""" 连续型——Hopfield神经网络求解TSP 1、初始化权值(A, D, U0) 2、计算N个城市的距离矩阵dxy 3、初始化神经网络的输入Uxi和输出Vxi 4、利用动力微分方程计算:dUxi / dt 5、由一阶欧拉方法更新计算:Uxi(t + 1) = Uxi(t) + dUxi / dt * step 6、由非线性函数sigmoid更新计算:Vxi(t) = 0.5 * (1 + th(Uxi / U0)) 7、计算能量函数E 8、检查路径是否合法 """ import numpy as np from matplotlib import pyplot as plt # 代价函数(具有三角不等式性质) def price_cn(vec1, vec2): # 元素的平方和再开根号 return np.linalg.norm(np.array(vec1) - np.array(vec2)) # 计算该方案下,总的路径长度 def calc_distance(path): dis = 0.0 for i in range(len(path) - 1): dis += distance[path[i]][path[i + 1]] return dis # 得到城市之间的距离矩阵 def get_distance(citys): N = len(citys) # 构造一个N*N的零矩阵 distance = np.zeros((N, N)) for i, curr_point in enumerate(citys): line = [] # 计算不同城市之间的距离 [line.append(price_cn(curr_point, other_point)) if i != j else line.append(0.0) for j, other_point in enumerate(citys)] # 把距离添加到矩阵相应的位置上 distance[i] = line return distance # 动态方程计算微分方程du def calc_du(V, distance): a = np.sum(V, axis=0) - 1 # 按列相加 - 1 b = np.sum(V, axis=1) - 1 # 按行相加 - 1 t1 = np.zeros((N, N)) t2 = np.zeros((N, N)) for i in range(N): for j in range(N): t1[i, j] = a[j] for i in range(N): for j in range(N): t2[j, i] = b[j] # 将第一列移动到最后一列 c_1 = V[:, 1:N] # 构造一个N行1列的零举证 c_0 = np.zeros((N, 1)) c_0[:, 0] = V[:, 0] # 把c_1和c_0在行方向上连接 c = np.concatenate((c_1, c_0), axis=1) c = np.dot(distance, c) return -A * (t1 + t2) - D * c # 更新神经网络的输入U # Uxi(t+1) = Uxi(t) + dUxi/dt * step def calc_U(U, du, step): return U + du * step # 更新神经网络的输出V # Vxi(t) = 0.5 * (1 + th(Uxi/U0)) def calc_V(U, U0): return 1 / 2 * (1 + np.tanh(U / U0)) # 计算当前网络的能量 def calc_energy(V, distance): t1 = np.sum(np.power(np.sum(V, axis=0) - 1, 2)) t2 = np.sum(np.power(np.sum(V, axis=1) - 1, 2)) idx = [i for i in range(1, N)] idx = idx + [0] Vt = V[:, idx] t3 = distance * Vt t3 = np.sum(np.sum(np.multiply(V, t3))) e = 0.5 * (A * (t1 + t2) + D * t3) return e # 检查路径的正确性 def check_path(V): newV = np.zeros([N, N]) route = [] for i in range(N): mm = np.max(V[:, i]) for j in range(N): if V[j, i] == mm: newV[j, i] = 1 route += [j] break return route, newV # 可视化画出哈密顿回路和能量趋势 def draw_H_and_E(citys, H_path, energys): fig = plt.figure() # 绘制哈密顿回路 ax1 = fig.add_subplot(121) # 设置x轴的数值显示范围 plt.xlim(0, 7) # 设置y轴的数值显示范围 plt.ylim(0, 7) for (from_, to_) in H_path: # 绘制城市点,大小为0.2,颜色为红色 p1 = plt.Circle(citys[from_], 0.2, color='red') p2 = plt.Circle(citys[to_], 0.2, color='red') ax1.add_patch(p1) ax1.add_patch(p2) ax1.plot((citys[from_][0], citys[to_][0]), (citys[from_][1], citys[to_][1]), color='red') ax1.annotate(text=chr(97 + to_), xy=citys[to_], xytext=(-8, -4), textcoords='offset points', fontsize=20) ax1.axis('equal') ax1.grid() # 绘制能量趋势图 ax2 = fig.add_subplot(122) ax2.plot(np.arange(0, len(energys), 1), energys, color='red') plt.show() # 定义城市坐标 citys = np.array([[2, 6], [2, 4], [1, 3], [4, 6], [5, 5], [4, 4], [6, 4], [3, 2], [7, 7], [9, 3]]) # 定义城市与城市之间的距离矩阵 distance = get_distance(citys) # 计算城市个数 N = len(citys) # 初始化参数A和D A = N * N D = N / 2 U0 = 0.0009 # 初始输入 step = 0.0001 # 步长 num_iter = 10000 # 迭代次数 # 初始化神经网络的输入状态(电路的输入U) U = 1 / 2 * U0 * np.log(N - 1) + (2 * (np.random.random((N, N))) - 1) # 初始化神经网络的输出状态(电路的输出V) V = calc_V(U, U0) energys = np.array([0.0 for x in range(num_iter)]) # 每次迭代的能量 best_distance = np.inf # 最优距离 best_route = [] # 最优路线 H_path = [] # 哈密顿回路 # 开始迭代训练网络 for n in range(num_iter): # 利用动态方程计算du du = calc_du(V, distance) # 由一阶欧拉法更新下一个时间的输入状态(电路的输入U) U = calc_U(U, du, step) # 由sigmoid函数更新下一个时间的输出状态(电路的输出V) V = calc_V(U, U0) # 计算当前网络的能量E energys[n] = calc_energy(V, distance) # 检查路径的合法性 route, newV = check_path(V) if len(np.unique(route)) == N: route.append(route[0]) dis = calc_distance(route) if dis < best_distance: # 如果dis小于现有最好的best_distance则把best_distance替换为dis H_path = [] # 更新dis best_distance = dis # 跟新route best_route = route [H_path.append((route[i], route[i + 1])) for i in range(len(route) - 1)] print('第{}次迭代找到的次优解距离为:{},能量为:{},路径为:'.format(n, best_distance, energys[n])) [print(chr(97 + v), end=',' if i < len(best_route) - 1 else '\n') for i, v in enumerate(best_route)] if len(H_path) > 0: draw_H_and_E(citys, H_path, energys) else: print('没有找到最优解')