| """Embed learned constitutive histories in a displacement-controlled bar FE test. |
| |
| This is a controlled one-dimensional structural deployment gate. The global |
| finite-element equilibrium is solved independently for a smooth notched bar, |
| while each element obtains its path-dependent generalized stress either from |
| the native AgentFEM Chaboche update or from a trained neural constitutive |
| model. It is not presented as a general three-dimensional learned-material |
| provider for AgentFEM. |
| """ |
|
|
| from __future__ import annotations |
|
|
| import argparse |
| import json |
| import time |
| from pathlib import Path |
|
|
| import matplotlib |
|
|
| matplotlib.use("Agg") |
| import matplotlib.pyplot as plt |
| import numpy as np |
| import torch |
| from scipy.optimize import least_squares |
|
|
| from agentfem import constitutive |
|
|
| try: |
| from src import train_t2_multiaxial_models as learning |
| from src import train_t2_physics_integrator as physics_integrator |
| except ModuleNotFoundError: |
| import train_t2_multiaxial_models as learning |
| import train_t2_physics_integrator as physics_integrator |
|
|
|
|
| ROOT = Path(__file__).resolve().parents[1] |
| MODEL_ROOT = ROOT / "models" / "t2_multiaxial_ood_v2" |
| ARTIFACT_ROOT = ROOT / "artifacts" / "t2_multiaxial_ood_v2" / "structural_validation" |
| BASIS = np.diag((1.0, -0.5, -0.5)) |
| BASIS_VOIGT = np.asarray((1.0, -0.5, -0.5, 0.0, 0.0, 0.0)) |
|
|
| MATERIAL_PARAMETERS = np.asarray( |
| ( |
| 190.0e9, |
| 0.30, |
| 280.0e6, |
| 0.0, |
| 35.0e9, |
| 60.0, |
| 8.0e9, |
| 8.0, |
| 70.0e6, |
| 8.0, |
| ), |
| dtype=float, |
| ) |
|
|
|
|
| def load_history(points: int = 81, *, scale: float = 1.0) -> np.ndarray: |
| anchors = np.asarray((0.0, 0.0035, -0.0025, 0.0055, -0.0035, 0.0065, 0.0)) |
| positions = np.linspace(0.0, len(anchors) - 1, points) |
| lower = np.minimum(np.floor(positions).astype(int), len(anchors) - 2) |
| fraction = positions - lower |
| return scale * ((1.0 - fraction) * anchors[lower] + fraction * anchors[lower + 1]) |
|
|
|
|
| def material() -> constitutive.ChabocheCombinedHardening: |
| p = MATERIAL_PARAMETERS |
| return constitutive.chaboche( |
| young=float(p[0]), |
| poisson=float(p[1]), |
| yield_stress=float(p[2]), |
| backstresses=((float(p[4]), float(p[5])), (float(p[6]), float(p[7]))), |
| isotropic_saturation=float(p[8]), |
| isotropic_rate=float(p[9]), |
| ) |
|
|
|
|
| def _normalization(values: dict[str, object]) -> learning.Normalization: |
| def tensor(name: str, shape: tuple[int, ...]) -> torch.Tensor: |
| return torch.tensor(values[name], dtype=torch.float32).reshape(shape) |
|
|
| return learning.Normalization( |
| strain_mean=tensor("strain_mean", (1, 1, 6)), |
| strain_std=tensor("strain_std", (1, 1, 6)), |
| parameter_mean=tensor("parameter_mean", (1, 10)), |
| parameter_std=tensor("parameter_std", (1, 10)), |
| stress_mean=tensor("stress_mean", (1, 1, 6)), |
| stress_std=tensor("stress_std", (1, 1, 6)), |
| plastic_scale=tensor("plastic_scale", (1, 1, 6)), |
| backstress_scale=tensor("backstress_scale", (1, 1, 6)), |
| peeq_scale=tensor("peeq_scale", (1, 1)), |
| ) |
|
|
|
|
| def load_checkpoint(name: str): |
| if name == physics_integrator.MODEL_NAME: |
| return physics_integrator.load_checkpoint("id") |
| path = MODEL_ROOT / f"id_{name}.pt" |
| checkpoint = torch.load(path, map_location="cpu", weights_only=False) |
| model = learning.build_model(str(checkpoint["model_name"]), int(checkpoint["input_size"])) |
| model.load_state_dict(checkpoint["state_dict"]) |
| model.eval() |
| return model, _normalization(checkpoint["normalization"]) |
|
|
|
|
| def neural_response( |
| model: torch.nn.Module, |
