scipy.integrate.ode¶

class
scipy.integrate.
ode
(f, jac=None)[source]¶ A generic interface class to numeric integrators.
Solve an equation system \(y'(t) = f(t,y)\) with (optional)
jac = df/dy
.Note: The first two arguments of
f(t, y, ...)
are in the opposite order of the arguments in the system definition function used byscipy.integrate.odeint
.Parameters: f : callable
f(t, y, *f_args)
Righthand side of the differential equation. t is a scalar,
y.shape == (n,)
.f_args
is set by callingset_f_params(*args)
. f should return a scalar, array or list (not a tuple).jac : callable
jac(t, y, *jac_args)
, optionalJacobian of the righthand side,
jac[i,j] = d f[i] / d y[j]
.jac_args
is set by callingset_jac_params(*args)
.See also
Notes
Available integrators are listed below. They can be selected using the
set_integrator
method.“vode”
Realvalued Variablecoefficient Ordinary Differential Equation solver, with fixedleadingcoefficient implementation. It provides implicit Adams method (for nonstiff problems) and a method based on backward differentiation formulas (BDF) (for stiff problems).
Source: http://www.netlib.org/ode/vode.f
Warning
This integrator is not reentrant. You cannot have two
ode
instances using the “vode” integrator at the same time.This integrator accepts the following parameters in
set_integrator
method of theode
class: atol : float or sequence absolute tolerance for solution
 rtol : float or sequence relative tolerance for solution
 lband : None or int
 uband : None or int Jacobian band width, jac[i,j] != 0 for ilband <= j <= i+uband. Setting these requires your jac routine to return the jacobian in packed format, jac_packed[ij+uband, j] = jac[i,j]. The dimension of the matrix must be (lband+uband+1, len(y)).
 method: ‘adams’ or ‘bdf’ Which solver to use, Adams (nonstiff) or BDF (stiff)
 with_jacobian : bool This option is only considered when the user has not supplied a Jacobian function and has not indicated (by setting either band) that the Jacobian is banded. In this case, with_jacobian specifies whether the iteration method of the ODE solver’s correction step is chord iteration with an internally generated full Jacobian or functional iteration with no Jacobian.
 nsteps : int Maximum number of (internally defined) steps allowed during one call to the solver.
 first_step : float
 min_step : float
 max_step : float Limits for the step sizes used by the integrator.
 order : int Maximum order used by the integrator, order <= 12 for Adams, <= 5 for BDF.
“zvode”
Complexvalued Variablecoefficient Ordinary Differential Equation solver, with fixedleadingcoefficient implementation. It provides implicit Adams method (for nonstiff problems) and a method based on backward differentiation formulas (BDF) (for stiff problems).
Source: http://www.netlib.org/ode/zvode.f
Warning
This integrator is not reentrant. You cannot have two
ode
instances using the “zvode” integrator at the same time.This integrator accepts the same parameters in
set_integrator
as the “vode” solver.Note
When using ZVODE for a stiff system, it should only be used for the case in which the function f is analytic, that is, when each f(i) is an analytic function of each y(j). Analyticity means that the partial derivative df(i)/dy(j) is a unique complex number, and this fact is critical in the way ZVODE solves the dense or banded linear systems that arise in the stiff case. For a complex stiff ODE system in which f is not analytic, ZVODE is likely to have convergence failures, and for this problem one should instead use DVODE on the equivalent real system (in the real and imaginary parts of y).
“lsoda”
Realvalued Variablecoefficient Ordinary Differential Equation solver, with fixedleadingcoefficient implementation. It provides automatic method switching between implicit Adams method (for nonstiff problems) and a method based on backward differentiation formulas (BDF) (for stiff problems).
