Geoscience Reference
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problem is
|+ gh
|
q
/
h
t
<
1
(9.57)
x
and for the 2-D problem is
gh
gh
|
U x
|+
+ |
U y
|+
t
<
1
(9.58)
x
y
However, the stability of each numerical scheme also may rely on its own formu-
lation, and the longest time step allowed for a stable solution varies among different
schemes.
To relax the restriction on time step imposed by the CFL conditions, Molls and
Chaudhry (1995) adopted the ADI method and Delis et al . (2000) established implicit
TVD schemes for 1-D St. Venant equations. It has been found that longer time steps can
be used in implicit algorithms, and the computational cost may be reduced. However,
implicit schemes may induce numerical diffusion. This is demonstrated in the following
example using the SIMPLEC algorithm
Figure 9.9 Dam-break waves at 30 s simulated using SIMPLEC.
 
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