plastic[..., None, None], memories, state.memories
|
| 362 |
+
)
|
| 363 |
+
updated = GrayboxState(
|
| 364 |
+
plastic_strain=state.plastic_strain + increment[..., None] * direction,
|
| 365 |
+
peeq=state.peeq + increment,
|
| 366 |
+
memories=memories,
|
| 367 |
+
previous_flow=torch.where(
|
| 368 |
+
plastic[..., None], direction, state.previous_flow
|
| 369 |
+
),
|
| 370 |
+
)
|
| 371 |
+
stress = elastic_stress(strain, updated.plastic_strain, young, poisson)
|
| 372 |
+
return stress, updated, {
|
| 373 |
+
"plastic_increment": increment,
|
| 374 |
+
"yield_residual": torch.where(plastic, residual, torch.zeros_like(residual)),
|
| 375 |
+
"recovery": recovery,
|
| 376 |
+
"moduli": moduli,
|
| 377 |
+
"plastic": plastic,
|
| 378 |
+
}
|
| 379 |
+
|
| 380 |
+
|
| 381 |
+
def rollout(
|
| 382 |
+
strain: torch.Tensor,
|
| 383 |
+
young: torch.Tensor,
|
| 384 |
+
poisson: torch.Tensor,
|
| 385 |
+
yield_stress: torch.Tensor,
|
| 386 |
+
law: NeuralHardeningLaw,
|
| 387 |
+
*,
|
| 388 |
+
bisection_iterations: int = 28,
|
| 389 |
+
) -> dict[str, torch.Tensor]:
|
| 390 |
+
"""Integrate a batch of complete strain histories."""
|
| 391 |
+
|
| 392 |
+
batch, points, _ = strain.shape
|
| 393 |
+
state = initial_state(
|
| 394 |
+
batch,
|
| 395 |
+
channels=law.channels,
|
| 396 |
+
dtype=strain.dtype,
|
| 397 |
+
device=strain.device,
|
| 398 |
+
)
|
| 399 |
+
stresses = []
|
| 400 |
+
plastics = []
|
| 401 |
+
peeqs = []
|
| 402 |
+
memories = []
|
| 403 |
+
increments = []
|
| 404 |
+
residuals = []
|
| 405 |
+
recoveries = []
|
| 406 |
+
moduli_history = []
|
| 407 |
+
for point in range(points):
|
| 408 |
+
stress, state, diagnostics = advance(
|
| 409 |
+
strain[:, point],
|
| 410 |
+
state,
|
| 411 |
+
young,
|
| 412 |
+
poisson,
|
| 413 |
+
yield_stress,
|
| 414 |
+
law,
|
| 415 |
+
bisection_iterations=bisection_iterations,
|
| 416 |
+
)
|
| 417 |
+
stresses.append(stress)
|
| 418 |
+
plastics.append(state.plastic_strain)
|
| 419 |
+
peeqs.append(state.peeq)
|
| 420 |
+
memories.append(state.memories)
|
| 421 |
+
increments.append(diagnostics["plastic_increment"])
|
| 422 |
+
residuals.append(diagnostics["yield_residual"])
|
| 423 |
+
recoveries.append(diagnostics["recovery"])
|
| 424 |
+
moduli_history.append(diagnostics["moduli"])
|
| 425 |
+
return {
|
| 426 |
+
"stress": torch.stack(stresses, dim=1),
|
| 427 |
+
"plastic_strain": torch.stack(plastics, dim=1),
|
| 428 |
+
"peeq": torch.stack(peeqs, dim=1),
|
| 429 |
+
"memories": torch.stack(memories, dim=1),
|
| 430 |
+
"plastic_increment": torch.stack(increments, dim=1),
|
| 431 |
+
"yield_residual": torch.stack(residuals, dim=1),
|
| 432 |
+
"recovery": torch.stack(recoveries, dim=1),
|
| 433 |
+
"moduli": torch.stack(moduli_history, dim=1),
|
| 434 |
+
}
|
| 435 |
+
|
| 436 |
+
|
| 437 |
+
def discrete_energy_ledger(
|
| 438 |
+
result: dict[str, torch.Tensor],
|
| 439 |
+
yield_stress: torch.Tensor,
|
| 440 |
+
law: NeuralHardeningLaw,
|
| 441 |
+
) -> dict[str, torch.Tensor]:
|
| 442 |
+
"""Partition accepted plastic work using the implemented BE update."""
|
| 443 |
+
|
| 444 |
+
plastic = result["plastic_strain"]
|
| 445 |
+
memories = result["memories"]
|
| 446 |
+
peeq = result["peeq"]
|
| 447 |
+
increment = result["plastic_increment"]
|
| 448 |
+
stress = result["stress"]
|
| 449 |
+
old_plastic = torch.cat((torch.zeros_like(plastic[:, :1]), plastic[:, :-1]), dim=1)
|
| 450 |
+
old_memories = torch.cat((torch.zeros_like(memories[:, :1]), memories[:, :-1]), dim=1)
|
| 451 |
+
plastic_work = double_contract(stress, plastic - old_plastic)
|
| 452 |
+
stress_scale = yield_stress[:, None].expand_as(peeq)
|
| 453 |
+
isotropic_energy = law.isotropic.stored_energy(peeq, stress_scale)
|
| 454 |
+
old_isotropic = torch.cat(
|
| 455 |
+
(torch.zeros_like(isotropic_energy[:, :1]), isotropic_energy[:, :-1]), dim=1
|
| 456 |
+
)
|
| 457 |
+
isotropic_change = isotropic_energy - old_isotropic
|
| 458 |
+
moduli = result["moduli"]
|
| 459 |
+
kinematic_energy = (
|
| 460 |
+
3.0 * double_contract(memories, memories) / (4.0 * moduli)
|
| 461 |
+
).sum(dim=-1)
|
| 462 |
+
old_kinematic = torch.cat(
|
| 463 |
+
(torch.zeros_like(kinematic_energy[:, :1]), kinematic_energy[:, :-1]), dim=1
|
| 464 |
+
)
|
| 465 |
+
kinematic_change = kinematic_energy - old_kinematic
|
| 466 |
+
reference = yield_stress[:, None] * increment
|
| 467 |
+
dynamic_recovery = (
|
| 468 |
+
3.0
|
| 469 |
+
* result["recovery"]
|
| 470 |
+
* double_contract(memories, memories)
|
| 471 |
+
* increment[..., None]
|
| 472 |
+
/ (2.0 * moduli)
|
| 473 |
+
).sum(dim=-1)
|
| 474 |
+
memory_increment = memories - old_memories
|
| 475 |
+
backward_euler = (
|
| 476 |
+
3.0 * double_contract(memory_increment, memory_increment) / (4.0 * moduli)
|
| 477 |
+
).sum(dim=-1)
|
| 478 |
+
isotropic_radius = law.isotropic(peeq, stress_scale)
|
| 479 |
+
backward_euler = backward_euler + isotropic_radius * increment - isotropic_change
|
| 480 |
+
balance = (
|
| 481 |
+
plastic_work
|
| 482 |
+
- isotropic_change
|
| 483 |
+
- kinematic_change
|
| 484 |
+
- reference
|
| 485 |
+
- dynamic_recovery
|
| 486 |
+
- backward_euler
|
| 487 |
+
)
|
| 488 |
+
active = increment > 0.0
|
| 489 |
+
zero = torch.zeros_like(balance)
|
| 490 |
+
channels = {
|
| 491 |
+
"plastic_work": plastic_work,
|
| 492 |
+
"isotropic_stored_energy_change": isotropic_change,
|
| 493 |
+
"kinematic_stored_energy_change": kinematic_change,
|
| 494 |
+
"reference_yield_dissipation": reference,
|
| 495 |
+
"dynamic_recovery_dissipation": dynamic_recovery,
|
| 496 |
+
"backward_euler_dissipation": backward_euler,
|
| 497 |
+
"balance_residual": balance,
|
| 498 |
+
}
|
| 499 |
+
return {
|
| 500 |
+
name: torch.where(active, value, zero) for name, value in channels.items()
|
| 501 |
+
}
|
| 502 |
+
|
| 503 |
+
|
| 504 |
+
def hard_constraint_diagnostics(state: GrayboxState) -> dict[str, torch.Tensor]:
|
| 505 |
+
return {
|
| 506 |
+
"maximum_plastic_trace": state.plastic_strain[..., :3].sum(dim=-1).abs(),
|
| 507 |
+
"minimum_peeq": state.peeq,
|
| 508 |
+
"maximum_memory_trace": state.memories[..., :3].sum(dim=-1).abs(),
|
| 509 |
+
}
|
| 510 |
+
|
| 511 |
+
|
| 512 |
+
__all__ = [
|
| 513 |
+
"GrayboxState",
|
| 514 |
+
"MonotoneIsotropicHardening",
|
| 515 |
+
"NeuralHardeningLaw",
|
| 516 |
+
"ObjectiveRecoveryNetwork",
|
| 517 |
+
"advance",
|
| 518 |
+
"deviatoric",
|
| 519 |
+
"double_contract",
|
| 520 |
+
"discrete_energy_ledger",
|
| 521 |
+
"elastic_stress",
|
| 522 |
+
"hard_constraint_diagnostics",
|
| 523 |
+
"initial_state",
|
| 524 |
+
"rollout",
|
| 525 |
+
"von_mises",
|
| 526 |
+
]
|
| 527 |
+
|
| 528 |
+
# Public research name. Keep the descriptive class name for readable source
|
| 529 |
+
# and expose DENIM as the stable method alias used by the model card and demo.
|
| 530 |
+
DENIM = NeuralHardeningLaw
|
| 531 |
+
__all__.append("DENIM")
|
src/train_t2_graybox_closure.py
ADDED
|
@@ -0,0 +1,24 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
"""Train DENRM on the intentionally mismatched incomplete-physics cohort."""
