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A body is placed on a rough inclined pla...

A body is placed on a rough inclined plane of inclination `theta`. As the angle `theta` is increased from `0^(@)` to `90^(@)` the contact force between the block and the plane

A

remains constant

B

first remains constant then decreases

C

first decreases then increases

D

first increases then decreases

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To analyze the contact force between a block and a rough inclined plane as the angle of inclination \(\theta\) increases from \(0^\circ\) to \(90^\circ\), we can follow these steps: ### Step 1: Understand the Forces Acting on the Block When the block is placed on the inclined plane, the forces acting on it are: - The gravitational force (\(mg\)) acting downwards. - The normal force (\(N\)) acting perpendicular to the surface of the incline. - The frictional force (\(f\)) acting parallel to the surface of the incline. ### Step 2: Resolve the Gravitational Force The gravitational force can be resolved into two components: - Perpendicular to the incline: \(mg \cos \theta\) - Parallel to the incline: \(mg \sin \theta\) ### Step 3: Analyze the Normal Force The normal force \(N\) is equal to the component of the gravitational force acting perpendicular to the incline: \[ N = mg \cos \theta \] ### Step 4: Analyze the Frictional Force The frictional force \(f\) can be expressed as: \[ f = \mu N = \mu (mg \cos \theta) \] where \(\mu\) is the coefficient of friction between the block and the inclined plane. ### Step 5: Consider the Motion of the Block As \(\theta\) increases: - At \(\theta = 0^\circ\): The block does not experience any inclination, and the contact force is simply the normal force \(N = mg\). - As \(\theta\) increases, the normal force decreases because \(N = mg \cos \theta\). - At \(\theta = 90^\circ\): The incline becomes vertical, and the normal force approaches zero, meaning the block would no longer be in contact with the incline. ### Step 6: Conclusion on Contact Force As \(\theta\) increases from \(0^\circ\) to \(90^\circ\): - The normal force \(N\) decreases from \(mg\) to \(0\). - The contact force between the block and the inclined plane also decreases from \(mg\) to \(0\). ### Summary The contact force between the block and the inclined plane decreases as the angle of inclination \(\theta\) increases from \(0^\circ\) to \(90^\circ\).
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