Engineering calculators · Pumping
Pump head, NPSH and power calculator
Size a pump for a water system from the suction tank to the delivery point. Enter both pipe runs, their fittings, the tank levels and pressures, and the calculator works out the total dynamic head, the NPSH available against the pump’s NPSHr, the pressure at each pump flange, and the power and yearly energy cost. Add three points from a pump curve to find where the pump will actually run, including at reduced speed on a variable-speed drive.
Results
Pump and system curves
Operating point: 54.2 m³/h at 20.8 m, drawing about 4.77 kW at the efficiencies above.
| Quantity | Suction | Discharge | Notes |
|---|---|---|---|
| Velocity | 0.786 m/s | 1.77 m/s | Q / (πD²/4) |
| Reynolds number | 117,486 | 176,229 | ρvD/μ |
| Darcy friction factor | 0.01746 | 0.01615 | Colebrook-White, or 64/Re when laminar [dff] |
| Pipe friction loss | 0.0183 m | 5.15 m | f (L/D) v²/2g |
| Fittings loss | 0.0611 m | 1.50 m | ΣK v²/2g [clark] |
| Pressure at pump flange | 18.5 kPa(g) | 210 kPa(g) | Static pressure at the inlet and outlet |
| Head build-up and NPSH | Value | Notes |
|---|---|---|
| Static lift | 13.0 m | Delivery level − suction level |
| Surface pressure difference | 0 m | (pdelivery − psuction) / ρg |
| All pipe and fitting losses | 6.72 m | Suction + discharge |
| Total dynamic head | 19.7 m | Sum of the three rows above |
| Atmospheric pressure at site | 100.7 kPa | Standard atmosphere at the site altitude [atm] |
| Vapour pressure of water | 2.34 kPa | At the water temperature [NIST] |
| Water density / viscosity | 998.2 kg/m³ / 1.002 mPa·s | [NIST] |
| NPSH available | 12.0 m | (patm + psuction − pvapour)/ρg + suction level − suction losses [npsh] |
How the calculation works
- Pipe losses. Each side is a single pipe run. Friction uses Darcy-Weisbach with a Colebrook-White friction factor (64/Re when laminar), and fittings add ΣK × v²/2g. This is the same method as the pipe pressure drop calculator. Water density and viscosity come from NIST at the water temperature [NIST].
- Fitting K values are published ranges [clark]. Real values depend on size, make and whether a fitting is screwed or flanged, so choose the low, middle or high end, and use the manufacturer’s figure where you have one. The entrance from a tank is treated as a sudden contraction (K = 0.42) and the exit into a tank as K = 1, which also accounts for the velocity head of a free discharge.
- Total dynamic head = static lift + surface pressure difference + suction losses + discharge losses. This is the head the pump must add at the design flow.
- Pump flange pressures come from Bernoulli along each line: the pressure at the tank surface, plus or minus the level, minus losses and the velocity head in the pipe.
- NPSH available = (atmospheric + suction surface gauge pressure − vapour pressure) / ρg + suction level − suction losses [npsh]. Atmospheric pressure falls with altitude, from the standard-atmosphere barometric formula [atm], and vapour pressure rises steeply with temperature [NIST]. A margin of at least 0.6 m over the pump’s NPSHr, and preferably 1.5 m, is commonly recommended [npsh].
- Power. Hydraulic power = ρ g Q H. Shaft power divides by pump efficiency and motor input divides again by motor efficiency. Yearly energy = motor input × running hours.
- Operating point. A pump runs where its curve crosses the system curve, not at the design duty. The three curve points are fitted with a quadratic, H = a + bQ + cQ². At a different speed the curve is scaled by the affinity laws (Q ∝ N, H ∝ N²) [aff], and the crossing is found numerically. The power at the operating point assumes the same efficiencies, which is only approximate away from the pump’s best efficiency point.
What this cannot tell you. It models one suction line and one discharge line in series, carrying clean water at steady flow. It does not handle branched networks, parallel pumps, sludge or other non-Newtonian liquids, entrained air, or surge and water hammer. A three-point quadratic is only a fit of the real pump curve, and it cannot predict efficiency or NPSHr across the curve. Use the manufacturer’s full curves to confirm the selection.
Sources
- Subramanian, R.S. Minor losses (loss coefficients for fittings, entrance and exit). Clarkson University
- NIST Chemistry WebBook: Saturation properties of water, 0–100 °C (vapour pressure, IAPWS-95)
- Wikipedia: Net positive suction head (NPSHa definition and margin over NPSHr)
- Wikipedia: Atmospheric pressure (barometric formula, troposphere)
- Wikipedia: Affinity laws for pumps (Q ∝ N, H ∝ N², P ∝ N³)
- Wikipedia: Darcy friction factor formulae (Colebrook-White, Swamee-Jain, flow regimes)
- Moody, L.F. (1944) Friction factors for pipe flow. Trans. ASME 66:671–684 (absolute roughness of commercial pipes)
- NIST Chemistry WebBook: Isobaric properties of water at 0.101325 MPa (density and viscosity, 0–100 °C)