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A tank of height H is fully filled with ...

A tank of height H is fully filled with water. If the water rushing from a hole made in the tank below the free surface , strikes the floor at a maximum horizontal distance , then the depth of the hole from the free surface must be

A

`3/4 H`

B

`2/3H`

C

`1/4H`

D

`1/2H`

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The correct Answer is:
To solve the problem of finding the depth of the hole from the free surface of a tank filled with water, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Problem**: We have a tank of height \( H \) filled with water. A hole is made below the free surface, and we need to find the depth \( h \) of this hole from the free surface such that the water strikes the floor at the maximum horizontal distance. 2. **Use Bernoulli's Equation**: We can apply Bernoulli's equation between two points: one just inside the hole (point 1) and one just outside the hole (point 2). The equation is given by: \[ P_1 + \frac{1}{2} \rho v_1^2 + \rho g h_1 = P_2 + \frac{1}{2} \rho v_2^2 + \rho g h_2 \] Here, \( P_1 \) and \( P_2 \) are the pressures at points 1 and 2, \( v_1 \) and \( v_2 \) are the velocities at those points, \( \rho \) is the density of water, and \( g \) is the acceleration due to gravity. 3. **Set Up the Equation**: For point 1 (just inside the hole): - Pressure \( P_1 = P_0 \) (atmospheric pressure) - Height \( h_1 = H - h \) (height from the bottom of the tank) - Velocity \( v_1 \) is negligible since the tank is large compared to the hole. For point 2 (just outside the hole): - Pressure \( P_2 = P_0 \) - Height \( h_2 = 0 \) (at the level of the hole) - Velocity \( v_2 \) is what we need to find. Thus, the equation simplifies to: \[ P_0 + \rho g (H - h) = P_0 + \frac{1}{2} \rho v_2^2 \] Canceling \( P_0 \) and rearranging gives: \[ \rho g (H - h) = \frac{1}{2} \rho v_2^2 \] Dividing by \( \rho \) gives: \[ g (H - h) = \frac{1}{2} v_2^2 \] Therefore, we can express \( v_2 \) as: \[ v_2 = \sqrt{2g(H - h)} \] 4. **Calculate the Time of Flight**: The time \( t \) it takes for the water to fall from height \( h \) to the ground can be calculated using the equation of motion: \[ h = \frac{1}{2} g t^2 \implies t = \sqrt{\frac{2h}{g}} \] 5. **Calculate the Horizontal Range**: The horizontal range \( R \) is given by the product of the horizontal velocity and the time of flight: \[ R = v_2 \cdot t = \sqrt{2g(H - h)} \cdot \sqrt{\frac{2h}{g}} = 2\sqrt{h(H - h)} \] 6. **Maximize the Range**: To find the maximum range, we can differentiate \( R \) with respect to \( h \) and set it to zero: \[ R = 2\sqrt{h(H - h)} \] Let \( R^2 = 4h(H - h) \). Differentiate: \[ \frac{d(R^2)}{dh} = 4(H - 2h) = 0 \implies H - 2h = 0 \implies h = \frac{H}{2} \] 7. **Conclusion**: The depth of the hole from the free surface for maximum horizontal distance is: \[ h = \frac{H}{2} \] ### Final Answer: The depth of the hole from the free surface must be \( \frac{H}{2} \). ---
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