fluid_mechanics
554 Chapter 10 ■ Open-Channel Flow where n eff is the effective value of n for this channel. With Q 16.8 ft 3 s as determined above, the value of is found to be n eff 1.49AR2 3 12 h S 0 Q 1.4916.4210.59322 3 10.0022 1 2 16.8 0.0179 As expected, the effective roughness 1Manning n2 is between the minimum 1n 2 0.0152 and maximum 1n 3 0.0302 values for the individual subsections. By repeating the calculations for various depths, y, the results shown in Fig. E10.6b are obtained. Note that there are two distinct portions of the graph—one when the water is contained entirely within the main, center channel 1y 6 0.8 ft2; the other when the water overflows into the side portions of the channel 1y 7 0.8 ft2. n eff Q, ft 3 /s 40 30 20 10 (1.4 ft, 16.8 ft 3 /s) 0 0 0.5 1 y, ft F I G U R E E10.6b 1.5 2 For a given flowrate, the channel of minimum area is denoted as the best hydraulic cross section. One type of problem often encountered in open-channel flows is that of determining the best hydraulic cross section defined as the section of the minimum area for a given flowrate, Q, slope, S 0 , and roughness coefficient, n. By using R h AP we can write Eq. 10.20 as which can be rearranged as Q k 23 n A aA P b S 1 2 0 k A 53 S 1 2 0 n P 2 3 A a nQ kS 1 2 0 35 b P 2 5 where the quantity in the parentheses is a constant. Thus, a channel with minimum A is one with a minimum P, so that both the amount of excavation needed and the amount of material to line the surface are minimized by the best hydraulic cross section. The best hydraulic cross section possible is that of a semicircular channel. No other shape has as small a wetted perimeter for a given area. It is often desired to determine the best shape for a class of cross sections. The results (given here without proof) for rectangular, trapezoidal (with 60° sides), and triangular shapes are shown in Fig. 10.11. For example, the best hydraulic cross section for a rectangle is one whose depth is half its width; for a triangle it is a 90° triangle. 10.5 Gradually Varied Flow In many situations the flow in an open channel is not of uniform depth 1y constant2 along the channel. This can occur because of several reasons: The bottom slope is not constant, the crosssectional shape and area vary in the flow direction, or there is some obstruction across a portion of the channel. Such flows are classified as gradually varying flows if dydx 1. If the bottom slope and the energy line slope are not equal, the flow depth will vary along the channel, either increasing or decreasing in the flow direction. In such cases dydx 0, dVdx 0, and the right-hand side of Eq. 10.10 is not zero. Physically, the difference between the b y = b/2 b y = √3b/2 60° 90° b F I G U R E 10.11 Best hydraulic cross sections for a rectangle, a 60º trapezoid, and a triangle.
10.6 Rapidly Varied Flow 555 component of weight and the shear forces in the direction of flow produces a change in the fluid momentum that requires a change in velocity and, from continuity considerations, a change in depth. Whether the depth increases or decreases depends on various parameters of the flow, with a variety of surface profile configurations [flow depth as a function of distance, y y 1x2] possible (Refs. 5, 9). 10.6 Rapidly Varied Flow In many cases the flow depth may change significantly in a short distance. V10.8 Erosion in a channel In many open channels, flow depth changes occur over a relatively short distance so that dydx 1. Such rapidly varied flow conditions are often quite complex and difficult to analyze in a precise fashion. Fortunately, many useful approximate results can be obtained by using a simple onedimensional model along with appropriate experimentally determined coefficients when necessary. In this section we discuss several of these flows. Some rapidly varied flows occur in constant area channels for reasons that are not immediately obvious. The hydraulic jump is one such case. As is indicated in Fig. 10.12, the flow may change from a relatively shallow, high-speed condition into a relatively deep, low-speed condition within a horizontal distance of just a few channel depths. Other rapidly varied flows may be due to a sudden change in the channel geometry such as the flow in an expansion or contraction section of a channel as is indicated in Fig. 10.13. In such situations the flow field is often two- or three-dimensional in character. There may be regions of flow separation, flow reversal, or unsteady oscillations of the free surface. For the purpose of some analyses, these complexities can be neglected and a simplified analysis can be undertaken. In other cases, however, it is the complex details of the flow that are the most important property of the flow; any analysis must include their effects. The scouring of a river bottom in the neighborhood of a bridge pier, as is indicated in Fig. 10.14, is such an example. A one- or two-dimensional model of this flow would not be sufficient to describe the complex structure of the flow that is responsible for the erosion near the foot of the bridge pier. Many open-channel flow-measuring devices are based on principles associated with rapidly varied flows. Among these devices are broad-crested weirs, sharp-crested weirs, critical flow flumes, and sluice gates. The operation of such devices is discussed in the following sections. F I G U R E 10.12 Hydraulic jump. V10.9 Bridge pier scouring Flow F I G U R E 10.13 Rapidly varied flow may occur in a channel transition section.
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10.6 Rapidly Varied Flow 555<br />
component of weight and the shear forces in the direction of flow produces a change in the <strong>fluid</strong><br />
momentum that requires a change in velocity and, from continuity considerations, a change in<br />
depth. Whether the depth increases or decreases depends on various parameters of the flow, with<br />
a variety of surface profile configurations [flow depth as a function of distance, y y 1x2] possible<br />
(Refs. 5, 9).<br />
10.6 Rapidly Varied Flow<br />
In many cases the<br />
flow depth may<br />
change significantly<br />
in a short distance.<br />
V10.8 Erosion in a<br />
channel<br />
In many open channels, flow depth changes occur over a relatively short distance so that dydx 1.<br />
Such rapidly varied flow conditions are often quite complex and difficult to analyze in a precise<br />
fashion. Fortunately, many useful approximate results can be obtained by using a simple onedimensional<br />
model along with appropriate experimentally determined coefficients when necessary.<br />
In this section we discuss several of these flows.<br />
Some rapidly varied flows occur in constant area channels for reasons that are not immediately<br />
obvious. The hydraulic jump is one such case. As is indicated in Fig. 10.12, the flow may change<br />
from a relatively shallow, high-speed condition into a relatively deep, low-speed condition within<br />
a horizontal distance of just a few channel depths. Other rapidly varied flows may be due to a<br />
sudden change in the channel geometry such as the flow in an expansion or contraction section of<br />
a channel as is indicated in Fig. 10.13.<br />
In such situations the flow field is often two- or three-dimensional in character. There may be<br />
regions of flow separation, flow reversal, or unsteady oscillations of the free surface. For the purpose<br />
of some analyses, these complexities can be neglected and a simplified analysis can be undertaken.<br />
In other cases, however, it is the complex details of the flow that are the most important property of<br />
the flow; any analysis must include their effects. The scouring of a river bottom in the neighborhood<br />
of a bridge pier, as is indicated in Fig. 10.14, is such an example. A one- or two-dimensional model<br />
of this flow would not be sufficient to describe the complex structure of the flow that is responsible<br />
for the erosion near the foot of the bridge pier.<br />
Many open-channel flow-measuring devices are based on principles associated with rapidly<br />
varied flows. Among these devices are broad-crested weirs, sharp-crested weirs, critical flow flumes,<br />
and sluice gates. The operation of such devices is discussed in the following sections.<br />
F I G U R E 10.12<br />
Hydraulic jump.<br />
V10.9 Bridge pier<br />
scouring<br />
Flow<br />
F I G U R E 10.13 Rapidly varied<br />
flow may occur in a channel transition section.