A block of mass m is at rest on a rough inclined plane of angle of inclination θ. If coefficient of friction between the block and the inclined plane is μ, then the minimum value of force along the plane required to move the block on the plane is
mg[μcosθ−sinθ]
mg[sinθ+μcosθ]
mg[μcosθ+sinθ]
mg[sinθ−μcosθ]
To solve the problem of determining the minimum force required to move a block of mass m resting on a rough inclined plane with an angle of inclination θ and a coefficient of friction μ, we can follow these steps:
Step 1: Identify the forces acting on the block
1. Weight of the block: The weight W of the block acts vertically downwards and is given by W=mg.
2. Components of weight:
- The component of weight acting parallel to the incline: W∥=mgsinθ.
- The component of weight acting perpendicular to the incline: W_{\perpendicular} = mg \cos \theta .
3. Normal force: The normal force N acts perpendicular to the inclined surface and balances the perpendicular component of the weight.
Step 2: Determine the frictional force
The frictional force f that opposes the motion is given by:
f=μN
Since the normal force N is equal to the perpendicular component of the weight, we have:
N=mgcosθ
Thus, the maximum frictional force can be expressed as:
f=μmgcosθ
Step 3: Set up the equilibrium condition
To move the block, the applied force F must overcome both the component of the weight acting down the incline and the frictional force. Therefore, we can write the equilibrium condition as:
F+mgsinθ=f
Substituting the expression for frictional force, we get:
F+mgsinθ=μmgcosθ
Step 4: Solve for the applied force F
Rearranging the equation to isolate F:
F=μmgcosθ−mgsinθ
Factoring out mg:
F=mg(μcosθ−sinθ)
Final Answer
The minimum value of the force F required to move the block along the inclined plane is:
F=mg(μcosθ−sinθ)
1. Weight of the block: The weight W of the block acts vertically downwards and is given by W=mg.
2. Components of weight:
- The component of weight acting parallel to the incline: W∥=mgsinθ.
- The component of weight acting perpendicular to the incline: W_{\perpendicular} = mg \cos \theta .
3. Normal force: The normal force N acts perpendicular to the inclined surface and balances the perpendicular component of the weight.
The frictional force f that opposes the motion is given by:
f=μN
Since the normal force N is equal to the perpendicular component of the weight, we have:
N=mgcosθ
Thus, the maximum frictional force can be expressed as:
f=μmgcosθ
To move the block, the applied force F must overcome both the component of the weight acting down the incline and the frictional force. Therefore, we can write the equilibrium condition as:
F+mgsinθ=f
Substituting the expression for frictional force, we get:
F+mgsinθ=μmgcosθ
Rearranging the equation to isolate F:
F=μmgcosθ−mgsinθ
Factoring out mg:
F=mg(μcosθ−sinθ)
The minimum value of the force F required to move the block along the inclined plane is:
F=mg(μcosθ−sinθ)
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