# Pump Affinity Laws

## Turbo machines affinity laws can be used to calculate volume capacity, head or power consumption in centrifugal pumps with changing speed or wheel diameters

**The Affinity Laws** of centrifugal pumps or fans indicates the influence on volume capacity, head (pressure) and/or power consumption of a pump or fan due to

- change in
**speed**of wheel - revolutions per minute (rpm) - geometrically similarity - change in
**impeller diameter**

Note that there are two sets of affinity laws:

- affinity laws for a specific centrifugal pump - to approximate head, capacity and power curves for different motor speeds and /or different diameter of impellers
- affinity laws for a family of geometrically similar centrifugal pumps - to approximate head, capacity and power curves for different motor speeds and /or different diameter of impellers

### Pump Affinity Laws for a Specific Centrifugal Pump

#### Volume Capacity

The volume capacity of a centrifugal pump can be expressed like

q_{1}/ q_{2}= (n_{1}/ n_{2}) (d_{1}/ d_{2}) (1)

where

q= volume flow capacity (m^{3}/s, gpm, cfm, ..)

n= wheel velocity - revolution per minute - (rpm)

d = wheel diameter (m, ft)

#### Head or Pressure

The head or pressure of a centrifugal pump can be expressed like

dp_{1}/ dp_{2}= (n_{1}/ n_{2})^{2}(d_{1}/ d_{2})^{2}(2)

where

dp= head or pressure (m, ft, Pa, psi, ..)

#### Power

The power consumption of a centrifugal pump can be expressed as

P_{1}/ P_{2}= (n_{1}/ n_{2})^{3}(d_{1}/ d_{2})^{3}(3)

where

P= power (W, bhp, ..)

**Changing Wheel Velocity**

If the **wheel diameter is constant** - change in pump wheel velocity can simplify the affinity laws to

##### Volume Capacity

q_{1}/ q_{2}= (n_{1}/ n_{2}) (1a)

##### Head or Pressure

dp_{1}/ dp_{2}= (n_{1}/ n_{2})^{2 }^{ }(2a)

##### Power

P_{1}/ P_{2}= (n_{1}/ n_{2})^{3}^{ }(3a)

**Note!** If the speed of a pump is increased with *10%*

- the volume flow increases with
*10%* - the head increases with
*21%* - the power increases with
*33 %*

If we want to increase the volume flow capacity of an existing system with *10%* we have to increase the power supply with *33%*.

#### Pump Affinity Laws Calculator - Changing Wheel Velocity

Replace the default values with the actual values. The calculator is generic and can be used with all common units as long as the use is consistent.

q_{1}- volume capacity - (m^{3}/s, gpm, cfm, ..)

dp_{1}- head or pressure (m, ft, Pa, psi, ..)

P_{1}- power (W, bhp)

n_{1}- initial wheel velocity (rpm)

n_{2}- final wheel velocity (rpm)

**Changing the Impeller Diameter**

If wheel velocity is constant **a change in impeller diameter** simplifies the affinity laws to

##### Volume Capacity

q_{1}/ q_{2}=d_{1}/ d_{2}(1b)

##### Head or Pressure

dp_{1}/ dp_{2}=(d_{1}/ d_{2})^{2}(2b)

##### Power

P_{1}/ P_{2}=(d_{1}/ d_{2})^{3}(3b)

#### Pump Affinity Laws Calculator - Changing Wheel Diameter

Replace the default values with the actual values. The calculator is generic and can be used with all common units as long as the use of units is consistent.

q_{1}- volume capacity - (m^{3}/s, gpm, cfm, ..)

dp_{1}- head or pressure (m, ft, Pa, psi, ..)

P_{1}- power (W, bhp)

d_{1}- initial wheel diameter (m, in, ft ...)

d_{2}- final wheel diameter (m, in, ft ..)

#### Example - Pump Affinity Laws - Changing Pump Speed

The pump speed is changed when the impeller size is constant. The initial flow is *100 gpm*, the initial head is *100 ft*, the initial power is *5 bhp*, the initial speed is *1750 rpm* and the final speed *3500 rpm*.

The final flow capacity can be calculated with (1a):

q_{2}= q_{1}n_{2}/ n_{1}

=(100 gpm) (3500 rpm) / (1750 rpm)

= 200 gpm

The final head can be calculated with (2a):

dp_{2}= dp_{1}(n_{2}/ n_{1})^{2}

= (100 ft) ((3500 rpm) / (1750 rpm))^{2}

= 400 ft

The final power consumption can be calculated with (3a):

P_{2}= P_{1}(n_{2}/ n_{1})^{3}

= (5 bhp) ((3500 rpm) / (1750 rpm))^{3}

= 40 bhp

#### Example - Pump Affinity Laws - Changing Impeller Diameter

The diameter of the pump impeller is reduced when the pump speed is constant. The diameter is changed from *8 to 6 inches*.

The final flow capacity can be calculated with *(1b)*:

q_{2}= q_{1}(d_{2}/ d_{1})

= (100 gpm) ((¨6 in) / (8 in))

= 75 gpm

The final head can be calculated with *(2b)*:

dp_{2}= dp_{1}(d_{2}/ d_{1})^{2}

= (100 ft) ((6 in) / (8 in))^{2}

= 56.3 ft

The final power consumption can be calculated with *(3b)*:

P_{2}= P_{1}(d_{2}/ d_{1})^{3}

= (5 bhp) ((6 in) / (8 in))^{3}

= 2.1 bhp

### Pump Affinity Laws for a Family of Geometrically Similar Pumps

The volume capacity can be expressed like

q_{1}/ q_{2}= (n_{1}/ n_{2})(d_{1}/ d_{2})^{3}(4)

where

q= volume flow capacity (m^{3}/s, gpm, cfm, ..)

n= wheel velocity - revolution per minute - (rpm)

d = wheel diameter

#### Head or Pressure

The head or pressure of a centrifugal pump can be expressed like

dp_{1}/ dp_{2}= (n_{1}/ n_{2})^{2}(d_{1}/ d_{2})^{2}(5)

where

dp= head or pressure (m, ft, Pa, psi, ..)

#### Power

The power consumption of a centrifugal pump can be expressed as

P_{1}/ P_{2}= (n_{1}/ n_{2})^{3}(d_{1}/ d_{2})^{5}(6)

where

P= power (W, bhp, ..)

Note that the affinity laws for fans are not identical with pumps.