Source: http://www.netlib.org/odepack
Warning
This integrator is not reentrant. You cannot have two
ode
instances using the “lsoda” integrator at the same time.This integrator accepts the following parameters in
set_integrator
method of theode
class: atol : float or sequence absolute tolerance for solution
 rtol : float or sequence relative tolerance for solution
 lband : None or int
 uband : None or int Jacobian band width, jac[i,j] != 0 for ilband <= j <= i+uband. Setting these requires your jac routine to return the jacobian in packed format, jac_packed[ij+uband, j] = jac[i,j].
 with_jacobian : bool Not used.
 nsteps : int Maximum number of (internally defined) steps allowed during one call to the solver.
 first_step : float
 min_step : float
 max_step : float Limits for the step sizes used by the integrator.
 max_order_ns : int Maximum order used in the nonstiff case (default 12).
 max_order_s : int Maximum order used in the stiff case (default 5).
 max_hnil : int Maximum number of messages reporting too small step size (t + h = t) (default 0)
 ixpr : int Whether to generate extra printing at method switches (default False).
“dopri5”
This is an explicit rungekutta method of order (4)5 due to Dormand & Prince (with stepsize control and dense output).
Authors:
E. Hairer and G. Wanner Universite de Geneve, Dept. de Mathematiques CH1211 Geneve 24, Switzerland email: ernst.hairer@math.unige.ch, gerhard.wanner@math.unige.chThis code is described in [HNW93].
This integrator accepts the following parameters in set_integrator() method of the ode class:
 atol : float or sequence absolute tolerance for solution
 rtol : float or sequence relative tolerance for solution
 nsteps : int Maximum number of (internally defined) steps allowed during one call to the solver.
 first_step : float
 max_step : float
 safety : float Safety factor on new step selection (default 0.9)
 ifactor : float
 dfactor : float Maximum factor to increase/decrease step size by in one step
 beta : float Beta parameter for stabilised step size control.
 verbosity : int Switch for printing messages (< 0 for no messages).
“dop853”
This is an explicit rungekutta method of order 8(5,3) due to Dormand & Prince (with stepsize control and dense output).
Options and references the same as “dopri5”.
References
[HNW93] (1, 2) E. Hairer, S.P. Norsett and G. Wanner, Solving Ordinary Differential Equations i. Nonstiff Problems. 2nd edition. Springer Series in Computational Mathematics, SpringerVerlag (1993) Examples
A problem to integrate and the corresponding jacobian:
>>> from scipy.integrate import ode >>> >>> y0, t0 = [1.0j, 2.0], 0 >>> >>> def f(t, y, arg1): ... return [1j*arg1*y[0] + y[1], arg1*y[1]**2] >>> def jac(t, y, arg1): ... return [[1j*arg1, 1], [0, arg1*2*y[1]]]
The integration:
>>> r = ode(f, jac).set_integrator('zvode', method='bdf') >>> r.set_initial_value(y0, t0).set_f_params(2.0).set_jac_params(2.0) >>> t1 = 10 >>> dt = 1 >>> while r.successful() and r.t < t1: ... print(r.t+dt, r.integrate(r.t+dt)) (1, array([0.71038232+0.23749653j, 0.40000271+0.j ])) (2.0, array([ 0.190985030.52359246j, 0.22222356+0.j ])) (3.0, array([ 0.47153208+0.52701229j, 0.15384681+0.j ])) (4.0, array([0.61905937+0.30726255j, 0.11764744+0.j ])) (5.0, array([ 0.023409970.61418799j, 0.09523835+0.j ])) (6.0, array([ 0.58643071+0.339819j, 0.08000018+0.j ])) (7.0, array([0.52070105+0.44525141j, 0.06896565+0.j ])) (8.0, array([0.159867330.61234476j, 0.06060616+0.j ])) (9.0, array([ 0.64850462+0.15048982j, 0.05405414+0.j ])) (10.0, array([0.38404699+0.56382299j, 0.04878055+0.j ]))
Attributes
t (float) Current time. y (ndarray) Current variable values. Methods
integrate
(t[, step, relax])Find y=y(t), set y as an initial condition, and return y. set_f_params
(*args)Set extra parameters for usersupplied function f. set_initial_value
(y[, t])Set initial conditions y(t) = y. set_integrator
(name, **integrator_params)Set integrator by name. set_jac_params
(*args)Set extra parameters for usersupplied function jac. set_solout
(solout)Set callable to be called at every successful integration step. successful
()Check if integration was successful.