A single acting reciprocating pump has a plunger diameter 0.15 m and stroke length 0.3 m. The centre of the pump is 4 m above the suction level. The atmospheric pressure in the suction level is 10.3 m of water. The pump is running at 40 rpm. The length and diameter of the suction pipe are 5 m and 0.1 m, respectively. Determine the pressure head due to acceleration in the cylinder at the beginning and at the middle of the stroke. Also find the absolute pressure head in the cylinder at the beginning of the suction stroke.
Given: D = 0.15 m, L = 0.3 m, H_{s} = 4 m, H_{at} = 10.3 m of water, N = 40 rpm, l_{s} = 5 m, d_{s} = 0.1 m
Now,
Angular speed of the crank, \omega={\frac{2\pi N}{60}}={\frac{2\times\pi\times40}{60}}=4.188\,{\mathrm{rad/s}}
Radius of the crank, r={\frac{L}{2}}={\frac{0.3}{2}}=0.15\,\mathrm{m}
Area of the piston, A={\frac{\pi}{4}}\times\left(0.15\right)^{2}=0.01767\,{\mathrm{m}}^{2}
Area of the suction pipe, a_{s}={\frac{\pi}{4}}\times(0.1)^{2}=0.007853\,{\mathrm{m}}^{2}
Thus, the equation of pressure head due to acceleration is
h_{s}={\frac{l_{s}}{g}}{\frac{A}{a_{s}}}\,r\omega^{2}\cos\thetaor h_{s}=\frac{5}{9.81}\times\frac{0.01767}{0.007853}\times0.15\times(4.188)^{2}\cos\theta
or h_{s}=3.01837\,\cos\theta
Again, at the beginning of stroke, θ = 0, cos θ = 1. Therefore,
h_{smax} = 3.01837 m
and at the middle of the stroke, θ = 90°, cos θ = 0. Therefore,
h_{s} = 0
Thus, the absolute pressure head in the cylinder at the beginning of the suction stroke is:
H_{at} – H_{s} – h_{smax}
= 10.3 – 4 – 3.01837 = 3.28163 m