Laws of Motion NCERT MCQ
Laws of Motion NCERT 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
(c) (d)
(d) 40 N 2 kg 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
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66 LAWS OF MOTION
m1g (m 2 m3 )g g P1 P2
= = (1 2 ) F1 = F2 =
m1m 2 m3 3 t1 t2
( m1 = m2 = m3 = m given) F1 × t1 = F2 × t2
81. (c) Change in momentum,
P1 = P2
p = Fdt Thus the same force for the same time causes the same
= Area of F-t graph change in momentum for different bodies.
= ar of – ar of + ar of
90. (d) Law of conservation of linear momentum is correct
1 when no external force acts. When bullet is fired form
= 2 6 3 2 4 3
2 a rifle then both should possess equal momentum
= 12 N-s
82. (a) p2
N cos but different kinetic energy. E = Kinetic
2m
N energy of the rifle is less than that of bullet because
f cos E 1/m
N sin 91. (a)
f 92. (a) The force acting on the body of mass M are its weight
mg
Mg acting vertically downward and air resistance F
f sin
acting vertically upward.
Clearly form the figure, N sin and f cos contribute to
F
the centripetal force. Acceration of the body , a g
M
2
N sin + f cos = mv Now M > m, therefore, the body with larger mass will
R have great acceleration and it will reach the ground first.
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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 Presultant
component is enough to provide the centripetal force.
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
= tan
f2 m
dy x 2 y
tan = =
mg sin
dx 2
mg sin
f1 mg cos mg cos (from question)
mg mg
Coefficient of friction = 0.5
LAWS OF MOTION 73
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 &
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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