I'm not sure if this belongs here or in the advanced applied math section, but here goes.

I'm trying to solve the equation

$\displaystyle \frac{\partial u}{\partial t} + \frac{\partial}{\partial x}\left(Cu\right) - \frac{\partial}{\partial x}\left(D\frac{\partial u}{\partial x}\right) = f(x,t)$


where C and D allow for linearity. I'm using a discontinuous Galerkin method in space and Backward Euler for the time-stepping. I currently have a working code for the equation WITHOUT the convection term:


$\displaystyle \frac{\partial u}{\partial t} - \frac{\partial}{\partial x}\left(D\frac{\partial u}{\partial x}\right) = f(x,t)$


However, I am unsure of how to properly implement the convection term. I currently have

$\displaystyle \int_{\Omega}\frac{\partial}{\partial x}(Cu)v = -\int_{\Omega}Cu\frac{\partial v}{\partial x} + \{Cu^{up}\}\left[v\right]$

where the { } indicate the average and the [ ] indicate the jump. My professor told me to implement the upwinding method like this:

if $\displaystyle {C} \ge 0$
$\displaystyle u^{up} = u(x^{-})$
else
$\displaystyle u^{up} = u(x^{+})$


I've implemented this as best as I can but it's already pretty terrible for the case when C = D = 1. I can get better accuracy with the plain old CG method for this case.


I know no one can help me with the code but is this scheme even correct?