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A solid uniform disc of mass m rolls wit...

A solid uniform disc of mass `m` rolls without slipping down a fixed inclined plank with an acceleration a. The frictional force on the disc due to surface of the plane is

A

2 ma

B

`(3)/(2)` ma

C

ma

D

`(1)/(2)` ma

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The correct Answer is:
To solve the problem of finding the frictional force on a solid uniform disc rolling down an inclined plane, we can follow these steps: ### Step-by-Step Solution: 1. **Identify the Forces Acting on the Disc**: - The weight of the disc, \( mg \), acts vertically downward. - This weight can be resolved into two components: - The component parallel to the incline: \( mg \sin \theta \) - The component perpendicular to the incline: \( mg \cos \theta \) 2. **Set Up the Equations of Motion**: - The vertical component \( mg \cos \theta \) is balanced by the normal force \( N \). - The net force acting down the incline is given by: \[ F_{\text{net}} = mg \sin \theta - F \] - Here, \( F \) is the frictional force acting up the incline. 3. **Relate Linear Acceleration to Angular Acceleration**: - Since the disc rolls without slipping, the linear acceleration \( a \) is related to the angular acceleration \( \alpha \) by: \[ a = R \alpha \] - Thus, we can express \( \alpha \) as: \[ \alpha = \frac{a}{R} \] 4. **Apply the Torque Equation**: - The torque \( \tau \) acting on the disc due to the frictional force is given by: \[ \tau = F \cdot R \] - This torque is also equal to the moment of inertia \( I \) times the angular acceleration \( \alpha \): \[ \tau = I \alpha \] - For a solid disc, the moment of inertia \( I \) about its center is: \[ I = \frac{1}{2} m R^2 \] 5. **Equate Torque Expressions**: - Setting the two expressions for torque equal gives: \[ F \cdot R = \frac{1}{2} m R^2 \cdot \frac{a}{R} \] - Simplifying this, we get: \[ F \cdot R = \frac{1}{2} m a R \] - Dividing both sides by \( R \) (assuming \( R \neq 0 \)): \[ F = \frac{1}{2} m a \] 6. **Conclusion**: - The frictional force \( F \) acting on the disc due to the surface of the inclined plane is: \[ F = \frac{1}{2} m a \] ### Final Answer: The frictional force on the disc due to the surface of the plane is \( \frac{1}{2} m a \).
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