Source code for rheojax.models.fluidity.nonlocal_model

"""Non-Local Fluidity Model Implementation.

This module implements the Non-Local (1D PDE, Coussot-Ovarlez) Fluidity model
for yield-stress fluids with spatial diffusion, supporting shear banding analysis.
"""

from __future__ import annotations

from typing import Any, cast

import numpy as np

from rheojax.core.inventory import Protocol
from rheojax.core.jax_config import lazy_import, safe_import_jax

diffrax = lazy_import("diffrax")
from rheojax.core.registry import ModelRegistry
from rheojax.core.test_modes import DeformationMode
from rheojax.logging import get_logger, log_fit
from rheojax.models.fluidity._base import FluidityBase
from rheojax.models.fluidity._kernels import (
    banding_ratio,
    fluidity_nonlocal_creep_pde_rhs,
    fluidity_nonlocal_pde_rhs,
    fluidity_nonlocal_steady_state,
    shear_banding_cv,
)

# Safe JAX import
jax, jnp = safe_import_jax()

# Logger
logger = get_logger(__name__)

# Sentinel for distinguishing "not provided" from falsy values (FL-009)
_MISSING = object()

# FL-006: kwargs to pop before forwarding to nlsq_optimize
_NLSQ_RESERVED = {
    "test_mode",
    "use_log_residuals",
    "smart_init",
    "use_multi_start",
    "n_starts",
    "perturb_factor",
    "gamma_dot",
    "sigma_applied",
    "gamma_0",
    "omega",
    "omega_laos",
    "t_wait",
    "n_cycles",
    "points_per_cycle",
    "deformation_mode",
    "poisson_ratio",
    "method",
    "callback",
}


[docs] @ModelRegistry.register( "fluidity_nonlocal", protocols=[ Protocol.FLOW_CURVE, Protocol.CREEP, Protocol.RELAXATION, Protocol.STARTUP, Protocol.OSCILLATION, Protocol.LAOS, ], deformation_modes=[ DeformationMode.SHEAR, DeformationMode.TENSION, DeformationMode.BENDING, DeformationMode.COMPRESSION, ], ) class FluidityNonlocal(FluidityBase): """Non-Local (1D PDE) Fluidity Model for yield-stress fluids. Implements the Coussot-Ovarlez non-local fluidity model where the fluidity field f(y,t) evolves across the gap (y-direction) via: ∂f/∂t = (f_loc(σ) - f)/θ + ξ²∂²f/∂y² where: - f_loc(σ) is the local equilibrium fluidity from HB flow curve - θ is the relaxation time - ξ is the cooperativity length (non-local diffusion) This captures shear banding: localized flow in yield-stress fluids where the cooperativity length ξ determines band width. Key features: - 1D Couette gap discretization (N_y points) - Neumann (zero-flux) boundary conditions at walls - Diffrax Dopri5 solver (explicit, robust) for PDE - Shear banding metrics: CV and max/min ratio Attributes: N_y: Number of grid points across gap gap_width: Physical gap width (m) """
[docs] def __init__(self, N_y: int = 64, gap_width: float = 1e-3): """Initialize Non-Local Fluidity Model. Args: N_y: Number of spatial grid points (default 64) gap_width: Physical gap width in meters (default 1 mm) """ super().__init__() # FL-011: Guard against N_y < 2 which causes ZeroDivisionError in dy if N_y < 2: raise ValueError(f"N_y must be >= 2 for spatial discretization, got {N_y}") self.N_y = N_y self.gap_width = gap_width self.dy = gap_width / (N_y - 1) # Add non-local specific parameter self._add_nonlocal_parameters() # Storage for fluidity field trajectory self._f_field_trajectory: np.ndarray | None = None
