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.
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).
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):
$$ V = \frac{\pi}{4} D^{3} \quad\Rightarrow\quad D = \sqrt[3]{\frac{4V}{\pi}}, \qquad L = D, \qquad r = \frac{D}{2} = \sqrt[3]{\frac{V}{2\pi}} $$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:
$$ d_{\text{DN}} \;=\; \mathrm{ceil}_{\text{DN}}\bigl(d_{\text{req}}\bigr), \qquad v_{\text{corr}} \;=\; \frac{Q}{A(d_{\text{DN}})} $$Convert backpressure \(\Delta p\) to head \(H\) (water):
$$ H \;=\; \frac{\Delta p}{\rho g}, \qquad \Delta p[\mathrm{Pa}] = \text{mbar}\times 100 $$Using the pump head coefficient \(\psi\) (0.6–1.0 typical):
$$ U_{\text{tip}} \;=\; \sqrt{\frac{g\,H}{\psi}}, \qquad \mathrm{RPM} \;=\; \frac{60\,U_{\text{tip}}}{\pi\,D_{\text{imp}}} $$Available head should at least cover exit velocity head:
$$ H_{\min} \;=\; \frac{v_{\text{pipe}}^{2}}{2g}, \qquad \text{passes} \;=\; \bigl(H \ge H_{\min}\bigr), \qquad \text{margin} \;=\; H - H_{\min} $$Viscous torque (above), geared by ratio \(G\) (e.g., 16 or 32):
$$ \tau_{\text{geared}} \;=\; \frac{\tau}{G} $$Mechanical power and electrical input (efficiency \(\eta\)):
$$ P_{\text{mech}} \;=\; \tau_{\text{geared}}\,\omega, \qquad P_{\text{elec}} \;=\; \frac{P_{\text{mech}}}{\eta} $$If energy is used only during off-time:
$$ m \;=\; \frac{T_{\text{off}}}{T_{\text{on}} + T_{\text{off}}}, \qquad \overline{P}_{\text{valve}} \;=\; m \; P_{\text{elec}} $$At operating point \((Q,H)\):
$$ P_{\text{hyd}} \;=\; \rho g Q H, \qquad P_{\text{elec,pump}} \;=\; \frac{P_{\text{hyd}}}{\eta_{\text{pump}}} $$
• 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.