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A block of mass m is placed at rest on a...

A block of mass `m` is placed at rest on a horizontal rough surface with angle of friction `phi`. The block is pulled with a force `F` at an angle `theta` with the horizontal. The minimum value of `F` required to move the block is

A

`(F)/(M) ( cos phi - sin phi) - mu g`

B

`(mu F)/(M)cos phi`

C

`(F)/(M) ( cos phi + sin phi) - mu g`

D

`(F)/(M)sin phi`

Text Solution

AI Generated Solution

The correct Answer is:
To find the minimum value of the force \( F \) required to move a block of mass \( m \) placed at rest on a horizontal rough surface with an angle of friction \( \phi \), we can follow these steps: ### Step 1: Understand the Forces Acting on the Block - The block experiences several forces: - Weight \( W = mg \) acting downwards. - Normal force \( N \) acting upwards. - Applied force \( F \) at an angle \( \theta \) with the horizontal, which can be resolved into two components: - Horizontal component: \( F \cos \theta \) - Vertical component: \( F \sin \theta \) - Frictional force \( f \) acting opposite to the direction of motion. ### Step 2: Determine the Normal Force - The normal force \( N \) is affected by the vertical component of the applied force: \[ N = mg - F \sin \theta \] ### Step 3: Express the Frictional Force - The limiting friction \( f_L \) can be expressed in terms of the normal force: \[ f_L = \mu N \] - Given that \( \tan \phi = \mu \), we can write: \[ f_L = \tan \phi \cdot N \] ### Step 4: Substitute for Normal Force - Substitute the expression for \( N \) into the frictional force equation: \[ f_L = \tan \phi \cdot (mg - F \sin \theta) \] ### Step 5: Set Up the Equation for Motion - For the block to start moving, the horizontal component of the applied force must equal the limiting friction: \[ F \cos \theta = f_L \] - Substitute \( f_L \): \[ F \cos \theta = \tan \phi \cdot (mg - F \sin \theta) \] ### Step 6: Rearranging the Equation - Rearranging gives: \[ F \cos \theta = \frac{\sin \phi}{\cos \phi} (mg - F \sin \theta) \] - This simplifies to: \[ F \cos \theta = mg \tan \phi - F \sin \theta \tan \phi \] ### Step 7: Collect Terms Involving \( F \) - Collect all terms involving \( F \) on one side: \[ F \cos \theta + F \sin \theta \tan \phi = mg \tan \phi \] - Factor out \( F \): \[ F (\cos \theta + \sin \theta \tan \phi) = mg \tan \phi \] ### Step 8: Solve for \( F \) - Finally, solve for \( F \): \[ F = \frac{mg \tan \phi}{\cos \theta + \sin \theta \tan \phi} \] ### Final Answer Thus, the minimum value of \( F \) required to move the block is: \[ F = \frac{mg \sin \phi}{\cos(\theta - \phi)} \]

To find the minimum value of the force \( F \) required to move a block of mass \( m \) placed at rest on a horizontal rough surface with an angle of friction \( \phi \), we can follow these steps: ### Step 1: Understand the Forces Acting on the Block - The block experiences several forces: - Weight \( W = mg \) acting downwards. - Normal force \( N \) acting upwards. - Applied force \( F \) at an angle \( \theta \) with the horizontal, which can be resolved into two components: - Horizontal component: \( F \cos \theta \) ...
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