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An Octave cookbook. Each entry should go in a separate section and have the following subsection: problem, solution, discussion and maybe a see also.
An Octave cookbook. Each entry should go in a separate section and have the following subsection: problem, solution, discussion and maybe a see also.
__FORCETOC__


== Programs, Libraries, and Packages ==
== Programs, Libraries, and Packages ==
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=== List all function in Octave ===
=== List all function in Octave ===
Use the following script (filename <code>list_func.m</code>)
Use the following script
<syntaxhighlight lang="Octave">
<syntaxhighlight lang="Octave">
## List of all builtin (C++) functions and m-file functions
## List of all builtin (C++) functions and m-file functions
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Check the [[Geometry package]] for many more distance functions (points, lines, polygons, etc.).
Check the [[Geometry package]] for many more distance functions (points, lines, polygons, etc.).


=== Find Algebraic Variables from ODE State Variables ===
==== Problem ====
When using lsode or other ODE solver to find the state variables x as a function of time t in a set of ODE's, there seems to be no simple way to return and tabulate algebraic variables y that are a function of the state variables x and time t, other than the derivatives.
Consider a modified version of the spring function defined above in the section on parametric functions:
<syntaxhighlight lang="Octave">
function sprime=dspring (s, t)
  k=1;
  tau=1;
  x = s(1);
  v = s(2);
  y=x+v*tau;
  sprime(1) = v;
  sprime(2) = -k * y;
endfunction
</syntaxhighlight>
What would be a way to way to use this function and lsode to tabulate not just the elements of x and sprime, but also (say) y as a function of time?
==== Solution ====
Modify the function sprime to return y as a second argument:
<syntaxhighlight lang="Octave">
function [sprime,y]=dspring (s, t)
  k=1;
  tau=1;
  x = s(1);
  v = s(2);
  y=x+v*tau;
  sprime(1) = v;
  sprime(2) = -k * y;
endfunction
</syntaxhighlight>
lsode will happily ignore the second return argument y, but after x has been tabulated, y can be tabulated using the second return argument of the spring function in a for loop, e.g.
<syntaxhighlight lang="Octave">
t = linspace (0, 10, 100);
x = lsode ('dspring',[1;0], t);
y=zeros(length(t),1);
for i=1:length(t)
  [xtmp,y(i,1)]=dspring(x(i,:),t(i));
end
</syntaxhighlight>
==== Discussion ====
This is a simple example with one algebraic variable. Others can be added by extending the second dimension of the y array.


[[Category:Examples]]
[[Category:Tutorials]]
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