chapter 3 hydraulics of open channel flow
chapter 3 hydraulics of open channel flow
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