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A graphical picture of the the pump pressure gain against volumetric flowrate aginst  (Fig. 1).In most practical cases the pump model can be   on the difference between intake and discharge pressure 

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body--uriencoded--p_%7B\rm out%7D - p_%7B\rm in%7D
 and called pump characteristic curve (see Fig. 1):

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anchorKD0ZN
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q = q(p_{\rm out} - p_{\rm in})

Image Modified

Fig. 1.

 
as function of delta pressure 
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body--uriencoded--p = p_%7B\rm out%7D-p_%7B\rm in%7D

.

The most general Pump model is given as a function of volumetric flowrate of the intake

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body--uriencoded--p_%7B\rm in%7D
 and discharge pressure 
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body--uriencoded--p_%7B\rm out%7D
:

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anchorpump
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q = q(p_{\rm out}, p_{\rm in})

The electrical power consumption  

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body--uriencoded--\displaystyle W = \frac%7BdE%7D%7Bdt%7D
is given by:

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anchoreta_pump
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W =  \eta(q) \cdot q \cdot (p_{\rm out}-p_{\rm in})

where

...

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body\eta

...

A popular pump proxy model is given by the quadratic equation:

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anchorq_pump
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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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anchorq_pump
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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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anchorQ056T
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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

maximum pressure gain that pump can exert over the input pressure 

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bodyp_{\rm in}

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bodyq_{\rm max}

maximum flowrate that pump can produce

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bodyk_f \in [0,1]

total hydraulic pump friction (dimensionless)

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body\eta

pump efficiency

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body\eta_{\rm max}

maximum pump efficiency

The plunger pump and centrifugal pumps are normally adjusted by working frequency 


See also

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Natural Science / Engineering / Device / Pump

[ Pump @model ]

Physics / Fluid Dynamics / Pipe Flow Dynamics / Pipe Flow Simulation (PFS)

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