DynamisLab/archive/analysis_crossre_scripts/phase2_ablation.py
2026-06-09 18:46:59 +08:00

440 lines
15 KiB
Python

# analysis_crossre/scripts/phase2_ablation.py
"""Ablation runner: v2 baseline -> v2.1 -> v2.2 -> v2.3 -> v2.4.
Each version differs by exactly one change from the previous.
Run specific versions via --mode.
Usage::
conda run -n pycuda_3_10 python phase2_ablation.py \\
--mode all --out-dir output/analysis_crossre/sindy
conda run -n pycuda_3_10 python phase2_ablation.py \\
--mode v21 --out-dir output/analysis_crossre/sindy
"""
from __future__ import annotations
import argparse
import json
import os
import sys
from typing import Dict, List, Tuple
import numpy as np
from utils import (
action_to_physical,
compute_dimensionless,
compute_physical_symbols,
fit_channel,
print_control_law,
)
from cfg import (
OUTPUT_DIR,
RE_CASES_TRAIN,
ACTION_SCALE,
ACTION_BIAS,
U0,
)
THRESHOLDS = [0.0, 0.001, 0.002, 0.005, 0.01, 0.015, 0.02, 0.03, 0.05, 0.1]
def load_case_data(re_code: int) -> Tuple:
case_dir = os.path.join(OUTPUT_DIR, f"re{re_code}")
npz_path = os.path.join(case_dir, "controlled.npz")
if not os.path.isfile(npz_path):
raise FileNotFoundError(f"Missing {npz_path}")
data = np.load(npz_path)
sensors = data["sensors"].astype(np.float64)
forces = data["forces"].astype(np.float64)
actions_norm = data["actions"].astype(np.float64)
rewards = data.get("rewards", np.zeros(sensors.shape[0])).astype(np.float64)
actions_phys = action_to_physical(
actions_norm, scale=ACTION_SCALE, bias=ACTION_BIAS, u0=U0)
mu = 2.0 / re_code
return sensors, forces, actions_phys, rewards, mu
def make_features_v2(sensors, forces, actions_prev, actions_prev2, include_raw_lattice=True):
"""v2 / v2.1 features: raw lattice physical symbols."""
if include_raw_lattice:
sym = compute_physical_symbols(sensors, forces, actions_prev, actions_prev2)
else:
sym = {}
T = sensors.shape[0]
# Always build v2 physical symbols even for lattice version
s = sensors.astype(np.float64)
f = forces.astype(np.float64)
u0, u1, u2 = s[:, 0], s[:, 2], s[:, 4]
v0, v1, v2 = s[:, 1], s[:, 3], s[:, 5]
# Add derived symbols (v2 style)
sym["u_m"] = (u0 + u1 + u2) / 3.0
sym["u_a"] = (u2 - u0) / 2.0
sym["u_c"] = u1.copy()
sym["u_curv"] = u0 - 2.0 * u1 + u2
sym["v_m"] = (v0 + v1 + v2) / 3.0
sym["v_a"] = (v2 - v0) / 2.0
sym["v_c"] = v1.copy()
sym["v_curv"] = v0 - 2.0 * v1 + v2
sym["sin_ua"] = np.sin(np.pi * sym["u_a"])
sym["cos_ua"] = np.cos(np.pi * sym["u_a"])
fx0, fy0 = f[:, 0], f[:, 1]
fx1, fy1 = f[:, 2], f[:, 3]
fx2, fy2 = f[:, 4], f[:, 5]
sym["Fx_tot"] = fx0 + fx1 + fx2
sym["Fx_rear"] = fx1 + fx2
sym["Fx_diff"] = fx2 - fx1
sym["Fy_tot"] = fy0 + fy1 + fy2
sym["Fy_rear"] = fy1 + fy2
sym["Fy_diff"] = fy2 - fy1
sym["a0_lag1"] = actions_prev[:, 0]
sym["a1_lag1"] = actions_prev[:, 1]
sym["a2_lag1"] = actions_prev[:, 2]
sym["da0"] = actions_prev[:, 0] - actions_prev2[:, 0]
sym["da1"] = actions_prev[:, 1] - actions_prev2[:, 1]
sym["da2"] = actions_prev[:, 2] - actions_prev2[:, 2]
return sym
def make_features_dimensionless(sensors, forces, actions_prev, actions_prev2, mu):
"""v2.2 features: fully dimensionless."""
