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Pump Hydraulic & Shaft Power

Water power from flow and head, and the shaft power once efficiency takes its cut.

InputP_hyd = ρ·g·Q·H P_shaft = P_hyd / η

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The engineering

Hydraulic power is the physics — lifting ρQ kilograms per second through H meters — and it doesn't negotiate. Efficiency is where the money goes: a mid-size centrifugal pump peaks around 70–85% at its best-efficiency point and falls off fast to either side, so a pump run far from BEP burns power and bearings alike.

Size the motor off *shaft* power at the worst expected operating point, then add service factor; and remember density matters — the same volumetric flow of brine (ρ ≈ 1200) costs 20% more power than water, while hydrocarbons run cheaper.

Where this math comes from

Leonhard Euler wrote the fundamental equation of turbomachinery in 1754 — how a spinning rotor exchanges energy with fluid — a century before anyone could build to it well. James Watt's horsepower (1782) is the other ancestor: defined by horses lifting water from mines, it made pumping power a commercial quantity, which is why this card still prints hp.

The centrifugal pump matured through the 1800s (John Appold's 1851 Great Exhibition demonstration of a curved-vane impeller tripled efficiency over straight blades), and the Hydraulic Institute — founded 1917 — standardized the test codes that make a vendor's η claim mean something.

  1. 1754Leonhard EulerEuler's turbomachine equation.
  2. 1782James WattHorsepower defined — pumping becomes a priced commodity.
  3. 1851John AppoldCurved-vane impeller shows efficiency is design, not luck.
  4. 1917Hydraulic InstitutePump test standards make efficiency claims comparable.

See the full timeline of the math behind every calculator →

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