Q 1 :

A block of mass m is on an inclined plane of angle θ. The coefficient of friction between the block and the plane is μ and tanθ>μ. The block is held stationary by applying a force P parallel to the plane. The direction of force pointing up the plane is taken to be positive. As P is varied from P1=mg(sinθ-μcosθ) to P2=mg(sinθ+μcosθ), the frictional force f versus P graph will look like                              [2010]

  • [IMAGE 46]

     

  • [IMAGE 47]

     

  • [IMAGE 48]

     

  • [IMAGE 49]

     

(1)

According to question, tanθ>μ, so block has a tendency to move down the incline. Force P is applied upwards along the incline to keep the block stationary.

Here, at equilibrium, P+f=mgsinθ    f=mgsinθ-P

Now as P increases, f decreases linearly with respect to P.

[IMAGE 50]

When P=mgsinθ, f=0.

When force P is increased further, the block has a tendency to move upwards along the incline and hence frictional force acts downwards along the incline.

Here, at equilibrium, P=f+mgsinθ

f=P-mgsinθ

Now as P increases, f increases linearly w.r.t P.

Hence graph (1) correctly depicts the situation.



Q 2 :

A block of base 10 cm×10 cm and height 15 cm is kept on an inclined plane. The coefficient of friction between them is 3. The inclination θ of this inclined plane from the horizontal plane is gradually increased from 0°. Then                        [2009]

  • at θ=30°, the block will start sliding down the plane

     

  • the block will remain at rest on the plane up to certain θ and then it will topple

     

  • at θ=60°, the block will start sliding down the plane and continue to do so at higher angles

     

  • at θ=60°, the block will start sliding down the plane and on further increasing θ, it will topple at certain θ

     

(2)

[IMAGE 51]

Maximum angle not to slide the block, angle of inclination = angle of repose,

i.e., tan-1μ=tan-13=60°

For the block to topple, the condition of the block has been shown in the figure.

In POMtanθ=PMOM=10/215/2=5 cm7.5 cm=23

So, θ<60°.

From this we can conclude that the block will topple at a lesser angle of inclination. Clearly the block will remain at rest on the plane up to a certain angle θ and then it will topple.



Q 3 :

What is the maximum value of the force F such that the block shown in the arrangement does not move?             [2003]

[IMAGE 52]

  • 20 N

     

  • 10 N

     

  • 12 N

     

  • 15 N

     

(1)

Since the block is not moving forward for the maximum force F applied, therefore

[IMAGE 53]

Fcos60°=f=μN

(Horizontal direction)

For vertical equilibrium of the block,

N=mg+Fsin60°

 Fcos60°=μN=μ(Fsin60°+mg)

F=μmgcos60°-μsin60°=123×3×1012-123×32=514=20 N



Q 4 :

An insect crawls up a hemispherical surface very slowly (see fig.). The coefficient of friction between the insect and the surface is 1/3. If the line joining the centre of the hemispherical surface to the insect makes an angle α with the vertical, the maximum possible value of α is given by                    [2001]

[IMAGE 54]

  • cotα=3

     

  • tanα=3

     

  • secα=3

     

  • cosecα=3

     

(1)

[IMAGE 55]

The two forces acting on the insect are mg and N.  

Two components of mg are

mgcosα balances N

mgsinα is balanced by the frictional force.

 N=mgcosα

       f=mgsinα

But, f=μN=μmgcosα

 μmgcosα=mgsinαcotα=1μcotα=3



Q 5 :

A block is moving on an inclined plane making an angle 45° with the horizontal and the coefficient of friction is μ. 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=10μ, then N is                     [2011]



(5)

[IMAGE 56]

For upward moving of block, pushing force F1=mgsinθ+f

 F1=mgsinθ+μmgcosθ=mg(sinθ+μcosθ)

The force required to just prevent it from sliding down or block just remains stationary,

F2=mgsinθ-μN=mg(sinθ-μcosθ)

Given, F1=3F2

 sinθ+μcosθ=3(sinθ-μcosθ)

 1+μ=3(1-μ)  [sinθ=cosθ]

 4μ=2    μ=0.5

 N=10μ=10×0.5=5 N



Q 6 :

A small block of mass of 0.1 kg lies on a fixed inclined plane PQ which makes an angle θ with the horizontal. A horizontal force of 1 N acts on the block through its centre of mass as shown in the figure.   

[IMAGE 57]                           

The block remains stationary if (take g=10 m/s2)           [2012]

  • θ=45°

     

  • θ>45° and a frictional force acts on the block towards P

     

  • θ>45° and a frictional force acts on the block towards Q

     

  • θ<45° and a frictional force acts on the block towards Q

     

Select one or more options

(1, 3)

[IMAGE 58]

The various forces acting on the block are as shown in the figure.

When θ=45°, sinθ=cosθ

The block will remain stationary and the frictional force is zero.

When θ>45°, sinθ>cosθ

Therefore a frictional force acts towards Q.

When θ<45°, cosθ>sinθ.

Therefore a frictional force acts towards P.



Q 7 :

A block of mass m1=1 kg and another mass m2=2 kg, are placed together (see figure) on an inclined plane with angle of inclination θ. Various values of θ are given in List-I. The coefficient of friction between the block m1 and plane is always zero. The coefficient of static and dynamic friction between the block m2 and the plane are equal to μ=0.3. In List-II expressions for the friction on block m2 are given. Match the correct expression of the friction in List-II with the angles given in List-I, and choose the correct option. The acceleration due to gravity is denoted by g.

Useful information: tan(5.5°)0.1; tan(11.5°)0.2; tan(16.5°)0.3                           [2014]

[IMAGE 59]

  List - I   List - II
P. θ=5° 1. m2gsinθ
Q. θ=10° 2. (m1+m2)gsinθ
R. θ=15° 3. μm2gcosθ
S. θ=20° 4. μ(m1+m2)gcosθ

Code:

  • P-1, Q-1, R-1, S-3

     

  • P-2, Q-2, R-2, S-3

     

  • P-2, Q-2, R-2, S-4

     

  • P-2, Q-2, R-3, S-3

     

(4)

Block will not slip or will be at rest if (m1+m2)gsinθμm2gcosθ

[IMAGE 60]

tanθμm2g(m1+m2)g

tanθμm2m1+m2

tanθ0.3×21+215

tanθ0.2  i.e.,  θ11.5°

i.e., If the angle θ<11.5°, the frictional force is less than μN2=μm2g=0.3×2×g=0.6g

and is equal to (m1+m2)gsinθ.

Blocks will not slip on the inclined plane and friction is static.

At θ>11.5°, the bodies start moving on the inclined plane and friction is kinetic and equal to μm2gcosθ.