Power Eng 2nd Class study materials
Power Eng 2nd Class study resources

Power Eng 2nd Class: Mechanical Equipment and Components (Pumps, Compressors, Turbines, Engines)

Power Eng 2nd Class · Work through your exam, one topic at a time.

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Mechanical Equipment and Components (Pumps, Compressors, Turbines, Engines)

This domain tests whether you can predict how rotating equipment behaves away from its design point: where a pump will actually operate, why a compressor surges, what limits a turbine, and how engines lose efficiency at part load. Expect affinity-law problems, NPSH calculations and fault-to-cause matching.

Pumps

  • Affinity laws: Q proportional to N, H proportional to N^2, P proportional to N^3. Trimming an impeller follows the same laws using diameter.
  • The operating point is where the pump curve crosses the system curve. Throttling moves the system curve; a VFD moves the pump curve.
  • NPSHa = (ps - pv)/(rho x g) + z - hf. It must exceed the pump's NPSHr with margin, or the pump cavitates: noise, falling head, vibration, impeller erosion.
  • Run near best efficiency point. Far left causes recirculation and radial loading; far right causes cavitation and motor overload.

Compressors and turbines

  • Positive displacement (reciprocating, screw, vane) suits high pressure and low flow; dynamic (centrifugal, axial) suits large flows.
  • Reciprocating machines need clearance-volume control; multi-stage intercooling pulls the path toward isothermal and cuts power.
  • Surge is a dynamic-machine instability where flow reverses. Anti-surge recycle opens as flow approaches the surge line.
  • Steam turbines: a condenser lowers exhaust pressure and raises output; gland seals keep air out, because air ingress destroys vacuum.

Engines

  • Four-stroke diesel: intake, compression, power, exhaust, with ignition by compression heat. Efficiency falls at light load; jacket-water and exhaust heat recovery matter.
  • Gas turbines: compressor, combustor, power turbine. Output drops as ambient temperature rises because mass flow falls.

Worked example

A pump delivers 60 L/s at 35 m head. Hydraulic power = rho x g x Q x H = 1000 x 9.81 x 0.060 x 35 = 20.6 kW. At 72% pump efficiency, shaft power = 20.6/0.72 = 28.6 kW. Doubling speed gives 120 L/s and 140 m head, and shaft power rises eightfold to about 229 kW. That third-power relationship is why overspeeding a motor or fitting a larger impeller can overload a drive that looked adequately sized.

Traps

  • Using discharge pressure instead of head, then mixing pressure units between pump curve and system curve.
  • Forgetting vapour pressure when the liquid is hot condensate - the classic deaerator extraction pump cavitation.
  • Confusing NPSHr (a pump property from the curve) with NPSHa (a system property you calculate).
  • Ignoring how steeply centrifugal compressor discharge temperature rises with pressure ratio.