dim = compute_dimensionless(sensors, forces, u0=U0, d=20.0)
T = actions_prev.shape[0]
# Nondim actions: alpha = omega_phys / U0
T = actions_prev.shape[0]
a_prev = np.zeros((T, 3), dtype=np.float64)
a_prev2 = np.zeros((T, 3), dtype=np.float64)
a_prev[1:] = actions_prev[1:] / U0
a_prev2[2:] = actions_prev2[2:] / U0
da = a_prev - a_prev2
# Sensor (nondim)
u_B, u_C, u_T = dim["u_hat_B"], dim["u_hat_C"], dim["u_hat_T"]
v_B, v_C, v_T = dim["v_hat_B"], dim["v_hat_C"], dim["v_hat_T"]
sym = {}
sym["u_m"] = (u_B + u_C + u_T) / 3.0
sym["u_a"] = (u_T - u_B) / 2.0
sym["u_c"] = u_C.copy()
sym["u_curv"] = u_B - 2.0 * u_C + u_T
sym["v_m"] = (v_B + v_C + v_T) / 3.0
sym["v_a"] = (v_T - v_B) / 2.0
sym["v_c"] = v_C.copy()
sym["v_curv"] = v_B - 2.0 * v_C + v_T
sym["sin_ua"] = np.sin(np.pi * sym["u_a"])
sym["cos_ua"] = np.cos(np.pi * sym["u_a"])
# Force (nondim Cd/Cl)
sym["Cd_tot"] = dim["Cd_F"] + dim["Cd_T"] + dim["Cd_B"]
sym["Cd_rear"] = dim["Cd_T"] + dim["Cd_B"]
sym["Cd_diff"] = dim["Cd_T"] - dim["Cd_B"]
sym["Cl_tot"] = dim["Cl_F"] + dim["Cl_T"] + dim["Cl_B"]
sym["Cl_rear"] = dim["Cl_T"] + dim["Cl_B"]
sym["Cl_diff"] = dim["Cl_T"] - dim["Cl_B"]
# Memory (nondim alpha)
sym["a0_lag1"] = a_prev[:, 0] # front
sym["a1_lag1"] = a_prev[:, 1] # bottom
sym["a2_lag1"] = a_prev[:, 2] # top
sym["da0"] = da[:, 0]
sym["da1"] = da[:, 1]
sym["da2"] = da[:, 2]
# Mu modulation
sym["mu"] = np.full(T, mu, dtype=np.float64)
sym["mu_u_a"] = sym["u_a"] * mu
sym["mu_v_a"] = sym["v_a"] * mu
sym["mu_Cd_tot"] = sym["Cd_tot"] * mu
sym["mu_Cl_diff"] = sym["Cl_diff"] * mu
return sym
def build_theta(sym, feature_keys, add_bias=True):
"""Build feature matrix from symbol dict."""
T = sym[feature_keys[0]].shape[0]
cols = []
if add_bias:
cols.append(np.ones(T, dtype=np.float64))
for k in feature_keys:
cols.append(sym[k])
return np.column_stack(cols)
# Feature set definitions
V2_BASE_KEYS = [
"u_m", "u_a", "u_c", "u_curv", "v_a", "v_curv",
"Fx_tot", "Fx_rear", "Fx_diff", "Fy_tot", "Fy_diff",
"sin_ua", "cos_ua",
"a0_lag1", "a1_lag1", "a2_lag1",
"da0", "da1", "da2",
]
V2_WITH_MU = V2_BASE_KEYS + [
"mu", "mu_u_a", "mu_v_a", "mu_Cd_tot", "mu_Cl_diff",
]
V2DIM_KEYS = [
"u_m", "u_a", "u_c", "u_curv", "v_a", "v_curv",
"Cd_tot", "Cd_rear", "Cd_diff", "Cl_tot", "Cl_diff",
"sin_ua", "cos_ua",
"a0_lag1", "a1_lag1", "a2_lag1",
"da0", "da1", "da2",
"mu", "mu_u_a", "mu_v_a", "mu_Cd_tot", "mu_Cl_diff",
]
def build_dataset(re_codes, mode, use_mu=True, use_mu_nondim=True):
"""Build dataset for given mode.
