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Scaling Laws; Affinity Laws

Fluid Mechanics · FE Reference Handbook section

Fluid Mechanics
13 formulas
10 exam-style examples
~60 min
All Fluid Mechanics lectures

Handbook notes for this section

Definitions and conditions exactly as the handbook states them.

  • Subscripts 1 and 2 refer to different but similar machines or to different operating conditions of the same machine.

Core formulas for this FE topic

Definitions, applicability, units, assumptions and worked examples for each relation.

Worked exam-style examples

The four ways this section is written on the real exam — thoughts first, then equations, then substitution.

Example 1
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws

A pump running at 1764 rpm delivers 0.140 m³/s at 16 m while absorbing 36.5 kW. The same impeller is run at 2961 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1764rpm,N2=2961rpmN_{1} = 1764 rpm, N_{2} = 2961 rpm
  • Q1=0.140m3/sQ_{1} = 0.140 m^{3}/s
  • H1=16mH_{1} = 16 m
  • P1=36.5kWP_{1} = 36.5 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2961/1764=1.6786N_{2}/N_{1} = 2961/1764 = 1.6786
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.140(1.6786)=0.235m3/sQ_{2} = 0.140(1.6786) = 0.235 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=16(1.6786)2=45.1mH_{2} = 16(1.6786)^{2} = 45.1 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=36.5(1.6786)3=172.6kWP_{2} = 36.5(1.6786)^{3} = 172.6 kW
Answer:
Q2=0.235m3/s,H2=45.1m,P2=172.6kWQ_{2} = 0.235 m^{3}/s, H_{2} = 45.1 m, P_{2} = 172.6 kW

Why the other options are there

  • H₂ = 26.9 m (linear scaling of head)
  • P₂ = 102.8 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 2
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (2)

A pump running at 1759 rpm delivers 0.050 m³/s at 21 m while absorbing 4.0 kW. The same impeller is run at 2446 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1759rpm,N2=2446rpmN_{1} = 1759 rpm, N_{2} = 2446 rpm
  • Q1=0.050m3/sQ_{1} = 0.050 m^{3}/s
  • H1=21mH_{1} = 21 m
  • P1=4.0kWP_{1} = 4.0 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2446/1759=1.3906N_{2}/N_{1} = 2446/1759 = 1.3906
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.050(1.3906)=0.070m3/sQ_{2} = 0.050(1.3906) = 0.070 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=21(1.3906)2=40.6mH_{2} = 21(1.3906)^{2} = 40.6 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=4.0(1.3906)3=10.8kWP_{2} = 4.0(1.3906)^{3} = 10.8 kW
Answer:
Q2=0.070m3/s,H2=40.6m,P2=10.8kWQ_{2} = 0.070 m^{3}/s, H_{2} = 40.6 m, P_{2} = 10.8 kW

Why the other options are there

  • H₂ = 29.2 m (linear scaling of head)
  • P₂ = 7.7 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 3
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (3)

A pump running at 1764 rpm delivers 0.030 m³/s at 23 m while absorbing 40.5 kW. The same impeller is run at 2662 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1764rpm,N2=2662rpmN_{1} = 1764 rpm, N_{2} = 2662 rpm
  • Q1=0.030m3/sQ_{1} = 0.030 m^{3}/s
  • H1=23mH_{1} = 23 m
  • P1=40.5kWP_{1} = 40.5 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2662/1764=1.5091N_{2}/N_{1} = 2662/1764 = 1.5091
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.030(1.5091)=0.045m3/sQ_{2} = 0.030(1.5091) = 0.045 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=23(1.5091)2=52.4mH_{2} = 23(1.5091)^{2} = 52.4 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=40.5(1.5091)3=139.2kWP_{2} = 40.5(1.5091)^{3} = 139.2 kW
Answer:
Q2=0.045m3/s,H2=52.4m,P2=139.2kWQ_{2} = 0.045 m^{3}/s, H_{2} = 52.4 m, P_{2} = 139.2 kW

Why the other options are there

  • H₂ = 34.7 m (linear scaling of head)
  • P₂ = 92.2 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 4
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (4)