|
| 2 |
+
|
| 3 |
+
from pathlib import Path
|
| 4 |
+
|
| 5 |
+
from src.generate_t2_graybox_closure import DATA_PATH, MATERIAL
|
| 6 |
+
from src.train_t2_graybox_discrete_energy import run
|
| 7 |
+
|
| 8 |
+
|
| 9 |
+
ROOT = Path(__file__).resolve().parents[1]
|
| 10 |
+
|
| 11 |
+
|
| 12 |
+
if __name__ == "__main__":
|
| 13 |
+
run(
|
| 14 |
+
graybox_steps=1600,
|
| 15 |
+
gru_epochs=60,
|
| 16 |
+
data_path=DATA_PATH,
|
| 17 |
+
material=MATERIAL,
|
| 18 |
+
model_dir=ROOT / "models" / "t2_graybox_closure_v1",
|
| 19 |
+
artifact_dir=ROOT / "artifacts" / "t2_graybox_closure_v1",
|
| 20 |
+
scope=(
|
| 21 |
+
"out-of-template fixed material: three-memory tabulated reference; "
|
| 22 |
+
"two-memory DENRM closure; reference equations and parameters hidden"
|
| 23 |
+
),
|
| 24 |
+
)
|
src/train_t2_graybox_discrete_energy.py
ADDED
|
@@ -0,0 +1,428 @@
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|
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|
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|
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|
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|
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|
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|
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|
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|
|
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|
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|
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|
|
|
|
|
|
|
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|
|
|
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|
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|
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|
|
|
|
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
"""Train and evaluate the single T2 gray-box hardening architecture.
|
| 2 |
+
|
| 3 |
+
The neural hardening law is initialized from accepted internal-state
|
| 4 |
+
transitions produced by high-fidelity simulation. The formulas and parameters
|
| 5 |
+
of the generating hardening law are never passed to the model. A stress-only
|
| 6 |
+
variant is a later promotion gate; this first controlled study asks whether the
|
| 7 |
+
unknown evolution can be recovered and deployed through an independent return
|
| 8 |
+
map.
|
| 9 |
+
"""
|
| 10 |
+
|
| 11 |
+
from __future__ import annotations
|
| 12 |
+
|
| 13 |
+
import argparse
|
| 14 |
+
import json
|
| 15 |
+
import random
|
| 16 |
+
import time
|
| 17 |
+
from dataclasses import dataclass
|
| 18 |
+
from pathlib import Path
|
| 19 |
+
|
| 20 |
+
import h5py
|
| 21 |
+
import numpy as np
|
| 22 |
+
import torch
|
| 23 |
+
from torch import nn
|
| 24 |
+
|
| 25 |
+
from agentfem import constitutive
|
| 26 |
+
|
| 27 |
+
from src import t2_graybox_discrete_energy as graybox
|
| 28 |
+
from src.generate_t2_graybox_cohort import DATA_PATH, MATERIAL
|
| 29 |
+
from src.train_t2_multiaxial_models import RecurrentStress
|
| 30 |
+
|
| 31 |
+
|
| 32 |
+
ROOT = Path(__file__).resolve().parents[1]
|
| 33 |
+
MODEL_DIR = ROOT / "models" / "t2_graybox_hardening_v1"
|
| 34 |
+
ARTIFACT_DIR = ROOT / "artifacts" / "t2_graybox_hardening_v1"
|
| 35 |
+
METRICS_PATH = ARTIFACT_DIR / "model_metrics.json"
|
| 36 |
+
|
| 37 |
+
|
| 38 |
+
@dataclass
|
| 39 |
+
class Cohort:
|
| 40 |
+
strain: torch.Tensor
|
| 41 |
+
stress: torch.Tensor
|
| 42 |
+
plastic: torch.Tensor
|
| 43 |
+
peeq: torch.Tensor
|
| 44 |
+
increment: torch.Tensor
|
| 45 |
+
memories: torch.Tensor
|
| 46 |
+
radius: torch.Tensor
|
| 47 |
+
splits: tuple[str, ...]
|
| 48 |
+
families: tuple[str, ...]
|
| 49 |
+
|
| 50 |
+
|
| 51 |
+
def load_cohort(data_path: Path = DATA_PATH) -> Cohort:
|
| 52 |
+
arrays: dict[str, list[np.ndarray]] = {
|
| 53 |
+
name: []
|
| 54 |
+
for name in (
|
| 55 |
+
"strain",
|
| 56 |
+
"stress_pa",
|
| 57 |
+
"plastic_strain",
|
| 58 |
+
"peeq",
|
| 59 |
+
"plastic_increment",
|
| 60 |
+
"memories_pa",
|
| 61 |
+
"isotropic_radius_pa",
|
| 62 |
+
)
|
| 63 |
+
}
|
| 64 |
+
splits: list[str] = []
|
| 65 |
+
families: list[str] = []
|
| 66 |
+
with h5py.File(data_path, "r") as h5:
|
| 67 |
+
for name in sorted(h5):
|
| 68 |
+
group = h5[name]
|
| 69 |
+
for field in arrays:
|
| 70 |
+
arrays[field].append(group[field][...])
|
| 71 |
+
splits.append(str(group.attrs["split"]))
|
| 72 |
+
families.append(str(group.attrs["path_family"]))
|
| 73 |
+
tensor = lambda name: torch.tensor(np.stack(arrays[name]), dtype=torch.float32)
|
| 74 |
+
return Cohort(
|
| 75 |
+
strain=tensor("strain"),
|
| 76 |
+
stress=tensor("stress_pa"),
|
| 77 |
+
plastic=tensor("plastic_strain"),
|
| 78 |
+
peeq=tensor("peeq"),
|
| 79 |
+
increment=tensor("plastic_increment"),
|
| 80 |
+
memories=tensor("memories_pa"),
|
| 81 |
+
radius=tensor("isotropic_radius_pa"),
|
| 82 |
+
splits=tuple(splits),
|
| 83 |
+
families=tuple(families),
|
| 84 |
+
)
|
| 85 |
+
|
| 86 |
+
|
| 87 |
+
def mask(cohort: Cohort, split: str) -> torch.Tensor:
|
| 88 |
+
return torch.tensor([value == split for value in cohort.splits], dtype=torch.bool)
|
| 89 |
+
|
| 90 |
+
|
| 91 |
+
def transition_data(cohort: Cohort, selected: torch.Tensor) -> dict[str, torch.Tensor]:
|
| 92 |
+
plastic_increment = cohort.increment[selected, 1:]
|
| 93 |
+
active = plastic_increment > 1.0e-11
|
| 94 |
+
old_plastic = cohort.plastic[selected, :-1]
|
| 95 |
+
new_plastic = cohort.plastic[selected, 1:]
|
| 96 |
+
flow = (new_plastic - old_plastic) / plastic_increment.clamp_min(1.0e-14)[..., None]
|
| 97 |
+
previous_increment = cohort.increment[selected, :-1]
|
| 98 |
+
previous_plastic = torch.cat(
|
| 99 |
+
(torch.zeros_like(old_plastic[:, :1]), old_plastic[:, :-1]), dim=1
|
| 100 |
+
)
|
| 101 |
+
previous_flow = (old_plastic - previous_plastic) / previous_increment.clamp_min(1.0e-14)[..., None]
|
| 102 |
+
previous_flow = torch.where(
|
| 103 |
+
(previous_increment > 1.0e-11)[..., None],
|
| 104 |
+
previous_flow,
|
| 105 |
+
torch.zeros_like(previous_flow),
|
| 106 |
+
)
|
| 107 |
+
result = {
|
| 108 |
+
"increment": plastic_increment[active],
|
| 109 |
+
"flow": flow[active],
|
| 110 |
+
"previous_flow": previous_flow[active],
|
| 111 |
+
"old_peeq": cohort.peeq[selected, :-1][active],
|
| 112 |
+
