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bU z
bU x U z
bU z )
( T zx
+ D zx
b p
∂(
)
+ ∂(
)
+ ∂(
1
ρ
1
ρ
[
b
) ]
=−
bg
z +
t
x
z
x
( T zz
+ D zz
1
ρ
[
b
) ]
1
ρ (
+
m 1
τ
+
m 2
τ
)
z 1
z 2
z
(2.97)
p and T ij
where
are the width-averaged pressure and stresses, respec-
tively; D ij are the dispersion momentum transports due to the lateral non-uniformity
of flow velocity, defined as D xx
(
i , j
=
x , z
)
=− b b 2
=− b b 2
U x
2 dy , D xz
= D zx
b 1 (
u x
)
b 1
=− b b 2
u x U x )(
u z U z )
dy , and D zz
u z U z )
2 dy ;
(
b 1 (
τ xl and
τ zl (
=
)
are the
shear stresses in the x - and z -directions on the two bank surfaces; and m l are the bank
slope coefficients, defined as m l =[
l
1, 2
2 .
For gradually varied flows, the effects of inertia, diffusion, and dispersion in the
vertical momentum equation (2.97) can be neglected, yielding the hydrostatic pressure
equation (2.65). The x -momentum equation (2.96) is then turned to
2
2
1
/
1
+ (∂
b l /∂
x
)
+ (∂
b l /∂
z
)
]
bU x )
bU x )
bU z U x )
( T xx + D xx ) ]
∂(
+ ∂(
+ ∂(
gb ˜
z s
1
ρ
[
b
=−
x +
t
x
z
x
( T xz
+ D xz
1
ρ
[
b
) ]
1
ρ (
+
m 1
τ
+
m 2
τ
)
x 1
x 2
z
(2.98)
where
z s is the laterally-averaged water surface elevation.
Integrating Eq. (2.72) over the flow width leads to the width-integrated suspended-
load transport equation:
˜
bC
bU x C
bU z C
s C
∂(
)
+ ∂(
)
+ ∂(
)
∂(
b
ω
)
t
x
z
z
b
x + D sx
b
+ D sz
s C
s C
=
+
ε
ε
+
S c
(2.99)
x
z
z
where C is the width-averaged concentration of suspended load; D sx and D sz are
the dispersion fluxes, defined as D sx
b b 2
U x
C
dy and D sz
1
1
b
=−
b 1 (
u x
)(
c
)
=−
b 2
u z U z )(
C
dy ; and S c includes the sediment exchange at banks and the side
discharge from tributaries.
The bed-load zone is so thin that it is not necessary to consider the vertical variation
of sediment concentration in this zone. The width-integrated bed-load transport is
determined using the 1-D transport equation introduced in the next subsection.
b 1 (
c
)
 
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