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r = (2.3.3b) t 2: x The initial and boundary conditions (2.3.1b, 2.3.1c) are
0 Uj =( j ) x j =0 1 ::: J (2.3.3c) 18 Finite Di erence Methods
n 0 U = n UJ =0 n> 0 (2.3.3d) : The computational stencil for (2.3.3a) is shown in Figure 2.3.2. The parameter
analogous to the Courant number (2.2.3) for the kinematic wave equation (2.2.1). 11
00 is n+1 11
00 j-1 r 11
00 j n j+1 Figure 2.3.2: Computational stencil of the forward time-centered space scheme (2.3.3a)
for the heat conduction equation (2.3.1a).
The solution of (2.3.3a) is obtained in the same manner as the nite di erence
solutions of (2.2.2b) and (2.2.4) for the kinematic wave equation (2.2.1). Thus, using the initial data (2.3.3c), we calculate a solution j1 at the interior mesh points,
; 1, of time level 1 using (2.3.3a) with ranging from 1 to ; 1. The
boundary conditions (2.3.3d) with = 1 determine 01 and J . Knowing the discrete
solution at time level 1, we proceed to determine it at time level 2, etc. in the sam...
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This document was uploaded on 03/16/2014 for the course CSCI 6840 at Rensselaer Polytechnic Institute.
- Spring '14