| model_name: str, |
| norm, |
| history: list[float], |
| ) -> tuple[float, float]: |
| previous = torch.tensor(history[:-1], dtype=torch.float32) |
| current = torch.tensor(float(history[-1]), dtype=torch.float32, requires_grad=True) |
| scalar = torch.cat((previous, current.reshape(1))) |
| strain = scalar[:, None] * torch.tensor(BASIS_VOIGT, dtype=torch.float32)[None, :] |
| parameters = torch.tensor(MATERIAL_PARAMETERS, dtype=torch.float32).reshape(1, 10) |
| if model_name == physics_integrator.MODEL_NAME: |
| parameter_mean, parameter_std, correction_steps = norm |
| output = physics_integrator.rollout( |
| strain[None, ...], parameters, model, |
| parameter_mean, parameter_std, |
| correction_steps=correction_steps, |
| )["stress"] |
| generalized = output[0, -1, 0] - 0.5 * output[0, -1, 1] - 0.5 * output[0, -1, 2] |
| tangent = torch.autograd.grad(generalized, current, create_graph=False)[0] |
| return float(generalized.detach()), float(tangent.detach()) |
| normalized_strain = (strain[None, ...] - norm.strain_mean) / norm.strain_std |
| normalized_parameters = (parameters - norm.parameter_mean) / norm.parameter_std |
| repeated = normalized_parameters[:, None, :].expand(1, len(scalar), -1) |
| indicator = torch.tensor((0.0, 1.0), dtype=torch.float32).reshape(1, 1, 2).expand(1, len(scalar), -1) |
| x = torch.cat((normalized_strain, repeated, indicator), dim=-1) |
| if model_name == "physics_state_gru": |
| output = model(x, strain[None, ...], parameters, norm)["stress"] |
| else: |
| output = model(x) * norm.stress_std + norm.stress_mean |
| generalized = ( |
| output[0, -1, 0] - 0.5 * output[0, -1, 1] - 0.5 * output[0, -1, 2] |
| ) |
| tangent = torch.autograd.grad(generalized, current, create_graph=False)[0] |
| return float(generalized.detach()), float(tangent.detach()) |
|
|
|
|
| def native_response( |
| law: constitutive.ChabocheCombinedHardening, |
| old_state, |
| strain: float, |
| ): |
| update = law.update(float(strain) * BASIS, old_state) |
| generalized = float(np.tensordot(update.stress, BASIS)) |
| tangent = float(np.einsum("ij,ijkl,kl", BASIS, update.algorithmic_tangent, BASIS)) |
| return generalized, tangent, update.state |
|
|
|
|
| def geometry(elements: int, notch_depth: float = 0.42) -> tuple[np.ndarray, np.ndarray]: |
| nodes = np.linspace(0.0, 1.0, elements + 1) |
| centers = 0.5 * (nodes[:-1] + nodes[1:]) |
| area = 1.0 - float(notch_depth) * np.exp(-((centers - 0.5) / 0.13) ** 2) |
| return nodes, area |
|
|
|
|
| def solve_native(elements: int, displacement: np.ndarray, *, notch_depth: float = 0.42) -> dict[str, np.ndarray | float | int]: |
| nodes, area = geometry(elements, notch_depth) |
| lengths = np.diff(nodes) |
| law = material() |
| states = [None] * elements |
| strain_histories = [[] for _ in range(elements)] |
| u = np.zeros(elements + 1) |
| reactions = [] |
| strains = [] |
| stresses = [] |
| iterations = [] |
| started = time.perf_counter() |
| for step, end_value in enumerate(displacement): |
| if step > 0: |
| u += np.linspace(0.0, end_value - u[-1], elements + 1) |
| u[0] = 0.0 |
| u[-1] = end_value |
| converged_states = None |
| for iteration in range(30): |
| internal = np.zeros(elements + 1) |
| stiffness = np.zeros((elements + 1, elements + 1)) |
| trial_states = [] |
| current_strain = np.diff(u) / lengths |
| current_stress = np.empty(elements) |
| for element in range(elements): |
| stress, tangent, state = native_response(law, states[element], current_strain[element]) |
| current_stress[element] = stress |
| trial_states.append(state) |
| b = np.asarray((-1.0 / lengths[element], 1.0 / lengths[element])) |
| dofs = (element, element + 1) |
| internal[list(dofs)] += area[element] * stress * b * lengths[element] |
