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Science of Water : Concepts and Applications

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<strong>Water</strong> Hydraulics 69<br />

•<br />

•<br />

•<br />

•<br />

•<br />

•<br />

V 1 2 /2g<br />

y 1<br />

z 1<br />

1<br />

Energy grade line<br />

Hydraulic grade line<br />

V 1<br />

Piezometers<br />

Center line <strong>of</strong> pipe<br />

Datum<br />

Pipe flow<br />

V 2<br />

2<br />

h L<br />

V 2<br />

1 /2g<br />

V 2 2 /2g<br />

y 2<br />

z 2<br />

Open channel flow<br />

V 2 2 /2g<br />

<strong>and</strong> the velocity head V 2 /2g. Figure 3.15 shows the energy grade line or energy gradient,<br />

which represents the energy from section to section. In the absence <strong>of</strong> frictional losses, the<br />

energy grade line remains horizontal, although the relative distribution <strong>of</strong> energy may vary<br />

between the elevation, pressure, <strong>and</strong> velocity heads. In all real systems, however, losses <strong>of</strong><br />

energy occur because <strong>of</strong> resistance to fl ow, <strong>and</strong> the resulting energy grade line is sloped<br />

(i.e., the energy grade line is the slope <strong>of</strong> the specifi c energy line).<br />

Specifi c energy (E)—Sometimes called specifi c head, is the sum <strong>of</strong> the pressure head<br />

y <strong>and</strong> the velocity head V 2 /2g. The specifi c energy concept is especially useful in analyzing<br />

fl ow in open channels.<br />

Steady fl ow—Occurs when the discharge or rate <strong>of</strong> fl ow at any cross section is constant.<br />

Uniform fl ow—Occurs when the depth, cross-sectional area, <strong>and</strong> other elements <strong>of</strong> fl ow<br />

are substantially constant from section to section.<br />

Nonuniform fl ow—Occurs when the slope, cross-sectional area, <strong>and</strong> velocity change from<br />

section to section. The fl ow through a Venturi section used for measuring fl ow is a good<br />

example.<br />

Varied fl ow—Flow in a channel is considered varied if the depth <strong>of</strong> fl ow changes along the<br />

length <strong>of</strong> the channel. The fl ow may be gradually varied or rapidly varied (i.e., when the<br />

depth <strong>of</strong> fl ow changes abruptly), as shown in Figure 3.16.<br />

Slope (gradient)—The head loss per foot <strong>of</strong> channel.<br />

y 1<br />

z 1<br />

1<br />

Energy grade line<br />

<strong>Water</strong> surface<br />

Channel bottom<br />

FIGURE 3.15 Comparison <strong>of</strong> pipe fl ow <strong>and</strong> open-channel fl ow. (Adapted from Metcalf & Eddy, Wastewater<br />

Engineering: Collection <strong>and</strong> Pumping <strong>of</strong> Wastewater, McGraw-Hill, New York, 1981.)<br />

FIGURE 3.16 Varied fl ow.<br />

RVF GVF RVF GVF RVF GVF RVF<br />

Sluice gate<br />

Hydraulic<br />

jump<br />

RVF – Rapidly varied flow<br />

GVF – Gradually varied flow<br />

V 1<br />

Flow over<br />

a weir<br />

V 2<br />

2<br />

h L<br />

y 2<br />

z 2<br />

Hydraulic<br />

drop

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