Problems

1. If cyclist moving with a speed of 4.9 m/s on a level road can take a sharp circular turn of radius 4 m, then what is the coefficient of friction between the cycle tyre and the road?

Solution:

To take a turn centripetal acceleration will be provided by frictional force

           =  μN

              =  rμg             ------ (1)

              μ  =                  ------ (2) 

Here radius of circular track,

      r  =  4 m

Velocity,

      =  4.9 m/s

Gravitational acceleration,

      g  =  9.8 m s−2

Substituting above values in eqn (2) we get

      μ  =  0.6125 

      μ  =  0.61

 

2. A motor cycle is going on an over bridge of radius R. The driver maintains a constant speed. As the motor cycle is ascending on the over bridge, what will be the normal force on it?

Solution:

d2.jpg

From figure reaction of normal force on the motor cyclist

   =   

                                R  = 

As motorcycle ascends on the over bridge, angle of inclination of motorcycle with vertical θ decreases and becomes zero at the highest point.

So cos θ goes on increasing and becomes 1 at highest point.

Value of R is continuously increasing while ascending.

 

3. One end of a string of length l is connected to a particle of mass m and the other to a small peg on a smooth horizontal table. If the particle moves in a circle with speed , then what will be the net force on the particle (directed towards the centre)?

Solution:

When a particle connected to a string revolves in a circular path around a centre, the centripetal force is provided by the tension produced in the string.

Hence, in the given case, the net force on the particle is the tension T, i.e.,

 =  T  = 

Where F is the net force acting on the particle.

 

4. A stone of mass 0.25 kg tied to the end of a string is whirled round in a circle of radius 1.5 m with a speed of 40 rev/min in a horizontal plane. What is the maximum speed with which the stone can be whirled around if the string can withstand a maximum tension of 200 N?

Solution:

Mass of the stone,    m  =  0.25 kg

Radius of the circle,   r  =  1.5 m

Maximum tension in the string, 

            =  200 N

            =  

∴                                 = 

         = 

         =   

         =  34.64 m/s

Therefore, the maximum speed of the stone is 34.64 m/s.

 

5. A weight W hangs from a rope that is tied to two other ropes that are fastened to the ceiling as shown in figure. 

lmq24.PNG

The upper ropes make angles θ and φ with the horizontal. What are the values of T1 and T2?

Solution:

lma24a.PNG

For equilibrium,

Along the horizontal direction

        T1 cos θ  =  T2 cos φ

       T2  =                    ------(1)

Along the vertical direction

T1 sin θ + T2 sin φ  =  W                           ------(2)

Substituting the value of T2 in eqn. (2)

T1 sin θ +  sin φ  =  W

   T1 (sin θ cos φ + cos θ sin φ)  =  W cos φ

       T1  = 

Similarly,                                    T2  = 

 

6. A mass of 5 kg is suspended in equilibrium, by two light inextensible strings S1 and S2, which make angle of 30° and 45° respectively with the horizontal. Then which of the following is correct? (Take g  =  10 m s−2)

(a) Tension in both the strings is same.

(b) Tension in S1 is more than that in S2.

(c) Tension in S1 is less than that in S2.

(d) Sum of tension in both is equal to 50 N.

Solution:

lma25a.PNG

From figure, we concluded

 T1 cos 30°  =  T2 cos 45°

           T1   =  T2

     T2  = 

      T2 > T1

            Tension in S1 is less than that in S2

 

7. A block of mass 200 kg is being pulled up by men on an inclined plane at angle of 45° as shown in figure.

lmq26.png

The coefficient of static friction is 0.5. Each man can only apply a maximum force of 500 N. Find the minimum number of men required to start moving the block up the plane.

Solution:

lma26a.PNG

Mass of the block,

      m  =  200 kg

Coefficient of static friction,

      μs  =  0.5

= 

Angle of incline plane,

       θ  =  45°

Maximum force that each man be apply,

       F  =  500 N

Let n be the number of men required to start moving the block up the plane. Then,

     nF  =  mg sin θ + f

=  mg sin θ + μsN

=  mg sin θ + μs mg cos θ

=  mg[sin θ + μs cos θ]

=  200 × 10

=  200 × 10

=      5

 

8. Which one of the following motions on a smooth plane surface does not involve force?

(a) Accelerated motion in a straight line.

(b) Retarded motion in a straight line.

(c) Motion with constant momentum along a straight line.

(d) Motion along a straight line with varying velocity.

Solution:

Motion with constant momentum along a straight line implies   =  constant.

So, according to Newton’s 2nd law

  =    =  (constant)  =  0

∴ Motion with constant momentum along a straight line is the correct statement.

 

9. The monkey B is holding on to the tail of monkey A which is climbing up a rope. The masses of the monkeys A and B are 5 kg and 2 kg respectively. If A can tolerate a tension of 30 N in its tail, what force should it apply on the rope in order to carry the monkey B with it? (Take g  =  10 m s−2).

