Number of equations.
Current status of the solver: 'running', 'finished' or 'failed'.
Boundary time.
Integration direction: +1 or -1.
Current time.
Current state.
Previous time. None if no steps were made yet.
Size of the last successful step. None if no steps were made yet.
Number of evaluations of the right-hand side.
Number of evaluations of the Jacobian.
Number of LU decompositions.
The implementation follows . The error is controlled with a third-order accurate embedded formula. A cubic polynomial which satisfies the collocation conditions is used for the dense output.
Right-hand side of the system. The calling signature is fun(t, y)
. Here t
is a scalar, and there are two options for the ndarray y
: It can either have shape (n,); then fun
must return array_like with shape (n,). Alternatively it can have shape (n, k); then fun
must return an array_like with shape (n, k), i.e., each column corresponds to a single column in y
. The choice between the two options is determined by :None:None:`vectorized`
argument (see below). The vectorized implementation allows a faster approximation of the Jacobian by finite differences (required for this solver).
Initial time.
Initial state.
Boundary time - the integration won't continue beyond it. It also determines the direction of the integration.
Initial step size. Default is None
which means that the algorithm should choose.
Maximum allowed step size. Default is np.inf, i.e., the step size is not bounded and determined solely by the solver.
Relative and absolute tolerances. The solver keeps the local error estimates less than atol + rtol * abs(y)
. HHere :None:None:`rtol`
controls a relative accuracy (number of correct digits), while atol
controls absolute accuracy (number of correct decimal places). To achieve the desired :None:None:`rtol`
, set atol
to be lower than the lowest value that can be expected from rtol * abs(y)
so that :None:None:`rtol`
dominates the allowable error. If atol
is larger than rtol * abs(y)
the number of correct digits is not guaranteed. Conversely, to achieve the desired atol
set :None:None:`rtol`
such that rtol * abs(y)
is always lower than atol
. If components of y have different scales, it might be beneficial to set different atol
values for different components by passing array_like with shape (n,) for atol
. Default values are 1e-3 for :None:None:`rtol`
and 1e-6 for atol
.
Jacobian matrix of the right-hand side of the system with respect to y, required by this method. The Jacobian matrix has shape (n, n) and its element (i, j) is equal to d f_i / d y_j
. There are three ways to define the Jacobian:
If array_like or sparse_matrix, the Jacobian is assumed to be constant.
If callable, the Jacobian is assumed to depend on both t and y; it will be called as
jac(t, y)
as necessary. For the 'Radau' and 'BDF' methods, the return value might be a sparse matrix.If None (default), the Jacobian will be approximated by finite differences.
It is generally recommended to provide the Jacobian rather than relying on a finite-difference approximation.
Defines a sparsity structure of the Jacobian matrix for a finite-difference approximation. Its shape must be (n, n). This argument is ignored if :None:None:`jac`
is not :None:None:`None`
. If the Jacobian has only few non-zero elements in each row, providing the sparsity structure will greatly speed up the computations . A zero entry means that a corresponding element in the Jacobian is always zero. If None (default), the Jacobian is assumed to be dense.
Whether :None:None:`fun`
is implemented in a vectorized fashion. Default is False.
Implicit Runge-Kutta method of Radau IIA family of order 5.
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