| stiffness[np.ix_(dofs, dofs)] += area[element] * tangent * np.outer(b, b) * lengths[element] |
| residual = internal[1:-1] |
| scale = max(float(np.linalg.norm(internal)), 1.0) |
| if np.linalg.norm(residual) <= 1.0e-8 * scale + 1.0e-3: |
| converged_states = trial_states |
| break |
| u[1:-1] -= np.linalg.solve(stiffness[1:-1, 1:-1], residual) |
| if converged_states is None: |
| raise RuntimeError(f"Native structural solve failed at step {step}.") |
| states = converged_states |
| current_strain = np.diff(u) / lengths |
| for element, value in enumerate(current_strain): |
| strain_histories[element].append(float(value)) |
| reactions.append(float(internal[-1])) |
| strains.append(current_strain.copy()) |
| stresses.append(current_stress.copy()) |
| iterations.append(iteration + 1) |
| return { |
| "displacement": displacement, |
| "reaction": np.asarray(reactions), |
| "strain": np.asarray(strains), |
| "stress": np.asarray(stresses), |
| "nodes": nodes, |
| "area": area, |
| "iterations": np.asarray(iterations), |
| "elapsed_seconds": time.perf_counter() - started, |
| } |
|
|
|
|
| def solve_neural( |
| elements: int, |
| displacement: np.ndarray, |
| model_name: str, |
| *, |
| notch_depth: float = 0.42, |
| ) -> dict[str, np.ndarray | float | int]: |
| if model_name == physics_integrator.MODEL_NAME: |
| return solve_physics_integrator( |
| elements, displacement, notch_depth=notch_depth |
| ) |
| nodes, area = geometry(elements, notch_depth) |
| lengths = np.diff(nodes) |
| loaded = load_checkpoint(model_name) |
| if model_name == physics_integrator.MODEL_NAME: |
| model, parameter_mean, parameter_std, correction_steps = loaded |
| norm = (parameter_mean, parameter_std, correction_steps) |
| else: |
| model, norm = loaded |
| histories = [[] for _ in range(elements)] |
| u = np.zeros(elements + 1) |
| reactions = [] |
| strains = [] |
| stresses = [] |
| iterations = [] |
| started = time.perf_counter() |
| for step, end_value in enumerate(displacement): |
| if step > 0: |
| u += np.linspace(0.0, end_value - u[-1], elements + 1) |
| u[0] = 0.0 |
| u[-1] = end_value |
| converged = False |
| for iteration in range(40): |
| internal = np.zeros(elements + 1) |
| stiffness = np.zeros((elements + 1, elements + 1)) |
| current_strain = np.diff(u) / lengths |
| current_stress = np.empty(elements) |
| for element in range(elements): |
| history = histories[element] + [float(current_strain[element])] |
| stress, tangent = neural_response(model, model_name, norm, history) |
| current_stress[element] = stress |
| |
| |
| if not np.isfinite(tangent) or tangent <= 0.0: |
| raise RuntimeError( |
| f"{physics_integrator.MODEL_NAME} produced an invalid tangent " |
| f"({tangent}) at step {step}." |
| ) |
| b = np.asarray((-1.0 / lengths[element], 1.0 / lengths[element])) |
| dofs = (element, element + 1) |
| internal[list(dofs)] += area[element] * stress * b * lengths[element] |
| stiffness[np.ix_(dofs, dofs)] += area[element] * tangent * np.outer(b, b) * lengths[element] |
| residual = internal[1:-1] |
| scale = max(float(np.linalg.norm(internal)), 1.0) |
| if np.linalg.norm(residual) <= 2.0e-6 * scale + 1.0e2: |
| converged = True |
| break |
| increment = np.linalg.solve(stiffness[1:-1, 1:-1], residual) |
| maximum = 0.20 * max(abs(end_value), 1.0e-5) |
| norm_increment = np.max(np.abs(increment)) |
| if norm_increment > maximum: |
| increment *= maximum / norm_increment |
| u[1:-1] -= increment |
| if not converged: |
| raise RuntimeError(f"{model_name} structural solve failed at step {step}.") |
| current_strain = np.diff(u) / lengths |
| for element, value in enumerate(current_strain): |
