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A stone of mass m tied to the end of a string revolves in a vertical circle of radius R. The net forces at the lowest and highest points of the circle directed vertically downwards are: [Choose the correct alternative] Lowest point Highest point
`T_(1)` and `V_(1)` denote the tension and speed at the lowest point `T_(2)` and `V_(2)` denote the corresponding values at the highest points.

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To solve the problem of a stone of mass \( m \) tied to a string revolving in a vertical circle of radius \( R \), we need to analyze the forces acting on the stone at both the lowest and highest points of the circle. ### Step-by-Step Solution: 1. **Identify Forces at the Lowest Point:** At the lowest point of the circle, the forces acting on the stone are: - The gravitational force acting downwards: \( mg \) - The tension in the string acting upwards: \( T_1 \) The net force \( F_{\text{net, low}} \) at the lowest point can be expressed as: \[ F_{\text{net, low}} = T_1 - mg \] 2. **Identify Forces at the Highest Point:** At the highest point of the circle, the forces acting on the stone are: - The gravitational force acting downwards: \( mg \) - The tension in the string acting downwards: \( T_2 \) The net force \( F_{\text{net, high}} \) at the highest point can be expressed as: \[ F_{\text{net, high}} = mg + T_2 \] 3. **Understand the Role of Centripetal Force:** For the stone to maintain circular motion, the net force at both points must provide the necessary centripetal force required to keep the stone moving in a circle. The centripetal force \( F_c \) is given by: \[ F_c = \frac{mv^2}{R} \] where \( v \) is the speed of the stone at that point. 4. **Set Up Equations for Circular Motion:** - At the lowest point: \[ T_1 - mg = \frac{mv_1^2}{R} \quad \text{(1)} \] - At the highest point: \[ mg + T_2 = \frac{mv_2^2}{R} \quad \text{(2)} \] 5. **Summarize the Net Forces:** From the above equations, we can summarize the net forces: - At the lowest point: \( T_1 = mg + \frac{mv_1^2}{R} \) - At the highest point: \( T_2 = \frac{mv_2^2}{R} - mg \) ### Conclusion: The net forces acting on the stone at the lowest and highest points are: - **Lowest Point:** \( T_1 - mg \) (upward) - **Highest Point:** \( mg + T_2 \) (downward)

To solve the problem of a stone of mass \( m \) tied to a string revolving in a vertical circle of radius \( R \), we need to analyze the forces acting on the stone at both the lowest and highest points of the circle. ### Step-by-Step Solution: 1. **Identify Forces at the Lowest Point:** At the lowest point of the circle, the forces acting on the stone are: - The gravitational force acting downwards: \( mg \) - The tension in the string acting upwards: \( T_1 \) ...
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