Laws of Motion - Ncert Extract MCQ
Laws of Motion - Ncert Extract MCQ
LAWS OF MOTION
T1
m 3F
(a) F3 = F1 + F2 (b) F3 = F F2 F3
1
T2
m 3F m 3F
(c) F3 = m m2 m3 (d) F3 = m
1 1 m2
W = 60N
79. Which of the following is true about acceleration, a for the
system?
(a) 30° (b) 45°
(c) 0° (d) 90° m2
76. The acceleration of the system shown in the figure is given m1
by the expression (ignore force of friction) T T B
F A
u g(1 – 2 )
(d)
2
30° 81. The force ‘F’ acting on a particle of mass ‘m’ is indicated by
u u 30° the force-time graph shown below. The change in momentum
u of the particle over the time interval from zero to 8 s is :
(a) (b) 6
3
(a) In (a) force is normal to the wall and in (b) force is
0
F(N)
1 1
1 2
(c) 1 (d) (a) m (b) m
6 3
n2 1 n2
1 1
130. The minimum force required to start pushing a body up rough (c) m (d) m
(frictional coefficient ) inclined plane is F1 while the 3 2
minimum force needed to prevent it from sliding down is F2. 137. Two bodies of masses 1 kg and 2 kg moving with same
If the inclined plane makes an angle from the horizontal velocities are stopped by the same force. Then the ratio of
F their stopping distances is
such that tan 2 then the ratio 1 is
F (a) 1 : 2 (b) 2 : 1
(a) 1 (b) 2 2
(c) 3 (d) 4 (c) 2 :1 (d) 1 : 2
131. A particle is acted upon by a force of constant magnitude
which is always perpendicular to the velocity of the 138. A block A of mass m1 rests on a horizontal table. A light
particle. The motion of the particle takes place in a plane. string connected to it passes over a frictionless pulley at the
It follows that edge of table and from its other end another block B of mass
(a) its velocity is constant m2 is suspended. The coefficient of kinetic friction between
(b) its acceleration is constant
the block and the table is µk. When the block A is sliding on
(c) its kinetic energy is constant
(d) it moves in a straight line. the table, the tension in the string is
132. If n bullets each of mass m are fired with a velocity v per
second from a machine gun, the force required to hold the (m 2 – k m1 ) g m1m 2 (1 k )g
(a) (m1 m 2 ) (b) (m1 m 2 )
gun in position is
mv m1m 2 (1 – k )g (m 2 km1 )g
(a) (n + 1) mv (b) (c) (d)
n2 (m1 m 2 ) (m1 m2 )
mv 139. The retarding acceleration of 7.35 m s–2 due to frictional
(c) (d) mnv
n force stops the car of mass 400 kg travelling on a road. The
133. A car moves at a speed of 20 ms–1 on a banked track and coefficient of friction between the tyre of the car and the
describes an arc of a circle of radius 40 3 m. The angle of road is
banking is (g = 10 ms–2 ) (a) 0.55 (b) 0.75
(a) 25° (b) 60°
(c) 0.70 (d) 0.65
(c) 45° (d) 30°
134. A ball of mass 10 g moving perpendicular to the plane of the 140. A hammer weighing 3 kg strikes the head of a nail with a
wall strikes it and rebounds in the same line with the same speed of 2 ms–1 drives it by l cm into the wall. The impulse
velocity. If the impulse experienced by the wall is 0.54 Ns, imparted to the wall is
the velocity of the ball is
(a) 6Ns (b) 3Ns
(a) 27 ms–1 (b) 3.7 ms–1
(c) 54 ms –1 (d) 37 ms–1 (c) 2Ns (d) l2 Ns
135. Two blocks of masses 2 kg and 4 kg are attached by an 141. A balloon with mass ‘m’ is descending down with an
inextensible light string as shown in the figure. If a force of acceleration ‘a’ (where a < g). How much mass should be
120 N pulls the blocks vertically upward, the tension in the removed from it so that it starts moving up with an
string is (take g = 10 ms–2) acceleration ‘a’?
