Home
Class 12
PHYSICS
A cubical block rests on a plane of mu= ...

A cubical block rests on a plane of `mu= sqrt(3)` . The angle through which the plane be inclined to the horizontal so that the block just slides down will be -

A

`30^(@)`

B

`45^(@)`

C

`60^(@)`

D

`75^(@)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem of determining the angle at which a cubical block will just start to slide down an inclined plane with a coefficient of friction (μ) equal to √3, we can follow these steps: ### Step 1: Understand the Forces Acting on the Block When the block is placed on the inclined plane, two main forces act on it: - The gravitational force (weight) acting downwards, which can be represented as \( mg \). - The normal force acting perpendicular to the surface of the inclined plane. ### Step 2: Resolve the Gravitational Force The gravitational force can be resolved into two components: - A component parallel to the incline: \( mg \sin \theta \) - A component perpendicular to the incline: \( mg \cos \theta \) ### Step 3: Write the Expression for Normal Force The normal force (N) acting on the block is equal to the perpendicular component of the gravitational force: \[ N = mg \cos \theta \] ### Step 4: Determine the Maximum Static Friction The maximum static friction force (F_friction) that can act on the block before it starts sliding is given by: \[ F_{friction} = \mu N = \mu (mg \cos \theta) \] ### Step 5: Set Up the Condition for Sliding The block will just start to slide when the component of the gravitational force parallel to the incline equals the maximum static friction force: \[ mg \sin \theta = \mu (mg \cos \theta) \] ### Step 6: Simplify the Equation We can cancel \( mg \) from both sides (assuming \( mg \neq 0 \)): \[ \sin \theta = \mu \cos \theta \] ### Step 7: Divide Both Sides by \( \cos \theta \) This gives us: \[ \tan \theta = \mu \] ### Step 8: Substitute the Value of μ Given that \( \mu = \sqrt{3} \): \[ \tan \theta = \sqrt{3} \] ### Step 9: Find the Angle θ To find θ, we take the arctangent (inverse tangent) of both sides: \[ \theta = \tan^{-1}(\sqrt{3}) \] ### Step 10: Calculate θ From trigonometric values, we know: \[ \tan 60^\circ = \sqrt{3} \] Thus, \[ \theta = 60^\circ \] ### Final Answer The angle through which the plane can be inclined to the horizontal so that the block just slides down is \( 60^\circ \). ---
Promotional Banner

Topper's Solved these Questions

  • NEWTON'S LAWS OF MOTION & FRICTION

    MOTION|Exercise Exercise - 2 SECTION-A:- String Constrained, Wedge Constrained, Newtons Law theory Question, Equillibrium Questions (Normal and Tension), Problems with Acceleration (F=ma), Wedge problems|23 Videos
  • NEWTON'S LAWS OF MOTION & FRICTION

    MOTION|Exercise Exercise - 2 SECTION-B :- Pulley Block System|7 Videos
  • NEWTON'S LAWS OF MOTION & FRICTION

    MOTION|Exercise Exercise - 1 SECTION-E:- Static friction, Kinetic friction|13 Videos
  • MODERN PHYSICS -1

    MOTION|Exercise EXERCISE-4 ( LEVEL- II)|39 Videos
  • NLM & FRICTION

    MOTION|Exercise EXERCISE-4 ( LEVEL-II)|15 Videos

Similar Questions

Explore conceptually related problems

A cubical block rests on an inclined plance of mu = (1)/sqrt(3) . Determine the angle at which the block just slides down the incline .

The angle which the rough inclined plane makes with the horizontal when the body placed on it just starts sliding down is called .

The coefficient of static friction between a block of mass m and an incline is mu_s=03 , a. What can be the maximum angle theta of the incline with the horizontal so that the block does not slip on the plane? b. If the incline makes an angle theta/2 with the horizontal, find the frictional force on the block.

A block of mass m rests on a rough inclined plane. The coefficient of friction between the surface and the block is µ. At what angle of inclination theta of the plane to the horizontal will the block just start to slide down the plane?

A block mass 'm' is placed on a frictionless inclined plane of inclination theta with horizontal. The inclined plane is accelerated horizontally so that the block does not slide down. In this situation vertical force exerted by the inclined plane on the block is:

A block of mass m is placed on a rough inclined plane. When the inclination of the plane is theta , the block just beging to slide down the plane under its own weight. The minimum force applied parallel to the plane, to move the block up the plane, is.