Ans) Apply Bernoulli equation between water surface of two reservoirs as :
P1/g + V12/2g + Z1 = P2/g + 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 = V D/
where, = 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
= (/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
= (/4) x 0.2 x 0.2 x 1.428
= 0.0448 m3/s
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