Question 21.19: The following details refer to working of a single-acting re......

The following details refer to working of a single-acting reciprocating pump with an air vessel fitted on the delivery pipe very close to the cylinder.

Piston diameter = 20 cm

Crank radius = 15 cm

Speed of the pump = 50 rpm.

Diameter of the delivery pipe = 10 cm

Length of the delivery pipe = 25 m

Darcy’s friction factor = 0.02

Atmospheric pressure head = 10.3 m of water

Find the power saved in overcoming the friction by fitting the air vessel.

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Diameter of piston                  D = 20 cm = 0.20 m

Crank radius                              r = 15 cm= 0.15 m

Speed of pump                          N = 50 rpm

Diameter of delivery pipe      ddd_{{d}}  =10 cm = 0.10 m

Length of delivery pipe         ld=25 ml_{d}=25{\mathrm{~m}}

Darcy’s friction factor            f = 0.02

Atmospheric pressure head  hatmh_{a t m} = 10.3 m of water

Area of piston is given by

A=π4D2=A=\frac{\pi}{4}D^{2}= π4(0.15)2=0.0177m2\frac{\pi}{4}(0.15)^{2}=0.0177\,{\mathrm{m}}^{2}

Area of delivery pipe is given by

ad=π4dd2=a_{d}=\frac{\pi}{4}d_{d}^{2}= π4(0.1)2=0.00785m2\frac{\pi}{4}(0.1)^{2}=0.00785\,{\mathrm{m}}^{2}

Angular speed is given by

ω=2πN60=\omega={\frac{2\pi N}{60}}=2π×5060=5.236rad/s{\frac{2\pi\times50}{60}}=5.236\,\mathrm{rad/}{s}

Without air vessel: The loss of head due to friction in delivery pipe is computed from Eq. (21.24) as

hfd,max=h_{f d,m a x}=flddd×2g ⁣(Aadωr)2\frac{{fl}_{d}}{d_{d}\times2g}\!\left(\frac{A}{a_{d}}\omega r\right)^{2}

=0.02×250.1×2×9.81={\frac{0.02\times25}{0.1\times2\times9.81}}(0.01770.00785×5.236×0.15)2\left({\frac{0.0177}{0.00785}}\times5.236\times0.15\right)^{2} = 0.7984 m

Power required in overcoming the friction is found to be

Pwithout=ρgQP_{w i t h o u t}=\rho g Q ×23hfd,max\times{\frac{2}{3}}h_{f d,m a x} =ρgALN60×23hfd,max={\frac{\rho g A L N}{60}}\times{\frac{2}{3}}h_{f d,m a x}           [Q=ALN60]\left[\because Q = \frac{ALN}{60} \right]

=1000×9.81×0.0177×0.3×4060={\frac{1000\times9.81\times0.0177\times0.3\times40}{60}} ×23×0.7984=18.484 W \times{\frac{2}{3}}\times0.7984=18.484{\mathrm{~W~}}

With air vessel: The loss of head due to friction in delivery pipe by fitting an air vessel is computed as

hfd=fldνaν2dd×2g=h_{f d}=\frac{fl_{d}\nu_{a\nu}^{2}}{d_{d}\times2g}= flddd×2g×(Aad×ωrπ)2{\frac{{\mathcal{fl}}_{d}}{d_{d}\times2g}}\times\left({\frac{A}{a_{d}}}\times{\frac{\omega r}{\pi}}\right)^{2}

=0.02×250.1×2×9.81×={\frac{0.02\times25}{0.1\times2\times9.81}}\times (0.01770.00785×5.236×0.15π)2=0.081m\left({\frac{0.0177}{0.00785}}\times{\frac{5.236\times0.15}{\pi}}\right)^{2}=0.081\,{\mathrm{m}}

Power required in overcoming the friction is found to be

Pwith=ρgQ×hfdP_{w i th}=\rho g Q\times h_{f d} =ρgALN60×hfd=\frac{\rho g A L N}{60}\times h_{f d}

=1000×9.8 1×0.0177×0.3×4060={\frac{1000\times9.8\ 1\times0.0177\times0.3\times40}{60}} ×0.081=2.183  W\times0.081=2.183\,\,\mathrm{W}

The power saved in overcoming the friction by fitting the air vessel is

PwithoutPwith=P_{w i t h o u t}-P_{w i t h}= 18.484 – 2.183 = 16.301 W

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