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The string of pendulum of length l is di...

The string of pendulum of length l is displaced through `90^(@)` from the vertical and released. Then the minimum strength of the string in order to withstand the tension, as the pendulum passes through the mean position is

A

mg

B

2mg

C

3mg

D

4mg

Text Solution

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The correct Answer is:
To find the minimum strength of the string required to withstand the tension as the pendulum passes through the mean position, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Problem**: - The pendulum is displaced through \(90^\circ\) from the vertical and then released. We need to find the tension in the string when the pendulum reaches the mean position (the lowest point). 2. **Applying Work-Energy Theorem**: - According to the work-energy theorem, the work done by gravity is equal to the change in kinetic energy. - When the pendulum is at the highest point (point A), its velocity is zero, and when it reaches the mean position (point B), it has maximum kinetic energy. 3. **Calculating Work Done by Gravity**: - The work done by gravity when the pendulum moves from point A to point B can be calculated as: \[ \text{Work done by gravity} = mgh \] - Here, \(h\) is the vertical height fallen, which is equal to the length of the pendulum \(L\) (since it falls a distance \(L\) when moving from the highest point to the lowest point). - Therefore, the work done by gravity is: \[ W = mgL \] 4. **Change in Kinetic Energy**: - The change in kinetic energy from point A to point B is given by: \[ \Delta KE = \frac{1}{2} mv^2 - 0 = \frac{1}{2} mv^2 \] 5. **Setting Work Done Equal to Change in Kinetic Energy**: - From the work-energy principle: \[ mgL = \frac{1}{2} mv^2 \] - Canceling \(m\) from both sides (assuming \(m \neq 0\)): \[ gL = \frac{1}{2} v^2 \] - Rearranging gives: \[ v^2 = 2gL \] 6. **Finding Tension at the Mean Position**: - At the mean position (point B), the forces acting on the pendulum bob are: - Tension \(T_B\) acting upwards. - Weight \(mg\) acting downwards. - The net force towards the center (centripetal force) is given by: \[ T_B - mg = \frac{mv^2}{L} \] - Substituting \(v^2\) from the previous calculation: \[ T_B - mg = \frac{m(2gL)}{L} \] - Simplifying gives: \[ T_B - mg = 2mg \] - Therefore: \[ T_B = 2mg + mg = 3mg \] 7. **Conclusion**: - The minimum strength of the string required to withstand the tension as the pendulum passes through the mean position is: \[ T_B = 3mg \]
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