Question 15

NUMERICALHARD

Liquid Efflux and Variable Dielectric Capacitance

A container of height 2 m2 \text{ m}, length 2 m2 \text{ m} and breadth 1 m1 \text{ m} is made of insulating vertical walls and two large area horizontal metal plates (M1M_1 and M2M_2) which extend far beyond the vertical walls in all directions. The container is partitioned into two equal chambers with a thin insulating vertical wall. The partition wall contains a small hole of cross-sectional area 10 cm2\sqrt{10} \text{ cm}^2 near its bottom edge. Initially the hole is closed and the left chamber of the container is completely filled with a liquid of dielectric constant ϵr=15\epsilon_r = 15 and the right chamber is empty (ϵr=1\epsilon_r = 1). At time t=0t = 0, the hole is opened and the liquid flows from the left chamber to the right chamber. In both the chambers, the space above the liquid has ϵr=1\epsilon_r = 1 and is maintained at atmospheric pressure. The schematic of the container at a time t>0t > 0 is shown in the figure. [Given: acceleration due to gravity is 10 ms−210 \text{ ms}^{-2}]

Passage

The height (in m) of the liquid in left chamber at t=500 st = 500 \text{ s} is:

Correct Answer: 1.25

Detailed Solution

Let h1h_1 and h2h_2 be the heights of the liquid in the left and right chambers respectively.

The base area of each chamber is A=1 m×1 m=1 m2A = 1 \text{ m} \times 1 \text{ m} = 1 \text{ m}^2.

Since the total volume of liquid is conserved, Ah1+Ah2=A×2A h_1 + A h_2 = A \times 2, so h1+h2=2h_1 + h_2 = 2.

The velocity of efflux through the hole of area a=10×10−4 m2a = \sqrt{10} \times 10^{-4} \text{ m}^2 is v=2g(h1−h2)v = \sqrt{2g(h_1 - h_2)}.

The rate of decrease of height in the left chamber is given by: Adh1dt=−a2g(h1−h2)A \frac{dh_1}{dt} = -a \sqrt{2g(h_1 - h_2)}

Substituting h2=2−h1h_2 = 2 - h_1:

dh1dt=−aA2g(2h1−2)=−2agAh1−1\frac{dh_1}{dt} = -\frac{a}{A} \sqrt{2g(2h_1 - 2)} = -\frac{2a\sqrt{g}}{A} \sqrt{h_1 - 1}

Separating variables and integrating from t=0t=0 (h1=2h_1=2) to t=500t=500 (h1=hh_1=h):

∫2h(h1−1)−1/2dh1=−∫05002agAdt\int_2^h (h_1 - 1)^{-1/2} dh_1 = -\int_0^{500} \frac{2a\sqrt{g}}{A} dt

[2h1−1]2h=−2agA(500)[2\sqrt{h_1 - 1}]_2^h = -\frac{2a\sqrt{g}}{A} (500)

h−1−2−1=−agA(500)\sqrt{h - 1} - \sqrt{2 - 1} = -\frac{a\sqrt{g}}{A} (500)

Using ag=10×10−4×10=10−3a\sqrt{g} = \sqrt{10} \times 10^{-4} \times \sqrt{10} = 10^{-3} and A=1A = 1:

h−1−1=−10−3×500=−0.5\sqrt{h - 1} - 1 = -10^{-3} \times 500 = -0.5

h−1=0.5  ⟹  h−1=0.25  ⟹  h=1.25 m\sqrt{h - 1} = 0.5 \implies h - 1 = 0.25 \implies h = 1.25 \text{ m}

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