def _add_nonlocal_parameters(self): """Add non-local specific parameters.""" # xi: Cooperativity length (m) self.parameters.add( name="xi", value=1e-5, bounds=(1e-9, 1e-3), units="m", description="Cooperativity length (non-local diffusion scale)", ) def _fit( self, X: np.ndarray, y: np.ndarray, **kwargs, ) -> FluidityNonlocal: """Fit Non-Local Fluidity model to data. Args: X: Independent variable (time, frequency, or shear rate) y: Dependent variable (stress, modulus, viscosity) **kwargs: Optimizer options. Must include 'test_mode'. """ test_mode = kwargs.get("test_mode") if test_mode is None: if hasattr(self, "_test_mode") and self._test_mode is not None: test_mode = self._test_mode else: raise ValueError("test_mode must be specified for Fluidity fitting") # FL-001: Normalize aliases early so self._test_mode is canonical if test_mode == "saos": test_mode = "oscillation" with log_fit(logger, model="FluidityNonlocal", data_shape=X.shape) as ctx: self._test_mode = cast(str, test_mode) ctx["test_mode"] = test_mode ctx["N_y"] = self.N_y if test_mode in ["steady_shear", "rotation", "flow_curve"]: self._fit_flow_curve(X, y, **kwargs) elif test_mode == "startup": self._fit_transient(X, y, mode="startup", **kwargs) elif test_mode == "relaxation": self._fit_transient(X, y, mode="relaxation", **kwargs) elif test_mode == "creep": self._fit_transient(X, y, mode="creep", **kwargs) elif test_mode == "oscillation": self._fit_oscillation(X, y, **kwargs) elif test_mode == "laos": self._fit_laos(X, y, **kwargs) else: raise ValueError(f"Unsupported test_mode: {test_mode}") self.fitted_ = True return self # ========================================================================= # Grid and Initial Conditions # ========================================================================= def _get_grid_args(self, params: dict | None = None) -> dict: """Get grid-related arguments for PDE solver. Args: params: Optional parameter dictionary Returns: Dictionary with grid parameters """ if params is None: params = self.get_parameter_dict() return { "N_y": self.N_y, "dy": self.dy, "xi": params.get("xi", 1e-5), } def _get_initial_f_field( self, f_init: float | None = None, N_y: int | None = None ) -> jnp.ndarray: """Get initial fluidity field (uniform across gap). Args: f_init: Initial fluidity value. If None, uses f_eq. N_y: Number of grid points override. If None, uses self.N_y. Returns: Fluidity field array, shape (N_y,) """ if f_init is None: f_init = self.get_initial_fluidity() n = N_y if N_y is not None else self.N_y return jnp.ones(n) * f_init def _get_initial_state( self, mode: str, params: dict, sigma_0: float | None = None, N_y: int | None = None, ) -> jnp.ndarray: """Get initial state vector for PDE solver. State vector: [Σ (or γ for creep), f[0], f[1], ..., f[N_y-1]] Args: mode: 'startup', 'relaxation', 'creep', or 'laos' params: Parameter dictionary sigma_0: Initial stress for relaxation Returns: Initial state vector """ f_eq = params["f_eq"] f_inf = params["f_inf"] if mode == "creep": # State: [γ, f_field] - strain starts at 0 f_field = self._get_initial_f_field(f_eq, N_y=N_y) return jnp.concatenate([jnp.array([0.0]), f_field]) elif mode == "relaxation": # State: [Σ, f_field] - stress starts at sigma_0, f at f_inf sigma_init = sigma_0 if sigma_0 is not None else params["tau_y"] f_field = self._get_initial_f_field(f_inf, N_y=N_y) # Just flowed return jnp.concatenate([jnp.array([sigma_init]), f_field]) else: # startup or laos # State: [Σ, f_field] - stress at 0, f at f_eq f_field = self._get_initial_f_field(f_eq, N_y=N_y) return jnp.concatenate([jnp.array([0.0]), f_field]) # ========================================================================= # Flow Curve (Steady State) # ========================================================================= def _fit_flow_curve( self, gamma_dot: np.ndarray, stress: np.ndarray, **kwargs ) -> None: """Fit steady-state flow curve. For homogeneous (non-banding) steady state, uses HB: σ = τ_y + K*|γ̇|^n Args: gamma_dot: Shear rate array (1/s) stress: Shear stress array (Pa) **kwargs: Optimizer options """ from rheojax.utils.optimization import ( create_least_squares_objective, nlsq_optimize, ) gamma_dot_jax = jnp.asarray(gamma_dot, dtype=jnp.float64) stress_jax = jnp.asarray(stress, dtype=jnp.float64) def model_fn(x_data, params): p_map = dict(zip(self.parameters.keys(), params, strict=True)) return fluidity_nonlocal_steady_state( x_data, p_map["G"], p_map["tau_y"], p_map["K"], p_map["n_flow"], p_map["f_eq"], p_map["f_inf"], p_map["theta"], ) objective = create_least_squares_objective( model_fn, gamma_dot_jax, stress_jax, use_log_residuals=kwargs.get("use_log_residuals", True), ) # FL-006: Pop protocol/meta kwargs before forwarding to nlsq_optimize nlsq_kwargs = {k: v for k, v in kwargs.items() if k not in _NLSQ_RESERVED} result = nlsq_optimize(objective, self.parameters, **nlsq_kwargs) if not result.success: logger.warning(f"Fluidity flow curve fit warning: {result.message}") # FL-013: _predict_flow_curve is not used by _predict() or model_function() # (flow curve routing goes through fluidity_nonlocal_steady_state directly). # Kept as a thin compatibility wrapper for external callers. def _predict_flow_curve(self, gamma_dot: np.ndarray) -> np.ndarray: """Predict steady-state flow curve (compatibility wrapper).""" return np.array(self._predict(gamma_dot, test_mode="flow_curve")) # ========================================================================= # Transient Protocols (Startup, Relaxation, Creep) # ========================================================================= def _fit_transient(self, t: np.ndarray, y: np.ndarray, mode: str, **kwargs) -> None: """Fit transient response using PDE solver. Args: t: Time array (s) y: Response data (stress for startup/relaxation, strain for creep) mode: 'startup', 'relaxation', or 'creep' **kwargs: Protocol-specific inputs and optimizer options """ from rheojax.utils.optimization import ( create_least_squares_objective, nlsq_optimize, ) t_jax = jnp.asarray(t, dtype=jnp.float64) # Preserve complex dtype for oscillation data (G* = G' + iG'') y_arr = np.asarray(y) if np.iscomplexobj(y_arr): y_jax = jnp.asarray(y_arr, dtype=jnp.complex128) else: y_jax = jnp.asarray(y_arr, dtype=jnp.float64) # Extract protocol-specific inputs gamma_dot = kwargs.pop("gamma_dot", None) sigma_applied = kwargs.pop("sigma_applied", None) sigma_0 = kwargs.pop("sigma_0", None) # FL-003: Use local variables for coarser grid instead of mutating self # This avoids thread-safety issues where concurrent access could corrupt # self.N_y and self.dy during fitting fit_N_y = kwargs.pop("fit_N_y", min(self.N_y, 32)) fit_dy = self.gap_width / (fit_N_y - 1) if mode == "startup" and gamma_dot is None: raise ValueError("startup mode requires gamma_dot in kwargs") if mode == "creep" and sigma_applied is None: raise ValueError("creep mode requires sigma_applied in kwargs") # Store for prediction self._gamma_dot_applied = gamma_dot self._sigma_applied = sigma_applied def model_fn(x_data, params): p_map = dict(zip(self.parameters.keys(), params, strict=True)) return self._simulate_pde( x_data, p_map, mode, gamma_dot, sigma_applied, sigma_0, N_y=fit_N_y, dy=fit_dy, ) objective = create_least_squares_objective( model_fn, t_jax, y_jax, use_log_residuals=kwargs.get("use_log_residuals", False), ) # FL-006: Pop protocol/meta kwargs before forwarding to nlsq_optimize nlsq_kwargs = {k: v for k, v in kwargs.items() if k not in _NLSQ_RESERVED} result = nlsq_optimize(objective, self.parameters, **nlsq_kwargs) if not result.success: logger.warning(f"Fluidity transient fit warning: {result.message}") def _simulate_pde( self, t: jnp.ndarray, params: dict, mode: str, gamma_dot: float | None, sigma_applied: float | None, sigma_0: float | None, N_y: int | None = None, dy: float | None = None, ) -> jnp.ndarray: """Simulate PDE response using Diffrax. Args: t: Time array params: Parameter dictionary mode: 'startup', 'relaxation', or 'creep' gamma_dot: Applied shear rate (for startup) sigma_applied: Applied stress (for creep) sigma_0: Initial stress (for relaxation) N_y: Grid points override (FL-003 thread safety). If None, uses self.N_y. dy: Grid spacing override (FL-003 thread safety). If None, uses self.dy. Returns: Primary output (stress for startup/relaxation, strain for creep) """ # FL-003: Use local variables instead of self.N_y/self.dy for thread safety N_y_local = N_y if N_y is not None else self.N_y dy_local = dy if dy is not None else self.dy # Build args for PDE RHS # FL-012: Removed dead "N_y" key — PDE kernels infer N_y from state vector shape args = { "G": params["G"], "tau_y": params["tau_y"], "K": params["K"], "n_flow": params["n_flow"], "theta": params["theta"], "xi": params.get("xi", 1e-5), "dy": dy_local, } # Mode-specific setup if mode == "creep": pde_fn = fluidity_nonlocal_creep_pde_rhs args["sigma_applied"] = sigma_applied if sigma_applied is not None else 0.0 else: pde_fn = fluidity_nonlocal_pde_rhs if mode == "startup": args["mode"] = 0 # rate_controlled args["gamma_dot"] = gamma_dot if gamma_dot is not None else 0.0 else: # relaxation args["mode"] = 0 # rate_controlled args["gamma_dot"] = 0.0 # Initial state (uses N_y_local for grid size) y0 = self._get_initial_state(mode, params, sigma_0, N_y=N_y_local) # Diffrax setup - use Dopri5 for stiff PDEs (explicit, avoids tracer issues) term = diffrax.ODETerm( jax.checkpoint(lambda ti, yi, args_i: pde_fn(cast(float, ti), yi, args_i)) ) solver = diffrax.Dopri5() stepsize_controller = diffrax.PIDController(rtol=1e-4, atol=1e-6) t0 = t[0] t1 = t[-1] dt0 = (t1 - t0) / max(len(t), 1000) saveat = diffrax.SaveAt(ts=t) sol = diffrax.diffeqsolve( term, solver, t0, t1, dt0, y0, args=args, saveat=saveat, stepsize_controller=stepsize_controller, max_steps=10_000_000, throw=False, # Return partial result on failure (for optimization) ) # Store trajectory for analysis (skip during JAX tracing, e.g. NUTS) # FL-007: Log exceptions instead of silently swallowing try: self._f_field_trajectory = np.array(sol.ys[:, 1:]) except Exception as e: logger.warning("Could not store fluidity field trajectory: %s", e) # Extract primary variable (index 0) # For creep: strain; for startup/relaxation: stress result = sol.ys[:, 0] # Handle solver failure by returning NaN (optimization will avoid this) result = jnp.where(sol.result == diffrax.RESULTS.successful, result, jnp.nan) return result def _predict_transient(self, t: np.ndarray, mode: str | None = None) -> np.ndarray: """Predict transient response.""" t_jax = jnp.asarray(t, dtype=jnp.float64) p = self.get_parameter_dict() mode = mode if mode is not None else self._test_mode if mode is None: raise ValueError("Test mode not specified for prediction") result = self._simulate_pde( t_jax, p, mode, self._gamma_dot_applied, self._sigma_applied, None, ) return np.array(result) # ========================================================================= # Shear Banding Analysis # =========================================================================
[docs] def get_fluidity_profile(self, time_idx: int = -1) -> np.ndarray: """Get fluidity profile at specified time index. Args: time_idx: Time index (default -1 for final time) Returns: Fluidity field across gap, shape (N_y,) """ if self._f_field_trajectory is None: raise ValueError("No trajectory available. Run simulation first.") return self._f_field_trajectory[time_idx]
