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2000 Hook-up Book - Spirax Sarco

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SYSTEM DESIGN<br />

48<br />

Condensate Pumping<br />

In nearly all steam-using plants,<br />

condensate must be pumped<br />

from the location where it is<br />

formed back to the boilerhouse,<br />

or in those cases where gravity<br />

drainage to the boilerhouse is<br />

practical, the condensate must be<br />

lifted into a boiler feed tank or<br />

deaerator. Even where deaerators<br />

are at low level, they usually<br />

operate at a pressure a few psi<br />

above atmospheric and again, a<br />

pump is needed to lift condensate<br />

from atmospheric pressure to<br />

deaerator tank pressure.<br />

Electric Condensate<br />

Return Pumps<br />

When using electric pumps to lift<br />

the condensate, packaged units<br />

comprising a receiver tank (usually<br />

vented to atmosphere) and<br />

one or more motorized pumps<br />

are commonly used. It is important<br />

with these units to make sure<br />

that the maximum condensate<br />

temperature specified by the<br />

manufacturer is not exceeded,<br />

and the pump has sufficient<br />

capacity to handle the load.<br />

Condensate temperature usually<br />

presents no problem with returns<br />

from low pressure heating systems.<br />

There, the condensate is<br />

often below 212°F as it passes<br />

through the traps, and a little further<br />

subcooling in the gravity<br />

return lines and in the pump<br />

receiver itself means that there is<br />

little difficulty in meeting the maximum<br />

temperature limitation. See<br />

Fig. II-74 (page 119).<br />

On high pressure systems,<br />

the gravity return lines often contain<br />

condensate at just above<br />

212°F, together with some flash<br />

steam. The cooling effect of the<br />

piping is limited to condensing a<br />

little of the flash steam, with the<br />

remainder passing through the<br />

vent at the pump receiver. The<br />

water must remain in the receiver<br />

for an appreciable time if it is to<br />

cool sufficiently, or the pump discharge<br />

may have to be throttled<br />

down to reduce the pump’s capacity<br />

if cavitation is to be avoided.<br />

See Fig. II-75 (page 119).<br />

The PUMP NPSH in any given application can readily be estimated<br />

from:<br />

NPSH = hsv = 144 (Pa - Pvp) + hs - hf<br />

W<br />

Where:<br />

Pa = Absolute pressure in<br />

receiver s<strong>up</strong>plying pump,<br />

in psi (that is at atmospheric<br />

pressure in the<br />

case of a vented receiver).<br />

Pvp= Absolute pressure of<br />

condensate at the liquid<br />

temperature, in psi.<br />

The absolute pressure at the<br />

inlet to the pump is usually the<br />

atmospheric pressure in the<br />

receiver, plus the static head from<br />

the water surface to the pump<br />

inlet, minus the friction loss<br />

through pipes, valves and fittings<br />

between the receiver and the<br />

pump. If this absolute pressure<br />

exceeds the vapor pressure of<br />

water at the temperature at which<br />

it enters the pump, then a Net<br />

Positive Suction Head exists.<br />

Providing this NPSH is above the<br />

value specified by the pump manufacturer,<br />

the water does not<br />

begin to boil as it enters the pump<br />

suction, and cavitation is avoided.<br />

If the water entering the pump is<br />

at high temperature, its vapor<br />

pressure is increased and a<br />

greater hydrostatic head over the<br />

pump suction is needed to ensure<br />

that the necessary NPSH is<br />

obtained.<br />

If the water does begin to boil<br />

in the pump suction, the bubbles<br />

of steam are carried with the<br />

water to a high pressure zone in<br />

the pump. The bubbles then<br />

implode with hammer-like blows,<br />

eroding the pump and eventually<br />

destroying it. The phenomenon is<br />

called cavitation and is readily<br />

recognized by its typical rattle-like<br />

noise, which usually diminishes<br />

as a valve at the pump outlet is<br />

closed down.<br />

However, since in most cases<br />

pumps are s<strong>up</strong>plied co<strong>up</strong>led to<br />

receivers and the static head<br />

hs = Total suction head in feet.<br />

(Positive for a head above<br />

the pump or negative for a<br />

lift to the pump)<br />

hf = Friction loss in suction piping.<br />

W = Density of water in pounds<br />

per cubic foot at the<br />

appropriate temperature.<br />

above the pump inlet is already<br />

fixed by the pump manufacturer, it<br />

is only necessary to ensure that<br />

the pump set has sufficient<br />

capacity at the water temperature<br />

expected at the pump. Pump<br />

manufacturers usually have a set<br />

of capacity curves for the pump<br />

when handling water at different<br />

temperatures and these should<br />

be consulted.<br />

Where steam systems operate<br />

at higher pressures than<br />

those used in LP space heating<br />

systems, as in process work, condensate<br />

temperatures are often<br />

212°F, or more where positive<br />

pressures exist in return lines.<br />

Electric pumps are then used<br />

only if their capacity is downrated<br />

by partial closure of a valve at the<br />

outlet; by using a receiver mounted<br />

well above the pump to ensure<br />

sufficient NPSH; or by subcooling<br />

the condensate through a heat<br />

exchanger of some type.<br />

Pressure Powered Condensate<br />

Pump<br />

All these difficulties are avoided<br />

by the use of non-electric condensate<br />

pumps, such as the<br />

Pressure Powered Pump . The<br />

Pressure Powered Pump is<br />

essentially an alternating receiver<br />

which can be pressurized, using<br />

steam, air or other gas. The gas<br />

pressure displaces the condensate<br />

(which can be at any<br />

temperature <strong>up</strong> to and including<br />

boiling point) through a check

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