Center of Mass and Collision

JEE Physics · 64 questions · Page 1 of 7 · Click an option or "Show Solution" to reveal answer

Q1
A bomb of mass 16kg16kg at rest explodes into two pieces of masses 44 kgkg and 1212 kg.kg. The velocity of the 1212 kgkg mass is 4ms1.4\,\,m{s^{ - 1}}. The kinetic energy of the other mass is
A 144144 JJ
B 288288 JJ
C 192192 JJ
D 9696 JJ
Correct Answer
Option B
Solution

Here linear momentum is conserved as no external force is acting on the bomb. Let the velocity and mass of

44
kgkg

piece be

v1{v_1}

and

m1{m_1}

and that of

1212
kgkg

piece be

v2{v_2}

and

m2{m_2}

. Applying conservation of linear momentum

0=m2v2m1v10 = {m_2}{v_2} - {m_1}{v_1}
v1=12×144=12ms1\Rightarrow {v_1} = {{12 \times 14} \over 4} = 12\,m{s^{ - 1}}

\therefore

K.E1=12m1v12=12×4×144=288JK.E{_1} = {1 \over 2}{m_1}v_1^2 = {1 \over 2} \times 4 \times 144 = 288\,J
Q2
Distance of the center of mass of a solid uniform cone from its vertex is z0z{}_0. If the radius of its base is RR and its height is hh then z0z{}_0 is equal to :
A 5h8{{5h} \over 8}
B 3h28R{{3{h^2}} \over {8R}}
C h24R{{{h^2}} \over {4R}}
D 3h4{{3h} \over 4}
Correct Answer
Option D
Solution

Let the density of solid cone ρ\rho.

dm=ρπr2dydm = \rho \pi {r^2}dy
ycm=ydmdm{y_{cm}} = {{\int {ydm} } \over {\int {dm} }}
=0hπr2dyρ×y13πR2hρ= {{\int\limits_0^h {\pi {r^2}} dy\rho \times y} \over {{1 \over 3}\pi {R^2}h\rho }}
=3h4= {{3h} \over 4}
Q3
A body of mass m1 moving with an unknown velocity of v1i{v_1}\mathop i\limits^ \wedge , undergoes a collinear collision with a body of mass m2 moving with a velocity v2i{v_2}\mathop i\limits^ \wedge . After collision, m1 and m2 move with velocities of v3i{v_3}\mathop i\limits^ \wedge and v4i{v_4}\mathop i\limits^ \wedge , respectively. If m2 = 0.5 m1 and v3 = 0.5 v1, then v1 is :-
A v4v22{v_4} - {{{v_2}} \over 2}
B v4v24{v_4} - {{{v_2}} \over 4}
C v4v2{v_4} - {v_2}
D v4+v2{v_4} + {v_2}
Correct Answer
Option C
Solution

Applying linear momentum conservation

m1v1i^+m2v2i^=m1v3i^+m2v4i^{m_1}{v_1}\widehat i + {m_2}{v_2}\widehat i = {m_1}{v_3}\widehat i + {m_2}{v_4}\widehat i

m1v1 + 0.5 m1v2 = m1(0.5 v1) + 0.5 m1v4 0.5 m1v1 = 0.5 m1(v4 - v2) v1 = v4 - v2

Q4
A particle of mass 'm' is moving with speed '2v' and collides with a mass '2m' moving with speed 'v' in the same direction. After collision, the first mass is stopped completely while the second one splits into two particles each of mass 'm', which move at angle 45° with respect to the origianl direction. The speed of each of the moving particle will be :-
A 2 2\sqrt2v
B v / (2 2\sqrt2 )
C v / 2\sqrt2
D 2\sqrt2v
Correct Answer
Option A
Solution

Initial momentum · Pi = 2mv + 2mv = 4 mv Let v' be the speed of

ll

particle

2mv2=4mv\therefore 2{{mv} \over {\sqrt 2 }} = 4mv

\Rightarrow v' =

22{2\sqrt 2 }

v

Q5
Particle A of mass m1 moving with velocity (3i^+j^)ms1\left( {\sqrt3\widehat i + \widehat j} \right)m{s^{ - 1}} collides with another particle B of mass m2 which is at rest initially. Let V1\overrightarrow {{V_1}} and V2\overrightarrow {{V_2}} be the velocities of particles A and B after collision respectively. If m1 = 2m2 and after collision V1=\overrightarrow {{V_1}} = (i^+3j^)\left( {\widehat i + \sqrt 3 \widehat j} \right) , the angle between V1\overrightarrow {{V_1}} and V2\overrightarrow {{V_2}} is :
A 105o
B 15o
C -45o
D 60o
Correct Answer
Option A
Solution

Given m1 = 2m2 So let, m2 = m and m1 = 2m From momentum conservation

pi{\overrightarrow p _i}

=

pf{\overrightarrow p _f}

\Rightarrow (2m)

(3i^+j^)\left( {\sqrt 3 \widehat i + \widehat j} \right)

+ 0 = 2m

(i^+3j^)\left( {\widehat i + \sqrt 3 \widehat j} \right)

+ m

V2{\overrightarrow V _2}

\Rightarrow

V2{\overrightarrow V _2}

= 2

(3i^+j^)\left( {\sqrt 3 \widehat i + \widehat j} \right)

