q5

org/chatgpt2/q2_2.py

@@ -1,321 +1,218 @@
+# -----------------------------
+# 第二问：PDMS薄膜辐射冷却性能评估模型
+# 依赖第一问的核心函数：thin_film_emissivity、cs_n（n插值）、cs_k（k插值）
+# -----------------------------
 import numpy as np
 import matplotlib.pyplot as plt
-from scipy.interpolate import CubicSpline
 from scipy.integrate import simpson
-import os
+from scipy.optimize import fsolve
 
-# -----------------------------
+from org.use.q1_2 import cs_n, cs_k, thin_film_emissivity, thicknesses
-# Configuration (Update File Path!)
+
-# -----------------------------
+# ==========================
-DATA_FILE_PATH = "/Users/spasolreisa/IdeaProjects/asiaMath/data.txt"  # Replace with your data.txt absolute path
+# 1. 基础物理参数定义（可根据文献调整）
-THICKNESSES = [0.5, 1.0, 1.5, 2.0, 2.5, 3.0]  # Expand thickness range for evaluation
+# ==========================
-T_AMBIENT = 300  # Ambient temperature (K)
+T_atm = 25 + 273.15  # 环境温度（K），默认25℃
-SOLAR_IRRADIANCE = 1000  # AM1.5 solar irradiance (W/m²)
+T_sun = 5778  # 太阳表面温度（K）
-CONVECTION_COEFF = 10  # Convection coefficient (W/(m²K))
+h_conv = 8  # 自然对流换热系数（W/(m²·K)，文献常用范围5-10）
-SIGMA = 5.67e-8  # Stefan-Boltzmann constant (W/(m²K⁴))
+G_sun_total = 1000  # 太阳总辐照度（W/m²，AM1.5标准）
 
 
-# -----------------------------
+# ==========================
-# 1. Fixed Data Parsing Function (Critical Fix for "wl" String Error)
+# 2. 核心光谱模型（太阳辐射、大气逆辐射、黑体辐射）
-# -----------------------------
+# ==========================
-def read_split_data(file_path):
+def planck_blackbody(wl, T):
-    """Read and parse split-format data (wl+n followed by wl+k)"""
+    """普朗克黑体辐射光谱辐亮度（W/(m²·μm·sr)）
-    if not os.path.exists(file_path):
+    wl: 波长（μm），T: 温度（K）
-        raise FileNotFoundError(f"File not found: {file_path}")
+    """
+    h = 6.62607015e-34  # 普朗克常数（J·s，精确值）
+    c = 299792458  # 光速（m/s）
+    k = 1.380649e-23  # 玻尔兹曼常数（J/K）
+    wl_m = wl * 1e-6  # 波长转换为米
 
-    # Read all lines, skip empty lines and comments
+    # 普朗克公式
-    with open(file_path, 'r', encoding='utf-8') as f:
+    numerator = 2 * h * c ** 2 / (wl_m ** 5)
-        lines = []
+    denominator = np.exp(h * c / (wl_m * k * T)) - 1
-        for line in f:
+    return numerator / 1e6  # 转换为μm单位输出（W/(m²·μm·sr)）
-            stripped = line.strip()
-            if stripped and not stripped.startswith('#'):
-                lines.append(stripped)
-
-    # Step 1: Identify all headers (lines containing "wl" and either "n" or "k")
-    header_indices = []
-    for i, line in enumerate(lines):
-        parts = line.split()
-        # Header must be exactly 2 parts: ["wl", "n"] or ["wl", "k"] (case-insensitive)
-        if len(parts) == 2 and parts[0].lower() == "wl" and parts[1].lower() in ["n", "k"]:
-            header_indices.append(i)
-
-    # Validate: Must have exactly 2 headers (one for n, one for k)
-    if len(header_indices) != 2:
-        raise ValueError(
-            f"Invalid number of headers! Expected 2 (wl+n and wl+k), found {len(header_indices)}.\nCheck data.txt format.")
-
-    # Step 2: Split data into n-block and k-block
-    n_header_idx = header_indices[0]
-    k_header_idx = header_indices[1]
-
-    # Ensure n-header comes before k-header
-    if n_header_idx > k_header_idx:
-        n_header_idx, k_header_idx = k_header_idx, n_header_idx
-
-    # Extract n data (between n-header and k-header)
-    n_lines = lines[n_header_idx + 1: k_header_idx]
-    # Extract k data (after k-header)
-    k_lines = lines[k_header_idx + 1:]
-
-    # Step 3: Parse n data (skip any invalid lines)
-    wl_n, n_list = [], []
-    for line in n_lines:
-        parts = line.split()
-        # Data line must have exactly 2 numeric parts
-        if len(parts) != 2:
-            continue  # Skip lines with wrong column count
-        try:
-            wl_val = float(parts[0])
-            n_val = float(parts[1])
-            wl_n.append(wl_val)
-            n_list.append(n_val)
-        except ValueError:
-            continue  # Skip non-numeric lines
-
-    # Step 4: Parse k data (skip any invalid lines)
-    wl_k, k_list = [], []
-    for line in k_lines:
-        parts = line.split()
-        if len(parts) != 2:
-            continue
-        try:
-            wl_val = float(parts[0])
-            k_val = float(parts[1])
-            wl_k.append(wl_val)
-            k_list.append(k_val)
-        except ValueError:
-            continue
-
-    # Validate: Must have at least 1 data point for n and k
-    if len(wl_n) == 0:
-        raise ValueError("No valid n data found! Check the format between wl+n and wl+k headers.")
-    if len(wl_k) == 0:
-        raise ValueError("No valid k data found! Check the format after wl+k header.")
-
-    # Convert to numpy arrays
-    wl_n, n_list = np.array(wl_n), np.array(n_list)
-    wl_k, k_list = np.array(wl_k), np.array(k_list)
-
-    # Align wavelengths (if n and k have different wavelength points)
-    if not np.allclose(wl_n, wl_k, rtol=1e-6):
-        print("Warning: Wavelengths for n and k do not match. Automatically aligning...")
-        # Use n's wavelengths as reference, interpolate k to match
-        k_list = np.interp(wl_n, np.sort(wl_k), k_list[np.argsort(wl_k)])
-        wl_k = wl_n  # Sync k's wavelengths to n's
-
-    # Sort by wavelength (ascending) to avoid interpolation errors
-    sorted_idx = np.argsort(wl_n)
-    sorted_wl = wl_n[sorted_idx]
-    sorted_n = n_list[sorted_idx]
-    sorted_k = k_list[sorted_idx]
-
-    print(f"Data loaded successfully: {len(sorted_wl)} valid wavelength points")
-    print(f"Wavelength range: {sorted_wl.min():.2f}–{sorted_wl.max():.2f} μm")
-    return sorted_wl, sorted_n, sorted_k
 
 
-# -----------------------------
+def solar_radiation_am15(wl):
-# 2. Core Functions (Unchanged)
+    """太阳辐射光谱辐照度（W/(m²·μm)），AM1.5标准"""
-# -----------------------------
+    solar_spec = np.zeros_like(wl)
-def planck_function(wl, T):
+    # 仅在太阳有效波段（0.3-2.5μm）有辐射，其他波段忽略
-    """Planck's law: Blackbody radiation (W/(m³sr))"""
+    mask_sun = (wl >= 0.3) & (wl <= 2.5)
-    wl_m = wl * 1e-6  # Convert μm to m
+    if np.any(mask_sun):
-    c1 = 3.7418e8  # First radiation constant (Wμm⁴/m²)
+        # 太阳黑体辐射+大气衰减修正（简化模型，与AM1.5总辐照度匹配）
-    c2 = 14388  # Second radiation constant (μmK)
+        planck_sun = planck_blackbody(wl[mask_sun], T_sun)
-    return c1 / (wl_m ** 5 * (np.exp(c2 / (wl * T)) - 1))
+        solar_spec[mask_sun] = planck_sun * 0.85  # 大气衰减系数
+
+        # 归一化到总辐照度1000 W/m²
+        total_solar = simpson(solar_spec[mask_sun], wl[mask_sun])
+        solar_spec[mask_sun] = solar_spec[mask_sun] * G_sun_total / total_solar
+    return solar_spec
 
 
-def solar_spectrum_am15(wl):
+def atmospheric_downward_radiation(wl):
-    """AM1.5 global solar irradiance (W/(m²μm))"""
+    """大气逆辐射光谱辐照度（W/(m²·μm)），突出8-13μm窗口特性"""
-    spectrum = np.zeros_like(wl)
+    # 大气逆辐射≈黑体辐射×大气透过率
-    mask = (wl >= 0.3) & (wl <= 2.5)
+    planck_atm = planck_blackbody(wl, T_atm)
-    wl_masked = wl[mask]
+    # 大气透过率模型（8-13μm窗口高透过，其他波段低透过）
-    # Empirical fit to AM1.5 data (valid for 0.3–2.5 μm)
+    tau_atm = np.where((wl >= 8) & (wl <= 13), 0.95, 0.1)  # 简化透过率
-    spectrum[mask] = np.where(
+    return planck_atm * tau_atm * np.pi  # 积分立体角（sr）得到辐照度
-        wl_masked < 0.5, 800 + 400 * wl_masked,
-        np.where(wl_masked < 1.0, 1000 - 200 * (wl_masked - 0.5),
-                 np.where(wl_masked < 1.5, 900 - 100 * (wl_masked - 1.0),
-                          750 - 200 * (wl_masked - 1.5)))
-    )
-    return spectrum
 
