Centrifugal Pumps Design and Application 2nd ed - Val S. Lobanoff, Robert R. Ross (Butterworth-Heinemann, 1992)
Vibration and Noise in Pumps 431 Figure 18-3. Cavitation effects on the dynamic pressure. sity results from backflow at the impeller eye or at the impeller discharge, or both. Every centrifugal pump has this recirculation under certain conditions of flow reduction. Operation in a recirculating condition can be damaging to the pressure side of the inlet and/or discharge impeller vanes (and also to casing vanes). Recirculation is evidenced by an increase in loudness of a banging type, random noise, and an increase in suction and/or discharge pressure pulsations as flow is decreased. Sound levels measured at the casing of an 8000 hp pump and near the suction piping during cavitation [2] are shown in Figure 18-4. The cavitation produced a wide-band shock that excited many frequencies; however, in this case, the vane passing frequency (number of impeller vanes
432 Centrifugal Pumps: Design and Application Figure 18-4. Noise spectra of cavitation in centrifugal pump. times revolutions per second) and multiples of it predominated. Cavita tion noise of this type usually produces very high frequency noise, best described as "crackling." Flashing is particularly common in hot water systems (feedwater pump systems) when the hot, pressurized water experiences a decrease in pressure through a restriction (i.e., flow control valve). This reduction of pressure allows the liquid to suddenly vaporize, or flash, which results in a noise similar to cavitation. To avoid flashing after a restriction, sufficient back pressure should be provided. Alternately, the restriction could be located at the end of the line so that the flashing energy can dissipate into a larger volume. Flow Turbulence. Pump generated dynamic pressure sources include turbulence (vortices or wakes) produced in the clearance space between impeller vane tips and the stationary diffuser or volute lips. Dynamic pressure fluctuations or pulsations produced in this manner can cause impeller vibrations or can result in shaft vibrations as the pressure pulses impinge on the impeller. Flow past an obstruction or restriction in the piping may produce turbulence or flow-induced pulsations [2]. These pulsations may produce both noise and vibration over a wide-frequency band. The frequencies are related to the flow velocity and geometry of the obstruction. These pulsations may cause a resonant interaction with other parts of the acoustic piping system. Most of these unstable flow patterns are produced by shearing at the boundary between a high-velocity and low-velocity region in a fluid
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432 <strong>Centrifugal</strong> <strong>Pumps</strong>: <strong>Design</strong> <strong>and</strong> <strong>Application</strong><br />
Figure 18-4. Noise spectra of cavitation in centrifugal pump.<br />
times revolutions per second) <strong>and</strong> multiples of it pr<strong>ed</strong>ominat<strong>ed</strong>. Cavita<br />
tion noise of this type usually produces very high frequency noise, best<br />
describ<strong>ed</strong> as "crackling."<br />
Flashing is particularly common in hot water systems (fe<strong>ed</strong>water pump<br />
systems) when the hot, pressuriz<strong>ed</strong> water experiences a decrease in pressure<br />
through a restriction (i.e., flow control valve). This r<strong>ed</strong>uction of<br />
pressure allows the liquid to suddenly vaporize, or flash, which results in<br />
a noise similar to cavitation. To avoid flashing after a restriction, sufficient<br />
back pressure should be provid<strong>ed</strong>. Alternately, the restriction could<br />
be locat<strong>ed</strong> at the end of the line so that the flashing energy can dissipate<br />
into a larger volume.<br />
Flow Turbulence. Pump generat<strong>ed</strong> dynamic pressure sources include<br />
turbulence (vortices or wakes) produc<strong>ed</strong> in the clearance space between<br />
impeller vane tips <strong>and</strong> the stationary diffuser or volute lips. Dynamic<br />
pressure fluctuations or pulsations produc<strong>ed</strong> in this manner can cause impeller<br />
vibrations or can result in shaft vibrations as the pressure pulses<br />
impinge on the impeller.<br />
Flow past an obstruction or restriction in the piping may produce turbulence<br />
or flow-induc<strong>ed</strong> pulsations [2]. These pulsations may produce<br />
both noise <strong>and</strong> vibration over a wide-frequency b<strong>and</strong>. The frequencies<br />
are relat<strong>ed</strong> to the flow velocity <strong>and</strong> geometry of the obstruction. These<br />
pulsations may cause a resonant interaction with other parts of the acoustic<br />
piping system.<br />
Most of these unstable flow patterns are produc<strong>ed</strong> by shearing at the<br />
boundary between a high-velocity <strong>and</strong> low-velocity region in a fluid