A pump running at 1153 rpm delivers 0.100 m³/s at 39 m while absorbing 38.0 kW. The same impeller is run at 2094 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1153rpm,N2=2094rpmN_{1} = 1153 rpm, N_{2} = 2094 rpm
  • Q1=0.100m3/sQ_{1} = 0.100 m^{3}/s
  • H1=39mH_{1} = 39 m
  • P1=38.0kWP_{1} = 38.0 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2094/1153=1.8161N_{2}/N_{1} = 2094/1153 = 1.8161
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.100(1.8161)=0.182m3/sQ_{2} = 0.100(1.8161) = 0.182 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=39(1.8161)2=128.6mH_{2} = 39(1.8161)^{2} = 128.6 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=38.0(1.8161)3=227.6kWP_{2} = 38.0(1.8161)^{3} = 227.6 kW
Answer:
Q2=0.182m3/s,H2=128.6m,P2=227.6kWQ_{2} = 0.182 m^{3}/s, H_{2} = 128.6 m, P_{2} = 227.6 kW

Why the other options are there

  • H₂ = 70.8 m (linear scaling of head)
  • P₂ = 125.3 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 5
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (5)

A pump running at 1680 rpm delivers 0.160 m³/s at 15 m while absorbing 36.0 kW. The same impeller is run at 2840 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1680rpm,N2=2840rpmN_{1} = 1680 rpm, N_{2} = 2840 rpm
  • Q1=0.160m3/sQ_{1} = 0.160 m^{3}/s
  • H1=15mH_{1} = 15 m
  • P1=36.0kWP_{1} = 36.0 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2840/1680=1.6905N_{2}/N_{1} = 2840/1680 = 1.6905
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.160(1.6905)=0.270m3/sQ_{2} = 0.160(1.6905) = 0.270 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=15(1.6905)2=42.9mH_{2} = 15(1.6905)^{2} = 42.9 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=36.0(1.6905)3=173.9kWP_{2} = 36.0(1.6905)^{3} = 173.9 kW
Answer:
Q2=0.270m3/s,H2=42.9m,P2=173.9kWQ_{2} = 0.270 m^{3}/s, H_{2} = 42.9 m, P_{2} = 173.9 kW

Why the other options are there

  • H₂ = 25.4 m (linear scaling of head)
  • P₂ = 102.9 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 6
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (6)

A pump running at 1614 rpm delivers 0.080 m³/s at 23 m while absorbing 55.5 kW. The same impeller is run at 2207 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1614rpm,N2=2207rpmN_{1} = 1614 rpm, N_{2} = 2207 rpm
  • Q1=0.080m3/sQ_{1} = 0.080 m^{3}/s
  • H1=23mH_{1} = 23 m
  • P1=55.5kWP_{1} = 55.5 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2207/1614=1.3674N_{2}/N_{1} = 2207/1614 = 1.3674
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.080(1.3674)=0.109m3/sQ_{2} = 0.080(1.3674) = 0.109 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=23(1.3674)2=43.0mH_{2} = 23(1.3674)^{2} = 43.0 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=55.5(1.3674)3=141.9kWP_{2} = 55.5(1.3674)^{3} = 141.9 kW
Answer:
Q2=0.109m3/s,H2=43.0m,P2=141.9kWQ_{2} = 0.109 m^{3}/s, H_{2} = 43.0 m, P_{2} = 141.9 kW

Why the other options are there

  • H₂ = 31.5 m (linear scaling of head)
  • P₂ = 103.8 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 7
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (7)

A pump running at 1466 rpm delivers 0.020 m³/s at 13 m while absorbing 6.5 kW. The same impeller is run at 2204 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1466rpm,N2=2204rpmN_{1} = 1466 rpm, N_{2} = 2204 rpm
  • Q1=0.020m3/sQ_{1} = 0.020 m^{3}/s
  • H1=13mH_{1} = 13 m
  • P1=6.5kWP_{1} = 6.5 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2204/1466=1.5034N_{2}/N_{1} = 2204/1466 = 1.5034
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.020(1.5034)=0.030m3/sQ_{2} = 0.020(1.5034) = 0.030 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=13(1.5034)2=29.4mH_{2} = 13(1.5034)^{2} = 29.4 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=6.5(1.5034)3=22.1kWP_{2} = 6.5(1.5034)^{3} = 22.1 kW
Answer:
Q2=0.030m3/s,H2=29.4m,P2=22.1kWQ_{2} = 0.030 m^{3}/s, H_{2} = 29.4 m, P_{2} = 22.1 kW

Why the other options are there

  • H₂ = 19.5 m (linear scaling of head)
  • P₂ = 14.7 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 8
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (8)