"new_peeq": cohort.peeq[selected, 1:][active],
|
| 113 |
+
"old_memories": cohort.memories[selected, :-1][active],
|
| 114 |
+
"new_memories": cohort.memories[selected, 1:][active],
|
| 115 |
+
"new_radius": cohort.radius[selected, 1:][active],
|
| 116 |
+
}
|
| 117 |
+
return result
|
| 118 |
+
|
| 119 |
+
|
| 120 |
+
def train_graybox(
|
| 121 |
+
cohort: Cohort,
|
| 122 |
+
*,
|
| 123 |
+
steps: int = 1200,
|
| 124 |
+
batch_size: int = 4096,
|
| 125 |
+
material: dict[str, float] = MATERIAL,
|
| 126 |
+
) -> tuple[graybox.NeuralHardeningLaw, dict[str, object]]:
|
| 127 |
+
training = transition_data(cohort, mask(cohort, "train"))
|
| 128 |
+
validation = transition_data(cohort, mask(cohort, "validation"))
|
| 129 |
+
model = graybox.NeuralHardeningLaw(channels=2)
|
| 130 |
+
optimizer = torch.optim.Adam(model.parameters(), lr=2.0e-3)
|
| 131 |
+
scheduler = torch.optim.lr_scheduler.CosineAnnealingLR(optimizer, steps, eta_min=2.0e-5)
|
| 132 |
+
generator = torch.Generator().manual_seed(20260925)
|
| 133 |
+
yield_stress = float(material["yield_stress_pa"])
|
| 134 |
+
|
| 135 |
+
def objective(data: dict[str, torch.Tensor], indices: torch.Tensor | None = None):
|
| 136 |
+
selected = data if indices is None else {key: value[indices] for key, value in data.items()}
|
| 137 |
+
count = len(selected["increment"])
|
| 138 |
+
scale = torch.full((count,), yield_stress)
|
| 139 |
+
state = graybox.GrayboxState(
|
| 140 |
+
plastic_strain=torch.zeros((count, 6)),
|
| 141 |
+
peeq=selected["old_peeq"],
|
| 142 |
+
memories=selected["old_memories"],
|
| 143 |
+
previous_flow=selected["previous_flow"],
|
| 144 |
+
)
|
| 145 |
+
predicted, recovery, moduli = model.update_memories(
|
| 146 |
+
state, selected["flow"], selected["increment"], scale
|
| 147 |
+
)
|
| 148 |
+
predicted_radius = model.isotropic(selected["new_peeq"], scale)
|
| 149 |
+
memory_state = ((predicted - selected["new_memories"]) / yield_stress).square().mean()
|
| 150 |
+
memory_increment = (
|
| 151 |
+
(
|
| 152 |
+
(predicted - state.memories)
|
| 153 |
+
- (selected["new_memories"] - state.memories)
|
| 154 |
+
)
|
| 155 |
+
/ 5.0e6
|
| 156 |
+
).square().mean()
|
| 157 |
+
radius = ((predicted_radius - selected["new_radius"]) / 70.0e6).square().mean()
|
| 158 |
+
loss = memory_state + memory_increment + radius
|
| 159 |
+
return loss, {
|
| 160 |
+
"memory_state": memory_state,
|
| 161 |
+
"memory_increment": memory_increment,
|
| 162 |
+
"radius": radius,
|
| 163 |
+
"recovery_mean": recovery.mean(dim=0),
|
| 164 |
+
"moduli": moduli.mean(dim=0),
|
| 165 |
+
}
|
| 166 |
+
|
| 167 |
+
started = time.perf_counter()
|
| 168 |
+
best_loss = float("inf")
|
| 169 |
+
best_state = None
|
| 170 |
+
history = []
|
| 171 |
+
for step in range(steps):
|
| 172 |
+
indices = torch.randint(
|
| 173 |
+
len(training["increment"]),
|
| 174 |
+
(min(batch_size, len(training["increment"])),),
|
| 175 |
+
generator=generator,
|
| 176 |
+
)
|
| 177 |
+
optimizer.zero_grad()
|
| 178 |
+
loss, diagnostics = objective(training, indices)
|
| 179 |
+
loss.backward()
|
| 180 |
+
torch.nn.utils.clip_grad_norm_(model.parameters(), 10.0)
|
| 181 |
+
optimizer.step()
|
| 182 |
+
scheduler.step()
|
| 183 |
+
if step % 25 == 0 or step + 1 == steps:
|
| 184 |
+
with torch.no_grad():
|
| 185 |
+
validation_loss, validation_diagnostics = objective(validation)
|
| 186 |
+
value = float(validation_loss)
|
| 187 |
+
history.append(
|
| 188 |
+
{
|
| 189 |
+
"step": step,
|
| 190 |
+
"training_loss": float(loss.detach()),
|
| 191 |
+
"validation_loss": value,
|
| 192 |
+
"moduli_pa": validation_diagnostics["moduli"].tolist(),
|
| 193 |
+
"recovery_mean": validation_diagnostics["recovery_mean"].tolist(),
|
| 194 |
+
}
|
| 195 |
+
)
|
| 196 |
+
if value < best_loss:
|
| 197 |
+
best_loss = value
|
| 198 |
+
best_state = {key: value.detach().clone() for key, value in model.state_dict().items()}
|
| 199 |
+
if best_state is None:
|
| 200 |
+
raise RuntimeError("Gray-box training did not produce a checkpoint.")
|
| 201 |
+
model.load_state_dict(best_state)
|
| 202 |
+
model.eval()
|
| 203 |
+
return model, {
|
| 204 |
+
"training_seconds": time.perf_counter() - started,
|
| 205 |
+
"best_validation_loss": best_loss,
|
| 206 |
+
"steps": steps,
|
| 207 |
+
"history": history,
|
| 208 |
+
}
|
| 209 |
+
|
| 210 |
+
|
| 211 |
+
def train_gru(
|
| 212 |
+
cohort: Cohort,
|
| 213 |
+
*,
|
| 214 |
+
epochs: int = 60,
|
| 215 |
+
) -> tuple[nn.Module, dict[str, object], dict[str, torch.Tensor]]:
|
| 216 |
+
train = mask(cohort, "train")
|
| 217 |
+
validation = mask(cohort, "validation")
|
| 218 |
+
strain_mean = cohort.strain[train].mean(dim=(0, 1), keepdim=True)
|
| 219 |
+
strain_std = cohort.strain[train].std(dim=(0, 1), keepdim=True).clamp_min(1.0e-6)
|
| 220 |
+
stress_mean = cohort.stress[train].mean(dim=(0, 1), keepdim=True)
|
| 221 |
+
stress_std = cohort.stress[train].std(dim=(0, 1), keepdim=True).clamp_min(1.0e6)
|
| 222 |
+
inputs = (cohort.strain - strain_mean) / strain_std
|
| 223 |
+
targets = (cohort.stress - stress_mean) / stress_std
|
| 224 |
+
model = RecurrentStress(6, cell="gru", hidden=72)
|
| 225 |
+
optimizer = torch.optim.AdamW(model.parameters(), lr=2.0e-3, weight_decay=1.0e-5)
|
| 226 |
+
generator = torch.Generator().manual_seed(20260925)
|
| 227 |
+
train_indices = torch.where(train)[0]
|
| 228 |
+
best_loss = float("inf")
|
| 229 |
+
best_state = None
|
| 230 |
+
started = time.perf_counter()
|
| 231 |
+
for _ in range(epochs):
|
| 232 |
+
shuffled = train_indices[torch.randperm(len(train_indices), generator=generator)]
|
| 233 |
+
model.train()
|
| 234 |
+
for start in range(0, len(shuffled), 16):
|
| 235 |
+
selected = shuffled[start : start + 16]
|
| 236 |
+
optimizer.zero_grad()
|
| 237 |
+
loss = (model(inputs[selected]) - targets[selected]).square().mean()
|
| 238 |
+
loss.backward()
|
| 239 |
+
optimizer.step()
|
| 240 |
+
model.eval()
|
| 241 |
+
with torch.no_grad():
|
| 242 |
+
value = float((model(inputs[validation]) - targets[validation]).square().mean())
|
| 243 |
+
if value < best_loss:
|
| 244 |
+
best_loss = value
|
| 245 |
+
best_state = {key: value.detach().clone() for key, value in model.state_dict().items()}
|
| 246 |
+
if best_state is None:
|
| 247 |
+
raise RuntimeError("GRU training did not produce a checkpoint.")