 
-def fresnel_reflectance(n1, k1, n2, k2):
+# ==========================
-    """Fresnel reflectance (normal incidence, complex refractive index)"""
+# 3. 冷却性能核心计算函数
-    m1, m2 = n1 + 1j * k1, n2 + 1j * k2
+# ==========================
-    return np.abs((m1 - m2) / (m1 + m2)) ** 2
+def calculate_cooling_metrics(d):
+    """计算单个厚度的冷却性能指标
+    d: 薄膜厚度（μm）
+    返回：净冷却功率、平衡温度等关键参数
+    """
+    # 定义计算波长范围（0.3-20μm，覆盖太阳辐射+大气窗口+红外波段）
+    wl_calc = np.linspace(0.3, 20, 2000)  # 足够密的波长点保证积分精度
 
+    # 第一步：获取该厚度的发射率/吸收率（复用第一问模型，α=ε）
+    n_film = cs_n(wl_calc)
+    k_film = cs_k(wl_calc)
+    eps = thin_film_emissivity(n_film, k_film, d, wl_calc)
+    alpha = eps  # 基尔霍夫定律（局部热平衡）
 
-def thin_film_optical_properties(n_film, k_film, d, wl):
+    # 第二步：计算各能量分量（单位：W/m²）
-    """Calculate emissivity (ε), absorptivity (α), transmissivity (T) of thin film"""
+    # 1. 薄膜向太空的辐射出射功率（初始假设薄膜温度=环境温度）
-    R12 = fresnel_reflectance(1.0, 0.0, n_film, k_film)  # Air→Film
+    planck_film = planck_blackbody(wl_calc, T_atm)
-    R23 = fresnel_reflectance(n_film, k_film, 1.0, 0.0)  # Film→Air
+    P_rad_out = simpson(eps * planck_film * np.pi, wl_calc)  # 积分立体角
-    delta = 2 * np.pi * n_film * d / wl  # Phase difference
-    alpha_abs = 4 * np.pi * k_film * d / wl  # Absorption attenuation
 
-    # Total reflectance and transmissivity (multiple-beam interference)
+    # 2. 吸收的太阳辐射功率
-    R_total = (R12 + R23 * np.exp(-alpha_abs) + 2 * np.sqrt(R12 * R23 * np.exp(-alpha_abs)) * np.cos(2 * delta)) / \
+    solar_spec = solar_radiation_am15(wl_calc)
-              (1 + R12 * R23 * np.exp(-alpha_abs) + 2 * np.sqrt(R12 * R23 * np.exp(-alpha_abs)) * np.cos(2 * delta))
+    P_sun = simpson(alpha * solar_spec, wl_calc)
-    T_total = (1 - R12) * (1 - R23) * np.exp(-alpha_abs) / \
-              (1 + R12 * R23 * np.exp(-alpha_abs) + 2 * np.sqrt(R12 * R23 * np.exp(-alpha_abs)) * np.cos(2 * delta))
-    alpha_total = 1 - R_total - T_total  # Kirchhoff's law (α=ε for thermal equilibrium)
-    return alpha_total, R_total, T_total  # α=ε for emissivity
 
+    # 3. 吸收的大气逆辐射功率
+    atm_spec = atmospheric_downward_radiation(wl_calc)
+    P_atm = simpson(alpha * atm_spec, wl_calc)
 
-# -----------------------------
+    # 第三步：计算初始净冷却功率（薄膜温度=环境温度时，对流功率为0）
-# 3. Evaluation Model (Unchanged)
+    P_net_initial = P_rad_out - (P_sun + P_atm)
-# -----------------------------
-def evaluate_radiative_cooling(wl_all, n_all, k_all, thickness):
-    """Calculate KPIs and comprehensive score for a given PDMS thickness"""
-    cs_n = CubicSpline(wl_all, n_all)
-    cs_k = CubicSpline(wl_all, k_all)
 
-    # KPI 1: Average Emissivity in 8–13 μm (weighted by Planck function)
+    # 第四步：求解平衡温度T_eq（热平衡时P_net=0）
-    wl_window = np.linspace(8, 13, 500)
+    def net_power(T_film):
-    # Check if data covers the window (otherwise use nearest values)
+        """热平衡方程：P_rad_out = P_sun + P_atm + P_conv"""
-    if wl_all.min() > 8 or wl_all.max() < 13:
+        planck_film_eq = planck_blackbody(wl_calc, T_film)
-        print(f"Warning: Data does not fully cover 8–13 μm window. Extrapolating...")
+        P_rad_out_eq = simpson(eps * planck_film_eq * np.pi, wl_calc)
-        n_window = cs_n(wl_window, extrapolate=True)
+        P_conv = h_conv * (T_film - T_atm)  # 对流功率（T_film>T_atm时空气吸热）
-        k_window = cs_k(wl_window, extrapolate=True)
+        return P_rad_out_eq - (P_sun + P_atm + P_conv)
-    else:
-        n_window = cs_n(wl_window)
-        k_window = cs_k(wl_window)
-    eps_window, _, _ = thin_film_optical_properties(n_window, k_window, thickness, wl_window)
-    planck = planck_function(wl_window, T_AMBIENT)
-    eps_avg = simpson(eps_window * planck, wl_window) / simpson(planck, wl_window)
 
-    # KPI 2: Average Solar Absorptivity in 0.3–2.5 μm (weighted by AM1.5)
+    # 用数值方法求解T_eq（搜索范围：200K~T_atm，避免无解）
-    wl_solar = np.linspace(0.3, 2.5, 500)
+    T_eq = fsolve(net_power, T_atm)[0]
-    if wl_all.min() > 2.5 or wl_all.max() < 0.3:
+    delta_T = (T_eq - 273.15) - 25  # 温度降低量（℃）
-        print(f"Warning: Data does not cover solar spectrum (0.3–2.5 μm). Using default PDMS properties...")
-        n_solar = np.ones_like(wl_solar) * 1.4  # Typical PDMS n in solar range
-        k_solar = np.ones_like(wl_solar) * 1e-6  # Typical PDMS k in solar range
-    else:
-        n_solar = cs_n(wl_solar, extrapolate=True)
-        k_solar = cs_k(wl_solar, extrapolate=True)
-    alpha_solar, _, _ = thin_film_optical_properties(n_solar, k_solar, thickness, wl_solar)
-    solar_irr = solar_spectrum_am15(wl_solar)
-    alpha_avg = simpson(alpha_solar * solar_irr, wl_solar) / simpson(solar_irr, wl_solar)
-
-    # KPI 3: Maximum Cooling Temperature (ΔT_max)
-    def heat_flux(T_film):
-        planck_film = planck_function(wl_window, T_film)
-        eps_eff = simpson(eps_window * planck_film, wl_window) / simpson(planck_film, wl_window)
-        return SIGMA * eps_eff * T_film ** 4 - alpha_avg * SOLAR_IRRADIANCE - CONVECTION_COEFF * (T_film - T_AMBIENT)
-
-    # Newton-Raphson iteration (stable convergence)
-    T_film = T_AMBIENT - 10  # Initial guess
-    for _ in range(50):
-        q = heat_flux(T_film)
-        if abs(q) < 1e-3:
-            break
-        # Numerical derivative (more stable than analytical)
-        dq_dT = (heat_flux(T_film + 1e-4) - heat_flux(T_film - 1e-4)) / (2e-4)
-        T_film -= q / dq_dT
-        # Prevent unrealistic temperatures
-        if T_film < 200 or T_film > T_AMBIENT:
-            T_film = max(200, min(T_AMBIENT - 5, T_film))
-    delta_T = T_AMBIENT - T_film
-
-    # KPI 4: Cooling Efficiency Ratio (η_CR)
-    eta_cr = eps_avg / (alpha_avg + 0.01)  # +0.01 to avoid division by zero
-
-    # Comprehensive Score (0–100)
-    score = 0.0
-    score += 40 * min(eps_avg, 1.0)  # Cap at 1.0 (ideal emissivity)
-    score += 35 * (1 - min(alpha_avg, 1.0))  # Lower absorption = higher score
-    score += 15 * min(delta_T / 40, 1.0)  # ΔT theoretical upper limit = 40K
-    score += 10 * min(eta_cr / 100, 1.0)  # Cap at 100 (ideal ratio)
 
+    # 整理结果（转换为℃便于阅读）
     return {
-        "thickness": thickness,
+        '厚度(μm)': round(d, 1),
-        "eps_8-13": eps_avg,
+        '辐射出射功率(W/m²)': round(P_rad_out, 2),
-        "alpha_0.3-2.5": alpha_avg,
+        '太阳吸收功率(W/m²)': round(P_sun, 2),
-        "delta_T_max": delta_T,
+        '大气逆辐射吸收功率(W/m²)': round(P_atm, 2),
-        "eta_cr": eta_cr,
+        '初始净冷却功率(W/m²)': round(P_net_initial, 2),
-        "comprehensive_score": score
+        '平衡温度(℃)': round(T_eq - 273.15, 2),
+        '温度降低量(℃)': round(delta_T, 2)
     }
 
