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Pumps & Rotating Equipment

System Curve vs Pump Curve

How the system curve and the pump curve interact, why the operating point is where they intersect, and how static head, friction, valve throttling, and speed move each curve — with what low flow can be telling you.

TypeEngineering guide — concept explainer

Definition

A pump curve and a system curve are two head-versus-flow relationships plotted on the same axes. The pump curve is the head a given pump delivers at each flow, falling as flow rises — it comes from the vendor for a fixed speed and impeller. The system curve is the head the piping demands at each flow: a fixed static (elevation/pressure) head plus friction and minor losses that grow roughly with the square of flow. Where the two curves cross is the operating point — the single flow and head at which the pump's delivery equals the system's demand. Everything in pump behaviour at steady state is a story about how those two curves move and where they intersect.

Why it matters

You cannot set the flow of a centrifugal pump directly; you can only change one of the two curves, and the operating point follows. Raise the static head or add friction (a partly shut valve, fouling, a longer line) and the system curve steepens or lifts, so the intersection slides up and to the left — less flow at more head. Change pump speed or impeller diameter and the whole pump curve scales by the affinity laws, moving the intersection the other way. This is why a pump rarely delivers its catalogue 'maximum' flow, why throttling a valve reduces flow without touching the pump, and why a flow problem is often a system-curve problem rather than a pump fault. Reading the two curves together is what turns a vague 'the pump is weak' into a specific, fixable cause.

Formula

System head (TDH form)
H_sys(Q) = H_static + K · Q²
Friction grows with flow
H_friction ∝ Q² (turbulent, fixed system)
Operating point
H_pump(Q) = H_sys(Q) → solve for Q
Speed change (affinity)
Q ∝ N, H ∝ N² (pump curve scales)

Units involved

  • Q — volumetric flow in m³/h, L/s, or gpm
  • H — head in metres (m) or feet (ft)
  • H_static — elevation/pressure head, independent of flow
  • K — lumped system resistance (head per flow², from friction + minor losses)
  • N — rotational speed in rpm (scales the pump curve)

Concept diagram

head (H)flow (Q)static headsystem curvepump curveoperating point

Worked example

A system has 12 m of static head and, at 50 m³/h, develops 7 m of friction + minor losses, so its resistance coefficient is K = 7 / 50² ≈ 0.0028 m per (m³/h)². The pump curve passes through (50 m³/h, 19 m). Check the operating point and see what throttling does.

  1. 01System head at 50 m³/h: H_sys = 12 + 0.0028 × 50² = 12 + 7 = 19 m
  2. 02Pump delivers 19 m at 50 m³/h → the curves intersect there: operating point ≈ 50 m³/h, 19 m
  3. 03Throttle a discharge valve (add ~5 m loss at 50 m³/h): the system curve steepens
  4. 04New intersection moves left — say to ~44 m³/h at a higher head — flow falls without changing the pump
  5. 05Slow the pump 10% instead (affinity): pump curve drops (H ∝ N²), intersection also moves to lower flow but at lower head, saving power
Result

Operating point ≈ 50 m³/h at 19 m. Throttling cuts flow by raising system resistance; slowing the pump cuts flow by lowering the pump curve — both move the intersection, but only the speed change saves energy.

Common mistakes

  • Expecting the pump to deliver its catalogue maximum flow — that is the curve's no-head end, not the operating point set by your system.
  • Treating static head and friction head as interchangeable — static head is flat with flow, friction rises with Q², and they move the operating point differently.
  • Throttling the suction side to control flow — this attacks NPSH available and invites cavitation; control on the discharge side.
  • Assuming a low flow means a faulty pump, when a steeper-than-expected system curve (closed valve, fouling, wrong line size) is the more common cause.
  • Comparing a measured duty against the pump curve without correcting for density, viscosity, or speed — the published curve is for clean water at the rated speed.

When to use the calculator

Build the system curve with the Total Dynamic Head calculator for the static and pressure terms, and the Pipe Head Loss, Darcy-Weisbach, and Minor Loss calculators for the flow-dependent friction. Use the Pump Affinity Laws calculator to see how a speed or impeller change scales the pump curve and moves the operating point.

FAQ

Why is the operating point at the intersection of the two curves?
At steady state the head the pump delivers must equal the head the system demands at the same flow. That equality holds at exactly one flow — the point where the pump curve and the system curve cross. Off that point, the pump and system heads disagree, so the flow adjusts until they meet.
What is the difference between static head and friction head?
Static head is the elevation (and any pressure) difference the pump must overcome regardless of flow — it is a flat line on the head-flow plot. Friction head is the loss in pipe and fittings, which grows roughly with the square of flow, so it is the rising part of the system curve. Together they make the total system head.
Why does throttling a valve reduce flow?
Closing a valve adds resistance, which steepens the system curve. The pump curve has not changed, so the intersection slides up and to the left: the pump produces more head at less flow. Throttling controls flow by reshaping the system, not by changing the pump.
How does changing pump speed move the curve?
By the affinity laws, flow scales with speed and head with speed squared, so reducing speed shifts the whole pump curve down and left. The system curve stays put, so the operating point moves to a lower flow and head — and because power scales with speed cubed, this is the efficient way to reduce flow.
Why do density and viscosity matter here?
A published pump curve is in head, which is largely density-independent, but it is measured on clean water at the rated speed. A viscous or slurry fluid raises friction (steeper system curve) and can derate the pump head and efficiency, so the real operating point sits away from where the clean-water curves predict.
My pump delivers low flow — is the pump or the system at fault?
It can be either, plus suction or measurement problems. A steeper-than-expected system curve (throttled valve, fouling, wrong line size) reduces flow with a healthy pump; a worn impeller, low speed, or wrong rotation lowers the pump curve; suction restriction or cavitation cuts delivery; and a faulty meter can make a normal duty look low. Work through the system-curve guide alongside the low-flow troubleshooting guide to isolate it.

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