[docs] def get_shear_banding_metric(self, f_field: np.ndarray | None = None) -> float: """Compute coefficient of variation as shear banding metric. CV = std(f) / mean(f) CV > 0.3 typically indicates significant shear banding. Args: f_field: Fluidity field. If None, uses final simulation state. Returns: Coefficient of variation (dimensionless) """ if f_field is None: f_field = self.get_fluidity_profile(-1) f_jax = jnp.asarray(f_field, dtype=jnp.float64) return float(shear_banding_cv(f_jax))
[docs] def get_banding_ratio(self, f_field: np.ndarray | None = None) -> float: """Compute max/min fluidity ratio as banding metric. ratio > 10 indicates strong localization. Args: f_field: Fluidity field. If None, uses final simulation state. Returns: Banding ratio (dimensionless) """ if f_field is None: f_field = self.get_fluidity_profile(-1) f_jax = jnp.asarray(f_field, dtype=jnp.float64) return float(banding_ratio(f_jax))
[docs] def is_banding( self, f_field: np.ndarray | None = None, cv_threshold: float = 0.3 ) -> bool: """Check if shear banding is occurring. Args: f_field: Fluidity field. If None, uses final simulation state. cv_threshold: CV threshold for banding (default 0.3) Returns: True if CV > threshold """ return self.get_shear_banding_metric(f_field) > cv_threshold
# ========================================================================= # Oscillatory Protocols # ========================================================================= def _fit_oscillation(self, X: np.ndarray, y: np.ndarray, **kwargs) -> None: """Fit SAOS data using linear viscoelastic approximation. For small amplitude, bulk response approximates Local model. """ from rheojax.utils.optimization import ( create_least_squares_objective, nlsq_optimize, ) omega_jax = jnp.asarray(X, dtype=jnp.float64) # Handle G_star format G_star_np = np.asarray(y) if np.iscomplexobj(G_star_np): G_star_2d = np.column_stack([np.real(G_star_np), np.imag(G_star_np)]) elif G_star_np.ndim == 2 and G_star_np.shape[1] == 2: G_star_2d = G_star_np else: raise ValueError(f"G_star must be complex or (M, 2), got {G_star_np.shape}") G_star_jax = jnp.asarray(G_star_2d, dtype=jnp.float64) def model_fn(x_data, params): p_map = dict(zip(self.parameters.keys(), params, strict=True)) return self._predict_saos_jit( x_data, p_map["G"], p_map["f_eq"], ) objective = create_least_squares_objective( model_fn, omega_jax, G_star_jax, normalize=True, ) # FL-006: Pop protocol/meta kwargs before forwarding to nlsq_optimize nlsq_kwargs = {k: v for k, v in kwargs.items() if k not in _NLSQ_RESERVED} result = nlsq_optimize(objective, self.parameters, **nlsq_kwargs) if not result.success: logger.warning(f"Fluidity SAOS fit warning: {result.message}") # TODO (FL-010): _predict_saos_jit is duplicated in FluidityLocal. # Consider extracting to a shared module-level function or into _base.py. @staticmethod @jax.jit def _predict_saos_jit( omega: jnp.ndarray, G: float, f_eq: float, theta: float = 0.0, # FL-005: dead parameter, kept for backward compatibility ) -> jnp.ndarray: """SAOS prediction using linear viscoelastic approximation. Note: theta parameter is unused (FL-005) but kept for backward compatibility with external callers. """ del theta # FL-005: explicitly unused tau_eff = 1.0 / (G * f_eq + 1e-30) omega_tau = omega * tau_eff denom = 1.0 + omega_tau**2 G_prime = G * omega_tau**2 / denom G_double_prime = G * omega_tau / denom return jnp.stack([G_prime, G_double_prime], axis=1) def _fit_laos(self, t: np.ndarray, sigma: np.ndarray, **kwargs) -> None: """Fit LAOS data using full PDE integration.""" from rheojax.utils.optimization import ( create_least_squares_objective, nlsq_optimize, ) gamma_0 = kwargs.pop("gamma_0", None) omega = kwargs.pop("omega", None) if gamma_0 is None or omega is None: raise ValueError("LAOS fitting requires gamma_0 and omega") self._gamma_0 = gamma_0 self._omega_laos = omega # FL-003: Use local variables for coarser grid instead of mutating self fit_N_y = kwargs.pop("fit_N_y", min(self.N_y, 32)) fit_dy = self.gap_width / (fit_N_y - 1) t_jax = jnp.asarray(t, dtype=jnp.float64) sigma_jax = jnp.asarray(sigma, dtype=jnp.float64) def model_fn(x_data, params): p_map = dict(zip(self.parameters.keys(), params, strict=True)) _, stress = self._simulate_laos_internal( x_data, p_map, gamma_0, omega, N_y=fit_N_y, dy=fit_dy, ) return stress objective = create_least_squares_objective( model_fn, t_jax, sigma_jax, normalize=True, ) # FL-006: Pop protocol/meta kwargs before forwarding to nlsq_optimize nlsq_kwargs = {k: v for k, v in kwargs.items() if k not in _NLSQ_RESERVED} result = nlsq_optimize(objective, self.parameters, **nlsq_kwargs) if not result.success: logger.warning(f"Fluidity LAOS fit warning: {result.message}") def _simulate_laos_internal( self, t: jnp.ndarray, params: dict, gamma_0: float, omega: float, N_y: int | None = None, dy: float | None = None, ) -> tuple[jnp.ndarray, jnp.ndarray]: """Simulate LAOS response using PDE solver. Args: t: Time array params: Parameter dictionary gamma_0: Strain amplitude omega: Angular frequency N_y: Grid points override (FL-003 thread safety). If None, uses self.N_y. dy: Grid spacing override (FL-003 thread safety). If None, uses self.dy. """ # FL-003: Use local variables instead of self.N_y/self.dy for thread safety N_y_local = N_y if N_y is not None else self.N_y dy_local = dy if dy is not None else self.dy # Base args # FL-012: Removed dead "N_y" key — PDE kernels infer N_y from state vector shape base_args = { "G": params["G"], "tau_y": params["tau_y"], "K": params["K"], "n_flow": params["n_flow"], "theta": params["theta"], "xi": params.get("xi", 1e-5), "dy": dy_local, "mode": 0, # rate_controlled } # Initial state (uses N_y_local for grid size) y0 = self._get_initial_state("laos", params, N_y=N_y_local) # PDE with time-varying gamma_dot def laos_pde(ti, yi, args_i): gamma_dot_t = gamma_0 * omega * jnp.cos(omega * ti) args_with_rate = {**args_i, "gamma_dot": gamma_dot_t} return fluidity_nonlocal_pde_rhs(ti, yi, args_with_rate) term = diffrax.ODETerm(jax.checkpoint(laos_pde)) solver = diffrax.Dopri5() stepsize_controller = diffrax.PIDController(rtol=1e-4, atol=1e-6) t0 = t[0] t1 = t[-1] dt0 = (t1 - t0) / max(len(t), 1000) saveat = diffrax.SaveAt(ts=t) sol = diffrax.diffeqsolve( term, solver, t0, t1, dt0, y0, args=base_args, saveat=saveat, stepsize_controller=stepsize_controller, max_steps=16_000_000, throw=False, # Return partial result on failure (for optimization) ) stress = sol.ys[:, 0] strain = gamma_0 * jnp.sin(omega * t) # Handle solver failure by returning NaN stress = jnp.where(sol.result == diffrax.RESULTS.successful, stress, jnp.nan) # Store trajectory only when not in JIT context (concrete arrays) # FL-008: Use ConcretizationTypeError (modern) instead of deprecated # TracerArrayConversionError try: # This will fail during JIT tracing self._f_field_trajectory = np.asarray(sol.ys[:, 1:]) except (TypeError, jax.errors.ConcretizationTypeError): # During JIT tracing, skip storage pass return strain, stress
[docs] def simulate_laos( self, gamma_0: float, omega: float, n_cycles: int = 2, n_points_per_cycle: int = 256, ) -> tuple[np.ndarray, np.ndarray]: """Simulate LAOS response. Args: gamma_0: Strain amplitude omega: Angular frequency (rad/s) n_cycles: Number of oscillation cycles n_points_per_cycle: Points per cycle Returns: (strain, stress) arrays """ self._gamma_0 = gamma_0 self._omega_laos = omega period = 2.0 * np.pi / omega t_max = n_cycles * period n_points = n_cycles * n_points_per_cycle t = np.linspace(0, t_max, n_points, endpoint=False) t_jax = jnp.asarray(t, dtype=jnp.float64) p = self.get_parameter_dict() strain, stress = self._simulate_laos_internal(t_jax, p, gamma_0, omega) return np.array(strain), np.array(stress)