F = 120 N 2ma 2ma
(a) 20 N
4 kg (a) g a (b) g a
(b) 15 N
(c) 35 N ma ma
2 kg (c) (d)
(d) 40 N g a g a
EBD_7208
64 LAWS OF MOTION
129. A given object takes n times as much time to slide down a 136. A block of mass m is placed on a surface with a vertical cross
45º rough incline as it takes to slide down a perfectly smooth
45º incline. The coefficient of kinetic friction between the x3
section given by y . If the coefficient of friction is 0.5,
object and incline is given by 6
1 1 the maximum height above the ground at which the block
(a) 1 (b)
n 2
1 n2 can be placed without slipping is:
1 1
1 2
(c) 1 (d) (a) m (b) m
6 3
n2 1 n2
1 1
130. The minimum force required to start pushing a body up rough (c) m (d) m
(frictional coefficient ) inclined plane is F1 while the 3 2
minimum force needed to prevent it from sliding down is F2. 137. Two bodies of masses 1 kg and 2 kg moving with same
If the inclined plane makes an angle from the horizontal velocities are stopped by the same force. Then the ratio of
F their stopping distances is
such that tan 2 then the ratio 1 is
F (a) 1 : 2 (b) 2 : 1
(a) 1 (b) 2 2
(c) 3 (d) 4 (c) 2 :1 (d) 1 : 2
131. A particle is acted upon by a force of constant magnitude
which is always perpendicular to the velocity of the 138. A block A of mass m1 rests on a horizontal table. A light
particle. The motion of the particle takes place in a plane. string connected to it passes over a frictionless pulley at the
It follows that edge of table and from its other end another block B of mass
(a) its velocity is constant m2 is suspended. The coefficient of kinetic friction between
(b) its acceleration is constant
the block and the table is µk. When the block A is sliding on
(c) its kinetic energy is constant
(d) it moves in a straight line. the table, the tension in the string is
132. If n bullets each of mass m are fired with a velocity v per
second from a machine gun, the force required to hold the (m 2 – k m1 ) g m1m 2 (1 k )g
(a) (m1 m 2 ) (b) (m1 m 2 )
gun in position is
mv m1m 2 (1 – k )g (m 2 km1 )g
(a) (n + 1) mv (b) (c) (d)
n2 (m1 m 2 ) (m1 m2 )
mv 139. The retarding acceleration of 7.35 m s–2 due to frictional
(c) (d) mnv
n force stops the car of mass 400 kg travelling on a road. The
133. A car moves at a speed of 20 ms–1 on a banked track and coefficient of friction between the tyre of the car and the
describes an arc of a circle of radius 40 3 m. The angle of road is
banking is (g = 10 ms–2 ) (a) 0.55 (b) 0.75
(a) 25° (b) 60°
(c) 0.70 (d) 0.65
(c) 45° (d) 30°
134. A ball of mass 10 g moving perpendicular to the plane of the 140. A hammer weighing 3 kg strikes the head of a nail with a
wall strikes it and rebounds in the same line with the same speed of 2 ms–1 drives it by l cm into the wall. The impulse
velocity. If the impulse experienced by the wall is 0.54 Ns, imparted to the wall is
the velocity of the ball is
(a) 6Ns (b) 3Ns
(a) 27 ms–1 (b) 3.7 ms–1
(c) 54 ms –1 (d) 37 ms–1 (c) 2Ns (d) l2 Ns
135. Two blocks of masses 2 kg and 4 kg are attached by an 141. A balloon with mass ‘m’ is descending down with an
inextensible light string as shown in the figure. If a force of acceleration ‘a’ (where a < g). How much mass should be
120 N pulls the blocks vertically upward, the tension in the removed from it so that it starts moving up with an
string is (take g = 10 ms–2) acceleration ‘a’?
F = 120 N 2ma 2ma
(a) 20 N
4 kg (a) g a (b) g a
(b) 15 N
(c) 35 N ma ma
2 kg (c) (d)
(d) 40 N g a g a
LAWS OF MOTION 65
142. The time required to stop a car of mass 800 kg, moving at a (a) have a horizontal inward component
speed of 20 ms–1 over a distance of 25 m is (b) be vertical
(a) 2s (b) 2.5s (c) equilibriate the centripetal force
(c) 4s (d) 4.5s
(d) be decreased
143. A particle rests on the top of a hemisphere of radius R.
Find the smallest horizontal velocity that must be imparted 148. A sphere is suspended by a thread of length . What
to the particle if it is to leave the hemisphere without minimum horizontal velocity has to be imparted to the sphere
sliding down is for it to reach the height of the suspension?