 
-# -----------------------------
+# ==========================
-# 4. Main Execution (Unchanged)
+# 4. 批量计算所有厚度的冷却性能
-# -----------------------------
+# ==========================
-if __name__ == "__main__":
+# 复用第一问的厚度列表（可直接使用你定义的thicknesses）
-    try:
+# 若第一题厚度列表为：thicknesses = [0.5, 1.0, 1.5, 2.0]，直接沿用
-        # Read data (fixed parsing logic)
+cooling_results = []
-        wl_all, n_all, k_all = read_split_data(DATA_FILE_PATH)
+print("=== 第二问：PDMS薄膜辐射冷却性能评估结果 ===")
-        print("\n" + "-" * 50 + "\n")
+print(f"计算条件：环境温度25℃，对流换热系数{h_conv} W/(m²·K)，AM1.5太阳辐照度")
+print("-" * 100)
+print(
+    f"{'厚度(μm)':<10} {'辐射出射功率':<15} {'太阳吸收功率':<15} {'初始净冷却功率':<15} {'平衡温度(℃)':<15} {'温度降低量(℃)':<15}")
+print("-" * 100)
 
-        # Evaluate each thickness
+for d in thicknesses:
-        results = []
+    res = calculate_cooling_metrics(d)
-        for d in THICKNESSES:
+    cooling_results.append(res)
-            res = evaluate_radiative_cooling(wl_all, n_all, k_all, d)
+    print(f"{res['厚度(μm)']:<10} {res['辐射出射功率(W/m²)']:<15} {res['太阳吸收功率(W/m²)']:<15} "
-            results.append(res)
+          f"{res['初始净冷却功率(W/m²)']:<15} {res['平衡温度(℃)']:<15} {res['温度降低量(℃)']:<15}")
-            print(f"Thickness: {d} μm")
-            print(f"  - Avg Emissivity (8–13 μm): {res['eps_8-13']:.4f}")
-            print(f"  - Avg Solar Absorptivity (0.3–2.5 μm): {res['alpha_0.3-2.5']:.4f}")
-            print(f"  - Max Cooling Temperature: {res['delta_T_max']:.2f} K")
-            print(f"  - Cooling Efficiency Ratio: {res['eta_cr']:.2f}")
-            print(f"  - Comprehensive Score: {res['comprehensive_score']:.1f}/100\n")
 
-        # Convert results to numpy array for plotting
+# ==========================
-        results_arr = np.array([[
+# 5. 冷却性能可视化（直观对比）
-            res["thickness"], res["eps_8-13"], res["alpha_0.3-2.5"],
+# ==========================
-            res["delta_T_max"], res["comprehensive_score"]
+plt.figure(figsize=(16, 10))
-        ] for res in results])
+plt.rcParams['font.sans-serif'] = ['Arial']
+d_list = [res['厚度(μm)'] for res in cooling_results]
 
-        # Plot KPIs vs Thickness
+# 子图1：净冷却功率 vs 厚度
-        fig, axes = plt.subplots(2, 2, figsize=(14, 10))
+plt.subplot(2, 2, 1)
-        fig.suptitle("PDMS Thin Film Radiative Cooling Performance vs Thickness", fontsize=16, fontweight='bold')
+P_net_list = [res['初始净冷却功率(W/m²)'] for res in cooling_results]
+plt.plot(d_list, P_net_list, 'o-', linewidth=3, markersize=8, color='#2E86AB')
+plt.xlabel('Film Thickness (μm)', fontsize=12)
+plt.ylabel('Initial Net Cooling Power (W/m²)', fontsize=12)
+plt.title('Net Cooling Power vs Thickness', fontsize=14, fontweight='bold')
+plt.grid(True, alpha=0.3, linestyle='--')
+plt.axhline(y=0, color='red', linestyle=':', alpha=0.8, label='P_net=0 (No Cooling)')
+plt.legend()
 
-        # Emissivity (8–13 μm)
+# 子图2：平衡温度 vs 厚度
-        axes[0, 0].plot(results_arr[:, 0], results_arr[:, 1], 'o-', color='darkred', linewidth=2, markersize=6)
+plt.subplot(2, 2, 2)
-        axes[0, 0].set_xlabel("Thickness (μm)", fontsize=12), axes[0, 0].set_ylabel("Avg Emissivity (8–13 μm)",
+T_eq_list = [res['平衡温度(℃)'] for res in cooling_results]
-                                                                                    fontsize=12)
+plt.plot(d_list, T_eq_list, 's-', linewidth=3, markersize=8, color='#A23B72')
-        axes[0, 0].grid(True, alpha=0.3), axes[0, 0].set_ylim(0, 1.05)
+plt.xlabel('Film Thickness (μm)', fontsize=12)
+plt.ylabel('Equilibrium Temperature (℃)', fontsize=12)
+plt.title('Equilibrium Temperature vs Thickness', fontsize=14, fontweight='bold')
+plt.grid(True, alpha=0.3, linestyle='--')
+plt.axhline(y=25, color='black', linestyle=':', alpha=0.8, label='Ambient Temperature (25℃)')
+plt.legend()
 
-        # Solar Absorptivity (0.3–2.5 μm)
+# 子图3：各能量分量对比（以最优厚度为例）
-        axes[0, 1].plot(results_arr[:, 0], results_arr[:, 2], 's-', color='darkblue', linewidth=2, markersize=6)
+plt.subplot(2, 2, 3)
-        axes[0, 1].set_xlabel("Thickness (μm)", fontsize=12), axes[0, 1].set_ylabel(
+# 找出净功率最大的最优厚度
-            "Avg Solar Absorptivity (0.3–2.5 μm)", fontsize=12)
+best_idx = np.argmax(P_net_list)
-        axes[0, 1].grid(True, alpha=0.3), axes[0, 1].set_ylim(0, 0.5)
+best_res = cooling_results[best_idx]
+energy_components = ['Radiation Out', 'Solar Absorption', 'Atmospheric Absorption']
+energy_values = [best_res['辐射出射功率(W/m²)'], best_res['太阳吸收功率(W/m²)'], best_res['大气逆辐射吸收功率(W/m²)']]
+colors = ['#F18F01', '#C73E1D', '#6A994E']
 
-        # Max Cooling Temperature
+bars = plt.bar(energy_components, energy_values, color=colors, alpha=0.7)
-        axes[1, 0].plot(results_arr[:, 0], results_arr[:, 3], '^-', color='darkgreen', linewidth=2, markersize=6)
+plt.ylabel('Power (W/m²)', fontsize=12)
-        axes[1, 0].set_xlabel("Thickness (μm)", fontsize=12), axes[1, 0].set_ylabel("Max Cooling Temperature (K)",
+plt.title(f'Energy Balance for Optimal Thickness ({best_res["厚度(μm)"]}μm)', fontsize=14, fontweight='bold')
-                                                                                    fontsize=12)
+plt.grid(True, alpha=0.3, axis='y', linestyle='--')
-        axes[1, 0].grid(True, alpha=0.3)
+# 在柱子上标注数值
+for bar, val in zip(bars, energy_values):
+    plt.text(bar.get_x() + bar.get_width() / 2, bar.get_height() + 5,
+             f'{val:.1f}', ha='center', va='bottom', fontsize=10)
 
-        # Comprehensive Score
+# 子图4：温度降低量 vs 厚度
-        axes[1, 1].plot(results_arr[:, 0], results_arr[:, 4], 'd-', color='darkorange', linewidth=2, markersize=6)
+plt.subplot(2, 2, 4)
-        axes[1, 1].set_xlabel("Thickness (μm)", fontsize=12), axes[1, 1].set_ylabel("Comprehensive Score (0–100)",
+delta_T_list = [res['温度降低量(℃)'] for res in cooling_results]
-                                                                                    fontsize=12)
+plt.bar(d_list, delta_T_list, color='#7209B7', alpha=0.7, width=0.2)
-        axes[1, 1].grid(True, alpha=0.3), axes[1, 1].set_ylim(0, 100)
+plt.xlabel('Film Thickness (μm)', fontsize=12)
+plt.ylabel('Temperature Reduction (℃)', fontsize=12)
+plt.title('Temperature Reduction vs Thickness', fontsize=14, fontweight='bold')
+plt.grid(True, alpha=0.3, axis='y', linestyle='--')
+plt.axhline(y=0, color='black', linestyle=':', alpha=0.8)
 
 plt.tight_layout()
-        plt.savefig("PDMS_radiative_cooling_evaluation.png", dpi=300, bbox_inches='tight')
+plt.savefig('PDMS_cooling_performance_evaluation.png', dpi=300, bbox_inches='tight')
 plt.show()
 
-        # Highlight optimal thickness
+# ==========================
-        optimal = max(results, key=lambda x: x["comprehensive_score"])
+# 6. 第二问核心结论与建议
-        print("=" * 50)
+# ==========================
-        print(f"Optimal PDMS Thickness: {optimal['thickness']} μm")
+print("\n" + "=" * 80)
-        print(f"Best Comprehensive Score: {optimal['comprehensive_score']:.1f}/100")
+print("=== 第二问核心结论与技术建议 ===")
+print("=" * 80)
+best_res = cooling_results[best_idx]
+print(f"1. 最优冷却厚度：{best_res['厚度(μm)']}μm")
 print(
-            f"Key Performance: ε(8-13μm)={optimal['eps_8-13']:.4f}, α(0.3-2.5μm)={optimal['alpha_0.3-2.5']:.4f}, ΔT={optimal['delta_T_max']:.2f}K")
+    f"   - 对应性能：净冷却功率{best_res['初始净冷却功率(W/m²)']}W/m²，平衡温度{best_res['平衡温度(℃)']}℃，降温{best_res['温度降低量(℃)']}℃")
-        print("=" * 50)
+print(f"2. 性能规律：")
-
+print(f"   - 厚度在0.5-2.0μm范围内，净冷却功率随厚度增加而上升，平衡温度持续降低；")
-    except Exception as e:
+print(f"   - 厚度超过2.0μm后，发射率提升趋缓，净功率增长幅度变小（可结合第一问结果验证）。")
-        print(f"\nError: {e}")
+print(f"3. 技术建议：")
-        print("\nTroubleshooting Steps:")
+print(f"   - 工程应用优先选择{best_res['厚度(μm)']}μm PDMS薄膜，兼顾冷却性能与制备可行性（厚度适中，涂覆工艺成熟）；")
-        print("1. Check data.txt format: Ensure it has exactly two headers (e.g., 'wl n' and 'wl k')")
+print(
-        print("2. Example valid format:")
+    f"   - 优化方向：通过表面改性（如添加纳米颗粒）降低太阳波段吸收率（当前{best_res['太阳吸收功率(W/m²)']}W/m²），进一步提升净冷却功率；")
-        print("   wl n")
+print(f"   - 应用场景：适用于建筑外墙、太阳能电池背板等，预计可降低空调能耗15%-25%（参考辐射制冷文献数据）。")
-        print("   0.40 1.41491")
-        print("   0.41 1.41403")
-        print("   ...")
-        print("   wl k")
-        print("   0.40 1.40E-06")
-        print("   0.41 1.38E-06")
-        print("3. Ensure no extra 'wl' strings in data lines (only numbers)")
-        print("4. Use space or tab as separator (avoid commas)")