Solution:

Let us make the free body diagram for both monkeys separately. As the monkey A, applies a force F downward on the rope, the rope applies a force F upward on the monkey A.

lma28.PNG

For A,            F − 5gT  =  5a ------ (1)

For B,                   T2g  =  2a ------ (2)

Dividing the two eqn.

    = 

     2(F − 5gT )  =  5(T − 2g)

    2F − 10g2T  =  5T − 10g

    2F  =  7T     or     T  = 

Now from eqn (2), for a  =  0

     =  2g  =  20 N;   =  30 N is given

Hence, 20 N ≤ 30 N

   20 N ≤  ≤ 30 N

   (20 N)    F     (30 N)

  70 N ≤ F ≤ 105 N

 

10. A gramophone record is revolving with an angular velocity (ω). A coin is placed at a distance r from the centre of the record. The coefficient of static friction is μ. The coin will revolve with the record if..?

Solution:

The coin will revolve with the record, if the centripetal force ≤ the force of friction

mrω2     or     r ≤

 

11. Block A of mass m and block B of mass 2 m are placed on a fixed triangular wedge by means of a massless, inextensible string and a frictionless pulley as shown in the figure. The wedge is inclined at 45° to the horizontal on both the sides. If the coefficient of friction between the block A and the wedge is  and that between the block B and the wedge is . Both A and B are released from rest, what will be the acceleration of A?

lmq30.PNG

Solution:

The free body diagram of the blocks is shown in the figure

lma30.PNG

The equation of motion of block B is

   2mg sin 45° − μ2N2T  =  2ma

or     2mg sin 45° −  2mg cos 45° − T  =  2ma

or                                                              2a  =  g   

or                                                                a  =   g

But                                (mB − mA)g sin θ  =   will be less than

   (μA mA + μB mB)g cos θ  = 

Therefore the masses will not move and hence acceleration of A or B will be Zero.

 

12. A body of 100 kg is placed on a truck. The coefficient of static friction between the body and the truck is 0.2. The truck suddenly decreases its speed from 90 km/h to 36 km/h in 5s. Which of the following is correct?

(a) The block does not move.

(b) The block slips forward and hit the driver's cabin.

(c) Nothing can be said about the block.

(d) Block shifts backward.

Solution:

Force of static friction     =  μmg

=  0.2 × 100 × 10

=  200 N

Deceleration                      = 

=  

=  3 m s−2

Force on the mass            =  100 kg × 3 m s−2

=  300 N

This is greater than the force due to static friction.

Therefore due to pseudo force, the block of mass m will go forward and hit the driver's cabin.

 

13. A boy stands on a weighing machine inside a lift. When the lift is going down with acceleration , the machine shows a reading 30 kg. When the lift goes upwards with acceleration , the reading would be?

Solution:

While going down, machine reading is 30 kg.

lma32b.PNG

        mg – N  =  m

    mg30g  = 

            3   =  30g

                  m  = 

=  40 kg

While going up, the reaction would be

lma32d.PNG

       N' – mg  =  m

                  N'  =  5

=   (40 kg)g

     N'  =  5 kgf

 

14. The rear side of a truck is open and a box of mass 20 kg is placed on the truck 4 m away from the open end. If μ is 0.15 and g  =  10 m s−2 and the truck starts from rest with an acceleration of 2 m s−2 on a straight road, then the box will fall off the truck when it is at a distance of  metre from the starting point. What is the value of ?

Solution:

a  =  2 m s−2, N  =  mg

lma34a.PNG

     maμN  =  m

           (maμmg)  =  m

     =  aμg

=  2 m s−2 – (0.15)(10 m s−2)

=  0.5 m s−2

For the box’s motion w.r.t. truck,

     =   · t +  · t2

       4  =  0 +  (0.5) t2

      t2  = 

        t  =  4 s

After 4 s, the box will fall off the truck. During 4 s, the truck travels,

         =   at2 

=  (2)(4)2

=  16 m.

 

15. An insect crawls up a hemispherical surface very slowly as shown in the figure. 

lmq35.PNG

The coefficient of friction between the insect and the surface is . If the line joining the centre of the hemispherical surface to the insect makes an angle α, with the vertical, what is the maximum possible value of α?

Solution:

lma35.PNG

The insect I is under the action of two forces. 

N denotes the normal reaction while mg denotes the weight of the insect. 

The weight mg can be resolved into two perpendicular components. For equilibrium

N  =  mg cos α,       f  =  mg sin α

where f denotes force of friction.

But       f  =  μN       μ(mg cos α)  =  mg sin α

or         μ  =  tan α     

                =     

      cot α  =  3

 

16. A weightless thread can bear tension up to 3.7 kg weight. A stone of mass 500 g is tied to it and revolves in a circular path of radius 4 m in vertical plane. If g  =  10 m s−2, then what will be the maximum angular velocity of the stone?

