I am wondering how to export MATLAB function ode45 to python. According to the documentation is should be as follows:
MATLAB: [t,y]=ode45(#vdp1,[0 20],[2 0]);
Python: import numpy as np
def vdp1(t,y):
dydt= np.array([y[1], (1-y[0]**2)*y[1]-y[0]])
return dydt
import scipy integrate
l=scipy.integrate.ode(vdp1([0,20],[2,0])).set_integrator("dopri5")
The results are completely different, Matlab returns different dimensions than Python.
As #LutzL mentioned, you can use the newer API, solve_ivp.
results = solve_ivp(obj_func, t_span, y0, t_eval = time_series)
If t_eval is not specified, then you won't have one record per one timestamp, which is mostly the cases I assume.
Another side note is that for odeint and often other integrators, the output array is a ndarray of a shape of [len(time), len(states)], however for solve_ivp, the output is a list(length of state vector) of 1-dimension ndarray(which length is equal to t_eval).
So you have to merge it if you want the same order. You can do so by:
Y =results
merged = np.hstack([i.reshape(-1,1) for i in Y.y])
First you need to reshape to make it a [n,1] array, and merge it horizontally.
Hope this helps!
The interface of integrate.ode is not as intuitive as of a simpler method odeint which, however, does not support choosing an ODE integrator. The main difference is that ode does not run a loop for you; if you need a solution at a bunch of points, you have to say at what points, and compute it one point at a time.
import numpy as np
from scipy import integrate
import matplotlib.pyplot as plt
def vdp1(t, y):
return np.array([y[1], (1 - y[0]**2)*y[1] - y[0]])
t0, t1 = 0, 20 # start and end
t = np.linspace(t0, t1, 100) # the points of evaluation of solution
y0 = [2, 0] # initial value
y = np.zeros((len(t), len(y0))) # array for solution
y[0, :] = y0
r = integrate.ode(vdp1).set_integrator("dopri5") # choice of method
r.set_initial_value(y0, t0) # initial values
for i in range(1, t.size):
y[i, :] = r.integrate(t[i]) # get one more value, add it to the array
if not r.successful():
raise RuntimeError("Could not integrate")
plt.plot(t, y)
plt.show()
The function scipy.integrate.solve_ivp uses the method RK45 by default, similar the method used by Matlab's function ODE45 as both use the Dormand-Pierce formulas with fourth-order method accuracy.
vdp1 = #(T,Y) [Y(2); (1 - Y(1)^2) * Y(2) - Y(1)];
[T,Y] = ode45 (vdp1, [0, 20], [2, 0]);
from scipy.integrate import solve_ivp
vdp1 = lambda T,Y: [Y[1], (1 - Y[0]**2) * Y[1] - Y[0]]
sol = solve_ivp (vdp1, [0, 20], [2, 0])
T = sol.t
Y = sol.y
Ordinary Differential Equations (solve_ivp)
Related
I am trying to solve this differential equation as part of my assignment. I am not able to understand on how can i put the condition for u in the code. In the code shown below, i arbitrarily provided
u = 5.
2dx(t)dt=−x(t)+u(t)
5dy(t)dt=−y(t)+x(t)
u=2S(t−5)
x(0)=0
y(0)=0
where S(t−5) is a step function that changes from zero to one at t=5. When it is multiplied by two, it changes from zero to two at that same time, t=5.
def model(x,t,u):
dxdt = (-x+u)/2
return dxdt
def model2(y,x,t):
dydt = -(y+x)/5
return dydt
x0 = 0
y0 = 0
u = 5
t = np.linspace(0,40)
x = odeint(model,x0,t,args=(u,))
y = odeint(model2,y0,t,args=(u,))
plt.plot(t,x,'r-')
plt.plot(t,y,'b*')
plt.show()
I do not know the SciPy Library very well, but regarding the example in the documentation I would try something like this:
def model(x, t, K, PT)
"""
The model consists of the state x in R^2, the time in R and the two
parameters K and PT regarding the input u as step function, where K
is the infimum of u and PT is the delay of the step.
"""
x1, x2 = x # Split the state into two variables
u = K if t>=PT else 0 # This is the system input
# Here comes the differential equation in vectorized form
dx = [(-x1 + u)/2,
(-x2 + x1)/5]
return dx
x0 = [0, 0]
K = 2
PT = 5
t = np.linspace(0,40)
x = odeint(model, x0, t, args=(K, PT))
plt.plot(t, x[:, 0], 'r-')
plt.plot(t, x[:, 1], 'b*')
plt.show()
You have a couple of issues here, and the step function is only a small part of it. You can define a step function with a simple lambda and then simply capture it from the outer scope without even passing it to your function. Because sometimes that won't be the case, we'll be explicit and pass it.
