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Handbook of air conditioning and refrigeration / Shan K

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7.38 CHAPTER SEVEN<br />

The wire-to-water efficiency <strong>of</strong> a water system � ww, expressed either in dimensionless form or as<br />

a percentage, is defined as the ratio <strong>of</strong> energy output from water to the energy input to the electric<br />

wire connected to the motor. It can be calculated as<br />

� ww � � p� dr� mot<br />

(7.15)<br />

The total efficiency <strong>of</strong> the centrifugal pump � p can be obtained from the pump manufacturer or calculated<br />

from Eq. (7.8). The pump efficiency � p depends on the type <strong>and</strong> size <strong>of</strong> pump as well as the<br />

percentage <strong>of</strong> design volume flow rate during operation. Pump efficiency usually varies from 0.7 to<br />

0.85 at the design volume flow rate. Drive efficiency � dr indicates the efficiency <strong>of</strong> a direct drive,<br />

belt drive, <strong>and</strong> various types <strong>of</strong> variable-speed drives. For direct drive, � dr � 1. Among variablespeed<br />

drives, an adjustable-frequency alternating-current (ac) drive has the highest drive efficiency.<br />

For a 25-hp (18.7-kW) motor, � dr <strong>of</strong>ten varies from 0.96 at design flow to 0.94 at 30 percent design<br />

flow to 0.80 at 20 percent design flow. Motor efficiency � mot depends on the type <strong>and</strong> size <strong>of</strong> motor.<br />

It normally varies from 0.91 for a 10-hp (7.5-kW) high-efficiency motor to 0.96 for a 250-hp (187kW)<br />

motor as listed in Table 6.2.<br />

7.9 OPERATING CHARACTERISTICS OF CHILLED<br />

WATER SYSTEM<br />

Many chilled <strong>and</strong> hot water systems used in commercial central hydronic <strong>air</strong> <strong>conditioning</strong> systems<br />

<strong>of</strong>ten have their central plant located in the basement, ro<strong>of</strong>top, or equipment floors <strong>of</strong> the building.<br />

The hot/chilled water from the boiler/chiller in the central plant is then supplied to the coils <strong>and</strong> terminals<br />

<strong>of</strong> various zones in one building or in adjacent buildings by means <strong>of</strong> supply main pipes.<br />

Water returns from the coils <strong>and</strong> terminals to the central plant via the return mains.<br />

Coil Load <strong>and</strong> Chilled Water Volume Flow<br />

In AHUs or fan coils, two-way control valves are currently widely used to modulate the water<br />

volume flow rate so as to maintain a predetermined <strong>air</strong> discharge temperature or space temperature<br />

at reduced system loads. Coils, especially oversized coils, operate at design load usually less than 5<br />

percent <strong>of</strong> their total operating time. For a typical coil, nearly 60 percent <strong>of</strong> the operating time may<br />

correspond to a coil load <strong>of</strong> 35 to 65 percent <strong>of</strong> the design value.<br />

During part-load operation, the required fraction <strong>of</strong> design volume flow rate <strong>of</strong> chilled water<br />

flowing through a coil V˙<br />

w is not equal to the fraction <strong>of</strong> design sensible coil load Qcs Btu/h (W)<br />

which is the sensible heat transfer from the coil to the conditioned <strong>air</strong>, as shown in Fig. 7.17a. In<br />

Fig. 7.17a, indicates the design chilled water volume flow rate, gpm (m 3 /min), <strong>and</strong> Q cs,d the<br />

V˙ w,d<br />

design sensible coil load, Btu/h (W). This is because <strong>of</strong> the characteristics <strong>of</strong> sensible heat transfer<br />

described by<br />

Qcs � AoUo�Tm where Ao � outer surface area <strong>of</strong> coil, ft2 (m2 )<br />

Uo � overall heat-transfer coefficient based on outer area, Btu/h�ft2�°F (W/m2�°C) �Tm � logarithmic temperature between conditioned <strong>air</strong> <strong>and</strong> chilled water,°F (°C)<br />

(7.16)<br />

When the volume flow rate <strong>of</strong> chilled water V˙<br />

w is reduced, the decrease in the product <strong>of</strong> AoUo�Tm is not the same as the reduction in the chilled water volume flow rate V˙<br />

w.<br />

When V˙ w drops, the outer<br />

surface area Ao remains the same <strong>and</strong> Uo is slightly reduced. Only a considerable rise in chilled<br />

water temperature across the coil �Tw,c � Twl � Twe, as shown in Fig. 7.17b, can reduce �Tm suffi-

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