The flow characteristics of the artificial large-scale roughness (bar roughness and block roughness) on a steep-slope channel were studied experimentally, with the following being obtained.
The flow over the roughness surface of a steep slope channel can be classified into tumbling flow, disturbed flow and quasi-smooth flow (each term is provisional).
The conditions of occurrence and flow characteristics of these flows were studied.
1. The conditions of occurrence of the tumbling flow were found due to the relation between the roughness arrangement (element height and spacing) and the flow properties for the cases of the bar roughness and the block roughness, respectively.
The discharge relationship of this flow was shown as a function of the overflow depth of the element at bar roughness or the overflow depth and element height at block roughness.
2. Regarding the quasi-smooth flow of the bar roughness, at first the boundary between the disturbed flow was shown as an experimental relationship related to the channel slope, element height and spacing and flow properties. The resistance of this flow was adjusted using the Knight-Macdonald's method for a mild slope bar roughness channel, that is, the tested data were regulated by resistance equation
V/U*=
k log (
h/χ) (where,
V: mean velocity,
U*: friction velocity,
h: depth of flow, χ; a parameter that depends upon the roughness states,
k coefficient). The tested data were classified into 2 groups of
k=6. 30 and
k=10. 50, depending on the roughness state and depth. The boundary relationships of these groups were found, and then the estimate methods of χ shown for each group. All tested data agreed with the resistance equation.
3. Regarding the quasi-smooth flow of the block roughness, at first the boundary between the disturbed flow was shown as an experimental relationship, and then, the resistance of this flow. was adjusted by the same method for bar roughness.
k is 5. 80 in this flow. The estimate method of χ was shown and it was shown that all tested data coincided with the resistance equation.
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