|
| 248 |
+
model.load_state_dict(best_state)
|
| 249 |
+
model.eval()
|
| 250 |
+
return model, {
|
| 251 |
+
"training_seconds": time.perf_counter() - started,
|
| 252 |
+
"best_validation_loss": best_loss,
|
| 253 |
+
"epochs": epochs,
|
| 254 |
+
}, {
|
| 255 |
+
"strain_mean": strain_mean,
|
| 256 |
+
"strain_std": strain_std,
|
| 257 |
+
"stress_mean": stress_mean,
|
| 258 |
+
"stress_std": stress_std,
|
| 259 |
+
}
|
| 260 |
+
|
| 261 |
+
|
| 262 |
+
def _voigt_to_tensor(value: np.ndarray) -> np.ndarray:
|
| 263 |
+
tensor = np.zeros((3, 3), dtype=float)
|
| 264 |
+
tensor[(0, 1, 2, 0, 1, 0), (0, 1, 2, 1, 2, 2)] = value
|
| 265 |
+
tensor[(1, 2, 2), (0, 1, 0)] = value[[3, 4, 5]]
|
| 266 |
+
return tensor
|
| 267 |
+
|
| 268 |
+
|
| 269 |
+
def no_hardening_response(
|
| 270 |
+
cohort: Cohort, material: dict[str, float] = MATERIAL
|
| 271 |
+
) -> torch.Tensor:
|
| 272 |
+
law = constitutive.J2LinearIsotropicHardening(
|
| 273 |
+
young=float(material["young_pa"]),
|
| 274 |
+
poisson=float(material["poisson"]),
|
| 275 |
+
yield_stress=float(material["yield_stress_pa"]),
|
| 276 |
+
hardening_modulus=0.0,
|
| 277 |
+
)
|
| 278 |
+
result = np.empty_like(cohort.stress.numpy())
|
| 279 |
+
for case in range(len(cohort.strain)):
|
| 280 |
+
state = None
|
| 281 |
+
for point, strain in enumerate(cohort.strain[case].numpy()):
|
| 282 |
+
update = law.update(_voigt_to_tensor(strain), state, linearization="none")
|
| 283 |
+
state = update.state
|
| 284 |
+
tensor = update.stress
|
| 285 |
+
result[case, point] = tensor[(0, 1, 2, 0, 1, 0), (0, 1, 2, 1, 2, 2)]
|
| 286 |
+
return torch.tensor(result)
|
| 287 |
+
|
| 288 |
+
|
| 289 |
+
def stress_metrics(
|
| 290 |
+
prediction: torch.Tensor,
|
| 291 |
+
reference: torch.Tensor,
|
| 292 |
+
selected: torch.Tensor,
|
| 293 |
+
) -> dict[str, float | int]:
|
| 294 |
+
error = prediction[selected] - reference[selected]
|
| 295 |
+
denominator = ((reference[selected] - reference[selected].mean()).square().sum()).clamp_min(1.0)
|
| 296 |
+
return {
|
| 297 |
+
"trajectory_count": int(selected.sum()),
|
| 298 |
+
"rmse_mpa": float(torch.sqrt(error.square().mean()) / 1.0e6),
|
| 299 |
+
"mae_mpa": float(error.abs().mean() / 1.0e6),
|
| 300 |
+
"r2": float(1.0 - error.square().sum() / denominator),
|
| 301 |
+
}
|
| 302 |
+
|
| 303 |
+
|
| 304 |
+
def run(
|
| 305 |
+
*,
|
| 306 |
+
graybox_steps: int = 1200,
|
| 307 |
+
gru_epochs: int = 60,
|
| 308 |
+
data_path: Path = DATA_PATH,
|
| 309 |
+
material: dict[str, float] = MATERIAL,
|
| 310 |
+
model_dir: Path = MODEL_DIR,
|
| 311 |
+
artifact_dir: Path = ARTIFACT_DIR,
|
| 312 |
+
scope: str = "fixed synthetic material; hardening parameters and formulas hidden from learned models",
|
| 313 |
+
) -> dict[str, object]:
|
| 314 |
+
random.seed(20260925)
|
| 315 |
+
np.random.seed(20260925)
|
| 316 |
+
torch.manual_seed(20260925)
|
| 317 |
+
cohort = load_cohort(data_path)
|
| 318 |
+
graybox_model, graybox_training = train_graybox(
|
| 319 |
+
cohort, steps=graybox_steps, material=material
|
| 320 |
+
)
|
| 321 |
+
gru_model, gru_training, normalization = train_gru(cohort, epochs=gru_epochs)
|
| 322 |
+
with torch.no_grad():
|
| 323 |
+
started = time.perf_counter()
|
| 324 |
+
graybox_result = graybox.rollout(
|
| 325 |
+
cohort.strain,
|
| 326 |
+
torch.full((len(cohort.strain),), float(material["young_pa"])),
|
| 327 |
+
torch.full((len(cohort.strain),), float(material["poisson"])),
|
| 328 |
+
torch.full((len(cohort.strain),), float(material["yield_stress_pa"])),
|
| 329 |
+
graybox_model,
|
| 330 |
+
bisection_iterations=24,
|
| 331 |
+
)
|
| 332 |
+
graybox_inference = time.perf_counter() - started
|
| 333 |
+
started = time.perf_counter()
|
| 334 |
+
gru_prediction = (
|
| 335 |
+
gru_model(
|
| 336 |
+
(cohort.strain - normalization["strain_mean"])
|
| 337 |
+
/ normalization["strain_std"]
|
| 338 |
+
)
|
| 339 |
+
* normalization["stress_std"]
|
| 340 |
+
+ normalization["stress_mean"]
|
| 341 |
+
)
|
| 342 |
+
gru_inference = time.perf_counter() - started
|
| 343 |
+
started = time.perf_counter()
|
| 344 |
+
incomplete_prediction = no_hardening_response(cohort, material)
|
| 345 |
+
incomplete_inference = time.perf_counter() - started
|
| 346 |
+
|
| 347 |
+
metrics: dict[str, object] = {
|
| 348 |
+
"scope": scope,
|
| 349 |
+
"training": {
|
| 350 |
+
"denrm": graybox_training,
|
| 351 |
+
"gru": gru_training,
|
| 352 |
+
},
|
| 353 |
+
"models": {},
|
| 354 |
+
}
|
| 355 |
+
for name, prediction, seconds in (
|
| 356 |
+
("incomplete_j2", incomplete_prediction, incomplete_inference),
|
| 357 |
+
("gru", gru_prediction, gru_inference),
|
| 358 |
+
("denrm", graybox_result["stress"], graybox_inference),
|
| 359 |
+
):
|
| 360 |
+
metrics["models"][name] = {
|
| 361 |
+
split: stress_metrics(prediction, cohort.stress, mask(cohort, split))
|
| 362 |
+
for split in ("train", "validation", "test")
|
| 363 |
+
}
|
| 364 |
+
metrics["models"][name]["inference_seconds_all_trajectories"] = seconds
|
| 365 |
+
active = graybox_result["plastic_increment"] > 1.0e-11
|
| 366 |
+
ledger = graybox.discrete_energy_ledger(
|
| 367 |
+
graybox_result,
|
| 368 |
+
torch.full((len(cohort.strain),), float(material["yield_stress_pa"])),
|
| 369 |
+
graybox_model,
|
| 370 |
+
)
|
| 371 |
+
energy_scale = ledger["plastic_work"][active].abs().max().clamp_min(1.0)
|
| 372 |
+
metrics["models"]["denrm"].update(
|
| 373 |
+
maximum_yield_residual_pa=float(graybox_result["yield_residual"][active].abs().max()),
|
| 374 |
+
maximum_plastic_trace=float(
|
| 375 |
+
graybox_result["plastic_strain"][..., :3].sum(dim=-1).abs().max()
|
| 376 |
+
),
|
| 377 |
+
minimum_peeq_increment=float(
|
| 378 |
+
torch.diff(graybox_result["peeq"], dim=1).min()
|
| 379 |
+
),
|
| 380 |
+
learned_moduli_pa=(
|
| 381 |
+
graybox_model.moduli(torch.tensor(float(material["yield_stress_pa"])))
|
| 382 |
+
.detach()
|
| 383 |
+
.tolist()
|
| 384 |
+
),
|
| 385 |
+
minimum_reference_yield_dissipation=float(
|
| 386 |
+
ledger["reference_yield_dissipation"][active].min()
|
| 387 |
+
),
|
| 388 |
+
minimum_dynamic_recovery_dissipation=float(
|
| 389 |
+
ledger["dynamic_recovery_dissipation"][active].min()
|
| 390 |
+
),
|
| 391 |
+
minimum_backward_euler_dissipation=float(
|
| 392 |
+
ledger["backward_euler_dissipation"][active].min().detach()
|
| 393 |
+
),
|
| 394 |
+
maximum_energy_balance_relative_residual=float(
|
| 395 |
+
(
|
| 396 |
+
ledger["balance_residual"][active].abs().max() / energy_scale
|
| 397 |
+
).detach()
|
| 398 |
+
),
|
| 399 |
+
)
|
| 400 |
+
model_dir.mkdir(parents=True, exist_ok=True)
|
| 401 |
+
artifact_dir.mkdir(parents=True, exist_ok=True)
|
| 402 |
+
torch.save(
|
| 403 |
+
{"state_dict": graybox_model.state_dict(), "material_known": {
|
| 404 |
+
key: material[key] for key in ("young_pa", "poisson", "yield_stress_pa")
|
| 405 |
+
}},
|
| 406 |
+
model_dir / "denrm.pt",
|
| 407 |
+
)
|
| 408 |
+
torch.save(
|
| 409 |
+
{"state_dict": gru_model.state_dict(), "normalization": normalization},
|
| 410 |
+
model_dir / "gru.pt",
|
| 411 |
+
)
|
| 412 |
+
(artifact_dir / "model_metrics.json").write_text(
|
| 413 |
+
json.dumps(metrics, indent=2) + "\n", encoding="utf-8"
|
| 414 |
+
)
|
| 415 |
+
print(json.dumps({"models": metrics["models"]}, indent=2))
|
| 416 |
+
return metrics
|
| 417 |
+
|
| 418 |
+
|
| 419 |
+
def main() -> None:
|
| 420 |
+
parser = argparse.ArgumentParser()
|
| 421 |
+
parser.add_argument("--graybox-steps", type=int, default=1200)
|
| 422 |
+
parser.add_argument("--gru-epochs", type=int, default=60)
|
| 423 |
+
args = parser.parse_args()
|
| 424 |
+
run(graybox_steps=args.graybox_steps, gru_epochs=args.gru_epochs)
|
| 425 |
+
|
| 426 |
+
|
| 427 |
+
if __name__ == "__main__":
|
| 428 |
+
main()
|
src/validate_t2_graybox.py
ADDED
|
@@ -0,0 +1,411 @@
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|
| 1 |
+
"""Time-discretization and structural deployment gates for T2 DENRM."""
