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An open cubical tank was initially fully...

An open cubical tank was initially fully filled with water. When the tank was accelerated on a horizontal plane along one of its side it was found that one thrid of volume of water was spilled out. The acceleration was

A

g/3

B

2g/3

C

g/2

D

g/4

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The correct Answer is:
To solve the problem of finding the acceleration of the open cubical tank that spills one-third of its water when accelerated, we can follow these steps: ### Step 1: Understand the Problem We have an open cubical tank filled with water. When the tank is accelerated horizontally, it spills out one-third of its volume of water. We need to find the acceleration of the tank. ### Step 2: Define the Variables Let: - \( H \) = side length of the cube - \( V \) = total volume of water in the tank = \( H^3 \) - The volume of water spilled = \( \frac{1}{3} V = \frac{1}{3} H^3 \) ### Step 3: Determine the Height of the Water Surface When the tank is accelerated, the water surface will tilt. Let \( h \) be the height to which the water surface dips due to acceleration. The volume of the spilled water can be expressed in terms of the height \( h \) and the area of the triangle formed by the tilted water surface. ### Step 4: Calculate the Volume of Water Spilled The volume of the spilled water can be calculated as: \[ \text{Volume of spilled water} = \text{Area of triangle} \times H \] The area of the triangle formed by the tilted water surface is: \[ \text{Area} = \frac{1}{2} \times h \times H \] Thus, the volume of spilled water becomes: \[ \text{Volume} = \frac{1}{2} \times h \times H^2 \] ### Step 5: Set Up the Equation From the previous steps, we can set up the equation: \[ \frac{1}{3} H^3 = \frac{1}{2} h H^2 \] Dividing both sides by \( H^2 \): \[ \frac{1}{3} H = \frac{1}{2} h \] Thus, we can express \( h \) in terms of \( H \): \[ h = \frac{2}{3} H \] ### Step 6: Relate the Angle and Acceleration The angle \( \theta \) that the water surface makes with the horizontal can be related to the acceleration \( a \) and gravitational acceleration \( g \) using: \[ \tan \theta = \frac{h}{H} \] Substituting \( h \): \[ \tan \theta = \frac{\frac{2}{3} H}{H} = \frac{2}{3} \] ### Step 7: Find the Acceleration Using the relationship \( \tan \theta = \frac{a}{g} \): \[ \frac{a}{g} = \frac{2}{3} \] Thus, the acceleration \( a \) can be expressed as: \[ a = \frac{2}{3} g \] ### Step 8: Conclusion The acceleration of the tank is: \[ \boxed{\frac{2g}{3}} \]
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