ASHRAE HVAC SYSTEMS AND EQUIPMENT IP CH 40-2012 COOLING TOWERS.pdf
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1、40.1CHAPTER 40COOLING TOWERSPrinciple of Operation . 40.1Design Conditions 40.2Types of Cooling Towers 40.2Materials of Construction 40.9Selection Considerations . 40.10Application. 40.10Performance Curves. 40.17Cooling Tower Thermal Performance . 40.18Cooling Tower Theory 40.18Tower Coefficients 40
2、.21Additional Information. 40.23OST air-conditioning systems and industrial processes gen-Merate heat that must be removed and dissipated. Water iscommonly used as a heat transfer medium to remove heat from re-frigerant condensers or industrial process heat exchangers. In thepast, this was accomplis
3、hed by drawing a continuous stream ofwater from a utility water supply or a natural body of water, heatingit as it passed through the process, and then discharging the waterdirectly to a sewer or returning it to the body of water. Water pur-chased from utilities for this purpose has become prohibiti
4、vely ex-pensive because of increased water supply and disposal costs.Similarly, cooling water drawn from natural sources is relativelyunavailable because the ecological disturbance caused by the in-creased temperature of discharge water has become unacceptable.Air-cooled heat exchangers cool water b
5、y rejecting heat directlyto the atmosphere, but the first cost and fan energy consumption ofthese devices are high and the plan area required is relatively large.They can economically cool water to within approximately 20F ofthe ambient dry-bulb temperature: too high for the cooling waterrequirement
6、s of most refrigeration systems and many industrialprocesses.Cooling towers overcome most of these problems and thereforeare commonly used to dissipate heat from refrigeration, air-conditioning, and industrial process systems. The water consump-tion rate of a cooling tower system is only about 5% of
7、 that of aonce-through system, making it the least expensive system tooperate with purchased water supplies. Additionally, the amountof heated water discharged (blowdown) is very small, so the eco-logical effect is greatly reduced. Lastly, cooling towers can coolwater to within 4 to 5F of the ambien
8、t wet-bulb temperature,which is always lower than the ambient dry-bulb, or approxi-mately 35F lower than can air-cooled systems of reasonable size(in the 250 to 500 ton range). This lower temperature improves theefficiency of the overall system, thereby reducing energy use sig-nificantly and increas
9、ing process output.PRINCIPLE OF OPERATIONA cooling tower cools water by a combination of heat and masstransfer. Water to be cooled is distributed in the tower by spray noz-zles, splash bars, or film-type fill, which exposes a very large watersurface area to atmospheric air. Atmospheric air is circul
10、ated by(1) fans, (2) convective currents, (3) natural wind currents, or(4) induction effect from sprays. A portion of the water absorbs heatto change from a liquid to a vapor at constant pressure. This heat ofvaporization at atmospheric pressure is transferred from the waterremaining in the liquid s
11、tate into the airstream.Figure 1 shows the temperature relationship between water andair as they pass through a counterflow cooling tower. The curvesindicate the drop in water temperature (A to B) and the rise in theair wet-bulb temperature (C to D) in their respective passagesthrough the tower. The
12、 temperature difference between the waterentering and leaving the cooling tower (A minus B) is the range.For a steady-state system, the range is the same as the water tem-perature rise through the load heat exchanger, provided the flowrate through the cooling tower and heat exchanger are the same.Ac
13、cordingly, the range is determined by the heat load and waterflow rate, not by the size or thermal capability of the cooling tower.The difference between the leaving water temperature and enter-ing air wet-bulb temperature (B minus C) in Figure 1 is the approachto the wet-bulb or simply the approach
14、 of the cooling tower. Theapproach is a function of cooling tower capability. A larger coolingtower produces a closer approach (colder leaving water) for a givenheat load, flow rate, and entering air condition. Therefore, theamount of heat transferred to the atmosphere by the cooling tower isalways
15、equal to the heat load imposed on the tower, whereas thetemperature level at which the heat is transferred is determined bythe thermal capability of the cooling tower and the entering air wet-bulb temperature.Thermal performance of a cooling tower depends mainly on theentering air wet-bulb temperatu
16、re. The entering air dry-bulb tem-perature and relative humidity, taken independently, have an insig-nificant effect on thermal performance of mechanical-draft coolingtowers, but do affect the rate of water evaporation in the coolingtower. A psychrometric analysis of the air passing through a cool-i
17、ng tower illustrates this effect (Figure 2). Air enters at the ambientcondition point A, absorbs heat and mass (moisture) from theThe preparation of this chapter is assigned to TC 8.6, Cooling Towers andEvaporative Condensers.Fig. 1 Temperature Relationship Between Water and Air in Counterflow Cooli
18、ng Tower40.2 2012 ASHRAE HandbookHVAC Systems and Equipment water, and exits at point B in a saturated condition (at very lightloads, the discharge air may not be fully saturated). The amount ofheat transferred from the water to the air is proportional to the dif-ference in enthalpy of the air betwe
19、en the entering and leaving con-ditions (hB hA). Because lines of constant enthalpy correspondalmost exactly to lines of constant wet-bulb temperature, thechange in enthalpy of the air may be determined by the change inwet-bulb temperature of the air.Air heating (vector AB in Figure 2) may be separa
20、ted into com-ponent AC, which represents the sensible portion of the heatabsorbed by the air as the water is cooled, and component CB,which represents the latent portion. If the entering air condition ischanged to point D at the same wet-bulb temperature but at a higherdry-bulb temperature, the tota
21、l heat transfer (vector DB) remains thesame, but the sensible and latent components change dramatically.DE represents sensible cooling of air, whereas EB represents latentheating as water gives up heat and mass to the air. Thus, for the samewater-cooling load, the ratio of latent to sensible heat tr
22、ansfer canvary significantly.The ratio of latent to sensible heat is important in analyzing waterusage of a cooling tower. Mass transfer (evaporation) occurs only inthe latent portion of heat transfer and is proportional to the changein specific humidity. Because the entering air dry-bulb temperatur
23、eor relative humidity affects the latent to sensible heat transfer ratio,it also affects the rate of evaporation. In Figure 2, the rate of evapo-ration in case AB (WB WA) is less than in case DB (WB WD)because the latent heat transfer (mass transfer) represents a smallerportion of the total.The evap
24、oration rate at typical design conditions is approximately1% of the water flow rate for each 12.5F of water temperature range;however, the average evaporation rate over the operating season isless than the design rate because the sensible component of total heattransfer increases as entering air tem
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