| histories[element].append(float(value)) |
| reactions.append(float(internal[-1])) |
| strains.append(current_strain.copy()) |
| stresses.append(current_stress.copy()) |
| iterations.append(iteration + 1) |
| return { |
| "displacement": displacement, |
| "reaction": np.asarray(reactions), |
| "strain": np.asarray(strains), |
| "stress": np.asarray(stresses), |
| "nodes": nodes, |
| "area": area, |
| "iterations": np.asarray(iterations), |
| "elapsed_seconds": time.perf_counter() - started, |
| } |
|
|
|
|
| def _detach_state(state: physics_integrator.State) -> physics_integrator.State: |
| return physics_integrator.State( |
| state.plastic.detach(), state.peeq.detach(), |
| state.alpha1.detach(), state.alpha2.detach(), |
| ) |
|
|
|
|
| def physics_increment_response( |
| model: torch.nn.Module, |
| parameter_mean: torch.Tensor, |
| parameter_std: torch.Tensor, |
| correction_steps: int, |
| committed: physics_integrator.State, |
| previous_strain: float, |
| current_strain: float, |
| ) -> tuple[float, float, physics_integrator.State]: |
| dtype = next(model.parameters()).dtype |
| basis = torch.tensor(BASIS_VOIGT, dtype=dtype).reshape(1, 6) |
| current = torch.tensor(float(current_strain), dtype=dtype) |
| strain = current.reshape(1, 1) * basis |
| previous = torch.tensor(float(previous_strain), dtype=dtype).reshape(1, 1) * torch.tensor( |
| BASIS_VOIGT, dtype=dtype |
| ).reshape(1, 6) |
| parameters = torch.tensor(MATERIAL_PARAMETERS, dtype=dtype).reshape(1, 10) |
| stress, updated, _ = physics_integrator.advance( |
| strain, previous, committed, parameters, model, |
| parameter_mean, parameter_std, correction_steps=correction_steps, |
| ) |
| generalized = stress[0, 0] - 0.5 * stress[0, 1] - 0.5 * stress[0, 2] |
| |
| |
| |
| |
| step = max(2.0e-8, 2.0e-5 * max(abs(float(current_strain)), 1.0e-3)) |
| neighboring = [] |
| with torch.no_grad(): |
| for value in (float(current_strain) - step, float(current_strain) + step): |
| neighbor_stress, _, _ = physics_integrator.advance( |
| torch.tensor(value, dtype=dtype).reshape(1, 1) * basis, |
| previous, committed, parameters, model, |
| parameter_mean, parameter_std, correction_steps=correction_steps, |
| ) |
| neighboring.append( |
| neighbor_stress[0, 0] - 0.5 * neighbor_stress[0, 1] - 0.5 * neighbor_stress[0, 2] |
| ) |
| tangent = (neighboring[1] - neighboring[0]) / (2.0 * step) |
| return float(generalized.detach()), float(tangent.detach()), _detach_state(updated) |
|
|
|
|
| def solve_physics_integrator( |
| elements: int, |
| displacement: np.ndarray, |
| *, |
| notch_depth: float, |
| ) -> dict[str, np.ndarray | float | int]: |
| nodes, area = geometry(elements, notch_depth) |
| lengths = np.diff(nodes) |
| model, parameter_mean, parameter_std, correction_steps = physics_integrator.load_checkpoint("id") |
| model = model.double() |
| parameter_mean = parameter_mean.double() |
| parameter_std = parameter_std.double() |
| correction_steps = max(correction_steps, 8) |
| states = [physics_integrator.initial_state(1, dtype=torch.float64) for _ in range(elements)] |
| previous_strains = np.zeros(elements) |
| u = np.zeros(elements + 1) |
| reactions, strains, stresses, iterations = [], [], [], [] |
| trust_region_fallback_steps: list[int] = [] |
| started = time.perf_counter() |
| for step, end_value in enumerate(displacement): |
| if step > 0: |
| u += np.linspace(0.0, end_value - u[-1], elements + 1) |
| u[0] = 0.0 |
| u[-1] = end_value |
| converged = False |
| converged_states = None |
| for iteration in range(40): |
| internal = np.zeros(elements + 1) |
| stiffness = np.zeros((elements + 1, elements + 1)) |
| current_strain = np.diff(u) / lengths |
| current_stress = np.empty(elements) |
