A liquid of density d is pumped by a pump p from situation (i) to situation (ii) as shown in the diagram. If the cross-section of each of the vessels is a, then the work done in pumping (neglecting friction effects) is
dgh2a
Potential energy of liquid column in first situation =Vdgh2+Vdgh2=Vdgh=ahdgh=dgh2a
We know that, the centre of mass of liquid column lies at height h2.
Potential energy of the liquid column in second situation =Vdg(2h2)=(A×2h)dgh=2dgh2a
Work done pumping = Change in potential energy =2dgh2a−dgh2a=dgh2a