Slay the P.E.
Well-known member
A little clarification seems to be in order here.
Equation 18.30 in MERM 13 (see attached photo) is based on the conditions at the fluid surface at the top of an open (to atmosphere) fluid source (e.g. tank, reservoir, etc). As this problem shows, that situation is by no means the only one that can be presented. We recommend using only equation 18.31 which is the actual definition of NPSHA: the actual total fluid energy at the pump inlet. Equation 18.31 is based on the conditions at the immediate entrance (suction, subscript s) to the pump.
In our practice problem (the one with the condenser above the pump) we don't know anything about the pump suction but we need the sum of pressure head h_p,s and velocity head h_v,s at the pump suction. However, we can get (h_p,s + h_v,s) by applying the extended Bernoulli equation between the free surface inside the condenser and the pump inlet.
Equation 18.30 in MERM 13 (see attached photo) is based on the conditions at the fluid surface at the top of an open (to atmosphere) fluid source (e.g. tank, reservoir, etc). As this problem shows, that situation is by no means the only one that can be presented. We recommend using only equation 18.31 which is the actual definition of NPSHA: the actual total fluid energy at the pump inlet. Equation 18.31 is based on the conditions at the immediate entrance (suction, subscript s) to the pump.
In our practice problem (the one with the condenser above the pump) we don't know anything about the pump suction but we need the sum of pressure head h_p,s and velocity head h_v,s at the pump suction. However, we can get (h_p,s + h_v,s) by applying the extended Bernoulli equation between the free surface inside the condenser and the pump inlet.