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A 1 kg solid sphere rolls without slippi...

A `1 kg` solid sphere rolls without slipping on a rough horizontal surface under the influence of a `7 N` force. The force acts tangentially at the highest point of the sphere. Which of the following statements are correct? (`7 N` force acts towards right).

A

The frictional force on the sphere acts towards right.

B

The value of the frictional force is `3 N`

C

The acceleration of the centre of the sphere is `9.8 m//s^(2)`

D

The acceleration of the centre of the sphere is `10 m//s^(2)`

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To solve the problem, we need to analyze the forces acting on the solid sphere and apply Newton's laws of motion. Let's break it down step by step. ### Step 1: Identify the Forces Acting on the Sphere The forces acting on the sphere are: - A tangential force \( F = 7 \, \text{N} \) acting to the right at the highest point of the sphere. - A frictional force \( f \) acting to the left at the point of contact with the ground. ### Step 2: Write the Equations of Motion Since the sphere rolls without slipping, we can apply Newton's second law for translation and rotation. 1. **Translational Motion:** \[ F - f = m a \] where \( m = 1 \, \text{kg} \) and \( a \) is the linear acceleration of the center of mass. 2. **Rotational Motion:** The torque \( \tau \) about the center of mass due to the forces is given by: \[ \tau = F \cdot r - f \cdot r = I \alpha \] where \( I \) is the moment of inertia of the sphere and \( \alpha \) is the angular acceleration. For a solid sphere, the moment of inertia is: \[ I = \frac{2}{5} m r^2 \] Since \( \alpha = \frac{a}{r} \) (due to rolling without slipping), we can substitute \( \alpha \) into the torque equation. ### Step 3: Substitute Values into the Equations Substituting the values into the equations: 1. From the translational motion: \[ 7 - f = 1 \cdot a \quad \text{(1)} \] 2. From the rotational motion: \[ 7 \cdot r - f \cdot r = \frac{2}{5} m r^2 \cdot \frac{a}{r} \] Simplifying gives: \[ 7 - f = \frac{2}{5} a \quad \text{(2)} \] ### Step 4: Solve the Equations Now we have two equations: 1. \( 7 - f = a \) (from equation 1) 2. \( 7 - f = \frac{2}{5} a \) (from equation 2) From equation (1), we can express \( a \) in terms of \( f \): \[ a = 7 - f \] Substituting this into equation (2): \[ 7 - f = \frac{2}{5}(7 - f) \] ### Step 5: Solve for \( f \) Multiplying through by 5 to eliminate the fraction: \[ 5(7 - f) = 2(7 - f) \] Expanding gives: \[ 35 - 5f = 14 - 2f \] Rearranging terms: \[ 35 - 14 = 5f - 2f \] \[ 21 = 3f \] Thus, we find: \[ f = 7 \, \text{N} \] ### Step 6: Calculate the Acceleration Substituting \( f \) back into equation (1): \[ 7 - 7 = a \implies a = 0 \, \text{m/s}^2 \] ### Conclusion The sphere does not accelerate, and the friction force acts to the left. The correct statements based on our calculations are: - The acceleration of the sphere is \( 0 \, \text{m/s}^2 \). - The friction force acts to the left.

To solve the problem, we need to analyze the forces acting on the solid sphere and apply Newton's laws of motion. Let's break it down step by step. ### Step 1: Identify the Forces Acting on the Sphere The forces acting on the sphere are: - A tangential force \( F = 7 \, \text{N} \) acting to the right at the highest point of the sphere. - A frictional force \( f \) acting to the left at the point of contact with the ground. ### Step 2: Write the Equations of Motion ...
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