(a) g (b) 2 g
(a) gR (b) 2g R
(c) g (d) 2g
(c) 3g R (d) 5g R
149. A car when passes through a bridge exerts a force on it
144. A train is moving with a speed of 36 km/hour on a curved which is equal to
path of radius 200 m. If the distance between the rails is 1.5
m, the height of the outer rail over the inner rail is Mv 2 Mv 2
(a) 1 m (b) 0.5 m (a) Mg (b)
r r
(c) 0.75 m (d) 0.075 m
145. A car moving on a horizontal road may be thrown out of the Mv 2
road in taking a turn (c) Mg – (d) None of these
r
(a) by the gravitational force
150. A bridge is in the from of a semi-circle of radius 40m. The
(b) due to the lack of proper centripetal force
greatest speed with which a motor cycle can cross the bridge
(c) due to the rolling frictional force between the tyre and
without leaving the ground at the highest point is
road
(d) due to the reaction of the ground (g = 10 m s–2) (frictional force is negligibly small)
146. A car sometimes overturns while taking a turn. When it (a) 40 m s–1 (b) 20 m s–1
overturns, it is (c) 30 m s–1 (d) 15 m s–1
(a) the inner wheel which leaves the ground first 151. A particle tied to a string describes a vertical circular motion
(b) the outer wheel which leaves the ground first
of radius r continually. If it has a velocity 3 gr at the
(c) both the wheel leave the ground simultaneously
(d) either wheel will leave the ground first highest point, then the ratio of the respective tensions in
the string holding it at the highest and lowest points is
147. On a railway curve the outside rail is laid higher than the
(a) 4 : 3 (b) 5 : 4
inside one so that resultant force exerted on the wheels of
(c) 1 : 4 (d) 3 : 2
the rail car by the tops of the rails will
LAWS OF MOTION 67
26. (c) 48. (a) A thin cushion of air maintained between solid surfaces
27. (c) Swimming is a result of pushing water in the opposite in relative motion is another effective way or reducing
direction of the motion. friction
28. (a) Newton’s second and third laws of motion leads to the
conservation of linear momentum. Inflated balloon
29. (c) Hot gases with high velocity react against the rocket Plastic disc with hole
and push it up.
30. (c) The gun applied a force F12 on the bullet in forward
Air cushion
direction & according to Newton’s third law bullet surface
applies a reaction force on gun F21 in backward
Because of air cushion between plastic disc and surface,
direction. But the recoil speed of gun is very low in
there is very less friction between plastic disc and
comparison to bullet due to large mass.
surface. So plastic disc can be moved on surface with
31. (b)
very less frictional dissipation of energy. This is
32. (b) Since no nearby stars are there to exert gravitational because friction between solid and air is very small.
force on the astronaut, so the net force acting on him is
49. (c) When force is applied on a moving body in a direction
zero when he moves out of the spaceship. Thus in
perpendicular to the direction of motion, then it takes a
accordance with first law of motion the acceleration of circular path. Thus the direction of motion changes
astronaut will be zero. without changes in the speed.
33. (d) 50. (c) Normal reaction N = weight mg thus the centripetal
34. (a) It works on the principle of conservation of linear force required by the car for circular motion is provided
momentum. by the component of the force of friction b/w the road
35. (a) If m1, m2 are masses and u1, u2 are velocity then by and the car tyres.
conservation of momentum m 1u1 + m 2u2 = 0 or
N
| m1u1 | | m2 u 2 |
36. (c)
37. (c) Motion with constant momentum along a straight line. f
According to Newton's second law rate of change of
momentum is directly proportional to force applied. mg
38. (d) k < s coefficient of static friction is always greater 51. (a) Optimum speed is given by V0 = (Rg tan )1/2 on a
than kinetic friction. banked road, the normal reaction’s component is
39. (a) Since there in no resultant external force, linear enough to provide the necessary centripetal force to a
momentum of the system remains constant. car driven at optimum speed.
