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chapter 3 hydraulics of open channel flow

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3.22 Chapter Three<br />

V2<br />

1 V2<br />

2<br />

z1 � α1 �� � z2 � α2 �� � hf + he 2g<br />

2g<br />

(3.61)<br />

where z1 and z2 � elevation <strong>of</strong> the water surface above a datum at Stations 1 and 2, respectively,<br />

he � eddy and other losses incurred in the reach, and hf � reach friction loss.<br />

The friction loss can be obtained by multiplying a representative friction slope, Sf,by the length <strong>of</strong> the reach, L. Four equations can be used to approximate the friction loss<br />

between two cross sections:<br />

S� f � ⎛ ⎜ �<br />

⎝ Q1<br />

� Q2<br />

K �<br />

2<br />

(average conveyance) (3.62)<br />

and<br />

V2<br />

1<br />

α1 �� 2g<br />

z 1<br />

y 1<br />

HYDRAULICS OF OPEN CHANNEL FLOW<br />

FIGURE 3.7 Energy relationship between two <strong>channel</strong> sections.<br />

1<br />

�<br />

K2 ⎞ ⎟<br />

⎠<br />

S� f � � Sf1 � Sf2 � (average friction slope) (3.63)<br />

2<br />

2 Sf1<br />

S� f � �<br />

S �<br />

Sf2<br />

� (harmonic mean friction slope) (3.64)<br />

S<br />

f1<br />

Energy Grade Line (S f)<br />

Water Surface (S w)<br />

Channel Bottom (S o)<br />

f2<br />

�x�L<br />

h f ��x<br />

V2<br />

2<br />

α2 �� 2g<br />

S� f � �S� f1 �S� f2 � (geometric mean friction slope) (3.65)<br />

The selection <strong>of</strong> a method to estimate the friction slope in a reach is an important decision<br />

and has been discussed in the literature. Laurenson (1986) suggested that the “true”<br />

friction slope for an irregular cross section can be approximated by a third-degree poly-<br />

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y 2<br />

z 2

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