Solution:

Mass of stone  =  500 g

Radius               =  4 m

g  =  10 m s−2

For vertical motion, tension in the string is given by:

         =   mg

where m is the mass of the block attached to the string

Maximum tension is   T  =  3.7 × 9.8 N

     = 

      =  

           =  329.8

        =  18.14 m/s

we know                          =  ωr

ω is the angular velocity

     ω  =  

          =  4.53 rad/sec

 

17. Two fixed frictionless inclined planes making an angle 30° and 60° with the vertical are shown in the figure. Two blocks A and B are placed on the two planes. What is the relative vertical acceleration of A with respect to B?

lmq37.PNG

Solution:

The acceleration of the body down the smooth inclined plane is a  =  g sin θ

It is along the inclined plane.

where θ is the angle of inclination

The vertical component of acceleration a is

             =  (g sin θ)sin θ 

      =  g sin2 θ

For block A,

           =  g sin2 60°

For block B,

           =  g sin2 30°

The relative vertical acceleration of A with respect to B is

        =   

      =  g sin2 60° − g sin2 30°

      =  g

      =    =  4.9 m s−2 in vertical direction

 

18. A person sitting in an open car moving at constant velocity throws a ball vertically up into air. Where will the ball fall?

Solution:

Since the velocity is constant, the horizontal component of velocity for the car and the ball are the same.

They cover equal horizontal distances in the same time interval. 

Therefore the ball will land in the hands of the person in the car.

 

19. A man is standing stationarily with respect to a horizontal conveyor belt that is accelerating with 1 m s–2, as shown in figure. What is the net force on the man? If the coefficient of static friction between the man’s shoes and the belt is 0.2, up to what acceleration of the belt can the man continue to be stationary relative to the belt? (Mass of the man  =  65 kg.)

lmq38.PNG

Solution:

Mass of the man,                     m  =  65 kg

Acceleration of the belt,         a  =  1 m s–2

Coefficient of static friction, μ  =  0.2

The net force F, acting on the man is given by Newton’s second law of motion as:

   Fnet  =  ma 

 =  65 × 1

 =  65 N

The man will continue to be stationary with respect to the conveyor belt until the net force on the man is less than or equal to the frictional force fs, exerted by the belt, i.e.,

   Fnet  =  fs

    ma'  =  μmg

       a'  =  0.2 × 10

 =  2 m s–2

Therefore, the maximum acceleration of the belt up to which the man can stand stationarily is 2 m s−2.

 

20. A stream of water flowing horizontally with a speed of 15 m s–1 gushes out of a tube of cross-sectional area 10–2 m2, and hits a vertical wall nearby. What is the force exerted on the wall by the impact of water, assuming it does not rebound?

Solution:

Speed of the water stream, 

  =  15 m/s

Cross-sectional area of the tube,

A  =  10–2 m2

Volume of water coming out from the pipe per second,

V  =  A 

     =  15 × 10–2 m3/s

Density of water, 

ρ  =  103 kg/m3

Mass of water flowing out through the pipe per second,

     =  ρ × V

     =  150 kg/s

The water strikes the wall and does not rebound. Therefore, the force exerted by the water on the wall is given by Newton’s second law of motion as:

F  =  Rate of change of momentum

     =  

     =  

     =  150 × 15

     =  2250 N

 

21. An aircraft executes a horizontal loop at a speed of 720 km/h with its wings banked at 15°. What is the radius of the loop?

Solution:

Speed of the aircraft,                 =  720 km/h

 =  720 ×  

 =  200 m/s

Acceleration due to gravity,  g  =  10 m/s2

Angle of banking,                     θ  =  15°

For radius r, of the loop, we have the relation:

            tan θ  =  

        r  =   

=   

= 

=  14925.37 m

=  14.92 km

 

22. A 70 kg man stands in contact against the inner wall of a hollow cylindrical drum of radius 3 m rotating about its vertical axis with 200 rev/min. The coefficient of friction between the wall and his clothing is 0.15. What is the minimum rotational speed of the cylinder to enable the man to remain stuck to the wall (without falling) when the floor is suddenly removed?

Solution:

The cylinder being vertical, the normal reaction of the wall on the man acts horizontally and provides the necessary centripetal force which is given below,

  R  =  mr             ------ (1)

The frictional force F, acting upwards balances his weight, i.e.,

  F  =  mg                  ------ (2)

The man will remain stuck to the wall and continue to rotate with the cylinder without slipping,

when   μ   

  F    μR

            Substituting equations (1) and (2),

          mg    μ mr

  

 ω                      ------(3)

The minimum angular speed of rotation of the cylinder drum is given by

       ωmin                    ------ (4)

Here,   μ  =  0.15, r  =  3 m, g  =  9.8 m s−2

Substituting in equation (4),

       ωmin  =   rad s−1

       =  4.67 ≃ 5 rad s−1