| trial_states = [] |
| for element in range(elements): |
| stress, tangent, trial_state = physics_increment_response( |
| model, parameter_mean, parameter_std, correction_steps, |
| states[element], previous_strains[element], current_strain[element], |
| ) |
| current_stress[element] = stress |
| trial_states.append(trial_state) |
| tangent = float(np.clip(tangent, 1.0e7, 4.0e11)) |
| b = np.asarray((-1.0 / lengths[element], 1.0 / lengths[element])) |
| dofs = (element, element + 1) |
| internal[list(dofs)] += area[element] * stress * b * lengths[element] |
| stiffness[np.ix_(dofs, dofs)] += area[element] * tangent * np.outer(b, b) * lengths[element] |
| residual = internal[1:-1] |
| scale = max(float(np.linalg.norm(internal)), 1.0) |
| if np.linalg.norm(residual) <= 2.0e-6 * scale + 1.0e2: |
| converged = True |
| converged_states = trial_states |
| break |
| increment = np.linalg.solve(stiffness[1:-1, 1:-1], residual) |
| maximum = 0.20 * max(abs(end_value), 1.0e-5) |
| norm_increment = np.max(np.abs(increment)) |
| if norm_increment > maximum: |
| increment *= maximum / norm_increment |
| u[1:-1] -= increment |
| if not converged: |
| |
| |
| |
| |
| |
| end_fixed = float(end_value) |
|
|
| def equilibrium(interior: np.ndarray) -> np.ndarray: |
| candidate = np.concatenate(([0.0], interior, [end_fixed])) |
| candidate_strain = np.diff(candidate) / lengths |
| candidate_internal = np.zeros(elements + 1) |
| for local_element in range(elements): |
| local_stress, _, _ = physics_increment_response( |
| model, parameter_mean, parameter_std, correction_steps, |
| states[local_element], previous_strains[local_element], |
| candidate_strain[local_element], |
| ) |
| local_b = np.asarray( |
| (-1.0 / lengths[local_element], 1.0 / lengths[local_element]) |
| ) |
| local_dofs = (local_element, local_element + 1) |
| candidate_internal[list(local_dofs)] += ( |
| area[local_element] * local_stress * local_b * lengths[local_element] |
| ) |
| return candidate_internal[1:-1] / 1.0e8 |
|
|
| recovered = least_squares( |
| equilibrium, u[1:-1], method="trf", jac="3-point", |
| max_nfev=250, xtol=1.0e-12, ftol=1.0e-12, gtol=1.0e-12, |
| ) |
| if recovered.success: |
| u[1:-1] = recovered.x |
| current_strain = np.diff(u) / lengths |
| internal = np.zeros(elements + 1) |
| current_stress = np.empty(elements) |
| trial_states = [] |
| for element in range(elements): |
| stress, _, trial_state = physics_increment_response( |
| model, parameter_mean, parameter_std, correction_steps, |
| states[element], previous_strains[element], current_strain[element], |
| ) |
| current_stress[element] = stress |
| trial_states.append(trial_state) |
| b = np.asarray((-1.0 / lengths[element], 1.0 / lengths[element])) |
| dofs = (element, element + 1) |
| internal[list(dofs)] += area[element] * stress * b * lengths[element] |
| residual = internal[1:-1] |
| scale = max(float(np.linalg.norm(internal)), 1.0) |
| if np.linalg.norm(residual) <= 2.0e-6 * scale + 1.0e2: |
| converged = True |
| converged_states = trial_states |
| iteration = 40 + int(recovered.nfev) |
| trust_region_fallback_steps.append(step) |
| if not converged or converged_states is None: |
| raise RuntimeError( |
| f"{physics_integrator.MODEL_NAME} structural solve failed at step {step}; " |
| f"max_abs_element_strain={float(np.max(np.abs(current_strain))):.6g}." |
| ) |
| states = converged_states |
| previous_strains = np.diff(u) / lengths |
| reactions.append(float(internal[-1])) |
| strains.append(previous_strains.copy()) |
| stresses.append(current_stress.copy()) |
| iterations.append(iteration + 1) |
| return { |
| "displacement": displacement, |
| "reaction": np.asarray(reactions), |
| "strain": np.asarray(strains), |
