numbalsoda
numbalsoda is a python wrapper to the LSODA method in ODEPACK, which is for solving ordinary differential equation initial value problems. LSODA was originally written in Fortran. numbalsoda is a wrapper to a C++ re-write of the original code: https://github.com/dilawar/libsoda
numbalsoda also wraps the dop853 explicit Runge-Kutta method from this repository: https://github.com/jacobwilliams/dop853
This package is very similar to scipy.integrate.solve_ivp (see here), when you set method = 'LSODA' or method = DOP853. But, scipy.integrate.solve_ivp invokes the python interpreter every time step which can be slow. Also, scipy.integrate.solve_ivp can not be used within numba jit-compiled python functions. In contrast, numbalsoda never invokes the python interpreter during integration and can be used within a numba compiled function which makes numbalsoda a lot faster than scipy for most problems, and achieves similar performance to Julia's DifferentialEquations.jl in some cases (see benchmark folder).
Installation
Conda:
conda install -c conda-forge numbalsoda
Pip:
python -m pip install numbalsoda
Basic usage
from numbalsoda import lsoda_sig, lsoda, dop853
from numba import njit, cfunc
import numpy as np
@cfunc(lsoda_sig)
def rhs(t, u, du, p):
du[0] = u[0]-u[0]*u[1]
du[1] = u[0]*u[1]-u[1]*p[0]
funcptr = rhs.address # address to ODE function
u0 = np.array([5.,0.8]) # Initial conditions
data = np.array([1.0]) # data you want to pass to rhs (data == p in the rhs).
t_eval = np.linspace(0.0,50.0,1000) # times to evaluate solution
# integrate with lsoda method
usol, success = lsoda(funcptr, u0, t_eval, data = data)
# integrate with dop853 method
usol1, success1 = dop853(funcptr, u0, t_eval, data = data)
# usol = solution
# success = True/False
The variables u, du and p in the rhs function are pointers to an array of floats. Therefore, operations like np.sum(u) or len(u) will not work. However, you can use the function nb.carray() to make a numpy array out of the pointers. For example:
import numba as nb
@cfunc(lsoda_sig)
def rhs(t, u, du, p):
u_ = nb.carray(u, (2,))
p_ = nb.carray(p, (1,))
# ... rest of rhs goes here using u_ and p_
Above, u_ and p_ are numpy arrays build out of u and p, and so functions like np.sum(u_) will work.
Also, note lsoda can be called within a jit-compiled numba function (see below). This makes it much faster than scipy if a program involves many integrations in a row.
@njit
def test():
usol, success = lsoda(funcptr, u0, t_eval, data = data)
return usol
usol = test() # this works!
@njit
def test_sp():
sol = solve_ivp(f_scipy, t_span, u0, t_eval = t_eval, method='LSODA')
return sol
sol = test_sp() # this does not work :(
Passing data to the right-hand-side function
In the examples shown above, we passed a an single array of floats to the right-hand-side function:
# ...
data = np.array([1.0])
usol, success = lsoda(funcptr, u0, t_eval, data = data)
However, sometimes you might want to pass more data types than just floats. For example, you might want to pass several integers, an array of floats, and an array of integers. One way to achieve this is with generating the cfunc using a function like this:
def make_lsoda_func(param1, param2, param3):
@cfunc(lsoda_sig)
def rhs(t, x, du, p):
# Here param1, param2, and param3
# can be accessed.
du[0] = param1*t
# etc...
return rhs
rhs = make_lsoda_func(10.0, 5, 10000)
funcptr = rhs.address
# etc...
The only drawback of this approach is if you want to do many successive integrations where the parameters change because it would required re-compiling the cfunc between each integration. This could be slow.
But! It is possible to pass arbitrary parameters without re-compiling the cfunc, but it is a little tricky. The notebook passing_data_to_rhs_function.ipynb gives an example that explains how.
![[lsoda] 500 steps taken before reaching tout](https://avatars.githubusercontent.com/u/100946992?v=4)
69 Nov 28, 2022
263 Jan 07, 2023
96 Nov 05, 2022
131 Jan 08, 2023
15 Aug 29, 2022
26 Oct 25, 2022
21 Oct 19, 2022
87 Sep 24, 2022
3 May 01, 2022
57 Dec 15, 2022
27 Dec 08, 2022
8 Nov 26, 2022
64 Dec 12, 2022
99 Dec 12, 2022
18 Nov 16, 2022
40 Oct 30, 2022
43 Jan 08, 2023
1 Dec 15, 2021
1.4k Dec 25, 2022
21 Sep 27, 2022