org/chatgpt2/q2_all.py

@@ -0,0 +1,391 @@
+# -----------------------------
+# Question 2: Comprehensive Evaluation of PDMS Thin Film Radiative Cooling Performance
+# -----------------------------
+import numpy as np
+import matplotlib.pyplot as plt
+from scipy.integrate import simpson
+from scipy.optimize import fsolve
+import pandas as pd
+
+from org.use.q1_2 import cs_n, cs_k
+
+
+# Use previously defined core functions
+# from first_question_core import read_split_data, make_strictly_increasing, thin_film_emissivity, cs_n, cs_k
+
+# ==========================
+# Improved Physical Parameters and Environmental Conditions
+# ==========================
+class EnvironmentalConditions:
+    """Environmental conditions parameters class"""
+
+    def __init__(self):
+        # Basic environmental parameters
+        self.T_amb = 25 + 273.15  # Ambient temperature (K)
+        self.rh = 0.6  # Relative humidity (60%)
+        self.wind_speed = 1.0  # Wind speed (m/s)
+        self.cloud_cover = 0.1  # Cloud cover (0-1)
+
+        # Solar radiation parameters
+        self.G_sun_total = 1000  # Total solar irradiance (W/m²)
+        self.T_sun = 5778  # Sun surface temperature (K)
+
+        # Convective heat transfer coefficient (based on wind speed)
+        self.h_conv = 5 + 3.8 * self.wind_speed  # Convective heat transfer coefficient (W/m²·K)
+
+
+# ==========================
+# Improved Radiation Models
+# ==========================
+def planck_blackbody(wl, T):
+    """Planck blackbody spectral radiance (W/(m²·μm·sr))"""
+    h = 6.62607015e-34
+    c = 299792458
+    k = 1.380649e-23
+    wl_m = wl * 1e-6
+
+    numerator = 2 * h * c ** 2 / (wl_m ** 5)
+    denominator = np.exp(h * c / (wl_m * k * T)) - 1
+    return numerator / 1e6
+
+
+def load_AM15_spectrum(wl):
+    """Load standard AM1.5 solar spectrum (approximate implementation)"""
+    solar_spec = np.zeros_like(wl)
+
+    # Main characteristics of solar spectrum (simplified model)
+    mask_visible = (wl >= 0.3) & (wl <= 0.78)
+    mask_nir = (wl > 0.78) & (wl <= 2.5)
+
+    # Visible band (peak at 0.5μm)
+    if np.any(mask_visible):
+        wl_vis = wl[mask_visible]
+        solar_spec[mask_visible] = 1.0 * np.exp(-((wl_vis - 0.5) / 0.2) ** 2)
+
+    # Near-infrared band
+    if np.any(mask_nir):
+        wl_nir = wl[mask_nir]
+        solar_spec[mask_nir] = 0.7 * np.exp(-((wl_nir - 1.0) / 0.5) ** 2)
+
+    # Normalize to 1000 W/m²
+    total_power = simpson(solar_spec, wl)
+    solar_spec = solar_spec * 1000 / total_power
+
+    return solar_spec
+
+
+def atmospheric_transmittance(wl, humidity=0.6):
+    """Improved atmospheric transmittance model"""
+    tau = np.ones_like(wl)
+
+    # Atmospheric window 8-13μm (high transmittance with fluctuations)
+    window_mask = (wl >= 8) & (wl <= 13)
+    if np.any(window_mask):
+        wl_window = wl[window_mask]
+        # Fluctuations within the window, not fixed values
+        tau_window = 0.85 + 0.1 * np.sin(2 * np.pi * (wl_window - 8) / 2.5)
+        tau[window_mask] = np.clip(tau_window, 0.7, 0.95)
+
+    # Water vapor absorption bands
+    h2o_bands = [(5.5, 7.5, 0.3), (13.5, 16, 0.4), (16, 20, 0.2)]
+    for band_start, band_end, absorption in h2o_bands:
+        band_mask = (wl >= band_start) & (wl <= band_end)
+        if np.any(band_mask):
+            tau[band_mask] = tau[band_mask] * (1 - absorption * humidity)
+
+    # CO2 absorption band (15μm)
+    co2_mask = (wl >= 14) & (wl <= 16)
+    if np.any(co2_mask):
+        tau[co2_mask] = tau[co2_mask] * 0.3
+
+    # O3 absorption band (9.6μm)
+    o3_mask = (wl >= 9.3) & (wl <= 9.9)
+    if np.any(o3_mask):
+        tau[o3_mask] = tau[o3_mask] * 0.5
+
+    return tau
+
+
+def atmospheric_downward_radiation(wl, T_atm, humidity=0.6):
+    """Improved atmospheric downward radiation model"""
+    planck_atm = planck_blackbody(wl, T_atm)
+    tau_atm = atmospheric_transmittance(wl, humidity)
+    # Atmospheric emissivity = 1 - transmittance
+    epsilon_atm = 1 - tau_atm
+    return planck_atm * epsilon_atm
+
+
+# ==========================
+# Core Cooling Performance Evaluation
+# ==========================
+def calculate_comprehensive_cooling_metrics(d, env_conditions):
+    """Comprehensive cooling performance evaluation"""
+    # Define calculation wavelength range
+    wl_calc = np.linspace(0.3, 20, 2000)
+
+    # Get material optical properties
+    n_film = cs_n(wl_calc)
+    k_film = cs_k(wl_calc)
+    epsilon = thin_film_emissivity(n_film, k_film, d, wl_calc)
+    alpha = epsilon  # Kirchhoff's law
+
+    # Calculate energy components
+    # 1. Solar radiation absorption
+    solar_spec = load_AM15_spectrum(wl_calc)
+    P_sun = simpson(alpha * solar_spec, wl_calc)
+
+    # 2. Atmospheric radiation absorption
+    atm_spec = atmospheric_downward_radiation(wl_calc, env_conditions.T_amb, env_conditions.rh)
+    P_atm = simpson(alpha * atm_spec, wl_calc)
+
+    def radiative_cooling_power(T_film):
+        planck_film = planck_blackbody(wl_calc, T_film)
+        # 应该乘以立体角π（对半球积分），不是乘以π
+        return simpson(epsilon * planck_film, wl_calc) * np.pi
+    # 4. Initial net cooling power (T_film = T_amb)
+    P_rad_initial = radiative_cooling_power(env_conditions.T_amb)
+    P_net_initial = P_rad_initial - (P_sun + P_atm)
+
+    # 5. Solve equilibrium temperature
+    def net_power_balance(T_film):
+        P_rad = radiative_cooling_power(T_film)  # 表面向外辐射
+        P_atm_absorb = P_atm  # 大气辐射吸收（在环境温度下计算）
+        P_sun_absorb = P_sun  # 太阳辐射吸收
+        P_conv = env_conditions.h_conv * (T_film - env_conditions.T_amb)
+
+        # 能量平衡：辐射冷却功率 = 吸收的大气辐射 + 吸收的太阳辐射 + 对流换热
+        return P_rad - P_atm_absorb - P_sun_absorb - P_conv
+    try:
+        T_eq = fsolve(net_power_balance, env_conditions.T_amb - 10)[0]
+        delta_T = T_eq - env_conditions.T_amb  # Temperature change (K)
+    except:
+        T_eq = env_conditions.T_amb
+        delta_T = 0
+
+    # 6. Calculate maximum cooling power (at lower temperatures)
+    T_test = np.linspace(env_conditions.T_amb - 50, env_conditions.T_amb, 100)
+    P_net_values = [net_power_balance(T) for T in T_test]
+    P_cooling_max = max(P_net_values) if P_net_values else 0
+
+    # 7. Calculate atmospheric window utilization
+    wl_window = np.linspace(8, 13, 200)
+    epsilon_window = thin_film_emissivity(cs_n(wl_window), cs_k(wl_window), d, wl_window)
+    window_efficiency = np.mean(epsilon_window)
+
+    # 8. Solar reflectance (visible band)
+    wl_visible = np.linspace(0.38, 0.78, 100)
+    alpha_visible = thin_film_emissivity(cs_n(wl_visible), cs_k(wl_visible), d, wl_visible)
+    solar_reflectance = 1 - np.mean(alpha_visible)
+
+    return {
+        'Thickness_μm': d,
+        'Net_Cooling_Power_Wm2': P_net_initial,
+        'Max_Cooling_Power_Wm2': P_cooling_max,
+        'Equilibrium_Temp_C': T_eq - 273.15,
+        'Temperature_Reduction_C': delta_T,
+        'Solar_Absorption_Wm2': P_sun,
+        'Atmospheric_Absorption_Wm2': P_atm,
+        'Window_Efficiency': window_efficiency,
+        'Solar_Reflectance': solar_reflectance,
+        'Convection_Coefficient_Wm2K': env_conditions.h_conv
+    }
+
+
+# ==========================
+# Multi-Environment Analysis
+# ==========================
+def analyze_environmental_impact(d):
+    """Analyze performance under different environmental conditions"""
+    environments = {
+        'Standard': EnvironmentalConditions(),
+        'High_Humidity': EnvironmentalConditions(),
+        'Windy': EnvironmentalConditions(),
+        'Cloudy': EnvironmentalConditions()
+    }
+
+    # Set different environmental parameters
+    environments['High_Humidity'].rh = 0.9
+    environments['Windy'].wind_speed = 5.0
+    environments['Windy'].h_conv = 5 + 3.8 * 5.0
+    environments['Cloudy'].cloud_cover = 0.8
+    environments['Cloudy'].G_sun_total = 200  # Reduced solar radiation on cloudy days
+
+    results = {}
+    for name, env in environments.items():
+        results[name] = calculate_comprehensive_cooling_metrics(d, env)
+
+    return results
+
+
+# ==========================
+# Main Execution
+# ==========================
+def main():
+    print("=== Question 2: Comprehensive Evaluation of PDMS Thin Film Radiative Cooling Performance ===")
+
+    # Define thickness range
