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Question: In the diagram shown below, the difference between the tubes of the manometer is 5 cm, the cross-sec...

In the diagram shown below, the difference between the tubes of the manometer is 5 cm, the cross-sections at A and B are 6 sq mm and 10 sq mm respectively. The rate at which water flows through the tube is;(g=10ms2g = 10m{\operatorname{s} ^{ - 2}})

(A) 7.5 cc/sec
(B) 8.0 cc/sec.
(C) 10.0 cc/sec.
(D) 12.5 cc/sec.

Explanation

Solution

This problem uses Bernoulli's theorem. Bernoulli's theorem is the pressure version of energy conservation. It is also similar to conservation of momentum.

Complete solution:
Bernoulli’s principle: In fluid dynamics, Bernoulli's principle states that an increase in the speed of a fluid occurs simultaneously with a decrease in static pressure or a decrease in the fluid's potential energy. Bernoulli's principle can be applied to various types of fluid flow, resulting in various forms of Bernoulli's equation; there are different forms of Bernoulli's equation for different types of flow.
The simplest one being;
P+12ρv2=CP + \dfrac{1}{2}\rho {v^2} = C.
Here, PP is the pressure at the surface of the liquid due to air, ρ\rho is the density of the fluid and v is the velocity of the fluid and C is constant.
Bernoulli's theorem also describes the relationship between a fluid's velocity and cross-sectional area. Mathematically it is written as A1v1=A2v2{A_1}{v_1} = {A_2}{v_2}.
Now in this case, the difference between the tubes is given viz. 5cm= 0.05 meters.
So first we find the velocity relation in the two tubes.
Hence by applying Bernoulli’s theorem we get;
A1v1=A2v2{A_1}{v_1} = {A_2}{v_2} here, A1=6mm2{A_1} = 6m{m^2} and A2=10mm2{A_2} = 10m{m^2} ;
Thus, 6v1=10v26{v_1} = 10{v_2}
Thus v1=53v2{v_1} = \dfrac{5}{3}{v_2} (equation:1)
Now apply Bernoulli’s theorem of conservation of pressure;
P1+12ρv12=P2+12ρv22{P_1} + \dfrac{1}{2}\rho {v_1}^2 = {P_2} + \dfrac{1}{2}\rho {v_2}^2
Solving the equation further we get;
P1P2=12ρ(v22v12){P_1} - {P_2} = \dfrac{1}{2}\rho \left( {{v_2}^2 - {v_1}^2} \right)
P1P2=12ρ(v22259v22){P_1} - {P_2} = \dfrac{1}{2}\rho \left( {{v_2}^2 - \dfrac{{25}}{9}{v_2}^2} \right) (from equation: 1)
Now we know that, P2P1=ρg(h2h1)=0.05ρg{P_2} - {P _1} = \rho g({h_2} - {h_1}) = 0.05\rho g (given)
0.05ρg=12ρ(169v22)0.05\rho g = \dfrac{1}{2}\rho \left( {\dfrac{{16}}{9}{v_2}^2} \right)
Solving the above equation we get,
v2=0.75ms2{v_2} = 0.75m{s^{ - 2}}
Therefore, rate of flow is mathematically Area X velocity;
Rate=A2v2=75×101cm3sec1{A_2}{v_2} = 75 \times {10^{ - 1}}c{m^3}{\sec ^{ - 1}}

Hence option A is correct.

Note: (1) The units must be converted very carefully
(2) Av is the rate of flow of fluid so Bernoulli’s principle states that rate of flow is constant.