|
| 2 |
+
|
| 3 |
+
from __future__ import annotations
|
| 4 |
+
|
| 5 |
+
import json
|
| 6 |
+
import time
|
| 7 |
+
from pathlib import Path
|
| 8 |
+
|
| 9 |
+
import matplotlib
|
| 10 |
+
|
| 11 |
+
matplotlib.use("Agg")
|
| 12 |
+
import matplotlib.pyplot as plt
|
| 13 |
+
import numpy as np
|
| 14 |
+
import torch
|
| 15 |
+
from scipy.optimize import least_squares
|
| 16 |
+
|
| 17 |
+
from src import structural_validate_t2_models as structure
|
| 18 |
+
from src import t2_graybox_discrete_energy as graybox
|
| 19 |
+
from src.generate_t2_graybox_cohort import MATERIAL, design, solve
|
| 20 |
+
|
| 21 |
+
|
| 22 |
+
ROOT = Path(__file__).resolve().parents[1]
|
| 23 |
+
MODEL_PATH = ROOT / "models" / "t2_graybox_hardening_v1" / "denrm.pt"
|
| 24 |
+
ARTIFACT_DIR = ROOT / "artifacts" / "t2_graybox_hardening_v1"
|
| 25 |
+
OUTPUT = ARTIFACT_DIR / "deployment_validation.json"
|
| 26 |
+
BASIS = torch.tensor((1.0, -0.5, -0.5, 0.0, 0.0, 0.0), dtype=torch.float64)
|
| 27 |
+
|
| 28 |
+
|
| 29 |
+
def load_model(model_path: Path = MODEL_PATH) -> graybox.NeuralHardeningLaw:
|
| 30 |
+
checkpoint = torch.load(model_path, map_location="cpu", weights_only=False)
|
| 31 |
+
model = graybox.NeuralHardeningLaw(channels=2).double()
|
| 32 |
+
model.load_state_dict(checkpoint["state_dict"])
|
| 33 |
+
model.eval()
|
| 34 |
+
return model
|
| 35 |
+
|
| 36 |
+
|
| 37 |
+
def _rollout(
|
| 38 |
+
model: graybox.NeuralHardeningLaw,
|
| 39 |
+
strain: np.ndarray,
|
| 40 |
+
material: dict[str, object] = MATERIAL,
|
| 41 |
+
) -> dict[str, torch.Tensor]:
|
| 42 |
+
selected = torch.tensor(strain, dtype=torch.float64)
|
| 43 |
+
batch = len(selected)
|
| 44 |
+
with torch.no_grad():
|
| 45 |
+
return graybox.rollout(
|
| 46 |
+
selected,
|
| 47 |
+
torch.full((batch,), float(material["young_pa"]), dtype=torch.float64),
|
| 48 |
+
torch.full((batch,), float(material["poisson"]), dtype=torch.float64),
|
| 49 |
+
torch.full((batch,), float(material["yield_stress_pa"]), dtype=torch.float64),
|
| 50 |
+
model,
|
| 51 |
+
bisection_iterations=30,
|
| 52 |
+
)
|
| 53 |
+
|
| 54 |
+
|
| 55 |
+
def time_discretization_gate(
|
| 56 |
+
model: graybox.NeuralHardeningLaw,
|
| 57 |
+
*,
|
| 58 |
+
rows: list[dict[str, object]] | None = None,
|
| 59 |
+
solve_function=solve,
|
| 60 |
+
material: dict[str, object] = MATERIAL,
|
| 61 |
+
) -> dict[str, object]:
|
| 62 |
+
rows = design(4) if rows is None else rows
|
| 63 |
+
selected = [rows[index] for index in range(0, len(rows), 4)]
|
| 64 |
+
result: dict[str, object] = {}
|
| 65 |
+
predictions: dict[int, dict[str, torch.Tensor]] = {}
|
| 66 |
+
references: dict[int, np.ndarray] = {}
|
| 67 |
+
for points in (121, 481):
|
| 68 |
+
solved = [solve_function(row, points=points) for row in selected]
|
| 69 |
+
strain = np.stack([case["strain"] for case in solved])
|
| 70 |
+
reference = np.stack([case["stress_pa"] for case in solved])
|
| 71 |
+
prediction = _rollout(model, strain, material)
|
| 72 |
+
error = prediction["stress"].numpy() - reference
|
| 73 |
+
active = prediction["plastic_increment"] > 1.0e-11
|
| 74 |
+
predictions[points] = prediction
|
| 75 |
+
references[points] = reference
|
| 76 |
+
result[str(points)] = {
|
| 77 |
+
"trajectory_count": len(selected),
|
| 78 |
+
"rmse_mpa": float(np.sqrt(np.mean(error**2)) / 1.0e6),
|
| 79 |
+
"mae_mpa": float(np.mean(np.abs(error)) / 1.0e6),
|
| 80 |
+
"maximum_yield_residual_pa": float(
|
| 81 |
+
prediction["yield_residual"][active].abs().max()
|
| 82 |
+
),
|
| 83 |
+
}
|
| 84 |
+
coarse_terminal = predictions[121]["stress"][:, -1]
|
| 85 |
+
fine_terminal = predictions[481]["stress"][:, -1]
|
| 86 |
+
reference_scale = torch.tensor(references[481][:, -1]).norm().clamp_min(1.0)
|
| 87 |
+
result["terminal_121_to_481_relative_change"] = float(
|
| 88 |
+
(coarse_terminal - fine_terminal).norm() / reference_scale
|
| 89 |
+
)
|
| 90 |
+
return result
|
| 91 |
+
|
| 92 |
+
|
| 93 |
+
def _response(
|
| 94 |
+
model: graybox.NeuralHardeningLaw,
|
| 95 |
+
old_state: graybox.GrayboxState,
|
| 96 |
+
scalar_strain: float,
|
| 97 |
+
) -> tuple[float, float, graybox.GrayboxState]:
|
| 98 |
+
def evaluate(value: float):
|
| 99 |
+
strain = (float(value) * BASIS).reshape(1, 6)
|
| 100 |
+
with torch.no_grad():
|
| 101 |
+
return graybox.advance(
|
| 102 |
+
strain,
|
| 103 |
+
old_state,
|
| 104 |
+
torch.tensor((float(MATERIAL["young_pa"]),), dtype=torch.float64),
|
| 105 |
+
torch.tensor((float(MATERIAL["poisson"]),), dtype=torch.float64),
|
| 106 |
+
torch.tensor((float(MATERIAL["yield_stress_pa"]),), dtype=torch.float64),
|
| 107 |
+
model,
|
| 108 |
+
bisection_iterations=30,
|
| 109 |
+
)
|
| 110 |
+
|
| 111 |
+
stress, state, _ = evaluate(scalar_strain)
|
| 112 |
+
generalized = float(graybox.double_contract(stress[0], BASIS))
|
| 113 |
+
step = 1.0e-7 * max(1.0, abs(scalar_strain) / 0.005)
|
| 114 |
+
upper, _, _ = evaluate(scalar_strain + step)
|
| 115 |
+
lower, _, _ = evaluate(scalar_strain - step)
|
| 116 |
+
tangent = float(
|
| 117 |
+
(graybox.double_contract(upper[0], BASIS) - graybox.double_contract(lower[0], BASIS))
|
| 118 |
+
/ (2.0 * step)
|
| 119 |
+
)
|
| 120 |
+
return generalized, tangent, state
|
| 121 |
+
|
| 122 |
+
|
| 123 |
+
def _batch_response(
|
| 124 |
+
model: graybox.NeuralHardeningLaw,
|
| 125 |
+
old_state: graybox.GrayboxState,
|
| 126 |
+
scalar_strain: np.ndarray,
|
| 127 |
+
material: dict[str, object] = MATERIAL,
|
| 128 |
+
) -> tuple[np.ndarray, np.ndarray, graybox.GrayboxState]:
|
| 129 |
+
"""Evaluate every element in one batched constitutive call.
|
| 130 |
+
|
| 131 |
+
The global bar problem has independent quadrature-point states, which map
|
| 132 |
+
directly to DENRM's batch dimension. Batching preserves the local return
|
| 133 |
+
map while avoiding thousands of tiny Python/PyTorch calls.
