System Curves & the Duty Point
Where the pump’s capability meets the system’s demand.
You don’t choose flow and head independently—the system and pump negotiate an operating point where their curves intersect.
System curve: what the piping “asks for”
A piping system requires head to (1) overcome any static elevation change and (2) overcome losses due to friction and fittings.
Many loss terms scale with velocity squared (v²). Since v ∝ Q for a given diameter, it is common to model the total loss as proportional to Q².
Darcy–Weisbach gives hf ∝ f(L/D)(v²/2g), and minor losses give hm ∝ K(v²/2g). For a fixed diameter, v is proportional to Q, so both terms scale approximately as Q².
Finding the duty point algebraically
If you approximate both curves with simple equations, you can solve for Q directly. At the duty point, Hpump(Q) = Hsys(Q).
- Set H_pump = H_sys: 50 − 200 Q² = 20 + 100 Q².
- Rearrange: 50 − 20 = 300 Q² → 30 = 300 Q².
- Solve for Q²: Q² = 30/300 = 0.10.
- Take the square root: Q = √0.10 = 0.316 m³/s (3 significant figures).
- Compute head at duty point using either curve: H = 20 + 100(0.10) = 30 m.
- Set curves equal: 45 − 200 Q² = 20 + 50 Q².
- Rearrange: 45 − 20 = 250 Q² → 25 = 250 Q².
- Solve: Q² = 25/250 = 0.10.
- Compute Q: Q = √0.10 = 0.316 m³/s.
When you solve for Q², take the positive root for physical flow. Also do a quick check by substituting back into both curves to confirm they match.
Check your understanding
- A system curve combines static lift and Q² loss terms.
- At the duty point, H_pump(Q) equals H_sys(Q).
- Increasing system resistance shifts the duty point to lower flow.
- Simple algebraic models let you solve duty points cleanly by solving for Q² first.