I am trying to adapt this example using the method of lines so solve a pde for a system of des. This is not the system I am trying to solve, just an example.
How do I incorporate a second de? I have tried modifying odefunc
to be
def odefunc(u,t):
dudt = np.zeros(X.shape)
dvdt = np.zeros(X.shape)
dudt[0] = 0 # constant at boundary condition
dudt[-1] = 0
dvdt[0] = 0
dvdt[-1] = 0
# for the internal nodes
for i in range (1, N-1):
dudt[i] = k* (u[i+1] - 2*u[i] + u[i-1]) / h**2
dvdt[i] = u[i]
return [dudt,dvdt]
based on a couple of example solutions of systems of odes I found - but as I already had an array for dudt I suspect this might be my problem. I also don't know what my initial conditions should now look like so they are the correct dimensions etc.
The error I get is
The array return by func must be one-dimensional, but got ndim=2.
at line sol = odeint(odefunc, init, tspan)
Example with a single pde
import numpy as np
from scipy.integrate import odeint
import matplotlib.pyplot as plt
plt.interactive(False)
N = 5 # number of points to discretise
L = 1.0 # length of the rod
X = np.linspace(0,L,N)
h = L/ (N - 1)
k = 0.02
def odefunc(u,t):
dudt = np.zeros(X.shape)
dudt[0] = 0 # constant at boundary condition
dudt[-1] = 0
# for the internal nodes
for i in range (1, N-1):
dudt[i] = k* (u[i+1] - 2*u[i] + u[i-1]) / h**2
return dudt
init = 150.0 * np.ones(X.shape) # initial temperature
init[0] = 100.0 # boundary condition
init[-1] = 200.0 # boundary condition
tspan = np.linspace(0.0, 5.0, 100)
sol = odeint(odefunc, init, tspan)
for i in range(0, len(tspan), 5):
plt.plot(X,sol[i], label = 't={0:1.2f}'.format(tspan[i]))
# legend outside the figure
plt.legend(loc='center left', bbox_to_anchor=(1,0.5))
plt.xlabel('X position')
plt.ylabel('Temperature')
# adjust figure edges so the legend is in the figure
plt.subplots_adjust(top=0.89, right = 0.77)
plt.show()
From the odeint documentation of the ode function defines y to be a vector, but you have it defined as a list of vectors.
Solves the initial value problem for stiff or non-stiff systems of first order odes:
dy/dt = func(y, t, ...) [or func(t, y, ...)]
where y can be a vector.
You can simply use the ravel
function to create a vector from a list of vectors. Here is an example from your code:
import numpy as np
from scipy.integrate import odeint
import matplotlib.pyplot as plt
plt.interactive(False)
N = 5 # number of points to discretise
L = 1.0 # length of the rod
X = np.linspace(0,L,N)
h = L/ (N - 1)
k = 0.02
def odefunc2(y,t):
u = y[:N]
v = y[N:]
dudt = np.zeros_like(u)
dvdt = np.zeros_like(v)
dudt[0] = 0 # constant at boundary condition
dudt[-1] = 0
dvdt[0] = 0
dvdt[-1] = 0
# for the internal nodes
for i in range (1, N-1):
dudt[i] = k* (u[i+1] - 2*u[i] + u[i-1]) / h**2
dvdt[i] = u[i]
return np.ravel([dudt, dvdt])
initu = 150.0 * np.ones(X.shape) # initial temperature
initu[0] = 100.0 # boundary condition
initu[-1] = 200.0 # boundary condition
initv = np.zeros(X.shape) # initial v
init = np.ravel([initu, initv])
tspan = np.linspace(0.0, 5.0, 100)
sol = odeint(odefunc2, init, tspan)
fig, (ax1, ax2) = plt.subplots(nrows=1, ncols=2)
for i in range(0, len(tspan)):
ax1.plot(X, sol[i, :N], label = 't={0:1.2f}'.format(tspan[i]))
ax2.plot(X, sol[i, N:], label = 't={0:1.2f}'.format(tspan[i]))
plt.show()