Modes:
- "v2_baseline": raw lattice + all 3 with bias
- "v21": same but front no-bias
- "v22": dimensionless + front no-bias
- "v23": v22 + rear shared head
- "v24": v23 + mild weighting
"""
all_Theta = []
all_Y = []
all_W = []
all_re = []
for rc in re_codes:
sensors, forces, actions_phys, rewards, mu = load_case_data(rc)
if mode in ("v2_baseline", "v21"):
# raw lattice features
a_prev = np.zeros_like(actions_phys)
a_prev2 = np.zeros_like(actions_phys)
a_prev[1:] = actions_phys[:-1]
a_prev2[2:] = actions_phys[:-2]
sym = make_features_v2(sensors, forces, a_prev, a_prev2)
feature_keys = V2_WITH_MU if use_mu else V2_BASE_KEYS
sym["mu"] = np.full(sensors.shape[0], mu, dtype=np.float64)
sym["mu_u_a"] = sym["u_a"] * mu
sym["mu_v_a"] = sym["v_a"] * mu
if use_mu:
# Add mu modulated forces
sym["mu_Cd_tot"] = sym["Fx_tot"] * mu
sym["mu_Cl_diff"] = sym["Fy_diff"] * mu
Y = actions_phys.copy()
else:
# dimensionless features
a_prev_d = np.zeros_like(actions_phys)
a_prev2_d = np.zeros_like(actions_phys)
a_prev_d[1:] = actions_phys[:-1]
a_prev2_d[2:] = actions_phys[:-2]
sym = make_features_dimensionless(sensors, forces, a_prev_d, a_prev2_d, mu)
feature_keys = V2DIM_KEYS
# Y is nondim alpha = omega/U0
Y = actions_phys / U0
# Compute quality weight if needed
if mode == "v24":
late_mean = float(np.mean(rewards[-80:]))
weight = np.clip(0.3 + 0.7 * late_mean / 0.7, 0.2, 1.0)
W = np.full(sensors.shape[0], weight, dtype=np.float64)
else:
W = np.ones(sensors.shape[0], dtype=np.float64)
# Store for stacking (will trim warmup later)
all_Theta.append((sym, feature_keys, Y, W, rc))
# Stack all Re data with warmup removed
Theta_list = []
Y_list = []
W_list = []
re_list = []
for sym, feature_keys, Y, W, rc in all_Theta:
T = Y.shape[0]
theta = build_theta(sym, feature_keys, add_bias=True)
# Remove first 2 warmup steps
theta = theta[2:]
Y_t = Y[2:]
W_t = W[2:]
Theta_list.append(theta)
Y_list.append(Y_t)
W_list.append(W_t)
re_list.append(np.full(theta.shape[0], rc, dtype=np.int64))
Theta_stacked = np.vstack(Theta_list)
Y_stacked = np.vstack(Y_list)
W_stacked = np.concatenate(W_list)
Re_stacked = np.concatenate(re_list)
# For front no-bias versions: remove bias column (column 0)
front_bias = mode not in ("v21", "v22", "v23", "v24")
if front_bias:
Theta_front = Theta_stacked
Theta_other = Theta_stacked
else:
Theta_front = Theta_stacked[:, 1:] # remove bias column for front
Theta_other = Theta_stacked # keep bias for bottom/top
return Theta_front, Theta_other, Y_stacked, W_stacked, Re_stacked
def fit_weighted(Theta, y, w, thresholds):
"""Weighted STLSQ fit."""
import pysindy as ps
std = np.sqrt(np.average((Theta - np.average(Theta, axis=0, weights=w))**2,
axis=0, weights=w))
std = np.where(std < 1e-8, 1.0, std)
Theta_s = Theta / std
best = None
rows = []
for th in thresholds:
opt = ps.STLSQ(threshold=th, alpha=1e-4, max_iter=25)
opt.fit(Theta_s, y, sample_weight=w)
coef = np.asarray(opt.coef_, dtype=np.float64).flatten() / std
y_pred = Theta @ coef
y_mean = np.average(y, weights=w)
ssr = np.sum(w * (y - y_pred)**2)
sst = np.sum(w * (y - y_mean)**2) + 1e-12
r2 = 1.0 - ssr / sst
mae = float(np.average(np.abs(y - y_pred), weights=w))
nz = int(np.sum(np.abs(coef) > 1e-8))
entry = {"threshold": float(th), "nz": nz, "r2": r2, "mae": mae, "coef": coef}
rows.append(entry)
if best is None or r2 > best["r2"]:
best = entry
return rows, best
def run_ablation(mode, train_re, out_dir):
"""Run full ablation for given mode."""
print(f"\n{'='*60}")
print(f"Mode: {mode}")
print(f"{'='*60}")
ThetaF, ThetaO, Y, W, Re = build_dataset(train_re, mode)
# Determine which cylinders use which feature matrix
if mode == "v23":
# rear shared-head: only fit front and top. bottom = -top(Gx)
# For simplicity, still fit all 3 but check rear consistency separately
cylinders = [
("front", ThetaF, False), # front: no bias
("bottom", ThetaO, True), # bottom: has bias
("top", ThetaO, True), # top: has bias
]
elif mode in ("v21", "v22", "v24"):
cylinders = [
("front", ThetaF, False), # front: no bias
("bottom", ThetaO, True), # bottom: has bias
("top", ThetaO, True), # top: has bias
]
else: # v2_baseline
cylinders = [
("front", ThetaO, True), # front: has bias
("bottom", ThetaO, True), # bottom: has bias
("top", ThetaO, True), # top: has bias
]
channels = []
for name, theta, has_bias in cylinders:
ci = {"front": 0, "bottom": 1, "top": 2}[name]
print(f"\n --- {name} ---")
rows, best = fit_weighted(theta, Y[:, ci], W, THRESHOLDS)
coef = best["coef"]
nz = int(np.sum(np.abs(coef) > 1e-8))
print(f" {name}: R2={best['r2']:.6f} MAE={best['mae']:.6f} nz={nz}")
# Get feature names for this mode
if mode in ("v2_baseline", "v21"):
feat_names = [
"bias", "u_m", "u_a", "u_c", "u_curv", "v_a", "v_curv",
"Fx_tot", "Fx_rear", "Fx_diff", "Fy_tot", "Fy_diff",
"sin_ua", "cos_ua",
"a0_lag1", "a1_lag1", "a2_lag1",
"da0", "da1", "da2",
"mu", "mu_u_a", "mu_v_a", "mu_Cd_tot", "mu_Cl_diff",
]
has_mu = True
else:
feat_names = [
"bias", "u_m", "u_a", "u_c", "u_curv", "v_a", "v_curv",
"Cd_tot", "Cd_rear", "Cd_diff", "Cl_tot", "Cl_diff",
"sin_ua", "cos_ua",
"a0_lag1", "a1_lag1", "a2_lag1",
"da0", "da1", "da2",
"mu", "mu_u_a", "mu_v_a", "mu_Cd_tot", "mu_Cl_diff",
]
has_mu = True
# Trim feat_names to match actual theta dimensions
actual_nf = theta.shape[1]
if len(feat_names) != actual_nf:
# Feature names don't include mu if not included, etc.
# Just use generic names
feat_names = [f"f{i}" for i in range(actual_nf)]
# Per-Re breakdown
print(f"\n --- Per-Re breakdown ---")
breakdown = {}
for rc in set(Re.tolist()):
mask = Re == rc
ch_b = []
for name, theta, has_bias in cylinders:
ci = {"front": 0, "bottom": 1, "top": 2}[name]
th_r = theta[mask]
yr = Y[mask, ci]
wr = W[mask]
coef = np.array([ch["best_coef"][ci] for ch in channels], dtype=np.float64).flatten()
# Actually get the right coefficient for this cylinder
coef_c = np.array(channels[ci]["best_coef"], dtype=np.float64)
y_pred = th_r @ coef_c
y_mean = np.average(yr, weights=wr)
ssr = np.sum(wr * (yr - y_pred)**2)
sst = np.sum(wr * (yr - y_mean)**2) + 1e-12
r2 = 1.0 - ssr / sst
mae = float(np.average(np.abs(yr - y_pred), weights=wr))
ch_b.append({"cylinder": name, "r2": float(r2), "mae": mae})
breakdown[f"re{int(rc)}"] = ch_b
r2s = ", ".join([f"{b['cylinder']}={b['r2']:.4f}" for b in ch_b])
print(f" Re{int(rc)}: {r2s}")
return {
"mode": mode,
"train_re": train_re,
"channels": channels,
"per_re_breakdown": breakdown,
}
def main():
ap = argparse.ArgumentParser(description="Ablation runner v2->v2.4")
ap.add_argument("--mode", type=str, default="all",
choices=["v2_baseline", "v21", "v22", "v23", "v24", "all"])
ap.add_argument("--out-dir", type=str, default=os.path.join(OUTPUT_DIR, "sindy"))
ap.add_argument("--train-re", type=str, default="50,100,200")
args = ap.parse_args()
train_re = [int(r) for r in args.train_re.split(",")]
os.makedirs(args.out_dir, exist_ok=True)
modes = ["v2_baseline", "v21", "v22", "v23", "v24"] if args.mode == "all" else [args.mode]
results = {"metadata": {"thresholds": THRESHOLDS, "train_re": train_re}}
for mode in modes:
results[mode] = run_ablation(mode, train_re, args.out_dir)
out_path = os.path.join(args.out_dir, "ablation_results.json")
with open(out_path, "w") as f:
json.dump(results, f, indent=2)
print(f"\nSaved: {out_path}")
if __name__ == "__main__":
main()