Pump & Fan Affinity Law Calculator Pumps & Fans

One operating point and a speed (or impeller) change, scaled by the affinity laws.
Flow tracks the ratio, head tracks its square, and power tracks its cube — which is the whole reason a VFD slowing a pump saves so much more energy than it gives up in flow. By speed is the VFD case; By impeller diameter is the trim case, exact for speed and approximate for small trims of the same casing.

Inputs are seeded with an example — edit them to your numbers.

Speeds take any consistent unit (RPM, Hz, %). Flow, head, and power pass through unchanged, so the outputs carry whatever units you entered — head (ft) for pumps, static pressure (in. w.c.) for fans, power in bhp or kW.

Speed ratio N₂/N₁
Flow Q₂  (∝ ratio)
Head / pressure H₂  (∝ ratio²)
Power P₂  (∝ ratio³)

Q₂ / H₂ / P₂ carry the same units you entered above — this tool just scales the magnitudes.

A VFD slows a pump from 60 Hz to 50 Hz — 83 % speed — at an operating point of 100 GPM, 50 ft head, 10 bhp.

  1. Ratio: 50 ÷ 60 = 0.833.
  2. Flow: 100 × 0.833 = 83.3 GPM (linear).
  3. Head: 50 × 0.833² = 34.7 ft (square).
  4. Power: 10 × 0.833³ = 5.8 bhp (cube).

A 17 % speed cut costs about 17 % of flow but nearly halves the power. The cube law is the energy case for variable-speed pumping — and the reason the savings shrink fast once you stop riding the curve down (see Pump Control).

The laws scale points on the pump or fan’s own curve; whether the machine actually rides down the affinity parabola is a system question. The cube-law payoff assumes a mostly-friction system curve — little or no static lift — with efficiency holding roughly constant. Add real static head — an open cooling tower, irrigation, anything that lifts water out of a sump (open-loop work; a closed loop recovers its own elevation and carries none) — and the operating point leaves the parabola, so the savings flatten short of the cube. Speed is the exact case for the curve; the system decides how much of it you keep.

Diameters take any consistent unit (in, mm). The diameter laws hold only for modest trims of the same casing — past roughly 10–15 % the efficiency falls off and the simple ratios drift.

Diameter ratio D₂/D₁
Flow Q₂  (∝ ratio)
Head / pressure H₂  (∝ ratio²)
Power P₂  (∝ ratio³)

Q₂ / H₂ / P₂ carry the same units you entered above — this tool just scales the magnitudes.

QuantityBy speed (N)By diameter (D)
Flow Q∝ N₂/N₁∝ D₂/D₁
Head / pressure H∝ (N₂/N₁)²∝ (D₂/D₁)²
Power P∝ (N₂/N₁)³∝ (D₂/D₁)³

Speed is the exact, reversible case — slow a pump and speed it back up and it returns to the same point. Impeller trim is permanent metal and only approximate: good for a one-time match of an oversized pump to its duty, not for control.

Before acting on P₂, check the motor. The cube law works both ways: a 10 % speed increase asks the motor for 33 % more power. This page scales the load — as a cross-check and a teaching aid — but whether the motor survives the new speed is decided by the nameplate HP, the service factor, and the overload settings. Confirm those before raising a maximum frequency; the calculator predicts the load, it doesn’t protect the motor.

What are the pump and fan affinity laws?

They scale a known operating point to a new speed (or impeller / sheave diameter) — flow varies with the ratio, head or pressure with its square, and power with its cube. Q₂ = Q₁·(N₂/N₁), H₂ = H₁·(N₂/N₁)², P₂ = P₁·(N₂/N₁)³.

Why does a VFD save so much energy?

Because power follows the cube of speed. Slowing a pump or fan to 80% speed drops flow to 80% but power to 0.8³ ≈ 51% — roughly half the energy for 80% of the flow. That cube is the whole energy case for variable-speed drives.

Do the affinity laws hold with static head?

Only the friction-head portion follows the cube. On a system with real static head (open loops, vertical lift), the operating point rides a flatter system curve, so actual power savings fall short of the ideal cube — model the static head separately.
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