Geoscience Reference
In-Depth Information
n
+
1
n
Numerical stability requires r
=| δ
1
|
, which implies that for the implicit
scheme,
Q n + 1
tk , i
θ(
1
e k )
t
+
1
2 A n + 1
m , i
A b , i + 1
(5.154)
+
1
L n + 1
t , i
p m )
(
1
+
1
and for the explicit scheme,
Q n + 1
tk , i
θ(
e k )
1
1
t
+
2 A n + 1
m , i
A b , i + 1
(5.155)
+
1
L n + 1
t , i
(
1
p m )
+
1
A n + 1
m , i
1 , then p bk , i + 1 is the bed-material
gradation in the second layer, the influence of which is assumed to be negligible on
the numerical stability of the bed-material gradation in the mixing layer. Thus, the
bed-material gradation error is governed by
A m , i + 1 <
For erosion, usually
A b , i + 1 +
+
Q n + 1
tk , i
n A m , i + 1 (
f 2
f 1 e k )(
1
θ
)
p
+
1
n
+
1
δ
= δ
(5.156)
A n + 1
m , i
f 1 e k p Q n + 1
tk , i
+ (
f 2
+
1
+
1
from which it is known that the implicit scheme is unconditionally stable, and the
stability condition for the explicit scheme is
Q n + 1
tk , i
θ(
1
e k
)
t
+
1
A m , i + 1 +
A n + 1
m , i
(5.157)
L n + 1
t , i
+
1
(
p m )
1
+
1
By definition, the mixing layer should be thicker than the change in bed elevation,
i.e., A n + 1
m
1, the stability condition (5.154) for the implicit
scheme is automatically satisfied; conditions (5.155) and (5.157) require upper limits
for the time step
≥|
A b
|
. Because e k
<
t in the explicit scheme. It is evident that the implicit scheme is
much more stable than the explicit scheme.
Requirement of non-negative bed-material gradation
In calculating bed-material gradation, negative values may occur under certain
conditions. Of course, this is a non-physical phenomenon and must be eliminated.
The condition p n + 1
bk , i
1
0 for Eq. (5.152) implies that
+
A m , i + 1 (
Q n + 1
tk , i
p bk , i + 1
f 1 e 0 k
+
f 0 k
+[
f 2
f 1 e k
)(
1
θ
)
]
p
+
1
A n + 1
m , i
A m , i + 1
p bk , i + 1
+ (
A b , i + 1 )
0
(5.158)
+
1
 
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