# ========================================================================= # Bayesian / Model Function Interface # =========================================================================
[docs] def model_function(self, X, params, test_mode=None, **kwargs): """NumPyro/BayesianMixin model function. Accepts protocol-specific kwargs (gamma_dot, sigma_applied, etc.). """ p_values = dict(zip(self.parameters.keys(), params, strict=True)) mode = test_mode if test_mode is not None else self._test_mode if mode is None: mode = "oscillation" # FL-001: Normalize aliases if mode == "saos": mode = "oscillation" X_jax = jnp.asarray(X, dtype=jnp.float64) # FL-009: Use sentinel pattern to avoid swallowing falsy values (e.g. 0.0) gamma_dot = kwargs.get("gamma_dot", _MISSING) if gamma_dot is _MISSING: gamma_dot = getattr(self, "_gamma_dot_applied", None) sigma_applied = kwargs.get("sigma_applied", _MISSING) if sigma_applied is _MISSING: sigma_applied = getattr(self, "_sigma_applied", None) gamma_0 = kwargs.get("gamma_0", _MISSING) if gamma_0 is _MISSING: gamma_0 = getattr(self, "_gamma_0", None) omega = kwargs.get("omega", _MISSING) if omega is _MISSING: omega = getattr(self, "_omega_laos", None) if mode in ["steady_shear", "rotation", "flow_curve"]: return fluidity_nonlocal_steady_state( X_jax, p_values["G"], p_values["tau_y"], p_values["K"], p_values["n_flow"], p_values["f_eq"], p_values["f_inf"], p_values["theta"], ) elif mode == "oscillation": return self._predict_saos_jit( X_jax, p_values["G"], p_values["f_eq"], ) elif mode in ["startup", "relaxation", "creep"]: return self._simulate_pde( X_jax, p_values, mode, gamma_dot, sigma_applied, None, ) elif mode == "laos": if gamma_0 is None or omega is None: raise ValueError("LAOS mode requires gamma_0 and omega") _, stress = self._simulate_laos_internal(X_jax, p_values, gamma_0, omega) return stress return jnp.zeros_like(X_jax)
# ========================================================================= # Prediction Interface # ========================================================================= def _predict(self, X: np.ndarray, **kwargs: Any) -> np.ndarray: """Predict based on fitted state.""" X_jax = jnp.asarray(X, dtype=jnp.float64) p = self.get_parameter_dict() # Get test_mode from kwargs or instance attribute _kw_mode = kwargs.get("test_mode") test_mode = ( _kw_mode if _kw_mode is not None else getattr(self, "_test_mode", None) ) if test_mode is None: raise ValueError("test_mode must be specified for prediction") # FL-001: Normalize aliases if test_mode == "saos": test_mode = "oscillation" if test_mode in ["steady_shear", "rotation", "flow_curve"]: result = fluidity_nonlocal_steady_state( X_jax, p["G"], p["tau_y"], p["K"], p["n_flow"], p["f_eq"], p["f_inf"], p["theta"], ) return np.array(result) elif test_mode == "oscillation": result = self._predict_saos_jit( X_jax, p["G"], p["f_eq"], ) # Convert (N,2) [G', G''] to complex G* for consistent API result = np.array(result) return result[:, 0] + 1j * result[:, 1] elif test_mode in ["startup", "relaxation", "creep"]: return self._predict_transient(X, mode=test_mode) elif test_mode == "laos": # Get gamma_0 and omega from kwargs or instance attributes gamma_0 = kwargs.get("gamma_0", self._gamma_0) omega = kwargs.get("omega", self._omega_laos) if gamma_0 is None or omega is None: raise ValueError("LAOS prediction requires gamma_0 and omega") _, stress = self._simulate_laos_internal(X_jax, p, gamma_0, omega) return np.array(stress) return np.zeros_like(X)