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108 Chapter 3
Table 3.2.4 Specified Variables - Cooling Tower Analysis
Variable Quantity Units
m 3 291300 Ibmol/h
t 1 94.0 °F
tiw 80.0 °F
ts 109.0 °F
tR 32.0 °F
19350 Btu/lbmol
Ah v,32 F
P 14.7 psia
C P1 1 « Cpj 1 8.2 Btu/lbmol-°F
Cpi 2 * Cp2,2 7.2 Btu/lbmol-°F
Cpa * Cp4 18.0 Btu/lbmol-°F
h/k 5.93 Btu/lbmol-°F
R 1.986 Btu/lbmol-°F
Table 3.2.4 lists the specified variables. The cooling tower is processing 40
rrrVmin (1410 fWrnin) of water at 109 °F (43.8 °C), which from the steam tables,
has a specific volume of 0.01616 ft3/lb (l.OlxlO" 3 m3/kg). Thus,
40.0 m 3 60 min 35.31 ft 3 1 Ib 1 Ibmol Ibmol
1 min 1 h 1m 3 0.01616 ft 3 18 Ib h
Finally, we can solve the equations listed in Table 3.2.2 simultaneously using
POLYMATH [19] or some other suitable mathematical software. The solution
procedure used in POLYMATH is the bounded Newton-Raphson method de-
scribed by Shacham and Shacham [20]. Table 3.2.5 lists the stream properties,
which include the solution to the equations and specified temperatures and pres-
sures at each line. The difference in the water flow rates into and out of the cooling
tower is the water evaporated. Thus, to cool 164,700 Ibmol/h (74,700 kg mol/h)
water requires evaporating 5,200 Ibmol/h (2,360 kg mol/h) of water. The evapo-
rated water, along with water lost because of leaks, blowdown, and drift are a cost
of operation.
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