Step 1: Understanding the Question:
We need to find the minimum force required to push a block up an inclined plane, overcoming both gravity and friction.
Step 2: Key Formula or Approach:
We will use a free-body diagram and apply Newton's First Law (for the condition of impending motion, acceleration is zero). The main forces are the applied force, gravity, normal force, and friction.
Step 3: Detailed Explanation:
Let's analyze the forces acting on the block along axes parallel and perpendicular to the inclined plane.
1.
Gravitational Force (Weight): \(mg\), acting vertically downwards.
- Component parallel to the incline: \(mg \sin \theta\) (acting down the incline).
- Component perpendicular to the incline: \(mg \cos \theta\) (acting into the incline).
2.
Normal Force (N): Acts perpendicular to the surface, outwards. From equilibrium in the perpendicular direction, \(N = mg \cos \theta\).
3.
Frictional Force (f): Opposes the motion (or impending motion) up the plane, so it acts down the plane. The maximum static friction (or kinetic friction) is \(f = \mu N = \mu mg \cos \theta\).
4.
Applied Force (F): The force required to move the block up the plane, acting parallel to the incline, upwards.
For the block to move up, the applied force F must overcome the sum of the forces pulling it down the incline.
\[ F = (\text{Gravitational component down the incline}) + (\text{Frictional force down the incline}) \]
\[ F = mg \sin \theta + f \]
Substitute \(f = \mu mg \cos \theta\):
\[ F = mg \sin \theta + \mu mg \cos \theta \]
Step 4: Final Answer:
The force required to move the block up the inclined plane is \(mg \sin \theta + \mu mg \cos \theta\).