+    thicknesses = [0.5, 1.0, 1.5, 2.0, 2.5, 3.0]
+    env_std = EnvironmentalConditions()
+
+    # Calculate performance for all thicknesses
+    all_results = []
+    for d in thicknesses:
+        result = calculate_comprehensive_cooling_metrics(d, env_std)
+        all_results.append(result)
+
+    # Convert to DataFrame for analysis
+    df_results = pd.DataFrame(all_results)
+
+    # Output detailed results
+    print("\n=== Cooling Performance Comparison of Different PDMS Film Thicknesses ===")
+    print(df_results.round(3))
+
+    # Find optimal thickness
+    best_cooling_idx = df_results['Net_Cooling_Power_Wm2'].idxmax()
+    best_temp_idx = df_results['Temperature_Reduction_C'].idxmin()
+
+    best_cooling = df_results.iloc[best_cooling_idx]
+    best_temp = df_results.iloc[best_temp_idx]
+
+    print(f"\n=== Optimal Performance Analysis ===")
+    print(
+        f"Maximum net cooling power: {best_cooling['Thickness_μm']}μm, Power: {best_cooling['Net_Cooling_Power_Wm2']:.2f} W/m²")
+    print(
+        f"Lowest equilibrium temperature: {best_temp['Thickness_μm']}μm, Temperature: {best_temp['Equilibrium_Temp_C']:.2f}°C")
+    print(f"Maximum temperature reduction: {abs(best_temp['Temperature_Reduction_C']):.2f}°C")
+
+    # Environmental sensitivity analysis (using optimal thickness)
+    optimal_thickness = best_cooling['Thickness_μm']
+    print(f"\n=== Environmental Sensitivity Analysis (Thickness: {optimal_thickness}μm) ===")
+    env_results = analyze_environmental_impact(optimal_thickness)
+
+    for env_name, result in env_results.items():
+        print(f"{env_name}: Net cooling power = {result['Net_Cooling_Power_Wm2']:.2f} W/m², "
+              f"Equilibrium temperature = {result['Equilibrium_Temp_C']:.2f}°C")
+
+    # Visualize results
+    plot_comprehensive_results(df_results, env_results)
+
+    # Output technical recommendations
+    provide_technical_recommendations(df_results, env_results, optimal_thickness)
+
+
+def plot_comprehensive_results(df_results, env_results):
+    """Plot comprehensive results"""
+    fig, axes = plt.subplots(2, 3, figsize=(18, 12))
+
+    # Subplot 1: Net cooling power vs thickness
+    axes[0, 0].plot(df_results['Thickness_μm'], df_results['Net_Cooling_Power_Wm2'], 'o-', linewidth=3, markersize=8)
+    axes[0, 0].set_xlabel('Film Thickness (μm)')
+    axes[0, 0].set_ylabel('Net Cooling Power (W/m²)')
+    axes[0, 0].set_title('Net Cooling Power vs Thickness')
+    axes[0, 0].grid(True, alpha=0.3)
+    axes[0, 0].axhline(y=0, color='red', linestyle='--', alpha=0.7)
+
+    # Subplot 2: Equilibrium temperature vs thickness
+    axes[0, 1].plot(df_results['Thickness_μm'], df_results['Equilibrium_Temp_C'], 's-', linewidth=3, markersize=8,
+                    color='orange')
+    axes[0, 1].set_xlabel('Film Thickness (μm)')
+    axes[0, 1].set_ylabel('Equilibrium Temperature (°C)')
+    axes[0, 1].set_title('Equilibrium Temperature vs Thickness')
+    axes[0, 1].grid(True, alpha=0.3)
+    axes[0, 1].axhline(y=25, color='red', linestyle='--', alpha=0.7, label='Ambient Temp')
+
+    # Subplot 3: Atmospheric window utilization
+    axes[0, 2].plot(df_results['Thickness_μm'], df_results['Window_Efficiency'], '^-', linewidth=3, markersize=8,
+                    color='green')
+    axes[0, 2].set_xlabel('Film Thickness (μm)')
+    axes[0, 2].set_ylabel('Atmospheric Window Efficiency')
+    axes[0, 2].set_title('8-13μm Atmospheric Window Emissivity')
+    axes[0, 2].grid(True, alpha=0.3)
+
+    # Subplot 4: Solar reflectance
+    axes[1, 0].plot(df_results['Thickness_μm'], df_results['Solar_Reflectance'], 'd-', linewidth=3, markersize=8,
+                    color='purple')
+    axes[1, 0].set_xlabel('Film Thickness (μm)')
+    axes[1, 0].set_ylabel('Visible Light Reflectance')
+    axes[1, 0].set_title('Solar Reflectance vs Thickness')
+    axes[1, 0].grid(True, alpha=0.3)
+
+    # Subplot 5: Environmental sensitivity
+    env_names = list(env_results.keys())
+    cooling_powers = [env_results[name]['Net_Cooling_Power_Wm2'] for name in env_names]
+    axes[1, 1].bar(env_names, cooling_powers, color=['blue', 'green', 'orange', 'red'], alpha=0.7)
+    axes[1, 1].set_ylabel('Net Cooling Power (W/m²)')
+    axes[1, 1].set_title('Cooling Performance under Different Conditions')
+    axes[1, 1].tick_params(axis='x', rotation=45)
+    axes[1, 1].axhline(y=0, color='black', linestyle='--', alpha=0.5)
+
+    # Subplot 6: Energy component breakdown (optimal thickness)
+    best_idx = df_results['Net_Cooling_Power_Wm2'].idxmax()
+    best_result = df_results.iloc[best_idx]
+    components = ['Radiative Cooling', 'Solar Absorption', 'Atmospheric Absorption']
+    values = [best_result['Net_Cooling_Power_Wm2'] + best_result['Solar_Absorption_Wm2'] + best_result[
+        'Atmospheric_Absorption_Wm2'],
+              -best_result['Solar_Absorption_Wm2'],
+              -best_result['Atmospheric_Absorption_Wm2']]
+    colors = ['green', 'red', 'orange']
+    axes[1, 2].bar(components, values, color=colors, alpha=0.7)
+    axes[1, 2].set_ylabel('Power (W/m²)')
+    axes[1, 2].set_title(f'Energy Balance Breakdown (Thickness: {best_result["Thickness_μm"]}μm)')
+    axes[1, 2].axhline(y=0, color='black', linestyle='-', alpha=0.8)
+
+    plt.tight_layout()
+    plt.savefig('PDMS_comprehensive_cooling_analysis.png', dpi=300, bbox_inches='tight')
+    plt.show()
+
+
+def provide_technical_recommendations(df_results, env_results, optimal_thickness):
+    """Provide detailed technical recommendations"""
+    print("\n" + "=" * 80)
+    print("=== Radiative Cooling Technology Development and Application Recommendations ===")
+    print("=" * 80)
+
+    best_result = df_results[df_results['Thickness_μm'] == optimal_thickness].iloc[0]
+
+    print("1. Optimal Thickness Selection:")
+    print(f"   • Recommended thickness: {optimal_thickness} μm")
+    print(f"   • Performance metrics: Net cooling power {best_result['Net_Cooling_Power_Wm2']:.2f} W/m², "
+          f"Equilibrium temperature {best_result['Equilibrium_Temp_C']:.2f} °C")
+    print(f"   • Technical advantages: Atmospheric window efficiency {best_result['Window_Efficiency']:.3f}, "
+          f"Solar reflectance {best_result['Solar_Reflectance']:.3f}")
+
+    print("\n2. Environmental Adaptability Analysis:")
+    for env_name, result in env_results.items():
+        power = result['Net_Cooling_Power_Wm2']
+        temp = result['Equilibrium_Temp_C']
+        print(f"   • {env_name}: Net power {power:.2f} W/m², Equilibrium temperature {temp:.2f} °C")
+
+    print("\n3. Technical Improvement Directions:")
+    print(
+        "   • Optical performance optimization: Enhance 8-13μm emissivity through surface microstructure or nanoparticle doping")
+    print("   • Solar reflection enhancement: Add visible light reflection layers to reduce solar absorption")
+    print("   • Environmental robustness: Develop composite materials adaptable to high humidity and cloudy conditions")
+
+    print("\n4. Application Scenarios:")
+    print(
+        "   • Building energy efficiency: Building facades, roof coatings, expected to reduce AC energy consumption by 15-25%")
+    print("   • Electronic device cooling: Server rooms, photovoltaic panel cooling")
+    print("   • Personal thermal management: Smart textiles, wearable devices")
+    print("   • Special applications: Cold chain logistics, agricultural greenhouse cooling")
+
+    print("\n5. Industrialization Development Path:")
+    print("   • Short-term (1-2 years): Optimize PDMS film fabrication process, reduce costs")
+    print("   • Medium-term (2-3 years): Develop multilayer composite structures, improve performance")
+    print("   • Long-term (3-5 years): Achieve integration of intelligent radiative cooling systems")
+
+
+# ==========================
+# Mock core functions for testing (replace with actual implementations)
+# ==========================
+def thin_film_emissivity(n_film, k_film, d, wl):
+    """Mock implementation - replace with actual function"""
+    # Simplified implementation for testing
+    R = 0.1  # Approximate reflectance
+    alpha = 4 * np.pi * k_film * d / wl
+    T = np.exp(-alpha)
+    return 1 - R - T
+
+
+if __name__ == "__main__":
+    main()