| "stress": np.asarray(stresses), |
| "nodes": nodes, |
| "area": area, |
| "iterations": np.asarray(iterations), |
| "trust_region_fallback_steps": trust_region_fallback_steps, |
| "elapsed_seconds": time.perf_counter() - started, |
| } |
|
|
|
|
| def compare(reference: dict[str, object], predicted: dict[str, object]) -> dict[str, float | int]: |
| reaction_reference = np.asarray(reference["reaction"]) |
| reaction_predicted = np.asarray(predicted["reaction"]) |
| strain_reference = np.asarray(reference["strain"]) |
| strain_predicted = np.asarray(predicted["strain"]) |
| stress_reference = np.asarray(reference["stress"]) |
| stress_predicted = np.asarray(predicted["stress"]) |
| reaction_scale = max(float(np.max(np.abs(reaction_reference))), 1.0) |
| stress_scale = max(float(np.max(np.abs(stress_reference))), 1.0) |
| result = { |
| "reaction_relative_l2": float(np.linalg.norm(reaction_predicted - reaction_reference) / max(np.linalg.norm(reaction_reference), 1.0)), |
| "reaction_max_relative_error": float(np.max(np.abs(reaction_predicted - reaction_reference)) / reaction_scale), |
| "strain_relative_l2": float(np.linalg.norm(strain_predicted - strain_reference) / max(np.linalg.norm(strain_reference), 1.0e-15)), |
| "stress_relative_l2": float(np.linalg.norm(stress_predicted - stress_reference) / max(np.linalg.norm(stress_reference), 1.0)), |
| "stress_max_relative_error": float(np.max(np.abs(stress_predicted - stress_reference)) / stress_scale), |
| "maximum_newton_iterations": int(np.max(predicted["iterations"])), |
| "mean_newton_iterations": float(np.mean(predicted["iterations"])), |
| "elapsed_seconds": float(predicted["elapsed_seconds"]), |
| } |
| if "trust_region_fallback_steps" in predicted: |
| result["trust_region_fallback_count"] = len(predicted["trust_region_fallback_steps"]) |
| result["trust_region_fallback_steps"] = list(predicted["trust_region_fallback_steps"]) |
| return result |
|
|
|
|
| def run( |
| elements: int = 12, |
| points: int = 81, |
| model_names: tuple[str, ...] = ("gru", "physics_state_gru", "physics_integrator_nn"), |
| case_name: str = "severe_ood", |
| ) -> dict[str, object]: |
| if case_name == "mild_id": |
| notch_depth = 0.12 |
| load_scale = 0.65 |
| elif case_name == "moderate_ood": |
| notch_depth = 0.30 |
| load_scale = 0.85 |
| elif case_name == "severe_ood": |
| notch_depth = 0.42 |
| load_scale = 1.0 |
| else: |
| raise ValueError(f"Unknown structural case: {case_name}") |
| displacement = load_history(points, scale=load_scale) |
| print("solving native AgentFEM Chaboche reference", flush=True) |
| reference = solve_native(elements, displacement, notch_depth=notch_depth) |
| learned = {} |
| metrics = {} |
| failures = {} |
| for model_name in model_names: |
| print(f"solving learned structural model: {model_name}", flush=True) |
| try: |
| result = solve_neural( |
| elements, |
| displacement, |
| model_name, |
| notch_depth=notch_depth, |
| ) |
| except RuntimeError as error: |
| failures[model_name] = str(error) |
| print(f"recorded structural failure: {error}", flush=True) |
| else: |
| learned[model_name] = result |
| metrics[model_name] = compare(reference, result) |
|
|
| output_directory = ARTIFACT_ROOT / case_name |
| output_directory.mkdir(parents=True, exist_ok=True) |
| figure, axes = plt.subplots(1, 3, figsize=(14.0, 4.2), constrained_layout=True) |
| axes[0].plot(displacement, np.asarray(reference["reaction"]) / 1.0e6, color="#111827", lw=2.2, label="AgentFEM Chaboche") |
| colors = {"gru": "#2563eb", "physics_state_gru": "#dc2626", "physics_integrator_nn": "#059669"} |
| labels = {"gru": "GRU", "physics_state_gru": "Physics-state GRU", "physics_integrator_nn": "Physics-integrator NN"} |