40. (c) Frictional force that opposes relative motion between 52. (a) Material forces like friction, gravitational force etc. act
surfaces in contact is called kinetic friction and denoted on the body and provide the centripetal force. The
by fk. centripetal force cannot be regarded as any kind of
force acting externally. It is simple name given to the
force of friction force that provides inward radial acceleration to a body
41. (a) Coefficient of static friction =
normal reaction in circular motion.
Therefore, coefficient of static friction depends upon v2 1
the normal reaction. 53. (a) Acceleration (centripetal) a i.e., a
r r
42. (c) Friction does not depend on area of surfaces in 54. (d)
contact. 55. (b) Due to centrifugal force, the inner wheel will be left up
43. (d) Coefficient of friction is independent of normal force. when car is taking a circular turn. Due to this, the reaction
44. (b) When a box is in stationary position with respect to on outer wheel is more than that on inner wheel.
train moving with acceleration, then relative motion is 56. (b) The cyclist bends while taking turn in order to provide
opposed by the static friction. necessary centripetal force.
45. (c)
46. (d) When brakes are on, the wheels of the cycle will slide STATEMENT TYPE QUESTIONS
on the road instead of rolling there. It means the sliding
friction will come into play instead of rolling friction. 57. (b) A breeze causes branches of tree to swing. In general
The value of sliding friction is more than that of rolling force is required to put a stationary object in motion.
friction. 58. (d) Newton’s 2nd law of motion gives F = ma. Thus it is a
47. (d) measure of force. Newton’s first law of motion simply
gives a qualitative definition of force.
LAWS OF MOTION 67
26. (c) 48. (a) A thin cushion of air maintained between solid surfaces
27. (c) Swimming is a result of pushing water in the opposite in relative motion is another effective way or reducing
direction of the motion. friction
28. (a) Newton’s second and third laws of motion leads to the
conservation of linear momentum. Inflated balloon
29. (c) Hot gases with high velocity react against the rocket Plastic disc with hole
and push it up.
30. (c) The gun applied a force F12 on the bullet in forward
Air cushion
direction & according to Newton’s third law bullet surface
applies a reaction force on gun F21 in backward
Because of air cushion between plastic disc and surface,
direction. But the recoil speed of gun is very low in
there is very less friction between plastic disc and
comparison to bullet due to large mass.
surface. So plastic disc can be moved on surface with
31. (b)
very less frictional dissipation of energy. This is
32. (b) Since no nearby stars are there to exert gravitational because friction between solid and air is very small.
force on the astronaut, so the net force acting on him is
49. (c) When force is applied on a moving body in a direction
zero when he moves out of the spaceship. Thus in
perpendicular to the direction of motion, then it takes a
accordance with first law of motion the acceleration of circular path. Thus the direction of motion changes
astronaut will be zero. without changes in the speed.
33. (d) 50. (c) Normal reaction N = weight mg thus the centripetal
34. (a) It works on the principle of conservation of linear force required by the car for circular motion is provided
momentum. by the component of the force of friction b/w the road
35. (a) If m1, m2 are masses and u1, u2 are velocity then by and the car tyres.
conservation of momentum m 1u1 + m 2u2 = 0 or
N
| m1u1 | | m2 u 2 |
36. (c)
37. (c) Motion with constant momentum along a straight line. f
According to Newton's second law rate of change of
momentum is directly proportional to force applied. mg
38. (d) k < s coefficient of static friction is always greater 51. (a) Optimum speed is given by V0 = (Rg tan )1/2 on a
than kinetic friction. banked road, the normal reaction’s component is
39. (a) Since there in no resultant external force, linear enough to provide the necessary centripetal force to a
momentum of the system remains constant. car driven at optimum speed.
40. (c) Frictional force that opposes relative motion between 52. (a) Material forces like friction, gravitational force etc. act
surfaces in contact is called kinetic friction and denoted on the body and provide the centripetal force. The
by fk. centripetal force cannot be regarded as any kind of
force acting externally. It is simple name given to the
force of friction force that provides inward radial acceleration to a body
41. (a) Coefficient of static friction =
normal reaction in circular motion.
