Pump Affinity Laws Back
Fluid Analysis

Pump Affinity Laws Simulator

Interactively explore centrifugal pump scaling laws Q∝n, H∝n², P∝n³. Overlay H-Q and power curves at rated and reduced speeds to quantify variable-frequency drive (VFD) energy savings.

m³/h
m
kW
(80%)
Results
New Flow Q₂ (m³/h)
New Head H₂ (m)
New Power P₂ (kW)
Power Reduction (%)
H-Q Curve (Head vs. Flow)
P-Q Curve (Shaft Power vs. Flow)
Theory & Key Formulas
$$\frac{Q_2}{Q_1}= \frac{n_2}{n_1}$$ $$\frac{H_2}{H_1}= \left(\frac{n_2}{n_1}\right)^2$$ $$\frac{P_2}{P_1}= \left(\frac{n_2}{n_1}\right)^3$$

Power scales as the cube of speed ratio. Reducing to 80% speed saves ~49% power (0.8³ ≈ 0.512). This is the basis for VFD energy savings in pumping systems.

What are Pump Affinity Laws?

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What exactly are the "affinity laws" for a pump? I've heard they're important for saving energy.
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Basically, they're a set of three simple rules that predict how a pump's performance changes when you change its rotational speed. In practice, if you slow a pump down, you don't just get less flow—the pressure it can generate and the power it needs drop by even more. Try moving the "Speed Ratio" slider in the simulator above from 1.0 down to 0.8 and watch what happens to Power.
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Wait, really? The power drops that much? So if I need less flow, it's way more efficient to slow the pump than to just throttle a valve?
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Exactly! Throttling a valve wastes energy by creating a pressure drop. Slowing the pump with a Variable Frequency Drive (VFD) reduces the energy going into the fluid from the start. For instance, in the simulator, set your rated power to 100 kW and the speed ratio to 0.7. You'll see the new power is only about 34 kW—that's a 66% savings!
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That's huge. But are these laws always accurate? What if I change the impeller diameter instead of the speed?
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Great question. The laws are very accurate for a given pump at different speeds, assuming the fluid and system don't change. They are the foundation for VFD control. For impeller trimming, similar but slightly different laws apply—the exponents change. The simulator here focuses on speed change, which is the most common way to achieve these dramatic savings. Play with different Rated Flow and Head values to see how the savings scale universally.

Physical Model & Key Equations

The affinity laws are derived from the principles of fluid dynamics and fan/pump similarity. The first law states that the volumetric flow rate (Q) is directly proportional to the rotational speed (n).

$$\frac{Q_2}{Q_1}= \frac{n_2}{n_1}$$

Where $Q_1$, $n_1$ are the initial flow and speed, and $Q_2$, $n_2$ are the new values.

The pressure or head (H) developed by the pump is proportional to the square of the speed. This comes from the centrifugal force ($\omega^2 r$). The required shaft power (P) is the product of flow and head, leading to a cubic relationship with speed.

$$\frac{H_2}{H_1}= \left(\frac{n_2}{n_1}\right)^2 \quad ; \quad \frac{P_2}{P_1}= \left(\frac{n_2}{n_1}\right)^3$$

$H$ is pump head in meters, $P$ is power in kW. The cubic law for power is why energy savings are so significant with even small speed reductions.

Real-World Applications

HVAC Building Systems: In large office towers, cooling water pumps run continuously. Using VFDs to slow pumps at night or during mild weather, following the affinity laws, can cut their energy consumption by over 50%, drastically reducing operating costs.

Water & Wastewater Treatment: Plant inflow varies daily. Instead of constantly turning large pumps on and off, treatment plants use VFDs to modulate pump speed, matching flow demand precisely and avoiding water hammer while saving energy.

Industrial Process Control: In a chemical plant, a process may require different flow rates for different batches. Adjusting pump speed via the affinity laws provides accurate, energy-efficient flow control without needing complex valve networks or bypass lines.

Irrigation Systems: Large agricultural irrigation pumps can be slowed during periods of lower water demand or at the ends of irrigation lines where pressure requirements are lower. This reduces power demand and protects pipelines from excessive pressure.

Common Misconceptions and Points to Note

The affinity laws are powerful, but there are several pitfalls in their application. First, the fundamental assumption is "similarity". Significantly changing the rotational speed alters the flow conditions inside the pump (Reynolds number), changing its efficiency. For example, reducing the speed of a pump from its rated 1750 min⁻¹ down to 500 min⁻¹ tends to result in actual shaft power being slightly higher than predicted by the cube law. The simulator assumes ideal similarity, so detailed efficiency changes in actual machines require separate consideration.

Next, do not overlook the relationship with the system resistance curve. Even if the pump performance curve shifts according to the affinity laws, the actual operating flow rate and head are determined by the intersection with the piping system's resistance curve. For instance, if you lower the speed too close to shut-off (zero flow), a situation can occur where the head becomes insufficient and no water is delivered at all. When using the tool to manipulate the performance curve, always imagine, "Where will this new curve intersect with my actual piping system?"

Finally, note that "reducing speed does not always save energy". While the pump's power consumption alone decreases dramatically, the story is different when looking at the entire process. For example, if the cooling water flow rate drops too much, the heat exchanger's thermal performance may decline, causing the chiller to work harder and potentially increasing the overall power consumption. Always use the results from this tool as part of a system optimization effort.

What is Pump Affinity Laws Simulator?

Pump Affinity Laws Simulator is a fundamental topic in engineering and applied physics. This interactive simulator lets you explore the key behaviors and relationships by directly manipulating parameters and observing real-time results.

By combining numerical computation with visual feedback, the simulator bridges the gap between abstract theory and physical intuition — making it an effective learning tool for students and a rapid-verification tool for practicing engineers.

How to Use

  1. Enter baseline pump conditions: flow rate (q1 in m³/h), head (h1 in m), and power consumption (p1 in kW) from your pump curve or nameplate data.
  2. Set the speed ratio (ratioValNum) representing the ratio of new operating speed to baseline speed—for example, 0.8 for 80% speed on a VFD-driven pump.
  3. The simulator applies the three affinity laws: flow scales linearly with speed, head scales with speed squared, and power scales with speed cubed—then displays new operating parameters and energy consumption.

Worked Example

A centrifugal pump operating at 1450 rpm delivers 150 m³/h at 45 m head while consuming 22 kW. When reduced to 75% speed (ratio=0.75) via VFD: flow becomes 112.5 m³/h (150×0.75), head drops to 25.3 m (45×0.75²), and power consumption falls to 9.3 kW (22×0.75³). This 58% power reduction translates to significant energy savings in HVAC and industrial circulation systems.

Practical Notes

  1. VFD installation on existing 1750 rpm motors becomes cost-effective when affinity calculations show >12% speed reduction potential, typical in oversized distribution systems.
  2. Affinity laws assume constant fluid properties and pump efficiency within ±10% of design point; deviation increases beyond 50% speed reduction.
  3. System curve interaction matters: for constant-pressure systems, actual power savings exceed cube-law predictions; for friction-dominated piping, savings match theoretical values closely.
  4. Verify pump NPSHR at reduced speeds—cavitation risk increases if suction head becomes inadequate despite lower flow demand.