Question 11.5: A pipeline conveys 8.33 litre per second of water from an ov...

A pipeline conveys 8.33 litre per second of water from an overhead tank to a building. The pipe is 2 km long and 0.15 m in diameter. It is desired to increase the discharge by 30% by installing another pipeline in parallel with this over half the length. Suggest a suitable diameter of the pipe to be installed. Is there any upper limit on discharge augmentation by this arrangement? (Take friction factor f = 0.03.)

The blue check mark means that this solution has been answered and checked by an expert. This guarantees that the final answer is accurate.
Learn more on how we answer questions.

The height H of the overhead tank above the building can be determined from the conditions with a single pipe.

 

H=h_{f}=0.03 \frac{2000}{0.15}\left[\frac{(4 \times 0.00833)}{\pi(0.15)^{2}}\right]^{2} \frac{1}{2 \times 9.81}=4.53 m

 

In the new plan as shown in Fig. 11.17

 

h_{f}=4.53=h_{f_{A B}}+h_{f_{B C}} (11.39)

 

again,

 

h_{f_{B C}}=h_{f_{B D}}=\frac{f L_{1}}{2 g d_{1}}\left[\frac{4 Q_{1}}{\pi\left(d_{1}\right)^{2}}\right]^{2}=\frac{f L_{2}}{2 g d_{2}}\left[\frac{4 Q_{2}}{\pi\left(d_{2}\right)^{2}}\right]^{2}

 

Here, L_{1}=L_{2}=1000 m

 

Therefore, \left(Q_{1} / Q_{2}\right)^{2}=\left(d_{1} / d_{2}\right)^{5} (11.40)

 

h_{f_{A B}}=\frac{0.03 \times 1000}{2 g(0.15)}\left[\frac{4 Q}{\pi(0.15)^{2}}\right]^{2}

 

Therefore, Eq. (11.39) can be written as

 

\frac{0.03 \times 1000 \times 8 Q^{2}}{9.81 \times \pi^{2} \times(0.15)^{5}}+\frac{0.03 \times 1000 \times 8 \times Q_{1}^{2}}{9.81 \times \pi^{2} \times(0.15)^{5}}=4.53 (11.41)

 

In this case, Q=1.3 \times 0.00833=0.0108 m ^{3} / s

 

Then, from Eq. (11.41), we get

 

Q_{1}^{2}=0.00014-(0.0108)^{2}

 

which gives Q_{1}=0.0048 m ^{3} / s

 

From continuity, Q_{2}=0.0108-0.0048=0.006 m ^{3} / s

 

From Eq. (11.40), we have d_{2}=\left(\frac{0.006}{0.0048}\right)^{2 / 5} \times 0.15

 

= 0.164 m

 

It can be observed from Eq. (11.41) that

 

Q_{1}^{2}=0.00014-Q^{2}

 

or Q^{2}=0.00014-Q_{1}^{2}

 

Now Q will be maximum when & \dot{Q}_{1} will be minimum. For a physically possible situation, the minimum value of & \dot{Q}_{1} will be zero. Therefore, the maximum value of Q will be

 

Q_{\max }=\sqrt{0.00014}=0.0118 m ^{3} / s

 

which is 41.6% more than the initial value. The case \left(Q_{1}=0, Q=0.0118 m ^{3} / s \right) corresponds to a situation of an infinitely large branched pipe, i.e. d_{2} \rightarrow \infty \text {. }

1.5

Related Answered Questions