A pump running at 1555 rpm delivers 0.030 m³/s at 13 m while absorbing 58.5 kW. The same impeller is run at 1990 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1555rpm,N2=1990rpmN_{1} = 1555 rpm, N_{2} = 1990 rpm
  • Q1=0.030m3/sQ_{1} = 0.030 m^{3}/s
  • H1=13mH_{1} = 13 m
  • P1=58.5kWP_{1} = 58.5 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=1990/1555=1.2797N_{2}/N_{1} = 1990/1555 = 1.2797
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.030(1.2797)=0.038m3/sQ_{2} = 0.030(1.2797) = 0.038 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=13(1.2797)2=21.3mH_{2} = 13(1.2797)^{2} = 21.3 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=58.5(1.2797)3=122.6kWP_{2} = 58.5(1.2797)^{3} = 122.6 kW
Answer:
Q2=0.038m3/s,H2=21.3m,P2=122.6kWQ_{2} = 0.038 m^{3}/s, H_{2} = 21.3 m, P_{2} = 122.6 kW

Why the other options are there

  • H₂ = 16.6 m (linear scaling of head)
  • P₂ = 95.8 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 9
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (9)

A pump running at 1406 rpm delivers 0.180 m³/s at 13 m while absorbing 21.5 kW. The same impeller is run at 2796 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1406rpm,N2=2796rpmN_{1} = 1406 rpm, N_{2} = 2796 rpm
  • Q1=0.180m3/sQ_{1} = 0.180 m^{3}/s
  • H1=13mH_{1} = 13 m
  • P1=21.5kWP_{1} = 21.5 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2796/1406=1.9886N_{2}/N_{1} = 2796/1406 = 1.9886
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.180(1.9886)=0.358m3/sQ_{2} = 0.180(1.9886) = 0.358 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=13(1.9886)2=51.4mH_{2} = 13(1.9886)^{2} = 51.4 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=21.5(1.9886)3=169.1kWP_{2} = 21.5(1.9886)^{3} = 169.1 kW
Answer:
Q2=0.358m3/s,H2=51.4m,P2=169.1kWQ_{2} = 0.358 m^{3}/s, H_{2} = 51.4 m, P_{2} = 169.1 kW

Why the other options are there

  • H₂ = 25.9 m (linear scaling of head)
  • P₂ = 85.0 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

Example 10
Pump affinity laws for a change in impeller speed — Scaling Laws; Affinity Laws (10)

A pump running at 1291 rpm delivers 0.040 m³/s at 17 m while absorbing 5.5 kW. The same impeller is run at 2631 rpm. Use the affinity laws to predict discharge, head and power.

Given

  • N1=1291rpm,N2=2631rpmN_{1} = 1291 rpm, N_{2} = 2631 rpm
  • Q1=0.040m3/sQ_{1} = 0.040 m^{3}/s
  • H1=17mH_{1} = 17 m
  • P1=5.5kWP_{1} = 5.5 kW

Find

Q₂, H₂ and P₂

Start with the thinking

  • Flow scales linearly, head with the square and power with the cube of the speed ratio.
  • A modest 20% speed increase nearly doubles the power draw — this is why VFD savings are large.

Step-by-step solution

  1. Speed ratio

    N2/N1=2631/1291=2.0380N_{2}/N_{1} = 2631/1291 = 2.0380
  2. Formula

    Q2Q1=N2N1\dfrac{Q_2}{Q_1}=\dfrac{N_2}{N_1}
  3. Substituting

    Q2=0.040(2.0380)=0.082m3/sQ_{2} = 0.040(2.0380) = 0.082 m^{3}/s
  4. Formula

    H2H1=(N2N1)2\dfrac{H_2}{H_1}=\left(\dfrac{N_2}{N_1}\right)^2
  5. Substituting

    H2=17(2.0380)2=70.6mH_{2} = 17(2.0380)^{2} = 70.6 m
  6. Formula

    P2P1=(N2N1)3\dfrac{P_2}{P_1}=\left(\dfrac{N_2}{N_1}\right)^3
  7. Substituting

    P2=5.5(2.0380)3=46.6kWP_{2} = 5.5(2.0380)^{3} = 46.6 kW
Answer:
Q2=0.082m3/s,H2=70.6m,P2=46.6kWQ_{2} = 0.082 m^{3}/s, H_{2} = 70.6 m, P_{2} = 46.6 kW

Why the other options are there

  • H₂ = 34.6 m (linear scaling of head)
  • P₂ = 22.8 kW (squared instead of cubed)

Reference: FE Reference Handbook — Fluid Mechanics → Scaling Laws; Affinity Laws

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