Simple pump energy calculator

This calculator automates most of the pump math, making it a simple tool to estimate the pump’s energy use. Default values are based on our pilot test and approximate what a well-tuned system would deliver.

  1. Enter the desired flow.
  2. Estimate pipe friction for your layout and enter the resulting backpressure (keep it as low as practical).
  3. Set the switching time. A typical starting point is 10 s. Longer times increase the required housing volume but reduce valve actuation energy per hour; faster switching allows a smaller housing but increases valve actuation energy.
  4. Motor RPM & gear ratio mainly affect speed/torque, and energy reductions on low RPM's.

Flow

This input sets the target flow and automatically sizes the pump volume based on flow and switching time.

Automatic pump sizing may not be practical for final design, but it is included here for simplicity.

The calculations depend primarily on the specified flow and the backpressure from the pipework.

The flow sets the pipe diameter using a fixed 1.3 m/s design velocity, then rounds up to the nearest metric DN size. This may increase the selected valve size.

Example: From the default values from our pilot test, it may be difficult to see the real efficiency and cost effects unless you increase the flow to 240 m3. Change the flow to 240 m3 and increase elevation to 10 meter, and you will better understand the pumps efficiency.

Backpressure

This value is the pressure loss your system imposes, calculated from the pipework (friction in straight runs plus losses in fittings/valves) at the chosen flow.

Keep this as low as possible (< 80 millibar) since it directly reduces pump power

How to reduce backpressure:
• Increase pipe diameter (DN): lowers velocity and friction (Δp ∝ v²).
• Shorten pipe runs; avoid unnecessary loops.
• Minimize fittings/valves; use long-radius bends and smooth transitions.
• Use smoother pipe/linings; keep throttling to a minimum and valves fully open where possible.
• Split flow into parallel lines if a single line forces high velocity.

Recalculate after changes: upsizing the pipe will reduce backpressure and may allow a lower required RPM.

Switching time

The switching time is how often the valves change position; it sets the exchange rate and the required pump volume (we size the housing for the flow moved during one switching period).

Longer switching times increases the required housing volume and typically lower the valve duty cycle. For example, with a 10 second switching time, the pump circulates for 10 seconds before the valve switches side.
Increasing the motor RPM alters the duty cycle. Higher valve energy and faster switching help balance energy consumption and may allow for a smaller pump.

Example: For the pilot test, when optimized properly, the switching time is quite high, which significantly reduces the duty cycle and lowers overall valve energy use.

Note: If you do not understand this value, set it to 10 seconds or higher and observe how the valve energy use and calculated pump size changes for that switching time.

Valve input - Motor RPM

To rotate the valve 90° (open/close), the valve motor output shaft must turn 4 or 8 revolutions with a gear ratio of 1/16 or 1/32.

Examples: at 1/16 gearing, 240 RPM gives 90° in 1.0 s; 480 RPM gives 90° in 0.5 s. With 1/32 gearing, bigger valves may have better operational conditions.

Increasing RPM makes the actuation faster: the valve motor draws more instantaneous power for a shorter duration, so the energy per actuation is roughly unchanged. For low RPM operations this will affect energy usage.

Elevation

Enter the elevation (pump head) you expect for water circulation. This helps illustrate the energy efficiency of the pump. At very low elevations (around 1 meter), efficiency decreases, but from 2 meters and above, efficiency improves. The key principle of the Zero Gravity Pump is to minimize pumping against hydrostatic pressure, focusing instead on circulating water rather than lifting it.

Example: In our pilot test, water was circulated to a height of 2.3 meters (the default setting). If you add 20 meters of straight piping (raising the elevation to 12.3 m), this only adds about 16 millibar of backpressure at the measured flow.

To test this effect, set the elevation to 12.3 meters and the backpressure to 66 millibar. You’ll see that energy efficiency increases, while only a small amount of additional power is required.

Multiplier

The pump multiplier distributes the total flow across several pumps arranged in parallel and recalculates the dimensions of each pump accordingly. The pump size is then automatically adjusted based on the selected multiplier.

The multiplier can be used together with the switching rate to determine a reasonable pump size for operation.

NOTE: This multiplier scales the pump assuming equal length and height, which does not fully reflect an actual configuration.
Because of the pump’s low RPM, the effective flow and valve sizes may be smaller than shown here, which also affects the scaling.
Still, the calculation provides useful insight into the non-linear scaling behavior that the pump is subjected to.

