Question:

A vessel completely filled with water has holes A and B at depths \( h \) and \( 3h \) from the top, respectively. Hole A is a square of side \( L \), and B is a circle of radius \( r \). The water flowing out per second from both the holes is the same. Then \( L \) is equal to:

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Use Torricelli’s theorem \( v = \sqrt{2gh} \) to calculate efflux velocity and combine it with the area of the hole to equate flow rates.
Updated On: Jan 25, 2025
  • \( L = 2^{3/4} \pi^{1/2} r \)
  • \( L = 3^{1/4} \pi^{1/2} r \)
  • \( L = 4^{1/2} \pi^{1/2} r \)
  • \( L = 3^{1/2} \pi^{1/2} r \)
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The Correct Option is B

Solution and Explanation

Step 1: Apply Torricelli’s theorem for efflux velocity.
The velocity of efflux for a hole at depth \( h \) is given by: \[ v = \sqrt{2gh}, \] where \( g \) is the acceleration due to gravity. For hole A at depth \( h \): \[ v_A = \sqrt{2gh}. \] For hole B at depth \( 3h \): \[ v_B = \sqrt{2g(3h)} = \sqrt{6gh}. \] Step 2: Relating the flow rates.
The rate of flow (\( Q \)) is given by: \[ Q = \text{Area} \times \text{Velocity}. \] For hole A (square of side \( L \)): \[ Q_A = L^2 \cdot v_A = L^2 \cdot \sqrt{2gh}. \] For hole B (circle of radius \( r \)): \[ Q_B = \pi r^2 \cdot v_B = \pi r^2 \cdot \sqrt{6gh}. \] Given that the flow rates are equal (\( Q_A = Q_B \)): \[ L^2 \cdot \sqrt{2gh} = \pi r^2 \cdot \sqrt{6gh}. \] Step 3: Simplify the equation.
Cancel \( \sqrt{gh} \) from both sides: \[ L^2 \cdot \sqrt{2} = \pi r^2 \cdot \sqrt{6}. \] Divide both sides by \( \sqrt{2} \): \[ L^2 = \pi r^2 \cdot \sqrt{\frac{6}{2}} = \pi r^2 \cdot \sqrt{3}. \] Take the square root of both sides: \[ L = \sqrt{\pi r^2 \cdot \sqrt{3}} = r \cdot \pi^{1/2} \cdot (3^{1/4}). \] Thus, \( L = 3^{1/4} \pi^{1/2} r \).
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