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Engineering reference

Fluid Machinery & Systems: theory, method, and sources

This fluid mechanics workspace publishes 10 governing equations, 5 stated assumptions, 1 documented boundary, and 2 sources so the numbers it returns can be checked rather than taken on trust.

Calculations run locallyCalculation & source methodology

How this tool works

Ten modules cover pump and turbine power, system and pump curve intersection, affinity laws, net positive suction head, specific speed, series and parallel pump combinations, hydraulic cylinders, accumulators, and fan laws.

The operating point module solves the intersection of a quadratic pump curve with a system curve, which is the calculation that determines the flow a given pump will actually deliver rather than its rated flow.

Calculators and topics covered

  • pumps
  • turbines
  • hydraulics
  • fans
  • NPSH
  • pump curve
  • system curve
  • affinity laws
  • hydraulic cylinder

Core equations

pump hydraulic power:Ph=ρgQHshaft power:Ps=Phη\text{pump hydraulic power:}\quad \begin{gathered}P_{h} = \rho gQH\\\text{shaft power:}\quad P_{s} = \frac{P_{h}}{\eta }\end{gathered}turbine shaft power:Ps=ρgQHη\text{turbine shaft power:}\quad P_{s} = \rho gQH \cdot \eta system curve:Hsys=Hstatic+kQ2\text{system curve:}\quad H_{\mathrm{sys}} = H_{\mathrm{static}} + kQ^{2}operating point:H0aQ2=Hstatic+kQ2\text{operating point:}\quad H_{0} - aQ^{2} = H_{\mathrm{static}} + kQ^{2}affinity laws:Q2Q1=(N2N1)(D2D1)3,  H2H1=(N2N1)2(D2D1)2,  P2P1=(N2N1)3(D2D1)5\text{affinity laws:}\quad \frac{Q_{2}}{Q_{1}} = \left(\frac{N_{2}}{N_{1}}\right) \left(\frac{D_{2}}{D_{1}}\right)^{3},\; \frac{H_{2}}{H_{1}} = \left(\frac{N_{2}}{N_{1}}\right)^{2} \left(\frac{D_{2}}{D_{1}}\right)^{2},\; \frac{P_{2}}{P_{1}} = \left(\frac{N_{2}}{N_{1}}\right)^{3} \left(\frac{D_{2}}{D_{1}}\right)^{5}net positive suction head available:NPSHa=patmpvρg+zshLV22g\text{net positive suction head available:}\quad \mathrm{NPSH}_{a} = \frac{p_{\mathrm{atm}} - p_{v}}{\rho g} + z_{s} - h_{L} \frac{- V^{2}}{2 g}specific speed:Ns=NQH34\text{specific speed:}\quad N_{s} = \frac{N \sqrt{Q}}{H^{\frac{3}{4}}}hydraulic cylinder:F=pA,  v=QA,  Aannulus=π(Dbore2Drod2)4\text{hydraulic cylinder:}\quad F = pA,\; v = \frac{Q}{A},\; A_{\mathrm{annulus}} = \frac{\pi \left(D_{\mathrm{bore}}^{2} - D_{\mathrm{rod}}^{2}\right)}{4}accumulator energy:E=p1V1[(p2p1)n1n1]n1\text{accumulator energy:}\quad E = \frac{p_{1} V_{1} \left[\left(\frac{p_{2}}{p_{1}}\right)^{\frac{n - 1}{n}} - 1\right]}{n - 1}fan laws:QN,  ΔpN2,  PN3\text{fan laws:}\quad Q \propto N,\; \Delta p \propto N^{2},\; P \propto N^{3}

Method and assumptions

Assumptions

  • Pump and system curves are represented by simple quadratic forms rather than manufacturer-tabulated data.
  • Efficiency is a single constant value and does not vary with flow across the operating range.
  • Affinity laws assume geometric similarity and constant efficiency, which holds only over a limited speed range.
  • NPSH available is compared to a required value that must come from the pump manufacturer; cavitation margin is not assumed.
  • Series and parallel combinations assume identical pumps and neglect interaction losses in the manifold.

Limitations and design boundaries

  • Educational screening calculations only. Real systems require verified fluid properties, calibrated coefficients, uncertainty analysis, applicable codes and standards, and qualified engineering review.

Sources and references

Primary sources are preferred for ratings, standards, manufacturer data, and externally defined constants.

Source policy
  • Çengel and Cimbala, Fluid Mechanics: Fundamentals and Applications
  • Munson et al., Fundamentals of Fluid Mechanics