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Wu et al . (2005) applied the formula of Wu et al . (2000b) to compute the bed load
in vegetated channels, with the effective bed shear stress
τ b determined by
τ
= γ
R s S
(10.36)
b
where S is the channel slope; and R s is the hydraulic radius, defined in Eq. (10.17), as
suggested by Barfield et al . (1979). The computed values of bed-load transport rate
were compared with the measured data (Series A, q
0.0065 m 2 s 1 ) of Jordanova
and James (2003), as shown in Fig.10.8. An excellent agreement was observed.
=
Figure 10.8 Measured and predicted bed-load rates in a vegetated flume.
Okabe et al . (1997) investigated the bed-load transport in a flume covered by
submerged vegetation. They modeled the vegetation using curved, cylindrical silicone
tubes and branched, inclined brass lines. They used a vertical 1-D k -
turbulent flow
model to determine the effective bed shear stress and applied the formula of Ashida and
Michiue (1972) for the bed-load transport rate in vegetated channels. The agreement
between the measured and predicted values was generally good.
It can be seen fromOkabe et al . (1997) and Wu et al . (2005) that bed-load transport
is mainly related to bed shear rather than the drag force exerted on vegetation elements.
If the effective bed shear is used, some existing bed-load formulas developed for non-
vegetated channels can be extended to the case of vegetated channels.
However, the suspended-load transport in vegetated channels has been little investi-
gated. Because vegetation may reduce the mean flow velocity significantly but intensify
the turbulence in a vegetated zone, the effect of vegetation on suspended-load transport
is more complex. More experimental and theoretical studies are needed to quantify this
effect. As an approximation, one may apply some existing suspended load formulas
ε
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