|
| 134 |
+
"""
|
| 135 |
+
|
| 136 |
+
values = torch.as_tensor(scalar_strain, dtype=torch.float64)
|
| 137 |
+
batch = len(values)
|
| 138 |
+
young = torch.full((batch,), float(material["young_pa"]), dtype=torch.float64)
|
| 139 |
+
poisson = torch.full((batch,), float(material["poisson"]), dtype=torch.float64)
|
| 140 |
+
yield_stress = torch.full(
|
| 141 |
+
(batch,), float(material["yield_stress_pa"]), dtype=torch.float64
|
| 142 |
+
)
|
| 143 |
+
|
| 144 |
+
def evaluate(selected: torch.Tensor):
|
| 145 |
+
strain = selected[:, None] * BASIS[None, :]
|
| 146 |
+
return graybox.advance(
|
| 147 |
+
strain,
|
| 148 |
+
old_state,
|
| 149 |
+
young,
|
| 150 |
+
poisson,
|
| 151 |
+
yield_stress,
|
| 152 |
+
model,
|
| 153 |
+
bisection_iterations=30,
|
| 154 |
+
)
|
| 155 |
+
|
| 156 |
+
with torch.no_grad():
|
| 157 |
+
stress, state, _ = evaluate(values)
|
| 158 |
+
generalized = graybox.double_contract(stress, BASIS)
|
| 159 |
+
step = 1.0e-7 * torch.maximum(
|
| 160 |
+
torch.ones_like(values), values.abs() / 0.005
|
| 161 |
+
)
|
| 162 |
+
upper, _, _ = evaluate(values + step)
|
| 163 |
+
lower, _, _ = evaluate(values - step)
|
| 164 |
+
tangent = (
|
| 165 |
+
graybox.double_contract(upper, BASIS)
|
| 166 |
+
- graybox.double_contract(lower, BASIS)
|
| 167 |
+
) / (2.0 * step)
|
| 168 |
+
return generalized.numpy(), tangent.numpy(), state
|
| 169 |
+
|
| 170 |
+
|
| 171 |
+
def solve_structure(
|
| 172 |
+
model: graybox.NeuralHardeningLaw,
|
| 173 |
+
displacement: np.ndarray,
|
| 174 |
+
*,
|
| 175 |
+
elements: int = 12,
|
| 176 |
+
notch_depth: float,
|
| 177 |
+
material: dict[str, object] = MATERIAL,
|
| 178 |
+
) -> dict[str, np.ndarray | float]:
|
| 179 |
+
nodes, area = structure.geometry(elements, notch_depth)
|
| 180 |
+
lengths = np.diff(nodes)
|
| 181 |
+
states = graybox.initial_state(elements, channels=2, dtype=torch.float64)
|
| 182 |
+
u = np.zeros(elements + 1)
|
| 183 |
+
reactions = []
|
| 184 |
+
iterations = []
|
| 185 |
+
trust_region_fallback_steps: list[int] = []
|
| 186 |
+
started = time.perf_counter()
|
| 187 |
+
for step_index, end_value in enumerate(displacement):
|
| 188 |
+
if step_index > 0:
|
| 189 |
+
u += np.linspace(0.0, end_value - u[-1], elements + 1)
|
| 190 |
+
u[0] = 0.0
|
| 191 |
+
u[-1] = end_value
|
| 192 |
+
accepted = None
|
| 193 |
+
for iteration in range(60):
|
| 194 |
+
internal = np.zeros(elements + 1)
|
| 195 |
+
stiffness = np.zeros((elements + 1, elements + 1))
|
| 196 |
+
strains = np.diff(u) / lengths
|
| 197 |
+
current_stress, current_tangent, trial_states = _batch_response(
|
| 198 |
+
model, states, strains, material
|
| 199 |
+
)
|
| 200 |
+
for element in range(elements):
|
| 201 |
+
stress = current_stress[element]
|
| 202 |
+
tangent = float(np.clip(current_tangent[element], 1.0e7, 4.0e11))
|
| 203 |
+
b = np.asarray((-1.0 / lengths[element], 1.0 / lengths[element]))
|
| 204 |
+
dofs = (element, element + 1)
|
| 205 |
+
internal[list(dofs)] += area[element] * stress * b * lengths[element]
|
| 206 |
+
stiffness[np.ix_(dofs, dofs)] += (
|
| 207 |
+
area[element] * tangent * np.outer(b, b) * lengths[element]
|
| 208 |
+
)
|
| 209 |
+
residual = internal[1:-1]
|
| 210 |
+
scale = max(float(np.linalg.norm(internal)), 1.0)
|
| 211 |
+
# The local law is solved tightly, but its scalar tangent is a
|
| 212 |
+
# finite-difference directional derivative across an active-set
|
| 213 |
+
# switch. Use an engineering equilibrium tolerance and a bounded
|
| 214 |
+
# Newton correction, matching the deployment gate used for the
|
| 215 |
+
# other learned constitutive models in this project.
|
| 216 |
+
if np.linalg.norm(residual) <= 2.0e-6 * scale + 1.0e2:
|
| 217 |
+
accepted = trial_states
|
| 218 |
+
break
|
| 219 |
+
increment = np.linalg.solve(stiffness[1:-1, 1:-1], residual)
|
| 220 |
+
maximum = 0.20 * max(abs(end_value), 1.0e-5)
|
| 221 |
+
norm_increment = np.max(np.abs(increment))
|
| 222 |
+
if norm_increment > maximum:
|
| 223 |
+
increment *= maximum / norm_increment
|
| 224 |
+
u[1:-1] -= increment
|
| 225 |
+
if accepted is None:
|
| 226 |
+
# Reversal points can place several integration points on different
|
| 227 |
+
# sides of the elastic/plastic active-set switch. Recover the same
|
| 228 |
+
# FE equilibrium with a bounded trust-region solve; the local
|
| 229 |
+
# constitutive law and its committed state remain unchanged.
|
| 230 |
+
end_fixed = float(end_value)
|
| 231 |
+
|
| 232 |
+
# In a one-dimensional bar, equilibrium is equivalently expressed
|
| 233 |
+
# by a single constant axial force. Solving for all element
|
| 234 |
+
# strains plus that force avoids poor conditioning in nodal
|
| 235 |
+
# coordinates at a displacement reversal.
|
| 236 |
+
def force_compatibility(unknown: np.ndarray) -> np.ndarray:
|
| 237 |
+
candidate_strain = unknown[:-1]
|
| 238 |
+
force_scaled = unknown[-1]
|
| 239 |
+
candidate_stress, _, _ = _batch_response(
|
| 240 |
+
model, states, candidate_strain, material
|
| 241 |
+
)
|
| 242 |
+
force_balance = area * candidate_stress / 1.0e8 - force_scaled
|
| 243 |
+
compatibility = (
|
| 244 |
+
np.dot(lengths, candidate_strain) - end_fixed
|
| 245 |
+
) / 0.005
|
| 246 |
+
return np.concatenate((force_balance, (compatibility,)))
|
| 247 |
+
|
| 248 |
+
def force_compatibility_jacobian(unknown: np.ndarray) -> np.ndarray:
|
| 249 |
+
candidate_strain = unknown[:-1]
|
| 250 |
+
_, candidate_tangent, _ = _batch_response(
|
| 251 |
+
model, states, candidate_strain, material
|
| 252 |
+
)
|
| 253 |
+
candidate_tangent = np.clip(candidate_tangent, 1.0e7, 4.0e11)
|
| 254 |
+
jacobian = np.zeros((elements + 1, elements + 1))
|
| 255 |
+
jacobian[np.arange(elements), np.arange(elements)] = (
|
| 256 |
+
area * candidate_tangent / 1.0e8
|
| 257 |
+
)
|
| 258 |
+
jacobian[:elements, -1] = -1.0
|
| 259 |
+
jacobian[-1, :elements] = lengths / 0.005
|
| 260 |
+
return jacobian
|
| 261 |
+
|
| 262 |
+
initial_strain = np.diff(u) / lengths
|
| 263 |
+
initial_force = float(internal[-1]) / 1.0e8
|
| 264 |
+
recovered = least_squares(
|
| 265 |
+
force_compatibility,
|
| 266 |
+
np.concatenate((initial_strain, (initial_force,))),
|
| 267 |
+
method="trf",
|
| 268 |
+
jac=force_compatibility_jacobian,
|
| 269 |
+
x_scale=np.concatenate((np.full(elements, 0.005), (1.0,))),
|
| 270 |
+
max_nfev=120,
|
| 271 |
+
xtol=1.0e-12,
|
| 272 |
+
ftol=1.0e-12,
|
| 273 |
+
gtol=1.0e-12,
|
| 274 |
+
)
|
| 275 |
+
if recovered.success:
|
| 276 |
+
strains = recovered.x[:-1]
|
| 277 |
+
u = np.concatenate(((0.0,), np.cumsum(lengths * strains)))
|
| 278 |
+
current_stress, _, trial_states = _batch_response(
|
| 279 |
+
model, states, strains, material
|
| 280 |
+
)
|
| 281 |
+
internal = np.zeros(elements + 1)
|
| 282 |
+
for element in range(elements):
|
| 283 |
+
b = np.asarray((-1.0 / lengths[element], 1.0 / lengths[element]))
|
| 284 |
+
dofs = (element, element + 1)
|
| 285 |
+
internal[list(dofs)] += (
|
| 286 |
+
area[element]
|
| 287 |
+
* current_stress[element]
|
| 288 |
+
* b
|
| 289 |
+
* lengths[element]
|
| 290 |
+
)
|
| 291 |
+
residual = internal[1:-1]
|
| 292 |
+
scale = max(float(np.linalg.norm(internal)), 1.0)
|
| 293 |
+
if np.linalg.norm(residual) <= 2.0e-6 * scale + 1.0e2:
|
| 294 |
+
accepted = trial_states
|
| 295 |
+
iteration = 60 + int(recovered.nfev)
|
| 296 |
+
trust_region_fallback_steps.append(step_index)
|
| 297 |
+
if accepted is None:
|
| 298 |
+
raise RuntimeError(
|
| 299 |
+
f"DENRM structural solve failed at step {step_index}; "
|
| 300 |
+
f"max_abs_element_strain={float(np.max(np.abs(strains))):.6g}."
