NUEN-430 Lecture 4

Now we consider the equation we want to solve we

Info iconThis preview shows page 1. Sign up to view the full content.

View Full Document Right Arrow Icon
This is the end of the preview. Sign up to access the rest of the document.

Unformatted text preview: se its error is proportional to rather than . Now we consider the equation we want to solve: () () () () We assume a uniform grid of the following form Where , and We will initially assume consistent cross sections throughout the mesh. This simplifies matters considerable. An alternative is to require constant cross-sections within each cell, but allow the cross sections to vary between cells. This complicates matters, because we must build the interface conditions into the scheme. Since we are developing a finite volume scheme, we obtain the basic equation for a single cell by integrating the diffusion equation over the cell; ∫ ∫ This balance equation suggests that we have scalar fluxes at cell centers and currents at cell edges. The above equation is actually exact, but now we introduce an approximation through the cell-centered a flux. Next we further introduce approximations by using central-difference approximations for the currents: ( ) Substituting this expression into our approximate balance equation, we obtain our interior-mesh discretization: ( ) ( ) Now, we must derive a differe...
View Full Document

This note was uploaded on 10/06/2013 for the course NEUN 430 taught by Professor Morel during the Fall '10 term at Texas A&M.

Ask a homework question - tutors are online