The most general Pump model is given as a function of volumetric the mass flowrate of on the intake
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| body | --uriencoded--p_%7B\rm in%7D |
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and discharge pressure
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| body | --uriencoded--p_%7B\rm out%7D |
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:
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| anchor | pump_m |
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| alignment | left |
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\dot m = M(p_{\rm out}, p_{\rm in}) |
It's often presented in terms of intake volumetric flowrate:
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| anchor | pump_q |
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| alignment | left |
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q = q_{in} = \frac{\dot m}{\rho(p_{in})} = \frac{M(p_{\rm out}, p_{\rm in})}{\rho(p_{in})} |
where
| fluid density as a function of fluid pressure |
The electrical power consumption
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| body | --uriencoded--\displaystyle W = \frac%7BdE%7D%7Bdt%7D |
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is given by:
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In most practical cases the pump model the pump model
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depends depends on the diffference between difference between intake and discharge pressure | LaTeX Math Inline |
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| body | --uriencoded--p_%7B\rm out%7D - p_%7B\rm in%7D |
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and called pump characteristic curve called Pump Characteristic Curve (see Fig. 1):| LaTeX Math Block |
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q = q(p_{\rm out} - p_{\rm in}) |
A popular pump proxy model is given by the quadratic equation with 3 inputs (
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| 'rf max%7D, \delta p_%7B\rm |
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)A popular pump proxy model is given by quadratic equation:
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| anchor | q_pump |
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| alignment | left |
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| q = \frac{q_{\rm max}}{2 \cdot k_f} \cdot \left[ -1 + k_f + \sqrt{ (1 + k_f)^2 - 4 \cdot k_f \cdot (p_{\rm out}- p_{\rm in})/\delta p_{\rm max}) \ } \, \right] |
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| anchor | q_pump |
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| alignment | left |
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| p_{\rm out} = p_{\rm in} + \delta p_{\rm max} \cdot \left[ 1+
(k_f -1 ) \cdot \frac{q}{q_{\rm max}} - k_f \cdot \left( \frac{q}{q_{\rm max}} \right)^2
\right ] |
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\eta(q) = 4 \, \eta_{\rm max} \cdot q/q_{\rm max} \cdot ( 1 - q/q_{\rm max}) |
where
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| body | --uriencoded--\delta p_%7B\rm max%7D |
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| maximum pressure gain that pump can exert over the input pressure |
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| maximum flowrate that pump can produce |
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| total hydraulic pump friction (dimensionless) |
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| pump efficiency efficiency |
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| maximum pump efficiency |
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Real pumps have non-constant friction coefficient which often modelled as a 3rd order polynomial and the overall real-pump model taking 6-inputs.
Many pumps can be normally adjusted by the variation of the working frequency which affects the maximum pump flowrate and maximum pressure gain as:
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| q_{\rm max} = q^*_{\rm max} \cdot \frac{f}{f^*} |
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| \delta p_{\rm max} = \delta p^*_{\rm max} \cdot \left( \frac{f}{f^*} \right)^2 |
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where
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| body | --uriencoded--q_%7B\rm max%7D |
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| maximum intake flowrate at the working frequency | | LaTeX Math Inline |
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| body | --uriencoded--\delta p_%7B\rm max%7D |
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| maximum pressure gain at the working frequency | | adjusted working frequency |
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| body | --uriencoded--q%5e*_%7B\rm max%7D |
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| maximum intake flowrate at the nominal frequency | | LaTeX Math Inline |
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| body | --uriencoded--\delta p%5e*_%7B\rm max%7D |
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| maximum pressure gain at the nominal frequency | | nominal frequency |
See also
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Natural Science / Engineering / Device / Pump
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