Therefore, coefficient of static friction depends upon v2 1
the normal reaction. 53. (a) Acceleration (centripetal) a i.e., a
r r
42. (c) Friction does not depend on area of surfaces in 54. (d)
contact. 55. (b) Due to centrifugal force, the inner wheel will be left up
43. (d) Coefficient of friction is independent of normal force. when car is taking a circular turn. Due to this, the reaction
44. (b) When a box is in stationary position with respect to on outer wheel is more than that on inner wheel.
train moving with acceleration, then relative motion is 56. (b) The cyclist bends while taking turn in order to provide
opposed by the static friction. necessary centripetal force.
45. (c)
46. (d) When brakes are on, the wheels of the cycle will slide STATEMENT TYPE QUESTIONS
on the road instead of rolling there. It means the sliding
friction will come into play instead of rolling friction. 57. (b) A breeze causes branches of tree to swing. In general
The value of sliding friction is more than that of rolling force is required to put a stationary object in motion.
friction. 58. (d) Newton’s 2nd law of motion gives F = ma. Thus it is a
47. (d) measure of force. Newton’s first law of motion simply
gives a qualitative definition of force.
EBD_7208
68 LAWS OF MOTION
59. (d) If a body is moving with a constant velocity then the Applying Lami's equation, we have
net force on the body is zero. Also if net force is zero,
TBC W2 300
the body may be moving uniformly along a straight = =
sin150 sin120 sin 90
line. Thus both the given statements are false.
60. (b) There are three types of inertia. TAB W1 TBC
Inertia of rest : The resistance of a body to change its and
sin 90
=
sin150
=
sin120
state of rest is called inertia of rest.
After simplifying, we get
Inertia of motion : The resistance of a body to change
its state of motion is called inertia of motion. TAB = 173 N, TBC = 150 N, W1 = 87 N, W2 = 260 N.
Inertia of direction : The resistance of a body to change 71. (c) (A) (3); (B) (4); C (1); (D) (2)
its direction of motion is called inertia of direction.
61. (d) Action & reaction forces act simultaneously: There is DIAGRAM TYPE QUESTIONS
no cause effect relation between action and reaction as
any of the two mutual forces can be called action and 72. (c) Equilibrium under three concurrent forces F1, F2and F3
the other reaction since action & reaction act on requires that vector sum of the three forces is zero.
different bodies, so they cannot be cancelled out. F1 + F2 + F3 = 0.
62. (c) When the men push the rough surface on walking, R F1 F2 F1
then surface (from Newton’ third Law) applies reaction R
force in forward direction. It occurs because there is F3 R (In eqbm)
friction between men & surface. If surface is frictionless
(such as ice), then it is very difficult to move on it. F3 (F1 F2 )
F2
63. (a) Newton's laws of motion are applicable only for inertial
F1 F2 F3 = 0 F3
frames. All refrence frames present on surface of earth
are supposed to be inertial frame of refrence.
64. (a) According to third law of motion bullet experiences a
force F then, give experiences an equal and opposite 73. (c) In series each spring will have same force.
force F. According to second law, F t is change in Here it is 4 kg-wt.
momentum of the bullet, then – F t is change in
momentum of the gun. Since initially both are at rest, 74. (b) If a body slides down, then the force of friction acts
the final momentum = 0. Pb + Pg = 0. Thus the total upwards along the plane weight(mg) act vertically
momentum of (bullet + gun) is conserved. downwards.
65. (d) The static friction comes into play, the moment there is 75. (b)
an applied force. As the applied force increases, static
friction also increases, remaining equal and opposite
to the applied force upto a certain limit. But if the applied T1 cos
T1
force increases so much, it overcomes the static friction
and the body starts moving.
66. (c) Limiting friction is the maximum static friction beyond T1 sin T2
which the object starts moving. It decreases a little bit 2m
before the object comes into motion. Thus limiting T2
friction is less than the kinetic friction.
W = 60N
MATCHING TYPE QUESTIONS
In eqbm T1cos = T2 = 60N. …(1)
67. (b) (A) (4); (B) (3); C (1); (D) (2) T1sin = 60 N …(2)
68. (a) (A) (4); (B) (1); C (2); (D) (3) tan = 1
69. (d) (A) (4); (B) (3); C (1); (D) (2) = 45°.