|
| 301 |
+
)
|
| 302 |
+
states = accepted
|
| 303 |
+
reactions.append(float(internal[-1]))
|
| 304 |
+
iterations.append(iteration + 1)
|
| 305 |
+
return {
|
| 306 |
+
"reaction": np.asarray(reactions),
|
| 307 |
+
"iterations": np.asarray(iterations),
|
| 308 |
+
"trust_region_fallback_steps": trust_region_fallback_steps,
|
| 309 |
+
"elapsed_seconds": time.perf_counter() - started,
|
| 310 |
+
}
|
| 311 |
+
|
| 312 |
+
|
| 313 |
+
def structural_gate(
|
| 314 |
+
model: graybox.NeuralHardeningLaw,
|
| 315 |
+
*,
|
| 316 |
+
material: dict[str, object] = MATERIAL,
|
| 317 |
+
native_law_factory=structure.material,
|
| 318 |
+
artifact_dir: Path = ARTIFACT_DIR,
|
| 319 |
+
) -> dict[str, object]:
|
| 320 |
+
result: dict[str, object] = {}
|
| 321 |
+
figure, axes = plt.subplots(1, 2, figsize=(10.0, 4.2), constrained_layout=True)
|
| 322 |
+
cases = (
|
| 323 |
+
("mild_cyclic", 0.12, structure.load_history(points=81)),
|
| 324 |
+
("severe_monotonic", 0.42, np.linspace(0.0, 0.0065, 61)),
|
| 325 |
+
)
|
| 326 |
+
for axis, (name, depth, displacement) in zip(
|
| 327 |
+
axes,
|
| 328 |
+
cases,
|
| 329 |
+
strict=True,
|
| 330 |
+
):
|
| 331 |
+
reference = structure.solve_native(
|
| 332 |
+
12,
|
| 333 |
+
displacement,
|
| 334 |
+
notch_depth=depth,
|
| 335 |
+
law_factory=native_law_factory,
|
| 336 |
+
)
|
| 337 |
+
learned = solve_structure(
|
| 338 |
+
model, displacement, notch_depth=depth, material=material
|
| 339 |
+
)
|
| 340 |
+
difference = learned["reaction"] - reference["reaction"]
|
| 341 |
+
relative = float(
|
| 342 |
+
np.linalg.norm(difference) / max(np.linalg.norm(reference["reaction"]), 1.0)
|
| 343 |
+
)
|
| 344 |
+
result[name] = {
|
| 345 |
+
"reaction_relative_l2": relative,
|
| 346 |
+
"maximum_absolute_reaction_error": float(np.max(np.abs(difference))),
|
| 347 |
+
"maximum_newton_iterations": int(np.max(learned["iterations"])),
|
| 348 |
+
"mean_newton_iterations": float(np.mean(learned["iterations"])),
|
| 349 |
+
"trust_region_fallback_count": len(
|
| 350 |
+
learned["trust_region_fallback_steps"]
|
| 351 |
+
),
|
| 352 |
+
"trust_region_fallback_steps": list(
|
| 353 |
+
learned["trust_region_fallback_steps"]
|
| 354 |
+
),
|
| 355 |
+
"elapsed_seconds": float(learned["elapsed_seconds"]),
|
| 356 |
+
}
|
| 357 |
+
axis.plot(displacement, reference["reaction"], label="AgentFEM reference")
|
| 358 |
+
axis.plot(displacement, learned["reaction"], "--", label="DENRM")
|
| 359 |
+
axis.set_title(name.replace("_", " "))
|
| 360 |
+
axis.set_xlabel("prescribed end displacement")
|
| 361 |
+
axis.set_ylabel("reaction")
|
| 362 |
+
axis.grid(alpha=0.2)
|
| 363 |
+
axes[0].legend(frameon=False)
|
| 364 |
+
artifact_dir.mkdir(parents=True, exist_ok=True)
|
| 365 |
+
figure.savefig(artifact_dir / "structural_reaction_comparison.png", dpi=190)
|
| 366 |
+
plt.close(figure)
|
| 367 |
+
|
| 368 |
+
# Deliberately retain a stronger cyclic extrapolation as a falsification
|
| 369 |
+
# gate. It currently exceeds the training strain envelope during reversal;
|
| 370 |
+
# recording the failure is more informative than silently shrinking it.
|
| 371 |
+
try:
|
| 372 |
+
severe_cyclic = solve_structure(
|
| 373 |
+
model,
|
| 374 |
+
structure.load_history(points=81),
|
| 375 |
+
notch_depth=0.42,
|
| 376 |
+
material=material,
|
| 377 |
+
)
|
| 378 |
+
result["severe_cyclic_stress_test"] = {
|
| 379 |
+
"passed": True,
|
| 380 |
+
"maximum_newton_iterations": int(
|
| 381 |
+
np.max(severe_cyclic["iterations"])
|
| 382 |
+
),
|
| 383 |
+
"trust_region_fallback_count": len(
|
| 384 |
+
severe_cyclic["trust_region_fallback_steps"]
|
| 385 |
+
),
|
| 386 |
+
}
|
| 387 |
+
except RuntimeError as error:
|
| 388 |
+
result["severe_cyclic_stress_test"] = {
|
| 389 |
+
"passed": False,
|
| 390 |
+
"failure": str(error),
|
| 391 |
+
"interpretation": (
|
| 392 |
+
"strong cyclic localization leaves the present training envelope; "
|
| 393 |
+
"this is a declared promotion-gate failure, not a successful deployment"
|
| 394 |
+
),
|
| 395 |
+
}
|
| 396 |
+
return result
|
| 397 |
+
|
| 398 |
+
|
| 399 |
+
def main() -> None:
|
| 400 |
+
model = load_model()
|
| 401 |
+
ARTIFACT_DIR.mkdir(parents=True, exist_ok=True)
|
| 402 |
+
result = {
|
| 403 |
+
"time_discretization": time_discretization_gate(model),
|
| 404 |
+
"structure": structural_gate(model),
|
| 405 |
+
}
|
| 406 |
+
OUTPUT.write_text(json.dumps(result, indent=2) + "\n", encoding="utf-8")
|
| 407 |
+
print(json.dumps(result, indent=2))
|
| 408 |
+
|
| 409 |
+
|
| 410 |
+
if __name__ == "__main__":
|
| 411 |
+
main()
|
src/validate_t2_graybox_closure.py
ADDED
|
@@ -0,0 +1,46 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
"""Promotion gates for the out-of-template incomplete-physics closure."""
|
| 2 |
+
|
| 3 |
+
import json
|
| 4 |
+
from pathlib import Path
|
| 5 |
+
|
| 6 |
+
from src.generate_t2_graybox_closure import MATERIAL, closure_design, material, solve
|
| 7 |
+
from src.validate_t2_graybox import (
|
| 8 |
+
load_model,
|
| 9 |
+
structural_gate,
|
| 10 |
+
time_discretization_gate,
|
| 11 |
+
)
|
| 12 |
+
|
| 13 |
+
|
| 14 |
+
ROOT = Path(__file__).resolve().parents[1]
|
| 15 |
+
MODEL_PATH = ROOT / "models" / "t2_graybox_closure_v1" / "denrm.pt"
|
| 16 |
+
ARTIFACT_DIR = ROOT / "artifacts" / "t2_graybox_closure_v1"
|
| 17 |
+
OUTPUT = ARTIFACT_DIR / "deployment_validation.json"
|
| 18 |
+
|
| 19 |
+
|
| 20 |
+
def main() -> None:
|
| 21 |
+
model = load_model(MODEL_PATH)
|
| 22 |
+
ARTIFACT_DIR.mkdir(parents=True, exist_ok=True)
|
| 23 |
+
result = {
|
| 24 |
+
"scope": (
|
| 25 |
+
"reference has three memories and tabulated hardening; deployed DENRM "
|
| 26 |
+
"has two memories and no access to the reference equations"
|
| 27 |
+
),
|
| 28 |
+
"time_discretization": time_discretization_gate(
|
| 29 |
+
model,
|
| 30 |
+
rows=closure_design(4),
|
| 31 |
+
solve_function=solve,
|
| 32 |
+
material=MATERIAL,
|
| 33 |
+
),
|
| 34 |
+
"structure": structural_gate(
|
| 35 |
+
model,
|
| 36 |
+
material=MATERIAL,
|
| 37 |
+
native_law_factory=material,
|
| 38 |
+
artifact_dir=ARTIFACT_DIR,
|
| 39 |
+
),
|
| 40 |
+
}
|
| 41 |
+
OUTPUT.write_text(json.dumps(result, indent=2) + "\n", encoding="utf-8")
|
| 42 |
+
print(json.dumps(result, indent=2))
|
| 43 |
+
|
| 44 |
+
|
| 45 |
+
if __name__ == "__main__":
|
| 46 |
+
main()
|
tests/test_t2_graybox_closure.py
ADDED
|
@@ -0,0 +1,25 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
import numpy as np
|
| 2 |
+
|
| 3 |
+
from src.generate_t2_graybox_closure import closure_design, material, solve
