## octave-cvsupdate

 [Octave-cvsupdate] octave-forge/main/odepkg/inst odepkg_equations_lorenz.m, 1.3, 1.4 odepkg_equations_pendulous.m, 1.2, 1.3 odepkg_equations_roessler.m, 1.2, 1.3 From: David Bateman - 2006-10-22 21:20:33 ```Update of /cvsroot/octave/octave-forge/main/odepkg/inst In directory sc8-pr-cvs3.sourceforge.net:/tmp/cvs-serv9230 Modified Files: odepkg_equations_lorenz.m odepkg_equations_pendulous.m odepkg_equations_roessler.m Log Message: Fix texinfo errors. Don't include the TODO line outside of deftypefn block Index: odepkg_equations_pendulous.m =================================================================== RCS file: /cvsroot/octave/octave-forge/main/odepkg/inst/odepkg_equations_pendulous.m,v retrieving revision 1.2 retrieving revision 1.3 diff -u -d -r1.2 -r1.3 --- odepkg_equations_pendulous.m 22 Oct 2006 17:49:59 -0000 1.2 +++ odepkg_equations_pendulous.m 22 Oct 2006 21:20:30 -0000 1.3 @@ -18,7 +18,6 @@ %# -*- texinfo -*- %# @deftypefn {Function} {@var{[ydot]} =} odepkg_equations_pendulous (@var{tvar}, @var{xvar}) %# Returns the states of the differential equations from a pendulum implementation, i.e. the motion of a simple pendulum with damping. The first state variable @var{ydot(1,1)} describes the angular position and the second state variable @var{ydot(2,1)} describes the velocity of the pendulum. The variables @var{xvar} and @var{ydot} are column vectors, the variable @var{tvar} is the actual time stamp. There is no error handling implemented in this function to achieve the highest processing speed. -%# @end deftypefn %# %# Run %# @example Index: odepkg_equations_roessler.m =================================================================== RCS file: /cvsroot/octave/octave-forge/main/odepkg/inst/odepkg_equations_roessler.m,v retrieving revision 1.2 retrieving revision 1.3 diff -u -d -r1.2 -r1.3 --- odepkg_equations_roessler.m 22 Oct 2006 17:49:59 -0000 1.2 +++ odepkg_equations_roessler.m 22 Oct 2006 21:20:30 -0000 1.3 @@ -18,7 +18,6 @@ %# -*- texinfo -*- %# @deftypefn {Function} {@var{[y]} =} odepkg_equations_roessler (@var{t}, @var{x}) %# TODO -%# @end deftypefn %# %# Run %# @example @@ -28,6 +27,7 @@ %# @end deftypefn %# %# @seealso{odepkg} + %# %# - TODO - REWORK THE HELP TEXT ABOVE BECAUSE IT MAY NOT BE CORRECT - %# - TODO - REWORK THE DEMO TEXT BELOW BECAUSE IT MAY NOT BE CORRECT - @@ -59,4 +59,4 @@ %# Local Variables: *** %# mode: octave *** -%# End: *** \ No newline at end of file +%# End: *** Index: odepkg_equations_lorenz.m =================================================================== RCS file: /cvsroot/octave/octave-forge/main/odepkg/inst/odepkg_equations_lorenz.m,v retrieving revision 1.3 retrieving revision 1.4 diff -u -d -r1.3 -r1.4 --- odepkg_equations_lorenz.m 22 Oct 2006 17:49:59 -0000 1.3 +++ odepkg_equations_lorenz.m 22 Oct 2006 21:20:30 -0000 1.4 @@ -18,7 +18,6 @@ %# -*- texinfo -*- %# @deftypefn {Function} {@var{[y]} =} odepkg_equations_lorenz (@var{t}, @var{x}) %# Returns the states of the ordinary differential equations from the Lorenz equation implementation, ie. the force to a conductor caused by movement in a magnetic field, cf. @url{http://en.wikipedia.org/wiki/Lorenz_equation} for further details. The variable @var{x} has the values for the state variables, @var{y} has the results after each integration step. Both variables are column vectors, the variable @var{t} is the actual time stamp. There is no error handling implemented in this function to achieve the highest performance. -%# @end deftypefn %# %# Run %# @example @@ -28,6 +27,7 @@ %# @end deftypefn %# %# @seealso{odepkg} + %# %# - TODO - REWORK THE HELP TEXT ABOVE BECAUSE IT MAY NOT BE CORRECT - @@ -60,4 +60,4 @@ %# Local Variables: *** %# mode: octave *** -%# End: *** \ No newline at end of file +%# End: *** ```