- 2

(i^+3j^)\left( {\widehat i + \sqrt 3 \widehat j} \right)

\Rightarrow

V2{\overrightarrow V _2}

=

(232)i^j^(232)\left( {2\sqrt 3 - 2} \right)\widehat i - \widehat j\left( {2\sqrt 3 - 2} \right)

=

2(31)(i^j^)2\left( {\sqrt 3 - 1} \right)\left( {\widehat i - \widehat j} \right)

Also given after collision

V1=(i^+3j^)ms1\overrightarrow {{V_1}} = \left( {\widehat i + \sqrt3\widehat j} \right)m{s^{ - 1}}

For angle between

V1{\overrightarrow V _1}

&

V2{\overrightarrow V _2}

, cos θ\theta =

V1.V2V1V2{{{{\overrightarrow V }_1}.{{\overrightarrow V }_2}} \over {\left| {{{\overrightarrow V }_1}} \right|\left| {{{\overrightarrow V }_2}} \right|}}

=

2(31)×12(31)×32×22(31){{2\left( {\sqrt 3 - 1} \right) \times 1 - 2\left( {\sqrt 3 - 1} \right) \times \sqrt 3 } \over {2 \times 2\sqrt 2 \left( {\sqrt 3 - 1} \right)}}

=

2(31)(13)2×22(31){{2\left( {\sqrt 3 - 1} \right)\left( {1 - \sqrt 3 } \right)} \over {2 \times 2\sqrt 2 \left( {\sqrt 3 - 1} \right)}}

=

(13)22{{\left( {1 - \sqrt 3 } \right)} \over {2\sqrt 2 }}

\Rightarrow θ\theta = 105o

Q6
If 1022 gas molecules each of mass 10–26 kg collide with a surface (perpendicular to it) elastically per second over an area 1 m2 with a speed 104 m/s, the pressure exerted by the gas molecules will be of the order of :
A 108 N/m2
B 1016 N/m2
C 104 N/m2
D 2 N/m2
Correct Answer
Option D
Solution

Momentum imparted to the surface in one collision,

Δp=(pipf)=mv(mv)=2mv\Delta p = ({p_i} - {p_f}) = mv - ( - mv) = 2mv

..... (i) Force on the surface due to n collision per second,

F=nt(Δp)=nΔpF = {n \over t}(\Delta p) = n\Delta p

(\because

t=1st = 1s

) = 2 mnv [from Eq. (i)] So, pressure on the surface,

p=FA=2mnvAp = {F \over A} = {{2mnv} \over A}

Here, m = 10-26 kg, n = 1022 s-1, v = 104 ms-1, A = 1 m2 \therefore Pressure,

p=2×1026×1022×1041=2p = {{2 \times {{10}^{ - 26}} \times {{10}^{22}} \times {{10}^4}} \over 1} = 2

N/m2 So, pressure exerted is of order of 100.

Q7
A man (mass = 50 kg) and his son (mass = 20 kg) are standing on a frictionless surface facing each other. The man pushes his son so that he starts moving at a speed of 0.70 ms–1 with respect to the man. The speed of the man with respect to the surface is :
A 0.28 ms–1
B 0.47 ms–1
C 0.20 ms–1
D 0.14 ms–1
Correct Answer
Option C
Solution

50 V1 = 20 V2 V1 + V2 = 0.70 V1 = 0.20

Q8
Two blocks of masses 10 kg and 30 kg are placed on the same straight line with coordinates (0, 0) cm and (x, 0) cm respectively. The block of 10 kg is moved on the same line through a distance of 6 cm towards the other block. The distance through which the block of 30 kg must be moved to keep the position of centre of mass of the system unchanged is :
A 4 cm towards the 10 kg block
B 2 cm away from the 10 kg block
C 2 cm towards the 10 kg block
D 4 cm away from the 10 kg block
Correct Answer
Option C
Solution

For COM to remain unchanged, m1x1 = m2x2 \Rightarrow 10 ×\times 6 = 30 ×\times x2 \Rightarrow x2 = 2 cm towards 10 kg block.

Q9
If the Kinetic energy of a moving body becomes four times its initial Kinetic energy, then the percentage change in its momentum will be :
A 100%
B 200%
C 300%
D 400%
Correct Answer
Option A
Solution

K2 = 4K1

12{1 \over 2}

mv

22_2^2

= 4

12{1 \over 2}

mv

12_1^2

v2 = 2v1 P = mv P2 = mv2 = 2mv1 P1 = mv1 % change =

ΔPP1×100=2mv1mv1mv1×100=100%{{\Delta P} \over {{P_1}}} \times 100 = {{2m{v_1} - m{v_1}} \over {m{v_1}}} \times 100 = 100\%
Q10
Two billiard balls of mass 0.05 kg each moving in opposite directions with 10 ms-1 collide and rebound with the same speed. If the time duration of contact is t = 0.005 s, then what is the force exerted on the ball due to each other?
A 100 N
B 200 N
C 300 N
D 400 N
Correct Answer
Option B
Solution

Change in momentum of one ball = 2 ×\times (0.05)(10) kg m/s = 1 kg m/s

Favg=1Δt=10.005\Rightarrow {F_{avg}} = {1 \over {\Delta t}} = {1 \over {0.005}}

N = 200 N

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