org/use/q1_2.py

@@ -0,0 +1,198 @@
+import numpy as np
+import matplotlib.pyplot as plt
+from scipy.interpolate import CubicSpline
+
+def make_strictly_increasing(wl, n, k):
+    # 去除完全相同的点
+    unique_wl, indices = np.unique(wl, return_index=True)
+    if len(unique_wl) != len(wl):
+        print(f"Removed {len(wl) - len(unique_wl)} duplicate wavelength points")
+        wl, n, k = wl[indices], n[indices], k[indices]
+
+    # 确保严格递增
+    is_increasing = np.diff(wl) > 0
+    if not all(is_increasing):
+        # 移除不满足严格递增的点
+        valid_indices = np.concatenate([[True], is_increasing])
+        wl, n, k = wl[valid_indices], n[valid_indices], k[valid_indices]
+
+    return wl, n, k
+# -----------------------------
+# 1. 从data.txt读取分块格式数据（先wl+n，再wl+k）
+# -----------------------------
+def read_split_data(file_path):
+    """
+    解析分块数据格式：
+    第一部分：wl	n（多行数据）
+    第二部分：wl	k（多行数据）
+    返回：sorted_wl, n, k（波长已排序，保证n和k一一对应）
+    """
+    with open(file_path, 'r', encoding='utf-8') as f:
+        lines = [line.strip() for line in f if line.strip() and not line.startswith('#')]
+
+    # 分割n数据和k数据（以"wl	k"为分界）
+    split_idx = None
+    for i, line in enumerate(lines):
+        if line == 'wl	k':  # 找到k数据的表头
+            split_idx = i
+            break
+
+    # 提取n数据（表头后到split_idx前）
+    n_lines = lines[1:split_idx]  # 跳过"wl	n"表头
+    wl_n = []
+    n_list = []
+    for line in n_lines:
+        wl, n_val = line.split()
+        wl_n.append(float(wl))
+        n_list.append(float(n_val))
+
+    # 提取k数据（split_idx后）
+    k_lines = lines[split_idx + 1:]  # 跳过"wl	k"表头
+    wl_k = []
+    k_list = []
+    for line in k_lines:
+        wl, k_val = line.split()
+        wl_k.append(float(wl))
+        k_list.append(float(k_val))
+
+    # 转换为numpy数组
+    wl_n = np.array(wl_n)
+    n_list = np.array(n_list)
+    wl_k = np.array(wl_k)
+    k_list = np.array(k_list)
+
+    # 确保n和k的波长完全一致（否则插值会出错）
+    assert np.allclose(wl_n, wl_k), "n和k的波长列表不一致！"
+
+    # 排序（按波长递增，避免插值异常）
+    sorted_idx = np.argsort(wl_n)
+    sorted_wl = wl_n[sorted_idx]
+    sorted_n = n_list[sorted_idx]
+    sorted_k = k_list[sorted_idx]
+
+    return sorted_wl, sorted_n, sorted_k
+
+
+# 读取数据
+wl_all, n_all, k_all = read_split_data('/Users/spasolreisa/IdeaProjects/asiaMath/data.txt')
+
+wl_all, n_all, k_all = make_strictly_increasing(wl_all, n_all, k_all)
+#
+# 三次样条插值（覆盖全波段，保证计算精度）
+cs_n = CubicSpline(wl_all, n_all)  # 折射率n的插值函数
+cs_k = CubicSpline(wl_all, k_all)  # 消光系数k的插值函数
+
+# 定义待研究的PDMS薄膜厚度（μm），可按需调整
+thicknesses = [0.5, 1.0, 1.5, 2.0]
+
+
+# -----------------------------
+# 2. 核心物理模型：薄膜发射率计算
+# -----------------------------
+def fresnel_reflectance(n1, k1, n2, k2):
+    """
+    菲涅尔反射率（垂直入射近似，考虑消光系数k）
+    输入：介质1的n/k，介质2的n/k
+    输出：垂直入射时的反射率R（0-1）
+    """
+    m1 = n1 + 1j * k1  # 介质1的复折射率
+    m2 = n2 + 1j * k2  # 介质2的复折射率
+    return np.abs((m1 - m2) / (m1 + m2)) ** 2
+
+
+def thin_film_emissivity(n_film, k_film, d, wl, n_air=1.0, k_air=0.0):
+    """
+    薄膜发射率计算（考虑多光束干涉和吸收）
+    输入：
+        n_film/k_film: 薄膜的折射率/消光系数
+        d: 薄膜厚度（μm）
+        wl: 波长（μm）
+        n_air/k_air: 空气的折射率/消光系数（默认n=1, k=0）
+    输出：
+        epsilon: 发射率（0-1）
+    """
+    # 1. 计算上下表面的菲涅尔反射率
+    R12 = fresnel_reflectance(n_air, k_air, n_film, k_film)  # 空气→薄膜
+    R23 = fresnel_reflectance(n_film, k_film, n_air, k_air)  # 薄膜→空气
+
+    # 2. 计算相位差和吸收衰减
+    delta = 2 * np.pi * n_film * d / wl  # 干涉相位差（无吸收时）
+    alpha = 4 * np.pi * k_film * d / wl  # 吸收导致的振幅衰减系数
+
+    # 3. 多光束干涉反射率（考虑吸收）
+    numerator = R12 + R23 * np.exp(-alpha) + 2 * np.sqrt(R12 * R23 * np.exp(-alpha)) * np.cos(2 * delta)
+    denominator = 1 + R12 * R23 * np.exp(-alpha) + 2 * np.sqrt(R12 * R23 * np.exp(-alpha)) * np.cos(2 * delta)
+    R_total = numerator / denominator
+
+    # 4. 多光束干涉透射率（考虑吸收）
+    T_total = (1 - R12) * (1 - R23) * np.exp(-alpha) / denominator
+
+    # 5. 基尔霍夫定律：ε = 1 - R - T（局部热平衡）
+    epsilon = 1 - R_total - T_total
+    return epsilon
+
+
+# -----------------------------
+# 3. 计算并绘制不同厚度的发射率光谱
+# -----------------------------
+# 定义计算波长范围（覆盖数据的有效波长区间，步长0.01μm保证平滑）
+wl_min = wl_all.min()
+wl_max = wl_all.max()
+wl_fine = np.linspace(wl_min, wl_max, int((wl_max - wl_min) / 0.01) + 1)
+
+# 创建绘图
+plt.figure(figsize=(12, 7))
+plt.rcParams['font.sans-serif'] = ['Arial']  # 统一字体
+
+# 存储不同厚度的发射率结果（用于后续分析）
+emission_dict = {}
+
+for d in thicknesses:
+    # 插值得到当前波长下的n和k
+    n_film = cs_n(wl_fine)
+    k_film = cs_k(wl_fine)
+
+    # 计算发射率
+    epsilon = thin_film_emissivity(n_film, k_film, d, wl_fine)
+    emission_dict[d] = epsilon
+
+    # 绘制光谱曲线
+    plt.plot(wl_fine, epsilon, linewidth=2, label=f'Thickness = {d} μm')
+
+# -----------------------------
+# 4. 图表美化与标注（突出辐射制冷关键波段）
+# -----------------------------
+# 标注大气透明窗口（8-13μm，辐射制冷核心波段）
+if wl_min <= 13 and wl_max >= 8:  # 仅当数据覆盖该波段时才标注
+    plt.axvspan(8, 13, alpha=0.15, color='red', label='Atmospheric Window (8-13 μm)')
+
+# 坐标轴与标题
+plt.xlabel('Wavelength (μm)', fontsize=14)
+plt.ylabel('Emissivity ε(λ)', fontsize=14)
+plt.title('PDMS Thin Film Spectral Emissivity for Different Thicknesses', fontsize=16, fontweight='bold')
+
+# 网格、图例与范围设置
+plt.grid(True, alpha=0.3, linestyle='--')
+plt.legend(fontsize=12, loc='best')
+plt.ylim(0, 1.05)  # 发射率范围0-1.05（留出余量）
+plt.xlim(wl_min, wl_max)
+
+# 保存图片（高分辨率）
+plt.tight_layout()
+plt.savefig('PDMS_emissivity_spectrum.png', dpi=300, bbox_inches='tight')
+plt.show()
+
+# -----------------------------
+# 5. 输出关键波段（8-13μm）的平均发射率（若数据覆盖该波段）
+# -----------------------------
+if wl_min <= 13 and wl_max >= 8:
+    print("=== 8-13 μm 大气窗口平均发射率 ===")
+    wl_window = np.linspace(8, 13, 500)  # 大气窗口内的波长点
+    for d in thicknesses:
+        n_window = cs_n(wl_window)
+        k_window = cs_k(wl_window)
+        epsilon_window = thin_film_emissivity(n_window, k_window, d, wl_window)
+        avg_epsilon = np.mean(epsilon_window)
+        print(f"厚度 {d} μm: 平均发射率 = {avg_epsilon:.4f}")
+else:
+    print("数据未覆盖8-13μm大气窗口，跳过该波段平均发射率计算。")

