Octave has two built-in functions for solving differential equations. Both are based on reliable ODE solvers written in Fortran.

The function `lsode`

can be used Solve ODEs of the form

using Hindmarsh's ODE solver LSODE.

lsode (fcn,x0,t_out,t_crit)

The first argument is the name of the function to call to compute the vector of right hand sides. It must have the form

xdot= f (x,t)

where `xdot` and `x` are vectors and `t` is a scalar.

The second argument specifies the initial condition, and the third specifies a vector of output times at which the solution is desired, including the time corresponding to the initial condition.

The fourth argument is optional, and may be used to specify a set of times that the ODE solver should not integrate past. It is useful for avoiding difficulties with singularities and points where there is a discontinuity in the derivative.

Tolerances and other options for `lsode`

may be specified using the
function `lsode_options`

.

Here is an example of solving a set of two differential equations using
`lsode`

. The function

function xdot = f (x, t) r = 0.25; k = 1.4; a = 1.5; b = 0.16; c = 0.9; d = 0.8; xdot(1) = r*x(1)*(1 - x(1)/k) - a*x(1)*x(2)/(1 + b*x(1)); xdot(2) = c*a*x(1)*x(2)/(1 + b*x(1)) - d*x(2); endfunction

is integrated with the command

x = lsode ("f", [1; 2], (t = linspace (0, 50, 200)'));

producing a set of 200 values stored in the variable `x`. Note that
this example takes advantage of the fact that an assignment produces a
value to store the values of the output times in the variable `t`
directly in the function call The results can then be plotted using
the command

plot (t, x)

See Alan C. Hindmarsh, ODEPACK, A Systematized Collection of ODE Solvers, in Scientific Computing, R. S. Stepleman, editor, (1983) for more information about this family of ODE solvers.

The function `dassl`

can be used Solve DAEs of the form

dassl (fcn,x_0,xdot_0,t_out,t_crit)

The first argument is the name of the function to call to compute the vector of residuals. It must have the form

res= f (x,xdot,t)

where `x`, `xdot`, and `res` are vectors, and `t` is a
scalar.

The second and third arguments to `dassl`

specify the initial
condition of the states and their derivatives, and the fourth argument
specifies a vector of output times at which the solution is desired,
including the time corresponding to the initial condition.

The set of initial states and derivatives are not strictly required to be consistent. In practice, however, DASSL is not very good at determining a consistent set for you, so it is best if you ensure that the initial values result in the function evaluating to zero.

The fifth argument is optional, and may be used to specify a set of times that the DAE solver should not integrate past. It is useful for avoiding difficulties with singularities and points where there is a discontinuity in the derivative.

Tolerances and other options for `dassl`

may be specified using the
function `dassl_options`

.

See K. E. Brenan, et al., Numerical Solution of Initial-Value Problems in Differential-Algebraic Equations, North-Holland (1989) for more information about the implementation of DASSL.

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