| for name, result in learned.items(): |
| axes[0].plot(displacement, np.asarray(result["reaction"]) / 1.0e6, color=colors[name], lw=1.5, label=labels[name]) |
| axes[0].set_xlabel("End displacement / length") |
| axes[0].set_ylabel("Reaction (MN for unit area)") |
| axes[0].set_title("Structural force-displacement") |
| centers = 0.5 * (np.asarray(reference["nodes"])[:-1] + np.asarray(reference["nodes"])[1:]) |
| axes[1].plot(centers, np.asarray(reference["strain"])[-2], color="#111827", lw=2.2) |
| axes[2].plot(centers, np.asarray(reference["stress"])[-2] / 1.0e6, color="#111827", lw=2.2) |
| for name, result in learned.items(): |
| axes[1].plot(centers, np.asarray(result["strain"])[-2], color=colors[name], lw=1.4) |
| axes[2].plot(centers, np.asarray(result["stress"])[-2] / 1.0e6, color=colors[name], lw=1.4) |
| axes[1].set_title("Near-final element strain") |
| axes[1].set_xlabel("Bar coordinate") |
| axes[1].set_ylabel("Generalized strain") |
| axes[2].set_title("Near-final generalized stress") |
| axes[2].set_xlabel("Bar coordinate") |
| axes[2].set_ylabel("Stress (MPa)") |
| for axis in axes: |
| axis.grid(alpha=0.2) |
| axes[0].legend(frameon=False, fontsize=8) |
| figure.savefig(output_directory / "notched_bar_comparison.png", dpi=190) |
| plt.close(figure) |
|
|
| archive = { |
| "displacement": displacement, |
| "nodes": reference["nodes"], |
| "area": reference["area"], |
| "reference_reaction": reference["reaction"], |
| "reference_strain": reference["strain"], |
| "reference_stress": reference["stress"], |
| } |
| for name, result in learned.items(): |
| archive[f"{name}_reaction"] = result["reaction"] |
| archive[f"{name}_strain"] = result["strain"] |
| archive[f"{name}_stress"] = result["stress"] |
| np.savez_compressed(output_directory / "notched_bar_results.npz", **archive) |
| summary = { |
| "status": "completed" if not failures else "completed_with_model_failures", |
| "scope": "controlled one-dimensional notched-bar finite-element deployment", |
| "case_name": case_name, |
| "notch_depth_fraction": notch_depth, |
| "load_scale": load_scale, |
| "elements": elements, |
| "load_points": points, |
| "material_model": "chaboche_combined", |
| "native_elapsed_seconds": float(reference["elapsed_seconds"]), |
| "models": metrics, |
| "model_failures": failures, |
| "limitations": [ |
| "This is a reduced one-dimensional structural gate, not a general 3D learned AgentFEM material provider.", |
| "The physics-integrator uses a numerical tangent of its fully discrete update and records any trust-region fallback used when plain global Newton leaves its local basin.", |
| "The loading is proportional at each material point even though the training dataset is multiaxial.", |
| ], |
| } |
| (output_directory / "structural_validation.json").write_text(json.dumps(summary, indent=2, sort_keys=True) + "\n", encoding="utf-8") |
| print(json.dumps(summary, indent=2), flush=True) |
| return summary |
|
|
|
|
| def main() -> None: |
| parser = argparse.ArgumentParser(description=__doc__) |
| parser.add_argument("--elements", type=int, default=12) |
| parser.add_argument("--points", type=int, default=81) |
| parser.add_argument( |
| "--models", |
| nargs="+", |
| choices=("gru", "physics_state_gru", "physics_integrator_nn"), |
| default=("gru", "physics_state_gru", "physics_integrator_nn"), |
| ) |
| parser.add_argument("--case", choices=("mild_id", "moderate_ood", "severe_ood"), default="severe_ood") |
| args = parser.parse_args() |
| run( |
| elements=args.elements, |
| points=args.points, |
| model_names=tuple(args.models), |
| case_name=args.case, |
| ) |
|
|
|
|
| if __name__ == "__main__": |
| main() |
|
|