Responsive image
Pump Inputs
Valve Inputs
Elevation / (pump head)

Calculations

Calculations used

Navier–Stokes (viscous shear torque)

Viscometer

Idealized torque for viscous shear in a thin gap between radii \(r_1\) and \(r_2\):

$$ \tau \;=\; \pi\,\mu\,\frac{\omega}{h}\,\bigl(r_2^4 - r_1^4\bigr) $$

Here \(\mu\) is dynamic viscosity, \(\omega\) motor angular speed (rad/s), \(h\) the gap (m).

Flow & pump-housing volume

The housing is sized to hold one switching period worth of flow:

$$ V_{\text{cyl}} = Q \, t_{\text{sw}} $$

With a cylindrical chamber \( V = \pi r^{2} L = \frac{\pi}{4} D^{2} L \). If we choose \( L = D \) (stroke equals diameter):

$$ V = \frac{\pi}{4} D^{3} \quad\Rightarrow\quad D = \sqrt[3]{\frac{4V}{\pi}}, \qquad L = D, \qquad r = \frac{D}{2} = \sqrt[3]{\frac{V}{2\pi}} $$

Pipe sizing from flow

Choose a design velocity \(v_{\text{pipe}}\) (e.g. 0.6 m/s). From continuity \(Q=A\,v\):

$$ A_{\text{pipe}} = \frac{Q}{v_{\text{pipe}}}, \qquad d_{\text{req}} \;=\; \sqrt{\frac{4A}{\pi}} \;=\; \sqrt{\frac{4Q}{\pi\,v_{\text{pipe}}}} $$

Then round up to the nearest metric DN size:

$$ d_{\text{DN}} \;=\; \mathrm{ceil}_{\text{DN}}\bigl(d_{\text{req}}\bigr), \qquad v_{\text{corr}} \;=\; \frac{Q}{A(d_{\text{DN}})} $$

Backpressure to hydraulic head

Convert backpressure \(\Delta p\) to head \(H\) (water):

$$ H \;=\; \frac{\Delta p}{\rho g}, \qquad \Delta p[\mathrm{Pa}] = \text{mbar}\times 100 $$

Tip speed and RPM from head

Using the pump head coefficient \(\psi\) (0.6–1.0 typical):

$$ U_{\text{tip}} \;=\; \sqrt{\frac{g\,H}{\psi}}, \qquad \mathrm{RPM} \;=\; \frac{60\,U_{\text{tip}}}{\pi\,D_{\text{imp}}} $$

Velocity-head sanity check

Available head should at least cover exit velocity head:

$$ H_{\min} \;=\; \frac{v_{\text{pipe}}^{2}}{2g}, \qquad \text{passes} \;=\; \bigl(H \ge H_{\min}\bigr), \qquad \text{margin} \;=\; H - H_{\min} $$

Valve drive: torque, gearing, power

Viscous torque (above), geared by ratio \(G\) (e.g., 16 or 32):

$$ \tau_{\text{geared}} \;=\; \frac{\tau}{G} $$

Mechanical power and electrical input (efficiency \(\eta\)):

$$ P_{\text{mech}} \;=\; \tau_{\text{geared}}\,\omega, \qquad P_{\text{elec}} \;=\; \frac{P_{\text{mech}}}{\eta} $$

Duty-cycle multiplier (energy only during off-time)

If energy is used only during off-time:

$$ m \;=\; \frac{T_{\text{off}}}{T_{\text{on}} + T_{\text{off}}}, \qquad \overline{P}_{\text{valve}} \;=\; m \; P_{\text{elec}} $$

Pump hydraulic & electrical power

At operating point \((Q,H)\):

$$ P_{\text{hyd}} \;=\; \rho g Q H, \qquad P_{\text{elec,pump}} \;=\; \frac{P_{\text{hyd}}}{\eta_{\text{pump}}} $$

Notes

• Rounding up to DN reduces velocity \(v_{\text{corr}}\) and friction.
• The velocity-head check excludes friction and fittings since this pump's head calculations are solely based on friction and fittings: \( \Delta p = f \frac{L}{D}\frac{\rho v^2}{2} + \sum K \frac{\rho v^2}{2} \).
• Head coefficient \(\psi\) captures slip and geometry; refine with calibration or pump curves.