304 CHAPTER TWELVE
For pipes flowing full:
(12.29)
(12.30)
(12.31)
(12.32)
where Vvelocity, ft /s (m /s)
C 1 coefficient, dependent on surface roughness (given in engineering
handbooks)
Rhydraulic radius, ft (m)
Shead loss due to friction, ft/ft (m/m) of pipe
Ddiameter of pipe, ft (m)
Llength of pipe, ft (m)
Qdischarge, ft^3 /s (m^3 /s)
hffriction loss, ft (m)
Figure 12.7 shows a typical three-reservoir problem. The elevations of the
hydraulic grade lines for the three pipes are equal at point D. The Hazen–Williams
equation for friction loss can be written for each pipe meeting at D. With the conti-
nuity equation for quantity of flow, there are as many equations as there are
unknowns:
ZbZd
PD
w
4.727LB
D4.87B
QB
CB
1.85
ZaZd
PD
w
4.727LA
D4.87A
QA
CA
1.85
D
1.376
S0.205
Q
C 1
0.38
hf
4.727
D4.87
L
Q
C 1
1.85
Q0.432C 1 D2.63S0.54
V0.55C 1 D0.63S0.54
Za
Zc
Datum
Zd
Zb
A
C
PD
W
B
D
FIGURE 12.7 Flow between reservoirs.