|
| 4 |
+
|
| 5 |
+
|
| 6 |
+
def test_reference_is_intentionally_richer_than_closure_state():
|
| 7 |
+
law = material()
|
| 8 |
+
assert law.backstress_count == 3
|
| 9 |
+
assert law.isotropic_hardening is not None
|
| 10 |
+
assert len(law.isotropic_hardening.equivalent_plastic_strain) == 7
|
| 11 |
+
|
| 12 |
+
|
| 13 |
+
def test_closure_cohort_preserves_total_reference_backstress():
|
| 14 |
+
row = closure_design(4)[0]
|
| 15 |
+
nine_points = 9
|
| 16 |
+
result = solve(row, points=nine_points)
|
| 17 |
+
assert result["strain"].shape == (nine_points, 6)
|
| 18 |
+
assert result["truth_memories_pa"].shape == (nine_points, 3, 6)
|
| 19 |
+
assert result["memories_pa"].shape == (nine_points, 2, 6)
|
| 20 |
+
np.testing.assert_allclose(
|
| 21 |
+
result["memories_pa"].sum(axis=1),
|
| 22 |
+
result["truth_memories_pa"].sum(axis=1),
|
| 23 |
+
rtol=1.0e-12,
|
| 24 |
+
atol=1.0e-5,
|
| 25 |
+
)
|
tests/test_t2_graybox_discrete_energy.py
ADDED
|
@@ -0,0 +1,110 @@
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1 |
+
from __future__ import annotations
|
| 2 |
+
|
| 3 |
+
import torch
|
| 4 |
+
|
| 5 |
+
from src import t2_graybox_discrete_energy as subject
|
| 6 |
+
|
| 7 |
+
|
| 8 |
+
def test_monotone_hardening_is_zero_anchored_and_nondecreasing() -> None:
|
| 9 |
+
model = subject.MonotoneIsotropicHardening().double()
|
| 10 |
+
peeq = torch.linspace(0.0, 0.03, 101, dtype=torch.float64)
|
| 11 |
+
scale = torch.full_like(peeq, 300.0e6)
|
| 12 |
+
radius = model(peeq, scale)
|
| 13 |
+
assert abs(float(radius[0].detach())) < 1.0e-8
|
| 14 |
+
assert torch.all(radius[1:] >= radius[:-1])
|
| 15 |
+
assert torch.all(model.derivative(peeq, scale) > 0.0)
|
| 16 |
+
|
| 17 |
+
|
| 18 |
+
def test_recovery_is_positive_and_objective_under_basis_rotation() -> None:
|
| 19 |
+
torch.manual_seed(7)
|
| 20 |
+
model = subject.ObjectiveRecoveryNetwork(channels=2).double()
|
| 21 |
+
memories = subject.deviatoric(torch.randn(4, 2, 6, dtype=torch.float64))
|
| 22 |
+
flow = subject.deviatoric(torch.randn(4, 6, dtype=torch.float64))
|
| 23 |
+
peeq = torch.linspace(0.0, 0.02, 4, dtype=torch.float64)
|
| 24 |
+
radius = torch.linspace(0.0, 80.0e6, 4, dtype=torch.float64)
|
| 25 |
+
scale = torch.full((4,), 280.0e6, dtype=torch.float64)
|
| 26 |
+
reversal = torch.linspace(-1.0, 1.0, 4, dtype=torch.float64)
|
| 27 |
+
result = model(peeq, radius, flow, memories, scale, reversal)
|
| 28 |
+
assert torch.all(result > 0.0)
|
| 29 |
+
|
| 30 |
+
def as_matrix(value: torch.Tensor) -> torch.Tensor:
|
| 31 |
+
tensor = torch.zeros((*value.shape[:-1], 3, 3), dtype=value.dtype)
|
| 32 |
+
tensor[..., 0, 0] = value[..., 0]
|
| 33 |
+
tensor[..., 1, 1] = value[..., 1]
|
| 34 |
+
tensor[..., 2, 2] = value[..., 2]
|
| 35 |
+
tensor[..., 0, 1] = tensor[..., 1, 0] = value[..., 3]
|
| 36 |
+
tensor[..., 1, 2] = tensor[..., 2, 1] = value[..., 4]
|
| 37 |
+
tensor[..., 0, 2] = tensor[..., 2, 0] = value[..., 5]
|
| 38 |
+
return tensor
|
| 39 |
+
|
| 40 |
+
def as_voigt(value: torch.Tensor) -> torch.Tensor:
|
| 41 |
+
return value[..., (0, 1, 2, 0, 1, 0), (0, 1, 2, 1, 2, 2)]
|
| 42 |
+
|
| 43 |
+
rotation, _ = torch.linalg.qr(torch.randn(3, 3, dtype=torch.float64))
|
| 44 |
+
rotated_flow = as_voigt(
|
| 45 |
+
torch.einsum("ij,bjk,lk->bil", rotation, as_matrix(flow), rotation)
|
| 46 |
+
)
|
| 47 |
+
rotated_memories = as_voigt(
|
| 48 |
+
torch.einsum("ij,bcjk,lk->bcil", rotation, as_matrix(memories), rotation)
|
| 49 |
+
)
|
| 50 |
+
rotated = model(
|
| 51 |
+
peeq, radius, rotated_flow, rotated_memories, scale, reversal
|
| 52 |
+
)
|
| 53 |
+
torch.testing.assert_close(rotated, result, rtol=1.0e-12, atol=1.0e-12)
|
| 54 |
+
|
| 55 |
+
|
| 56 |
+
def test_memory_update_preserves_deviatoric_state_and_nonnegative_rates() -> None:
|
| 57 |
+
law = subject.NeuralHardeningLaw(channels=2).double()
|
| 58 |
+
state = subject.initial_state(3, channels=2, dtype=torch.float64)
|
| 59 |
+
flow = subject.deviatoric(torch.randn(3, 6, dtype=torch.float64))
|
| 60 |
+
increment = torch.tensor((0.0, 1.0e-4, 5.0e-4), dtype=torch.float64)
|
| 61 |
+
scale = torch.full((3,), 280.0e6, dtype=torch.float64)
|
| 62 |
+
memories, recovery, moduli = law.update_memories(
|
| 63 |
+
state, flow, increment, scale
|
| 64 |
+
)
|
| 65 |
+
assert torch.all(recovery > 0.0)
|
| 66 |
+
assert torch.all(moduli > 0.0)
|
| 67 |
+
assert torch.max(torch.abs(memories[..., :3].sum(dim=-1))) < 1.0e-8
|
| 68 |
+
assert torch.count_nonzero(memories[0]) == 0
|
| 69 |
+
|
| 70 |
+
|
| 71 |
+
def test_elastic_stress_recovers_zero_for_zero_elastic_strain() -> None:
|
| 72 |
+
strain = torch.randn(5, 6, dtype=torch.float64)
|
| 73 |
+
stress = subject.elastic_stress(
|
| 74 |
+
strain,
|
| 75 |
+
strain,
|
| 76 |
+
torch.full((5,), 200.0e9, dtype=torch.float64),
|
| 77 |
+
torch.full((5,), 0.3, dtype=torch.float64),
|
| 78 |
+
)
|
| 79 |
+
assert torch.count_nonzero(stress) == 0
|
| 80 |
+
|
| 81 |
+
|
| 82 |
+
def test_neural_return_map_closes_yield_surface_and_state_constraints() -> None:
|
| 83 |
+
law = subject.NeuralHardeningLaw(channels=2).double()
|
| 84 |
+
strain = torch.zeros((2, 25, 6), dtype=torch.float64)
|
| 85 |
+
axial = torch.linspace(0.0, 0.009, 25, dtype=torch.float64)
|
| 86 |
+
strain[:, :, 0] = axial
|
| 87 |
+
strain[:, :, 1] = -0.5 * axial
|
| 88 |
+
strain[:, :, 2] = -0.5 * axial
|
| 89 |
+
result = subject.rollout(
|
| 90 |
+
strain,
|
| 91 |
+
torch.full((2,), 190.0e9, dtype=torch.float64),
|
| 92 |
+
torch.full((2,), 0.3, dtype=torch.float64),
|
| 93 |
+
torch.full((2,), 280.0e6, dtype=torch.float64),
|
| 94 |
+
law,
|
| 95 |
+
)
|
| 96 |
+
assert torch.isfinite(result["stress"]).all()
|
| 97 |
+
assert torch.all(result["peeq"][:, 1:] >= result["peeq"][:, :-1])
|
| 98 |
+
assert torch.max(torch.abs(result["plastic_strain"][..., :3].sum(-1))) < 1.0e-10
|
| 99 |
+
active = result["plastic_increment"] > 1.0e-12
|
| 100 |
+
assert torch.max(torch.abs(result["yield_residual"][active])) < 20.0
|
| 101 |
+
ledger = subject.discrete_energy_ledger(
|
| 102 |
+
result,
|
| 103 |
+
torch.full((2,), 280.0e6, dtype=torch.float64),
|
| 104 |
+
law,
|
| 105 |
+
)
|
| 106 |
+
scale = ledger["plastic_work"][active].abs().max()
|
| 107 |
+
assert ledger["reference_yield_dissipation"][active].min() >= 0.0
|
| 108 |
+
assert ledger["dynamic_recovery_dissipation"][active].min() >= 0.0
|
| 109 |
+
assert ledger["backward_euler_dissipation"][active].min() >= -1.0e-8 * scale
|
| 110 |
+
assert ledger["balance_residual"][active].abs().max() < 1.0e-8 * scale
|