The Greenhouse-Gas Impact of Various Chiller Technologies
As more colleges and universities strive for climate neutrality, a look at the fundamentals of CO2 production
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The design operating conditions were a chiller-module size of 600 tons of cooling capacity, an evaporator design based on 1,200 gpm of chilled water cooled from 54F to 42F, and a condenser design based on 85F condenser water available at a flow rate capable of producing a 12F rise in the condenser-water stream.
Only full-load conditions were compared. For each chiller, the following were considered:
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Input energy -- the electricity, steam, or natural gas used to power the chiller and auxiliary equipment (e.g., pumps, cooling tower) or the natural gas used to power an engine creating electricity to power the chiller and auxiliary equipment.
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Recovered heat -- heat recovered from the condenser-water stream or the engine/generator producing the input electricity.
Input energy and recovered heat were determined using manufacturer data. Cooling-tower-fan power is the catalogued power needed for heat rejection. For absorption chillers, input energy included catalogued power needs for solution, refrigerant, and vacuum pumps. For chilled-water and condenser-water pumps, chiller input-power contribution was calculated based on catalogued evaporator or condenser head loss and the following formula:
Pump power (kw) = (gpm x ΔH x 0.746) (3,960 x η
where:
ΔH = evaporator or condenser head loss (feet) catalogued by chiller manufacturer
η
η
The catalogued values for each of the chiller options are given in Table 1.
High-efficiency electric centrifugal chiller
Figure 1 shows the pounds of CO
Standard-efficiency electric centrifugal chiller
Figure 2 shows the pounds of CO
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