Your next problem is the order of arguments in the function to integrate. As per the docs (y,t,...). Ie, First the function, then the time vector, then the other args arguments. So for the first part we get:
u = lambda t : 2 if t>5 else 0
def model(x,t,u):
dxdt = (-x+u(t))/2
return dxdt
x0 = 0
y0 = 0
t = np.linspace(0,40)
x = odeint(model,x0,t,args=(u,))
Moving to the next part, the trouble is, you can't feed x as an arg to y because it's a vector of values for x(t) for particular times and so y+x doesn't make sense in the function as you wrote it. You can follow your intuition from math class if you pass an x function instead of the x values. Doing so requires that you interpolate the x values using the specific time values you are interested in (which scipy can handle, no problem):
from scipy.interpolate import interp1d
xfunc = interp1d(t.flatten(),x.flatten(),fill_value="extrapolate")
#flatten cuz the shape is off , extrapolate because odeint will go out of bounds
def model2(y,t,x):
dydt = -(y+x(t))/5
return dydt
y = odeint(model2,y0,t,args=(xfunc,))
Then you get:
#Sven's answer is more idiomatic for vector programming like scipy/numpy. But I hope my answer provides a clearer path from what you know already to a working solution.
I have a system of ODEs that depend on a matrix of data. Each ODE should reference a different column of data in its evaluation.
import numpy as np
n_eqns = 20
coeffs = np.random.normal(0, 1, (n_eqns, 20))
def dfdt(_, f, idx):
return (f ** 2) * coeffs[idx, :].sum() - 2 * f * coeffs.sum()
from scipy.integrate import ode
f0 = np.random.uniform(-1, 1, n_eqns)
t0 = 0
tf = 1
dt = 0.001
r = ode(dfdt)
r.set_initial_value(f0, t0).set_f_params(range(n_eqns))
while r.successful() and r.t < tf:
print(r.t+dt, r.integrate(r.t+dt))
How can I specify that each ODE should use the idx value associated with its index in the system of ODEs? The first equation should be passed idx=0, the second idx=1, and so on.
The function dfdt takes and returns the state and derivative, respectively as arrays (or other iterables). Thus, all you have to do is to loop over all indices and apply your operations accordingly. For example:
def dfdt(t,f):
output = np.empty_like(f)
for i,entry in enumerate(f)
output[i] = f[i]**2 * coeffs[i,:].sum() - 2*f[i]*coeffs.sum()
return output
You can also write this using NumPy’s component-wise operations (which is quicker):
def dfdt(t,f):
return f**2 * coeffs.sum(axis=1) - 2*f*coeffs.sum()
Finally note that using f for your state may be somewhat confusing since this is how ode denotes the derivative (which you call dfdt).
On another thread, I saw someone manage to integrate the length of a arc using mathematica.They wrote:
In[1]:= ArcTan[3.05*Tan[5Pi/18]/2.23]
Out[1]= 1.02051
In[2]:= x=3.05 Cos[t];
In[3]:= y=2.23 Sin[t];
In[4]:= NIntegrate[Sqrt[D[x,t]^2+D[y,t]^2],{t,0,1.02051}]
Out[4]= 2.53143
How exactly could this be transferred to python using the imports of numpy and scipy? In particular, I am stuck on line 4 in his code with the "NIntegrate" function. Thanks for the help!
Also, if I already have the arc length and the vertical axis length, how would I be able to reverse the program to spit out the original paremeters from the known values? Thanks!
To my knowledge scipy cannot perform symbolic computations (such as symbolic differentiation). You may want to have a look at http://www.sympy.org for a symbolic computation package. Therefore, in the example below, I compute derivatives analytically (the Dx(t) and Dy(t) functions).