70. (b) (A) (2) ; (B) (1) ; (C) (4) ; (D) (3) 76. (a) Equations of motion of m1 & m2 are as:
T = m1a …(1)
300N
m2g – T = m2a …(2)
A Adding eqn. (i) and (ii)
150° 120°
C
m2g = (m1 + m2) a
B
TBC TBC
m2g
a= m m
2
w1 w2
EBD_7208
70 LAWS OF MOTION
93. (d) The net force on the block is zero, but action cannot 106. (c) When an elevator cabin falls down, it is accelerated down
cancel the reaction because these two act on different with respect to earth i.e. man standing on earth.
bodies. 107. (a)
94. (a) On a rainy day, the roads are wet. Wetting of roads
108. (b)
lowers the coefficient of friction between the types
109. (c) Impulse experienced by the body
and the road. Therefore, grip on a road of car reduces
and thus chances of skidding increases. = change in momentum
95. (d) = MV – (–MV)
96. (d) The man can exert force on block by pulling the rope. = 2MV.
The tension in rope will make the man move. Hence 110. (d) If rope of lift breaks suddenly, then acceleration
statement-1 is false. becomes equal to g so that tension T = m(g – g) = 0
97. (a) Friction causes wear & tear and loss of energy, so it is
an evil but without friction walking. Stopping a vehicle
etc. would not be possible. So it is necessary for us. 111. (a) y
98. (c) The assertion is true for a reason that when the car is 2 kg m2
driven at optimum speed. Then the normal reaction
8 m/sec
component is enough to provide the centripetal force. Presultant
99. (b) When a body is moving in a circle, its speed remains
12 m/sec
same but velocity changes due to change in the m1
c x
direction of motion of body. According to first law of /se 1 kg
motion, force is required to change the state of a 4m
3
body. As in circular motion the direction of velocity m
of body is changing so the acceleration cannot be
zero. But for a uniform motion acceleration is zero (for
rectilinear motion).
100. (c) In uniform circular motion, the direction of motion Presultant = 122 162
changes, therefore velocity changes.
= 144 256 = 20
As P = mv therefore momentum of a body also
changes uniform circular motion. m3v3 = 20 (momentum of third part)
101. (c) The purpose of bending is to acquire centripetal
force for circular motion. By doing so component of 20
or, m3 = = 5 kg
normal reaction will counter balance the centrifugal 4
force. 112. (d) According to law of conservation of momentum the
third piece has momentum
CRITICALTHINKING TYPE QUESTIONS
1 –(3iˆ 4j)
ˆ kg ms–1
102. (b) The apple will fall slightly away from the hand of his
brother in the direction of motion of the train due to Impulse = Average force × time
inertia of motion. When train is just going to stop, Impulse
the boy and his brother slows down with train but Average force
time
the apple which is in free fall continue to move with y
the same speed and therefore, falls slightly away
from the hand in the direction of motion of the train. Change in momentum
103. (d) Horizontal velocity of ball and person are same so time
1 4ˆj
both will cover equal horizontal distance in a given x
1 3iˆ
interval of time and after following the parabolic path –(3iˆ 4ˆj)kg ms –1 4j)
the ball falls exactly in the hand which threw it up. i +
10 –4 s (3
104. (a) After the stone is thrown out of the moving train, the (–
only force acting on it is the force of gravity i.e. its 1×
weight. 113. (b) From law of conservation of momentum
F = mg = 0.05 × 10 = 0.5 N.
MV = m1v1 + m2v2
105. (b) The pressure on rear side would be more due to fictious
force on the rear face. Consequently the pressure in Here, M = 100 kg, v = 104 m s–1
the front side would be lowered. m1 = 10 kg, v1 = 0
m2 = 90 kg, v2 = ?
LAWS OF MOTION 71
120. (b) When force is applied on m1
4
100 10 then T = m2a and when force is applied on m2, then
100 × 104 = 10 × 0 + 90 × v2 v2
90 T = m1a. Thus value of T is different for each case. And
v2 = 11.11 × 103 m s–1. it depends on whether the force is applied on m1, or m2.
