After reading two of my articles on power pump valves, valve springs and net positive suction head required (NPSHR), Brazilian engineer Ricardo Martuscelli emailed me to suggest that I create graphs that illustrate the effects of speed (rpm) and the density of the pumpage on the NPSH requirements of these machines. That sounded like a good idea. We had the published NPSHR curves (see Figure 2), which were based on tests, but I had not used my equations to calculate equivalent curves. Could my equations produce such curves? If so, how would the calculated curves compare to the published curves? Could we include the effect of the density (specific gravity) of the pumpage in this exercise?

The equations did produce curves, which answered both questions, and are of sufficient interest, I think, to share in this article.

The following is the nomenclature used in the calculations:

A_{s} = Flow area through valve seat (wings & webs are ignored), ft^{2} (m^{2}) = (π/4)(D_{3}^{2} – D_{2}^{2})

A_{2} = Valve area acted on by P_{2}, ft^{2} (m^{2}) = (π/4) (D_{3}^{2} – D_{1}^{2}) = A_{4} – A_{3}

A_{3} = Seating surface area exposed to P_{3}, ft^{2} (m^{2}) = (π/4) (D_{4}^{2} – D_{3}^{2})

A_{4} = Area of top of valve (that was exposed to P_{4}), ft^{2} (m^{2) = (π/4) (D42 – D12)}

C = Orifice coefficient of valve “escape” area

D_{p} = Diameter of plunger or piston, ft (m)

D_{1} = Diameter of hole in center of valve disc, ft (m)

D_{2} = OD of inner seating surface, ft (m) (ID of port opening in seat)

D_{3} = ID of outer seating surface, ft (m) (OD of port opening in seat)

D_{4} = OD of valve outer seating surface, ft (m)

F_{o} = Force from spring(s) when valve is closed, lb (N)

g = Acceleration of gravity, 32.2 ft/sec^{2} (9.8 m/sec^{2})

K_{c} = Clinging coefficient

for an OD flow valve = ((D_{4}/D_{3})^{2} + (D_{3}/D_{4})^{2} – 2) / 8π(sinα)^{2}

for an ID flow valve = (2 – (D_{2}/D_{1})^{2} – (D_{1}/D_{2})^{2}) / 8π(sinα)^{2}

K_{i} = Coefficient of inertial impact of pumpage on upstream side of valve

L_{S} = Stroke length of plunger, ft (m)

L_{90} = The lift of the valve at about 90 degrees of crank otation, ft (m)

N = Rotative speed of pump crankshaft, rev/min

NPSHR = Net positive suction head required to prevent cavitation across the valve, lb/ft^{2} (Pa)

P_{1} = Stagnation pressure upstream of valve assembly, lb/ft^{2} (Pa)

P_{2} = Static pressure acting on upstream disc area A_{2}, lb/ft^{2} (Pa) = P_{1} – ρ(V_{S})^{2} / 2

Q_{1} = Flow rate created by plunger at mid stroke (the peak) = Q_{90}, assuming pure sinusoidal movement of plunger, ft^{3}/sec (m^{3}/s) = π^{2}NL_{s}D_{P}^{2}/240

R = Spring rate, lb/ft (N/m)

V_{S} = Velocity of pumpage moving through seat, ft/sec (m/s) = (Q_{2})/(A_{S})

W_{1} = Weight of valve (in air), lb (N)

W_{2} = Weight of the valve if axis is vertical, minus the buoyant effect of the pumpage, lb (N) = W1(1 – W_{3} / W_{4}) (if axis is horizontal, W_{2} = 0)

W_{3} = Specific weight of pumpage, lb/ft^{3} (N/m^{3}) = ρg

W_{4} = Specific weight of the valve, lb/ft^{3} (N/m^{3})

α = Angle between valve seating surface and valve axis, degrees

ρ = Density of pumpage, slugs/ft^{3} (lb-s^{2}/ft^{4}) (kg/m^{3}) = W_{3}/g

ω = Angular velocity of pump crankshaft, radians/sec = πN/30

The following equations were incorporated into a computer program, which used Equations 1, 2 and 3 (from Reference 2) to calculate the maximum lift of the valve (at mid-stroke) for each speed, then Equation 4 to calculate the pressure drop across the valve (NPSHR). This pressure drop was then plotted as a function of the pump rotative speed. The equations assume fully turbulent flow through the valve “escape” area (the flow area between the seating surfaces). They do not compensate for viscous liquids.

(1) L_{90} = (A/B)^{0.5}

Where:

(2) A = ρQ_{1}^{2}[A_{2}/2(cπD_{3} sinα)^{2} – K_{C}]

(3) B = ρQ_{1}^{2}(A_{2}/2A_{S} – K_{i})/A_{S} + F_{0} + W_{2} + L_{90} [R – W_{1} (πN/30)^{2}/g]

Because L90 appears on both sides of the equation, iteration is required for a solution. A trial value is plugged into the right side of the equation for a first trial solution.

(4) NPSHR = ρ(Q_{1}/cπD_{3}L_{9O}sin α)^{2} / 2

Figure 1 is a cross-sectional drawing of the 3-inch-stroke triplex pump for which these calculations were performed. The pressure losses from the suction nozzle to the valve, through the valve seat, and from the valve to the plunger are minimal. Therefore, the pressure drop across the seating surfaces of the valve and seat of the suction valve represent the NPSHR of the pump. In this pump, the valve lift is limited to 0.282 inches by a stop.

Figure 2 shows a published NPSHR curve for the pump with strong valve springs and compares it to the calculated curve. I believe that the published curve contains a 0.5 lb/in^{2} margin of safety. If 0.5 is subtracted from the published curve, the two curves fall on top of each other. Similar comparisons of the curves for the standard valve springs, and for no suction valve springs, produced equivalent results. The results indicate that the equations produce reasonably accurate NPSH curves.

What I find intriguing is the different shape of the two curves in Figure 2. The published curve cups slightly upward, which initially seems correct. The calculated curve cups slightly downward, which seems wrong until we realize that, until the valve hits the stop, any increase in differential pressure across the valve is partially relieved by the valve lifting higher. After the valve hits the stop, the NPSHR curve becomes a squared parabola (cupped upward).

Figure 3 is a plot of NPSHR for three different liquids, with specific gravities of 0.5, 1 and 1.5. We see that, at a very low speed, the NPSHR, expressed in pressure units, is not affected by the density (specific gravity) of the pumpage.

In Figure 3, the valve hits the stop at a differential pressure of about 8 psi. If we compare the NPSH requirements at 350 rpm (before the valve hits the stop), a 50 percent reduction in density results in only a 15 percent reduction in NPSHR (expressed in pressure units). A 50 percent increase in pumpage density results in an increase in NPSHR (expressed in pressure units) of only about 11 percent. The NPSHR (expressed in pressure units) does not vary to the same degree as the liquid density. The NPSHR characteristics of reciprocating pumps are different than those of centrifugal pumps.

## References

- Henshaw, Terry, “Power Pump Valve Dynamics – A Study of the Velocity and Pressure Distribution in Outward-Flow Bevel-Face and Flat-Face Power Pump Valves,” a technical paper presented at the Texas A&M 25th International Pump Users Symposium, Houston, Texas, 2009.
- Henshaw, Terry, “Improve Power Pump Performance With Stronger Valve Springs,”
*COMPRESSOR TechTwo*, July 2010. - Henshaw, Terry, “The Vital Role of Valve Springs in Power Pumps,”
*Pumps & Systems*, March 2011.