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(b) Water flows under gravity between two reservoirs through a pipe of length 5000m. The diameter of the pipe is 0.2 m and th

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Ans) Apply Bernoulli equation between water surface of two reservoirs as :

P1/\rhog + V12/2g + Z1 = P2/\rhog + V22/2g + Z2 + Hf + Hm

where, P1 and P2 are pressures at point 1 and 2 respectively. Since , the reservoirs are open to atmosphere , pressue is only atmospheric pressure, hence gauge pressure P1 = P2 = 0

Also, velocities V1 and V2 at surface = 0

Z1 and Z2 are datum head. Let point 2 be datum , then

Z1 = 50 m and Z2 = 0

Hf = head loss due to friction

a) Since minor loss has to neglected, therefore, above equation reduces to,

0 + 0 + 50 = 0 + 0 + 0 + Hf

=> Hf =f L V2/ D(2g) = 50

where, f = Darcy friction factor

L = length of pipe

V = velocity of flow

D =diameter of pipe

To determine 'f' , let us find Reynold number (Re)

Re = \rho V D/ \mu

where, \mu = dynamic viscosity of water = 0.001 Ns/m2

Re = 1000 x V x 0.2 / 10-3

= 2V x 105

According to Moody diagram, approx value of friction factor can be determined by 'Re' and relative roughness = e/D

= 0.00004 / 0.2 = 0.0002

For Re = 2 x 105 and e/D = 0.0002 , 'f' = 0.016

=> 0.016 x 5000 x V2 / (0.2 x 2 x 9.81) = 50

=> V = 1.566 m/s

Discharge = Area x velocity

= (\pi/4) x 0.2 x 0.2 x 1.566

= 0.049 m3/s

Ans b) Now, if minor loss also be considered then,

Hf + Hm = 50 [from part (a)]

Friction loss + loss due to entry + loss due to exit + loss due to valve = 50

=> f L V2/ D(2g) + Ke V2/2g + Kv V2 /2g = 50

=> V2/2g ( 0016 x 5000/0.2 + 0.50 + 80) = 50

=> V2 = 0.104 x 2 x 9.81

=> V= 1.428 m/s

Discharge = area x velocity

= (\pi/4) x 0.2 x 0.2 x 1.428

= 0.0448 m3/s  

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