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A block is moving on an inclined plane m...

A block is moving on an inclined plane making an angle `45^@` with the horizontal and the coefficient of friction is `mu`. The force required to just push it up the inclined plane is 3 times the force required to just prevent it from sliding down. If we define `N=10mu`, then N is

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To solve the problem step by step, we will analyze the forces acting on the block on the inclined plane and derive the necessary equations. ### Step 1: Identify the forces acting on the block On an inclined plane at an angle θ (45 degrees in this case), the forces acting on the block include: - The gravitational force (mg) acting downward. - The normal force (N) acting perpendicular to the surface of the incline. - The frictional force (f) acting parallel to the incline, opposing the motion. ### Step 2: Resolve the gravitational force The gravitational force can be resolved into two components: - Parallel to the incline: \( mg \sin \theta \) - Perpendicular to the incline: \( mg \cos \theta \) Since θ = 45 degrees, we have: - \( \sin 45^\circ = \cos 45^\circ = \frac{1}{\sqrt{2}} \) ### Step 3: Write the equations for the forces 1. **Force required to just push the block up the incline (F1)**: \[ F_1 = mg \sin \theta + f \] where \( f = \mu N \) and \( N = mg \cos \theta \). Thus, substituting for f: \[ F_1 = mg \sin \theta + \mu (mg \cos \theta) \] 2. **Force required to just prevent the block from sliding down (F2)**: \[ F_2 = mg \sin \theta - f \] Again substituting for f: \[ F_2 = mg \sin \theta - \mu (mg \cos \theta) \] ### Step 4: Set up the relationship between F1 and F2 According to the problem, \( F_1 = 3 F_2 \). Substituting the expressions for F1 and F2: \[ mg \sin \theta + \mu (mg \cos \theta) = 3 \left( mg \sin \theta - \mu (mg \cos \theta) \right) \] ### Step 5: Simplify the equation Cancelling \( mg \) from both sides (assuming \( mg \neq 0 \)): \[ \sin \theta + \mu \cos \theta = 3 \left( \sin \theta - \mu \cos \theta \right) \] Expanding the right side: \[ \sin \theta + \mu \cos \theta = 3 \sin \theta - 3 \mu \cos \theta \] ### Step 6: Rearranging the equation Rearranging gives: \[ \mu \cos \theta + 3 \mu \cos \theta = 3 \sin \theta - \sin \theta \] This simplifies to: \[ 4 \mu \cos \theta = 2 \sin \theta \] ### Step 7: Substitute θ = 45 degrees Since \( \sin 45^\circ = \cos 45^\circ = \frac{1}{\sqrt{2}} \): \[ 4 \mu \left(\frac{1}{\sqrt{2}}\right) = 2 \left(\frac{1}{\sqrt{2}}\right) \] Cancelling \( \frac{1}{\sqrt{2}} \) from both sides: \[ 4 \mu = 2 \implies \mu = \frac{1}{2} \] ### Step 8: Calculate N Given \( N = 10 \mu \): \[ N = 10 \times \frac{1}{2} = 5 \] ### Final Answer Thus, the value of N is \( \boxed{5} \).

To solve the problem step by step, we will analyze the forces acting on the block on the inclined plane and derive the necessary equations. ### Step 1: Identify the forces acting on the block On an inclined plane at an angle θ (45 degrees in this case), the forces acting on the block include: - The gravitational force (mg) acting downward. - The normal force (N) acting perpendicular to the surface of the incline. - The frictional force (f) acting parallel to the incline, opposing the motion. ...
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