The flow characteristics of the large scale roughness on the mild slope channel were studied experimentally and the following facts were found.
1. On the flow over a sill, the relations among the flow surface profile classification, the energy loss and the flow conditions showed in a diagram.
2. As the expression of the energy loss of the large scale roughness, the form loss coefficient
f and the effective drag coefficient β
2CD (
CD: the form drag coefficient of roughness element, β: the ratio of degradation of fluid force acting on the element due to the covering by the upstream roughness element) were used for adjustment of test data. The relations of
f-
n (
n: the roughness setting rank number), and β
2CD-
n were found on each testing cases. In generally,
f increased and β
2CD-
n decreased with increasing
n.
3. On the sill group, the largest resistance were obtained at the case of
S1/
D=10 (
S1: flow-ward sill setting space,
D: height of sill). The relations of
f-n, β-
n and
CD-
Dr were obtaind by the experimental equations.(
Dr=
D/
H2,
H2: downstream station depth)
4. On the block roughness group, the 9 cases that combined the 4 arrangement patterns with the 4 block shapes were tested.
The relation between classification of overflow surface profile and the flow conditions are shown in diagram and these characteristics were about the same with the sill cases.
On the resistance characteristics, the relations
f-n, β-
n and
CD-
Dr, were obtained as the experimental equations for the each tested case.
5. The influence of the arrangement of blocks to the energy loss were tested under the same condition of the block shape, setting rank number, and flow condition.
The energy loss were afected largely by the
BrDr (
Br=Σ
b/
B,
B: the width of channel, Σ
b: the sum of each transverse-ward block width on a rank.) and
S1. At the
BrDr>0.103 of the zigzag arrangement, the energy loss increased with decreasing
S1 as far as some
S1. But at the
BrDr<0.103, the loss did not vary with
S1 variation and showed a nearly constant value.
The lattice looking arrangement showed a loss smaller than the zigzag's one at small
S1 but the difference of both the losses lessened with increase in
S1 and at last both the losses became the same.
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