114. (c) Change in momentum of the ball
= mv sin – (– mv sin ) 121. (b) Opposite force causes retardation.
= 2 mv sin 122. (d) In case (a) In case (b)
2vsin
= mg
g N mN N
F2
= weight of the ball × total time of flight
F1
115. (a) 49 mg mg
Mass 5 kg
9.8 mg Cos mN Sin mg Cos S in
W E
m = 1000 kg
S
x2 2ma
0.5 Therefore m =
2 g a
x=+1 u v
3
142. (b) As we know, S = t
x 1 2
Now, y m
6 6
0 20
137. (a) Energy of both bodies is given by 2
t = 25 t = 2.5s
KE1 = F.S1
143. (a) The velocity should be such that the centripetal
KE2 = F.S2
acceleration is equal to the acceleration due to gravity
As force is equal
v2
S1 m1v12 m1 1 g or v gR
v1 v2 R
S2 m 2 v 22 m2 2
144. (d) tan = v2 / rg, tan = H / 1.5, r = 200 m, b = 1.5 m
138. (b) For the motion of both the blocks v = 36 km/hour = 36 × (5/18) = 10 m/s.
m1a = T – Putting these values, we get H = 0.075 m.
km1g
145. (b) It means that car which is moving on a horizontal road
m2g – T = m2a
& the necessary centripetal force, which is provided
a
T by friction (between car & road) is not sufficient.
k m1g m1
If is friction between car and road, then max speed of
k safely turn on horizontal road is determined from figure.
m2
a
N
m2g car of
f mass m
m 2g – k m1g
a= m1 m 2 mg
m 2 g – k m1g
m2g – T = (m2) m1 m 2
solving we get tension in the string N = mg ...(i)
m1mg (1 k )g mv 2
T= f ...(ii)
m1 m 2 r
F Where f is frictional force between road & car, N is the
139. (b) As we know, coefficient of friction =
N normal reaction exerted by road on the car. We know
ma a that
= (a = 7.35 m s–2 given)
mg g f sN s mg ......(iii)
7.35 where s is static friction
= 0.75 so from eq (ii) & (iii) we have
9.8
140. (a) As we know, |impulse| = |change in momentum| mv 2
s mg v2 s rg or v s rg
= |p2 – p1| r
= |0 – mv1| = |0 – 3 × 2| = 6 Ns & v max s rg
141. (a) Let upthrust of air be Fa then If the speed of car is greater than vmax at that road,
For downward motion of balloon then it will be thrown out from road i.e., skidding.
Fa = mg – ma 146. (a) The car over turn, when reaction on inner wheel of car
mg – Fa = ma is zero, i.e., first the inner wheel of car leaves the ground
For upward motion (where G is C.G of car, h is height of C.G from the ground,
Fa – (m – m)g = (m – m)a f1 & f2 are frictional force exerted by ground on inner &
EBD_7208
74 LAWS OF MOTION
outer wheel respectively). The max. speed for no over Where is angle of banking of rail track, N is normal
turning is reaction exerted by rail track on rail.
G It is clear from the equation (i) & (ii) that N cos balance
N1 N2 the weight of the train & N sin provide the necessary
h centripetal force to turn.
f1 B
A If width of track is (OB) & h (AB) be height of outside
inner wheel f2 mg outer wheel
of car of track from the inside, then
of car
2a h v2 v2
tan or h .................(iv)
rg rg
gra So it is clear from the above analysis that if we increase
v max
h the height of track from inside by h metre then resultant
where r is radius of the path followed by car for turn & 2a force on rail is provided by railway track & whose
direction is inwards.
is distance between two wheels of car (i.e., AB)
147. (a) If the outside rail is h units higher than inside of rail track 1
148. (d) mv 2 m g or v (2 g )
as shown in figure then 2
N cos = mg....................(i) 149. (c) Force exerted by a car when passes through a bridge
Mv 2
F Mg .
N Ncos Train
r
1
sin A 150. (b) v gr 10 40 20 m s
N
O
h 151. (c) Tension at the highest point
mg B
inside mv2
Ttop – mg 2mg ( vtop = 3gr )
r
trrack
Rail