python PINN求解一维Sod的预测解并给出精确解以及代码
时间: 2023-12-20 11:23:55 浏览: 39
Sod问题是一个经典的气体动力学问题,它描述了一个强激波穿过气体的过程。在这里,我们将使用物理信息神经网络(PINN)来预测一维Sod问题的解,并将其与精确解进行比较。
首先,定义问题的初始和边界条件:
$$\begin{aligned} \rho(x,0) &= \begin{cases} 1 & x<0.5 \\ 0.125 & x\geq 0.5 \end{cases} \\ u(x,0) &= 0 \\ p(x,0) &= \begin{cases} 1 & x<0.5 \\ 0.1 & x\geq 0.5 \end{cases} \\ \rho(0,t) &= 1 \\ u(0,t) &= 0 \\ p(0,t) &= 1 \\ \rho(1,t) &= 0.125 \\ u(1,t) &= 0 \\ p(1,t) &= 0.1 \end{aligned} $$
接下来,我们将使用PINN来求解这个问题。首先,我们需要导入必要的库:
```python
import tensorflow as tf
import numpy as np
import matplotlib.pyplot as plt
```
然后,我们定义网络的结构和损失函数:
```python
class SodPINN(tf.keras.Model):
def __init__(self):
super(SodPINN, self).__init__()
self.dense1 = tf.keras.layers.Dense(50, activation=tf.nn.tanh, input_shape=(1,))
self.dense2 = tf.keras.layers.Dense(50, activation=tf.nn.tanh)
self.dense3 = tf.keras.layers.Dense(50, activation=tf.nn.tanh)
self.dense4 = tf.keras.layers.Dense(50, activation=tf.nn.tanh)
self.dense5 = tf.keras.layers.Dense(50, activation=tf.nn.tanh)
self.dense6 = tf.keras.layers.Dense(50, activation=tf.nn.tanh)
self.dense7 = tf.keras.layers.Dense(3)
def call(self, inputs):
x = inputs
x = self.dense1(x)
x = self.dense2(x)
x = self.dense3(x)
x = self.dense4(x)
x = self.dense5(x)
x = self.dense6(x)
return self.dense7(x)
def pinn_loss(model, x, rho, u, p, gamma):
with tf.GradientTape(persistent=True) as g:
g.watch(x)
# Forward pass
inputs = tf.concat([x, rho, u, p], axis=1)
pred = model(inputs)
# Extracting predictions
rho_pred = pred[:, 0:1]
u_pred = pred[:, 1:2]
p_pred = pred[:, 2:3]
# Computing gradients
drho_dx = g.gradient(rho_pred, x)
du_dx = g.gradient(u_pred, x)
dp_dx = g.gradient(p_pred, x)
# Computing residual terms
rho_res = drho_dx + rho_pred * (u_pred - u_pred[:, 0:1]) / (x - x[:, 0:1])
u_res = du_dx + (p_pred - p_pred[:, 0:1]) / (rho_pred * (x - x[:, 0:1])) - (gamma - 1) / gamma * (u_pred - u_pred[:, 0:1]) * (dp_dx / p_pred)
p_res = dp_dx + gamma * p_pred * (u_pred - u_pred[:, 0:1]) / (x - x[:, 0:1])
# Computing loss
loss = tf.reduce_mean(tf.square(rho_res) + tf.square(u_res) + tf.square(p_res))
return loss
```
接下来,我们将定义一些必要的变量,并初始化模型:
```python
# Defining constants
gamma = 1.4
N = 10000
x = np.linspace(0, 1, N)[:, None]
rho = np.zeros((N, 1))
u = np.zeros((N, 1))
p = np.zeros((N, 1))
for i in range(N):
if x[i] < 0.5:
rho[i] = 1
u[i] = 0
p[i] = 1
else:
rho[i] = 0.125
u[i] = 0
p[i] = 0.1
# Initializing model
model = SodPINN()
optimizer = tf.keras.optimizers.Adam(learning_rate=1e-3)
```
然后,我们将训练模型:
```python
# Training model
for epoch in range(10000):
with tf.GradientTape() as tape:
loss = pinn_loss(model, x, rho, u, p, gamma)
grads = tape.gradient(loss, model.trainable_variables)
optimizer.apply_gradients(zip(grads, model.trainable_variables))
if epoch % 1000 == 0:
print("Epoch: {}, Loss: {}".format(epoch, loss.numpy()))
```
最后,我们将绘制预测解和精确解的比较图:
```python
# Computing predictions
inputs = tf.concat([x, rho, u, p], axis=1)
pred = model(inputs)
rho_pred = pred[:, 0:1].numpy()
u_pred = pred[:, 1:2].numpy()
p_pred = pred[:, 2:3].numpy()
# Computing exact solution
rho_exact = np.zeros((N, 1))
u_exact = np.zeros((N, 1))
p_exact = np.zeros((N, 1))
for i in range(N):
if x[i] < 0.5:
rho_exact[i] = 1
u_exact[i] = 0
p_exact[i] = 1
else:
rho_exact[i] = 0.125
u_exact[i] = 0
p_exact[i] = 0.1
# Plotting results
plt.figure(1)
plt.plot(x, rho_pred, 'r-', label='PINN')
plt.plot(x, rho_exact, 'k--', label='Exact')
plt.xlabel('x')
plt.ylabel('Density')
plt.legend()
plt.figure(2)
plt.plot(x, u_pred, 'r-', label='PINN')
plt.plot(x, u_exact, 'k--', label='Exact')
plt.xlabel('x')
plt.ylabel('Velocity')
plt.legend()
plt.figure(3)
plt.plot(x, p_pred, 'r-', label='PINN')
plt.plot(x, p_exact, 'k--', label='Exact')
plt.xlabel('x')
plt.ylabel('Pressure')
plt.legend()
plt.show()
```
完整代码如下: