Updated to hopefully start handling single mode output correctly. Also added ability to use a -z option to specify the number of planes in the z-direction

Tidied up the LinearAdvection implementation (incluing removing the dealiasing). Also put ChanStability test in standard testing (rather than lengthy) as well as using an eigenvalue measure rather than a L2 norm. Finally also played with OutputTecplot so it would output the HalfMode as a 2D file

Chris Cantwell authored 9 years ago and Spencer Sherwin committed 9 years ago

time-offset errors when checkpointing over long periods.

Also moved base flow interpolation outside of loop.

of BodyForce to also be FieldForce. To incorporate this change I have slightly modified the EvalauteTimeFunction in Forcing

Updates to use a QueryStringAttribute rather than just an Attribute call and also important fix for initialisation of c.ptid in MeshPartition which was causing issues on SGI UV system since it was not intialised correctly

Re-arranged Part II of the documentation to put Preprocessing (MeshConvert), Postprocessing (FieldConvert) and the solvers into separate chapters. This has also mean reducing the section tags of all the solvers and adding a \subsubsubsection command which currently is using bold italic text

Modified the solution to a value that is almost an order of magnitude higher! This is because the introduction of the DGopt branch has used a different set of points (GLL-GLR vs GLL-GLL) to sample the boundary expansion points and this has reduced the accuracy of the boudnary approximation of a function. It does however still converge expoentially. So at a later stage we could look to improve the boundary projection of functions but have accepted this difference at this point