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A stone is rotated in a vertical circle....

A stone is rotated in a vertical circle. Speed at bottommost point is `sqrt(8gR)`, where R is the radius of circle. The ratio of tension at the top and the bottom is

A

`1:2`

B

`1:3`

C

`2:3`

D

`1:4`

Text Solution

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The correct Answer is:
To solve the problem, we need to find the ratio of the tension in the string at the topmost point (T_B) to the tension at the bottommost point (T_A) of the vertical circle in which the stone is rotating. ### Step-by-Step Solution: 1. **Identify the Given Information:** - Speed at the bottommost point (A): \( v_A = \sqrt{8gR} \) - Radius of the circle: \( R \) 2. **Calculate Tension at the Bottommost Point (T_A):** - At the bottommost point, the forces acting on the stone are: - Tension \( T_A \) acting upwards - Weight \( mg \) acting downwards - Centripetal force requirement: \( \frac{mv_A^2}{R} \) acting downwards - The equation of motion at point A can be written as: \[ T_A - mg = \frac{mv_A^2}{R} \] - Substitute \( v_A \): \[ T_A - mg = \frac{m(\sqrt{8gR})^2}{R} \] \[ T_A - mg = \frac{m \cdot 8gR}{R} \] \[ T_A - mg = 8mg \] - Therefore, we can solve for \( T_A \): \[ T_A = mg + 8mg = 9mg \] 3. **Calculate Speed at the Topmost Point (B):** - To find the speed at the topmost point (B), we can use the conservation of mechanical energy between points A and B. - At point A (bottom): - Kinetic Energy (KE_A) = \( \frac{1}{2} m v_A^2 = \frac{1}{2} m (8gR) = 4mgR \) - Potential Energy (PE_A) = 0 (taking this as the reference level) - At point B (top): - Kinetic Energy (KE_B) = \( \frac{1}{2} m u^2 \) - Potential Energy (PE_B) = \( mg(2R) = 2mgR \) - By conservation of energy: \[ KE_A + PE_A = KE_B + PE_B \] \[ 4mgR + 0 = \frac{1}{2} m u^2 + 2mgR \] - Rearranging gives: \[ 4mgR = \frac{1}{2} m u^2 + 2mgR \] \[ 2mgR = \frac{1}{2} m u^2 \] \[ 4gR = u^2 \] 4. **Calculate Tension at the Topmost Point (T_B):** - At the topmost point (B), the forces acting on the stone are: - Tension \( T_B \) acting downwards - Weight \( mg \) acting downwards - Centripetal force requirement: \( \frac{mu^2}{R} \) acting downwards - The equation of motion at point B can be written as: \[ T_B + mg = \frac{mu^2}{R} \] - Substitute \( u^2 \): \[ T_B + mg = \frac{m(4gR)}{R} \] \[ T_B + mg = 4mg \] - Therefore, we can solve for \( T_B \): \[ T_B = 4mg - mg = 3mg \] 5. **Calculate the Ratio of Tensions:** - Now, we can find the ratio of tensions: \[ \frac{T_B}{T_A} = \frac{3mg}{9mg} = \frac{1}{3} \] ### Final Answer: The ratio of tension at the topmost point to the tension at the bottommost point is \( \frac{1}{3} \).

To solve the problem, we need to find the ratio of the tension in the string at the topmost point (T_B) to the tension at the bottommost point (T_A) of the vertical circle in which the stone is rotating. ### Step-by-Step Solution: 1. **Identify the Given Information:** - Speed at the bottommost point (A): \( v_A = \sqrt{8gR} \) - Radius of the circle: \( R \) ...
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