>>> from scipy.integrate import quad
>>> import numpy as np
>>> Dx = lambda t: -3.05 * np.sin(t)
>>> Dy = lambda t: 2.23 * np.cos(t)
>>> quad(lambda t: np.sqrt(Dx(t)**2 + Dy(t)**2), 0, 1.02051)
(2.531432761012828, 2.810454936566873e-14)
EDIT: Second part of the question - inverting the problem
From the fact that you know the value of the integral (arc) you can now solve for one of the parameters that determine the arc (semi-axes, angle, etc.) Let's assume you want to solve for the angle. Then you can use one of the non-linear solvers in scipy, to revert the equation quad(theta) - arcval == 0. You can do it like this:
>>> from scipy.integrate import quad
>>> from scipy.optimize import broyden1
>>> import numpy as np
>>> a = 3.05
>>> b = 2.23
>>> Dx = lambda t: -a * np.sin(t)
>>> Dy = lambda t: b * np.cos(t)
>>> arc = lambda theta: quad(lambda t: np.sqrt(Dx(t)**2 + Dy(t)**2), 0, np.arctan((a / b) * np.tan(np.deg2rad(theta))))[0]
>>> invert = lambda arcval: float(broyden1(lambda x: arc(x) - arcval, np.rad2deg(arcval / np.sqrt((a**2 + b**2) / 2.0))))
Then:
>>> arc(50)
2.531419526553662
>>> invert(arc(50))
50.000031008458365
If you prefer a pure numerical approach, you could use the following barebones solution. This worked well for me given that I had two input numpy.ndarrays, x and y with no functional form available.
import numpy as np
def arclength(x, y, a, b):
"""
Computes the arclength of the given curve
defined by (x0, y0), (x1, y1) ... (xn, yn)
over the provided bounds, `a` and `b`.
Parameters
----------
x: numpy.ndarray
The array of x values
y: numpy.ndarray
The array of y values corresponding to each value of x
a: int
The lower limit to integrate from
b: int
The upper limit to integrate to
Returns
-------
numpy.float64
The arclength of the curve
"""
bounds = (x >= a) & (y <= b)
return np.trapz(
np.sqrt(
1 + np.gradient(y[bounds], x[bounds])
) ** 2),
x[bounds]
)
Note: I spaced the return variables out that way just to make it more readable and clear to understand the operations taking place.
As an aside, recall that the arc-length of a curve is given by:
I am totally new to python, and try to integrate following ode:
$\dot{x} = -2x-y^2$
$\dot{y} = -y-x^2
This results in an array with everything 0 though
What am I doing wrong? It is mostly copied code, and with another, not coupled ode it worked fine.
import numpy as np
import matplotlib.pyplot as plt
from scipy.integrate import ode
def fun(t, z):
"""
Right hand side of the differential equations
dx/dt = -omega * y
dy/dt = omega * x
"""
x, y = z
f = [-2*x-y**2, -y-x**2]
return f
# Create an `ode` instance to solve the system of differential
# equations defined by `fun`, and set the solver method to 'dop853'.
solver = ode(fun)
solver.set_integrator('dopri5')
# Set the initial value z(0) = z0.
t0 = 0.0
z0 = [0, 0]
solver.set_initial_value(z0, t0)
# Create the array `t` of time values at which to compute
# the solution, and create an array to hold the solution.
# Put the initial value in the solution array.
t1 = 2.5
N = 75
t = np.linspace(t0, t1, N)
sol = np.empty((N, 2))
sol[0] = z0
# Repeatedly call the `integrate` method to advance the
# solution to time t[k], and save the solution in sol[k].
k = 1
while solver.successful() and solver.t < t1:
solver.integrate(t[k])
sol[k] = solver.y
k += 1
# Plot the solution...
plt.plot(t, sol[:,0], label='x')
plt.plot(t, sol[:,1], label='y')
plt.xlabel('t')
plt.grid(True)
plt.legend()
plt.show()
Your initial state (z0) is [0,0]. The time derivative (fun) for this initial state is also [0,0]. Hence, for this initial condition, [0,0] is the correct solution for all times.
If you change your initial condition to some other value, you should observe more interesting result.
I am relatively new to Python and trying to use it to solve an integrator problem
x' = - L * x
Where L is the Laplacian Matrix, that is a matrix representation of a graph. This is part of my code:
def integrate_cons(x, t, l):
xdot = -l*x
return xdot;
t = np.linspace(0, 10, 101)
#laplacian is a 3x3 matrix
#initial_condition is a vector
solution = odeint(integrate_cons, initial_conditions, t, args=(laplacian,))
print solution
I'm having problems to pass a matrix like an argument in odeint. How can i solve?
import numpy as np
from scipy.integrate import odeint
def integrate_cons(x, t, l):
# unless you use np.matrix which I never do, you have to use np.dot
xdot = -np.dot(l,x)
return xdot;
t = np.linspace(0, 10, 101)
# just a random matrix
l = np.random.rand(3,3)
# initial conditions
x0 = np.array([1,1,1])
#laplacian is a 3x3 matrix
#initial_condition is a vector
solution = odeint(integrate_cons, x0, t, args=(l,))
print(solution)
Look at the scipy cookbook for examples.