NVAMediumJEE 2023Bernoulli's Theorem

JEE Physics 2023 Question with Solution

Glycerine of density 1.25×103kg/m31.25 \times 10^3 \, \text{kg/m}^{-3} is flowing through the conical section of pipe. The area of cross-section of the pipe at its ends is 10cm210 \, \text{cm}^2 and 5cm25 \, \text{cm}^2 and pressure drop across its length is 3N m23 \, \text{N m}^{-2}. The rate of flow of glycerine through the pipe is x×105m3s1x \times 10^{-5} \, \text{m}^3 \, \text{s}^{-1}. The value of xx is _____ .

Answer

Correct answer:4

Step-by-step solution

Standard Method

Given: Density of glycerine ρ=1.25×103kg/m3\rho = 1.25 \times 10^3 \, \text{kg/m}^3, areas A1=10×104m2=1×103m2A_1 = 10 \times 10^{-4} \, \text{m}^2 = 1 \times 10^{-3} \, \text{m}^2 and A2=5×104m2A_2 = 5 \times 10^{-4} \, \text{m}^2, and pressure drop ΔP=P1P2=3N/m2\Delta P = P_1 - P_2 = 3 \, \text{N/m}^2.

Find: The value of xx in Q=x×105m3/sQ = x \times 10^{-5} \, \text{m}^3\text{/s}.

Using continuity equation,

A1v1=A2v2A_1 v_1 = A_2 v_2

So,

v2=A1A2v1=10×1045×104v1=2v1v_2 = \frac{A_1}{A_2} v_1 = \frac{10 \times 10^{-4}}{5 \times 10^{-4}} v_1 = 2v_1

Now apply Bernoulli's equation,

P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2}\rho v_1^2 = P_2 + \frac{1}{2}\rho v_2^2

Therefore,

P1P2=12ρ(v22v12)P_1 - P_2 = \frac{1}{2}\rho \left(v_2^2 - v_1^2\right)

Substituting ΔP=3\Delta P = 3 and v2=2v1v_2 = 2v_1,

3=12ρ((2v1)2v12)3 = \frac{1}{2}\rho \left((2v_1)^2 - v_1^2\right) 3=12ρ(4v12v12)=32ρv123 = \frac{1}{2}\rho \left(4v_1^2 - v_1^2\right) = \frac{3}{2}\rho v_1^2

Putting ρ=1.25×103\rho = 1.25 \times 10^3,

3=32(1.25×103)v123 = \frac{3}{2}(1.25 \times 10^3)v_1^2 v12=21.25×103=1625v_1^2 = \frac{2}{1.25 \times 10^3} = \frac{1}{625} v1=1625=125=0.04m/sv_1 = \sqrt{\frac{1}{625}} = \frac{1}{25} = 0.04 \, \text{m/s}

Now the rate of flow is,

Q=A1v1=(1×103)(0.04)=4×105m3/sQ = A_1 v_1 = (1 \times 10^{-3})(0.04) = 4 \times 10^{-5} \, \text{m}^3\text{/s}

Comparing with Q=x×105m3/sQ = x \times 10^{-5} \, \text{m}^3\text{/s}, we get x=4x = 4.

Therefore, the value of xx is 44.

Using continuity and pressure-energy relation

Given: The liquid flows through a conical pipe section with different cross-sectional areas, so the speed changes from one end to the other.

Find: The numerical value of xx.

Because the pipe narrows from 10cm210 \, \text{cm}^2 to 5cm25 \, \text{cm}^2, the fluid speed at the smaller area must increase. From continuity,

A1v1=A2v2A_1 v_1 = A_2 v_2

Hence,

v2=2v1v_2 = 2v_1

The pressure drop is used to supply the increase in kinetic energy per unit volume. So Bernoulli's equation gives,

ΔP=12ρ(v22v12)\Delta P = \frac{1}{2}\rho\left(v_2^2 - v_1^2\right)

Substitute v2=2v1v_2 = 2v_1,

3=12(1.25×103)(4v12v12)3 = \frac{1}{2}(1.25 \times 10^3)\left(4v_1^2 - v_1^2\right) 3=32(1.25×103)v123 = \frac{3}{2}(1.25 \times 10^3)v_1^2 v12=21250=1625v_1^2 = \frac{2}{1250} = \frac{1}{625} v1=0.04m/sv_1 = 0.04 \, \text{m/s}

Now use discharge formula,

Q=A1v1=(1×103)(0.04)Q = A_1 v_1 = (1 \times 10^{-3})(0.04) Q=4×105m3/sQ = 4 \times 10^{-5} \, \text{m}^3\text{/s}

So the required coefficient is x=4x = 4.

Therefore, the final answer is 44.

Common mistakes

  • Using the area ratio in the wrong direction. From continuity, A1v1=A2v2A_1v_1 = A_2v_2, so when area decreases, speed increases. Here v2=2v1v_2 = 2v_1, not v1=2v2v_1 = 2v_2.

  • Forgetting to convert cm2\text{cm}^2 into m2\text{m}^2. The area 10cm210 \, \text{cm}^2 must be written as 10×104m210 \times 10^{-4} \, \text{m}^2. Using unconverted areas gives an incorrect flow rate.

  • Applying Bernoulli's equation with the pressure difference sign reversed. The correct relation from the given drop is P1P2=12ρ(v22v12)P_1 - P_2 = \frac{1}{2}\rho(v_2^2 - v_1^2) because the speed is higher at the narrower end.

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