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Hydraulics, open channels and fluid power

Available net positive suction head at a pump inlet

Head at the pump inlet above the vapour pressure of the liquid, from the static absolute suction pressure, vapour pressure and mean inlet speed.

Ref
HYD-36
Rev
v1
Field
Hydraulics, open channels and fluid power
Result
NPSHa [m]

Net positive suction head available is the head at the pump inlet above the liquid’s vapour pressure: NPSHa = (ps − pv)/(ρ g) + Vs²/(2g), using absolute pressures. A pump needs NPSHa above its required NPSH, with a margin, to avoid cavitation, which damages the impeller and drops the head. Vapour pressure rises quickly with temperature, so hot liquids have much less margin.

Head at the pump inlet above the vapour pressure of the liquid, from the static absolute suction pressure, vapour pressure and mean inlet speed. It must exceed the pump’s required value with a margin.

Calculator

Solve for
m
Pa
1,0001e7
Pa
1001,000,000
kg/m³
5002,000
m/s²
130
m/s
030
  • Pressure head above vapour, (ps − pv)/(ρ g)7.849 m
  • Velocity head at the inlet, Vs²/(2g)0.2039 m
  • Margin over a required NPSH of 5 m3.053 m

What drives the result

Each variable is moved across its typical range while the others stay at the values above. The longest bar is the key driver.

Available NPSH (m) current value 8.053 m
psAbsolute static pressure at the suction tapKey driver
01,020
pvVapour pressure of the liquid
−93.68.35
gGravitational acceleration
2.6379
VsMean speed at the inlet
7.8553.7
ρLiquid density
4.1315.9
  • The pump inlet has 8.053 m of head above vapour pressure, of which 0.204 m is velocity head.
  • Against a required NPSH of 5 m the margin would be 3.05 m; a ratio of NPSHa to NPSHr of 1.1 to 1.3 or more is commonly asked for.
Chart data as tables

Ranked variables

VariableTypical rangeLowest resultHighest resultSwing (m)Local stepChange in result
ps Absolute static pressure at the suction tap1,000 to 1e7 Pa01,0191,019+10%+10.1 %
pv Vapour pressure of the liquid100 to 1,000,000 Pa−93.588.349101.9+10%−0.38 %
g Gravitational acceleration1 to 30 m/s²2.6337976.37+10%−9.09 %
Vs Mean speed at the inlet0 to 30 m/s7.84953.7245.87+10%+0.532 %
ρ Liquid density500 to 2,000 kg/m³4.12815.911.77+10%−8.86 %

Sweep of Vapour pressure of the liquid

Vapour pressure of the liquid (Pa)Available NPSH (m)
1008.349
316.28.327
1,0008.257
3,1628.036
10,0007.339
31,6205.135
100,000−1.835
316,200−23.88
1,000,000−93.58

Sweep one variable

Available NPSH (m)Hover, touch, or use the arrow keys on the chart
−100−80−60−40−200 100100010k100k1M Vapour pressure of the liquid (Pa), log scale now 8.053

Variables and how each one contributes

NPSHa

Available NPSH

Result · m

What the equation gives you. Everything else feeds it.

ps

Absolute static pressure at the suction tap

Pa · typical 1,000 to 1e7

The absolute static pressure at the suction tap, in Pa. Raises the head in direct proportion to the pressure. Raising it by 10 % (to 88,000) moves the result by +10.1 %, from 8.053 to 8.869 m.

pv

Vapour pressure of the liquid

Pa · typical 100 to 1,000,000

The vapour pressure of the liquid at the pumping temperature, in Pa. A higher vapour pressure lowers the available head. Raising it by 10 % (to 3,300) moves the result by −0.38 %, from 8.053 to 8.022 m.

ρ

Liquid density

kg/m³ · typical 500 to 2,000

The liquid density, in kg/m³. A denser liquid gives less head for the same pressure. Raising it by 10 % (to 1,100) moves the result by −8.86 %, from 8.053 to 7.339 m.

g

Gravitational acceleration

m/s² · typical 1 to 30

The gravitational acceleration, in m/s². Lowers the head in inverse proportion. Raising it by 10 % (to 10.79) moves the result by −9.09 %, from 8.053 to 7.321 m.

Vs

Mean speed at the inlet

m/s · typical 0 to 30

The mean speed at the inlet, in m/s. Raises the head through the velocity-head term. Raising it by 10 % (to 2.2) moves the result by +0.532 %, from 8.053 to 8.096 m.

Worked example with the values above

  1. Pressure head: (ps − pv)/(ρ g) = (80,000 − 3,000) / (1,000 × 9.81) = 7.8491 m.
  2. Velocity head: 2² / (2 × 9.81) = 0.20387 m.
  3. NPSHa = 8.053 m.

Assumptions and limits

  • Steady incompressible flow with the pump curve and system curve both of quadratic form.
  • Ideal blade-guided flow for the velocity-triangle results, so the real head is lower.

Common mistakes

  • Using gauge pressure in place of absolute pressure.
  • Using the vapour pressure at the wrong temperature.
  • Forgetting that the available value must exceed the required value with a margin, not equal it.

Statistics and uncertainty

Vapour pressure changes by a factor of about two for every 15 to 20 K near ambient temperature, so the margin shrinks quickly with hot liquids, and suction level varies with tank level.

Where it is used

  • Choosing pumps and finding the duty point on a pipe system.
  • Checking cavitation margin and estimating head from impeller geometry.

Maths you need

  • Pump curve: head against flow for a pump at a fixed speed
  • System curve: head needed by the pipe system against flow
  • Velocity triangle: the vector diagram of blade and fluid velocities

Related formulas

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