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There are two holes P and Q at depths h ...

There are two holes P and Q at depths h and 4h from the top of a large vessel, completely filled with water. P is a square hole of side L and Q is a circular hole of radius r. If the same quantity of water flows out per second from both the holes, then the relation between L and r is

A

`L=r/2`

B

`L=sqrt(2pir)`

C

`L-2pir`

D

`L=(sqrt(2pi))/(r )`

Text Solution

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The correct Answer is:
To solve the problem, we need to find the relationship between the side length \( L \) of the square hole at depth \( h \) and the radius \( r \) of the circular hole at depth \( 4h \) when the same quantity of water flows out per second from both holes. ### Step-by-Step Solution: 1. **Identify the velocities at both holes**: - For hole P at depth \( h \), the velocity of water flowing out can be derived from Torricelli’s theorem: \[ v_P = \sqrt{2gh} \] - For hole Q at depth \( 4h \): \[ v_Q = \sqrt{2g(4h)} = \sqrt{8gh} = 2\sqrt{2gh} \] 2. **Calculate the areas of the holes**: - The area of the square hole P: \[ A_P = L^2 \] - The area of the circular hole Q: \[ A_Q = \pi r^2 \] 3. **Set up the volume flow rate equation**: - The volume flow rate (Q) for both holes must be equal: \[ Q_P = A_P \cdot v_P = L^2 \cdot \sqrt{2gh} \] \[ Q_Q = A_Q \cdot v_Q = \pi r^2 \cdot (2\sqrt{2gh}) \] 4. **Equate the flow rates**: \[ L^2 \cdot \sqrt{2gh} = \pi r^2 \cdot (2\sqrt{2gh}) \] 5. **Simplify the equation**: - Cancel \( \sqrt{2gh} \) from both sides: \[ L^2 = 2\pi r^2 \] 6. **Solve for \( L \)**: \[ L = \sqrt{2\pi} r \] ### Final Relation: The relationship between \( L \) and \( r \) is: \[ L = \sqrt{2\pi} r \]

To solve the problem, we need to find the relationship between the side length \( L \) of the square hole at depth \( h \) and the radius \( r \) of the circular hole at depth \( 4h \) when the same quantity of water flows out per second from both holes. ### Step-by-Step Solution: 1. **Identify the velocities at both holes**: - For hole P at depth \( h \), the velocity of water flowing out can be derived from Torricelli’s theorem: \[ v_P = \sqrt{2gh} ...
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