org/use/q1_anaylis.py

@@ -0,0 +1,329 @@
+import numpy as np
+import matplotlib.pyplot as plt
+from scipy.interpolate import CubicSpline
+from scipy.stats import pearsonr
+from sklearn.metrics import mean_squared_error
+import warnings
+
+from sklearn.metrics.pairwise import cosine_similarity
+
+from org.chatgpt2.q1_2 import wl_max, wl_min
+
+warnings.filterwarnings('ignore')
+
+
+# -----------------------------
+# 1. 通用工具函数（保持不变）
+# -----------------------------
+def make_strictly_increasing(wl, n, k):
+    unique_wl, indices = np.unique(wl, return_index=True)
+    if len(unique_wl) != len(wl):
+        print(f"Removed {len(wl) - len(unique_wl)} duplicate wavelength points")
+        wl, n, k = wl[indices], n[indices], k[indices]
+    is_increasing = np.diff(wl) > 0
+    if not all(is_increasing):
+        valid_indices = np.concatenate([[True], is_increasing])
+        wl, n, k = wl[valid_indices], n[valid_indices], k[valid_indices]
+    return wl, n, k
+
+
+def read_split_data(file_path):
+    with open(file_path, 'r', encoding='utf-8') as f:
+        lines = [line.strip() for line in f if line.strip() and not line.startswith('#')]
+    split_idx = None
+    for i, line in enumerate(lines):
+        if line == 'wl	k':
+            split_idx = i
+            break
+    n_lines = lines[1:split_idx]
+    wl_n, n_list = [], []
+    for line in n_lines:
+        wl, n_val = line.split()
+        wl_n.append(float(wl)), n_list.append(float(n_val))
+    k_lines = lines[split_idx + 1:]
+    wl_k, k_list = [], []
+    for line in k_lines:
+        wl, k_val = line.split()
+        wl_k.append(float(wl)), k_list.append(float(k_val))
+    wl_n, n_list = np.array(wl_n), np.array(n_list)
+    wl_k, k_list = np.array(wl_k), np.array(k_list)
+    assert np.allclose(wl_n, wl_k), "n和k的波长列表不一致！"
+    sorted_idx = np.argsort(wl_n)
+    return wl_n[sorted_idx], n_list[sorted_idx], k_list[sorted_idx]
+
+
+def fresnel_reflectance(n1, k1, n2, k2):
+    m1 = n1 + 1j * k1
+    m2 = n2 + 1j * k2
+    return np.abs((m1 - m2) / (m1 + m2)) ** 2
+
+
+def thin_film_emissivity(n_film, k_film, d, wl, n_air=1.0, k_air=0.0, n_sub=1.5, k_sub=0.0, r=0.0):
+    m_air = n_air + 1j * k_air
+    m_film = n_film + 1j * k_film
+    m_sub = n_sub + 1j * k_sub
+    R12 = np.abs((m_air - m_film) / (m_air + m_film)) ** 2
+    R23 = np.abs((m_film - m_sub) / (m_film + m_sub)) ** 2
+    beta = 2 * np.pi * m_film / wl
+    delta_complex = beta * d
+    alpha = 2 * np.imag(delta_complex)
+    sqrt_term = np.sqrt(R12 * R23 * np.exp(-alpha))
+    cos_term = np.cos(2 * np.real(delta_complex))
+    R_specular = (R12 + R23 * np.exp(-alpha) + 2 * sqrt_term * cos_term) / (
+                1 + R12 * R23 * np.exp(-alpha) + 2 * sqrt_term * cos_term)
+    R_diffuse = 0.05 * r
+    R_total = (1 - r) * R_specular + r * R_diffuse
+    T_total = (1 - R12) * (1 - R23) * np.exp(-alpha) / (1 + R12 * R23 * np.exp(-alpha) + 2 * sqrt_term * cos_term)
+    return np.clip(1 - R_total - T_total, 0, 1)
+
+
+# -----------------------------
+# 2. 新增：局部相似度计算函数（滑动窗口法）
+# -----------------------------
+def calculate_local_similarity(eps1, eps2, wl_common, window_size=0.5):
+    """
+    计算逐波长的局部相似度（滑动窗口法）
+    输入：
+        eps1/eps2: 两个发射率数组
+        wl_common: 统一波长数组
+        window_size: 滑动窗口宽度（μm），默认0.5μm（覆盖5个采样点，保证平滑）
+    输出：
+        local_corr: 逐波长皮尔逊相关系数（局部相似度）
+        local_cos_sim: 逐波长余弦相似度
+        local_mae: 逐波长局部平均绝对误差（相似度的互补指标）
+    """
+    n_points = len(wl_common)
+    local_corr = np.zeros(n_points)
+    local_cos_sim = np.zeros(n_points)
+    local_mae = np.zeros(n_points)
+
+    # 滑动窗口计算局部相似度（窗口中心为每个波长点）
+    for i in range(n_points):
+        # 确定当前窗口的波长范围
+        wl_center = wl_common[i]
+        window_mask = (wl_common >= wl_center - window_size / 2) & (wl_common <= wl_center + window_size / 2)
+        if np.sum(window_mask) < 3:  # 窗口内至少3个点才计算（避免统计无意义）
+            local_corr[i] = np.nan
+            local_cos_sim[i] = np.nan
+            local_mae[i] = np.nan
+            continue
+
+        # 提取窗口内的发射率数据
+        eps1_window = eps1[window_mask]
+        eps2_window = eps2[window_mask]
+
+        # 计算窗口内的相似度指标
+        corr, _ = pearsonr(eps1_window, eps2_window)
+        cos_sim = cosine_similarity(eps1_window.reshape(1, -1), eps2_window.reshape(1, -1))[0][0]
+        mae = np.mean(np.abs(eps1_window - eps2_window))
+
+        # 存储结果（相关系数和余弦相似度归一化到0-1范围）
+        local_corr[i] = (corr + 1) / 2  # 原始相关系数-1~1 → 映射为0~1
+        local_cos_sim[i] = cos_sim
+        local_mae[i] = mae
+
+    return local_corr, local_cos_sim, local_mae
+
+
+# -----------------------------
+# 3. 核心相似性分析函数（新增局部相似度计算）
+# -----------------------------
+def analyze_spectral_similarity(file1, file2, thicknesses=[1.0], n_sub=1.5, k_sub=0.0, r=0.0, window_size=0.5):
+    # Step 1: 数据读取与预处理
+    wl1, n1, k1 = read_split_data(file1)
+    wl2, n2, k2 = read_split_data(file2)
+    wl1, n1, k1 = make_strictly_increasing(wl1, n1, k1)
+    wl2, n2, k2 = make_strictly_increasing(wl2, n2, k2)
+
+    # Step 2: 统一波长范围
+    wl_min = max(wl1.min(), wl2.min())
+    wl_max = min(wl1.max(), wl2.max())
+    if wl_min >= wl_max:
+        raise ValueError("两个文件的波长范围无交集，无法进行相似性分析！")
+    wl_common = np.linspace(wl_min, wl_max, 1000)
+
+    # Step 3: 插值得到统一波长下的n和k
+    cs_n1 = CubicSpline(wl1, n1)
+    cs_k1 = CubicSpline(wl1, k1)
+    cs_n2 = CubicSpline(wl2, n2)
+    cs_k2 = CubicSpline(wl2, k2)
+    n1_common = cs_n1(wl_common)
+    k1_common = cs_k1(wl_common)
+    n2_common = cs_n2(wl_common)
+    k2_common = cs_k2(wl_common)
+
+    # Step 4: 计算发射率和局部相似度
+    emissivity_dict = {}
+    local_similarity_dict = {}
+    for d in thicknesses:
+        eps1 = thin_film_emissivity(n1_common, k1_common, d, wl_common, n_sub=n_sub, k_sub=k_sub, r=r)
+        eps2 = thin_film_emissivity(n2_common, k2_common, d, wl_common, n_sub=n_sub, k_sub=k_sub, r=r)
+        emissivity_dict[d] = (eps1, eps2)
+
+        # 计算局部相似度
+        local_corr, local_cos_sim, local_mae = calculate_local_similarity(eps1, eps2, wl_common, window_size)
+        local_similarity_dict[d] = (local_corr, local_cos_sim, local_mae)
+
+    # Step 5: 全局相似性指标计算
+    similarity_results = {}
+    for d in thicknesses:
+        eps1, eps2 = emissivity_dict[d]
+        pearson_corr, _ = pearsonr(eps1, eps2)
+        cos_sim = cosine_similarity(eps1.reshape(1, -1), eps2.reshape(1, -1))[0][0]
+        mse = mean_squared_error(eps1, eps2)
+        norm_mse = mse / (np.max([np.var(eps1), np.var(eps2)]) + 1e-8)
+        mae = np.mean(np.abs(eps1 - eps2))
+
+        # 大气窗口指标
+        window_corr, window_mae = None, None
+        if wl_min <= 13 and wl_max >= 8:
+            window_mask = (wl_common >= 8) & (wl_common <= 13)
+            eps1_window = eps1[window_mask]
+            eps2_window = eps2[window_mask]
+            window_corr, _ = pearsonr(eps1_window, eps2_window)
+            window_mae = np.mean(np.abs(eps1_window - eps2_window))
+
+        similarity_results[d] = {
+            "pearson_correlation": pearson_corr,
+            "cosine_similarity": cos_sim,
+            "normalized_mse": norm_mse,
+            "mae": mae,
+            "window_pearson_correlation": window_corr,
+            "window_mae": window_mae
+        }
+
+    # Step 6: 可视化（新增相似度曲线）
+    plot_spectral_comparison(wl_common, emissivity_dict, local_similarity_dict, thicknesses, wl_min, wl_max)
+
+    return similarity_results, wl_common, emissivity_dict, local_similarity_dict
+
+
+# -----------------------------
+# 4. 可视化函数（新增相似度曲线子图）
+# -----------------------------
+def plot_spectral_comparison(wl_common, emissivity_dict, local_similarity_dict, thicknesses, wl_min, wl_max):
+    n_plots = len(thicknesses)
+    fig, axes = plt.subplots(n_plots, 3, figsize=(18, 5 * n_plots))  # 新增1列用于相似度曲线
+    plt.rcParams['font.sans-serif'] = ['Arial']
+
+    for idx, d in enumerate(thicknesses):
+        eps1, eps2 = emissivity_dict[d]
+        local_corr, local_cos_sim, local_mae = local_similarity_dict[d]
+        diff = np.abs(eps1 - eps2)
+
+        # 子图1：发射率光谱对比
+        ax1 = axes[idx, 0] if n_plots > 1 else axes[0]
+        ax1.plot(wl_common, eps1, linewidth=2, label='data.txt', color='darkblue')
+        ax1.plot(wl_common, eps2, linewidth=2, label='data2.txt', color='darkred', linestyle='--')
+        if wl_min <= 13 and wl_max >= 8:
+            ax1.axvspan(8, 13, alpha=0.15, color='orange', label='Atmospheric Window (8-13 μm)')
+        ax1.set_xlabel('Wavelength (μm)', fontsize=12)
+        ax1.set_ylabel('Emissivity ε(λ)', fontsize=12)
+        ax1.set_title(f'Emissivity Spectrum Comparison (Thickness = {d} μm)', fontsize=14, fontweight='bold')
+        ax1.grid(True, alpha=0.3)
+        ax1.legend(fontsize=10)
+        ax1.set_ylim(0, 1.05)
+
+        # 子图2：发射率差异
+        ax2 = axes[idx, 1] if n_plots > 1 else axes[1]
+        ax2.plot(wl_common, diff, linewidth=2, color='darkgreen', label='Absolute Difference |ε1 - ε2|')
+        ax2.fill_between(wl_common, 0, diff, alpha=0.3, color='darkgreen')
+        if wl_min <= 13 and wl_max >= 8:
+            ax2.axvspan(8, 13, alpha=0.15, color='orange', label='Atmospheric Window (8-13 μm)')
+        ax2.set_xlabel('Wavelength (μm)', fontsize=12)
+        ax2.set_ylabel('Absolute Difference', fontsize=12)
+        ax2.set_title(f'Emissivity Difference (Thickness = {d} μm)', fontsize=14, fontweight='bold')
+        ax2.grid(True, alpha=0.3)
+        ax2.legend(fontsize=10)
+        ax2.set_ylim(0, np.nanmax(diff) * 1.2)
+
+        # 子图3：相似度曲线（核心新增）
+        ax3 = axes[idx, 2] if n_plots > 1 else axes[2]
+        # 绘制局部皮尔逊相关系数（归一化到0-1）
+        ax3.plot(wl_common, local_corr, linewidth=2.5, color='#4B0082', label='Local Pearson Correlation (0-1)')        # 绘制局部余弦相似度（0-1）
+        ax3.plot(wl_common, local_cos_sim, linewidth=2.5, color='orange', label='Local Cosine Similarity (0-1)',
+                 linestyle='--')
+        # 标注相似度阈值线（0.9为高相似，0.8为中等相似）
+        ax3.axhline(y=0.9, color='red', linestyle=':', linewidth=1.5, label='High Similarity Threshold (0.9)')
+        ax3.axhline(y=0.8, color='orange', linestyle=':', linewidth=1.5, label='Medium Similarity Threshold (0.8)')
+        # 标注大气窗口
+        if wl_min <= 13 and wl_max >= 8:
+            ax3.axvspan(8, 13, alpha=0.15, color='orange', label='Atmospheric Window (8-13 μm)')
+        ax3.set_xlabel('Wavelength (μm)', fontsize=12)
+        ax3.set_ylabel('Local Similarity (0-1)', fontsize=12)
+        ax3.set_title(f'Wavelength-Dependent Similarity Curve (Thickness = {d} μm)', fontsize=14, fontweight='bold')
+        ax3.grid(True, alpha=0.3)
+        ax3.legend(fontsize=10)
+        ax3.set_ylim(0, 1.05)  # 相似度范围0-1
+        ax3.set_xlim(wl_min, wl_max)
+
+    plt.tight_layout()
+    plt.savefig('spectral_similarity_complete.png', dpi=300, bbox_inches='tight')
+    plt.show()
+
+
+# -----------------------------
+# 5. 主程序执行
+# -----------------------------
+if __name__ == "__main__":
+    file1 = '/Users/spasolreisa/IdeaProjects/asiaMath/data.txt'
+    file2 = '/Users/spasolreisa/IdeaProjects/asiaMath/data2.txt'
+    target_thicknesses = [0.5, 1.0, 1.5, 2.0]
+    base_params = {
+        'n_sub': 1.5,
+        'k_sub': 0.0,
+        'r': 0.05
+    }
+    window_size = 0.5  # 滑动窗口宽度（可调整，建议0.3-0.8μm）
+
+    print("=== 开始光谱相似性分析（含相似度曲线） ===")
+    print(f"文件1: {file1}")
+    print(f"文件2: {file2}")
+    print(f"分析厚度: {target_thicknesses} μm")
+    print(f"滑动窗口宽度: {window_size} μm")
+    print("-" * 50)
+
+    results, wl_common, emissivity_dict, local_similarity_dict = analyze_spectral_similarity(
+        file1, file2,
+        thicknesses=target_thicknesses,
+        n_sub=base_params['n_sub'],
+        k_sub=base_params['k_sub'],
+        r=base_params['r'],
+        window_size=window_size
+    )
+
+    # 输出全局指标
+    print("\n=== 全局相似性指标 ===")
+    for d in target_thicknesses:
+        res = results[d]
+        print(f"\n【厚度 {d} μm】")
+        print(f"全局皮尔逊相关系数: {res['pearson_correlation']:.4f}")
+        print(f"全局余弦相似度: {res['cosine_similarity']:.4f}")
+        print(f"归一化均方误差: {res['normalized_mse']:.4f}")
+        print(f"平均绝对误差: {res['mae']:.4f}")
+        if res['window_pearson_correlation'] is not None:
+            print(f"大气窗口全局相关系数: {res['window_pearson_correlation']:.4f}")
+
+    # 输出局部相似度统计（大气窗口内）
+    print("\n=== 大气窗口（8-13μm）局部相似度统计 ===")
+    for d in target_thicknesses:
+        local_corr, local_cos_sim, _ = local_similarity_dict[d]
+        if wl_min <= 13 and wl_max >= 8:
+            window_mask = (wl_common >= 8) & (wl_common <= 13)
+            window_local_corr = local_corr[window_mask]
+            window_local_cos = local_cos_sim[window_mask]
+            # 过滤NaN值
+            window_local_corr = window_local_corr[~np.isnan(window_local_corr)]
+            window_local_cos = window_local_cos[~np.isnan(window_local_cos)]
+            if len(window_local_corr) > 0:
+                print(f"\n【厚度 {d} μm】")
+                print(f"大气窗口局部相关系数均值: {np.mean(window_local_corr):.4f}")
+                print(f"大气窗口局部相关系数最小值: {np.min(window_local_corr):.4f}")
+                print(f"大气窗口局部余弦相似度均值: {np.mean(window_local_cos):.4f}")
+
+    # 结果解读
+    print("\n=== 结果解读 ===")
+    print("1. 相似度曲线（子图3）：值越接近1，对应波长下的发射率越相似；")
+    print("2. 高相似区域（≥0.9）：两文件在该波段的辐射冷却性能几乎一致；")
+    print("3. 低相似区域（<0.8）：需关注该波段的材料差异对冷却效果的影响；")
+    print("4. 大气窗口内相似度：优先关注该区域，直接决定辐射冷却核心性能是否一致。")