LOGOS Engineering Workspace

LOGOS Learning · 4

NPSH available formula: why the pump cavitates

NPSH available is the head left at the pump inlet above the vapor pressure: NPSHa = p_atm/(rho*g) - p_v/(rho*g) + dz - hf_suc. The pump runs free of cavitation only while NPSHa stays above the NPSHr from the pump curve, with a margin.

Lower the suction tank relative to the pump. The inlet pressure falls until the water boils inside the impeller.

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Quick test

Three questions about this lesson. Got one wrong? The explanation shows right away.

1. Installing the pump well above the suction level…

2. What reduces NPSH available?

3. Why is NPSHa slightly above NPSHr not enough?

0 of 3 answered

Why this happens

Arrows compare with the suction level at the pump centerline (Δz = 0).

Lower the suction tank to see the chain

NPSH available

NPSHa = patmρg − pvρg + Δz − hf,suc
9.97 m = 10.36 − 0.32 + 0.0 − 0.07 m

The energy left at the pump inlet above vapor pressure. The atmosphere pushes water in; the elevation helps or hurts; suction loss always hurts.

Cavitation criterion

NPSHa ≥ NPSHr
ratio = NPSHaNPSHr
9.97 m · 4.89 m · 2.04

Catalog NPSHr is usually NPSH3: at that point the pump has already lost 3 % of head to cavitation. So a ratio above 1 is not enough; the LOGOS calculator requires a ratio of at least 1.1 and a 0.5 m margin as the floor for general service, in line with HI 9.6.1.

Suction pressure (PIT-02)

ps,abs = patm + ρg ( Δz − hf,suc − v22g )
100.2 kPa abs = -0.01 bar(g)

With the tank below the pump, suction pressure falls below atmospheric and PIT-02 shows vacuum. When it nears vapor pressure, water boils at the impeller eye and the bubbles collapse on the vanes.

More flow, less margin

hf,suc ∝ Q2 NPSHr ↑ with Q
Q = 60.1 m³/h · hf,suc = 0.07 m

On the chart NPSHa falls with flow and NPSHr rises. Lowering the tank shifts the whole NPSHa curve down until it crosses NPSHr near the operating point.

Illustrative NPSHr curve of the teaching pump.

Formulas in plain text

NPSH available
NPSHa = p_atm / (rho * g) - p_v / (rho * g) + dz - hf_suc
NPSHa = net positive suction head available (m) · p_atm = absolute pressure on the suction tank surface (Pa) · p_v = vapor pressure at pumping temperature (Pa) · rho = fluid density (kg/m3) · g = 9.81 m/s2 · dz = suction level minus pump centerline (m, negative for suction lift) · hf_suc = suction line head loss (m)
Cavitation criterion
NPSHa >= NPSHr ratio = NPSHa / NPSHr
NPSHr = NPSH required by the pump, usually NPSH3 (m) · ratio = NPSH margin ratio (-)
Absolute suction pressure
p_s,abs = p_atm + rho * g * (dz - hf_suc - v^2 / (2 * g))
p_s,abs = absolute pressure at the pump suction (Pa) · v = velocity in the suction pipe (m/s)
Effect of flow
hf_suc ~ Q^2 and NPSHr rises with Q
Q = pump flow (m3/h)

Frequently asked questions

Why must NPSH available exceed NPSH required?

Below NPSHr the pressure at the impeller eye reaches the vapor pressure and the water boils. The bubbles collapse on the vanes, causing loss of head, gravel-like noise and erosion.

How much NPSH margin is enough?

Catalog NPSHr is usually NPSH3, where the pump has already lost 3 % of head, so a ratio of 1 is not safe. ANSI/HI 9.6.1 recommends margin ratios from about 1.1 up to 2.5 depending on the service; the LOGOS calculator uses at least 1.1 and 0.5 m as the floor for general service.

How does a suction lift affect NPSHa?

Every metre the liquid level sits below the pump centerline subtracts one metre from NPSHa, and the suction loss subtracts more. A flooded suction, with the tank above the pump, adds the elevation in your favour.

How does liquid temperature change NPSH available?

Vapor pressure rises quickly with temperature, so the p_v/(rho*g) term grows and NPSHa falls. Water at 25 C has about 3.2 kPa of vapor pressure, while at 100 C it equals sea-level atmospheric pressure.

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