1. Two blocks with masses M and m are in contact with each other and are resting on a horizontal friction-less floor. When horizontal force is applied to the heavier, the blocks accelerate to the right. The force between the two blocks is
A. (M + m) F/m
B. MF/m
C. mF/M
D. mF/(M + m)
Answer - Option D
Explanation -
From free body diagram
F – N = Ma ...(i)
or N = ma ...(ii)
From equations (i) and (ii), we get
N = [latex]\frac{mF}{(m + M)}[/latex]
2. The combined motion of rotation and translation may be assumed to be a motion of pure rotation about some centre which goes on changing from time to time. The centre in question is known as
A. Shear centre
B. Meta centre
C. Instantaneous centre
D. Gravitational centre
Answer - Option C
Explanation -
The instantaneous centre of a link is the point about which all the points on the link appear to rotate at that instant.
3. Two bodies of mass [latex]{m}_{1}[/latex] and [latex]{m}_{2}[/latex] are dropped from different heights [latex]{h}_{1}[/latex] and [latex]{h}_{2}[/latex] respectively. Neglecting the effect of friction, the ratio of times taken to drop through the given heights would be
A. [latex]\frac{{m}_{1}}{{m}_{2}}[/latex]
B. [latex]\frac{{m}_{1}{h}_{1}}{{m}_{2}{h}_{2}}[/latex]
C. [latex]{(\frac{{h}_{1}}{{h}_{2}})}^{\frac{1}{2}}[/latex]
D. [latex]{(\frac{{h}_{1}}{{h}_{2}})}^{2}[/latex]
Answer - Option C
Explanation -
s = ut + [latex]\frac{1}{2}g {t}^{2}[/latex]
and u = 0
i.e, [latex]{h}_{1} = \frac{1}{2}g {{t}_{1}}^{2}[/latex], and [latex]{h}_{2} = \frac{1}{2}g {{t}_{2}}^{2}[/latex]
Hence [latex]\frac{{t}_{1}}{{t}_{2}} = {(\frac{{h}_{1}}{{h}_{2}})}^{\frac{1}{2}}[/latex]
4. A block slides down a smooth inclined plane in time t after having been released from its top. An identical block on being released from the same point and falling freely will reach the ground in time
A. [latex]\frac{t}{3}[/latex]
B. [latex]\frac{t}{\sqrt{3}}[/latex]
C. [latex]\frac{t}{2}[/latex]
D. [latex]\frac{t}{4}[/latex]
(Take inclination of plane = 30º)
Answer - Option C
Explanation -
For motion along the plane
a = g sin θ and l = [latex]\frac{h}{sinθ}[/latex]
i.e, [latex]\frac{h}{sin θ} = \frac{1}{2} (g sin θ){t}^{2}[/latex]
or [latex]{t}^{2} = \frac{2h}{g} \frac{1}{{sin}^{2}}θ[/latex] ......(i)
For vertical motion :
h = [latex] \frac{1}{2} g{T}^{2}[/latex]
[latex]{T}^{2} = \frac{2h}{g}[/latex] ......(ii)
From equations (i) and (ii), we get
T = t sin θ = t sin 30º = [latex] \frac{t}{2}[/latex]
5. AB is the vertical diameter of a circle in a vertical plane. Another diameter CD makes an angle of 60º with AB. Then the ratio of time taken by a particle to slide along AB to the time taken by it to slide along CD is
A. 1 : [latex]\sqrt{3} [/latex]
B. [latex]\sqrt{2}[/latex] : 1
C. 1 : [latex]\sqrt{2} [/latex]
D. [latex]\sqrt{3}[/latex] : [latex]\sqrt{2}[/latex]
Answer - Option C
Explanation -
For motion along the vertical diameter AB
s = d (diameter of circle) and a = g
i.e, d = [latex] \frac{1}{2} g{T}^{2}[/latex]
[latex]{t}^{2} = \frac{2d}{g}[/latex] ......(i)
For motion along the inclined diameter CD,
s = d
and a = g cos 60º = [latex]\frac{g}{2}[/latex]
i.e, d = [latex]\frac{1}{2} *\frac{g}{2} * {T}^{2}[/latex]
or [latex]{T}^{2} = \frac{4d}{g}[/latex] ......(ii)
From equations (i) and (ii) we get
[latex]\frac{t}{T} = \frac{1}{\sqrt{2}}[/latex]
6. Which of the following graphs represents the motion of an objects moving with a linearly increasing acceleration against time ?
Answer - Option B
Explanation -
The acceleration which varies linearly with time
can be expressed as
a = [latex]\frac{dv}{dt}[/latex]= [latex]{a}_{0}[/latex]+ kt
Hence no curve shows with acceleration versus time,
v = [latex]{v}_{0}{a}_{0}t + \frac{k{t}^{2}}{2} [/latex]
Curves (a), (d) are drawn with velocity against time. None of them satisfies the above relations.
However, s = [latex]{s}_{0} + {v}_{0}{a}_{0}t + \frac{{a}_{0}{t}^{2}}{2} + \frac{k{t}^{3}}{6}[/latex]
(B) satisfies this relation
7. Two particles with masses in the ratio 1 : 4 are moving with equal kinetic energies. The magnitude of their linear momentums wil l
conform to the ratio
A. 1 : 8
B. 1 : 2
C. [latex]\sqrt{2}[/latex] : 1
D. [latex]\sqrt{2}[/latex]
Answer - Option B
Explanation -
[latex]{(KE)}_{1} = \frac{1}{2} {m}_{1} {{v}_{1}}^{2}[/latex]
[latex]{(KE)}_{1} = \frac{1}{2} {m}_{1} {{v}_{2}}^{2}[/latex]
But kinetic energies are equal and [latex] \frac{{m}_{1}}{{m}_{2}} = \frac{1}{4}[/latex]
Now, [latex]{m}_{1} {{v}_{1}}^{2} = {m}_{2} {{v}_{1}}^{2} [/latex]
[latex] \frac{{v}_{1}}{{v}_{2}} = {(\frac{{m}_{1}}{{m}_{2}})}^{\frac{1}{2}} = 2[/latex]
Required ratio = [latex] \frac{{v}_{1}}{{v}_{2}}\frac{{m}_{1}}{{m}_{2}} = \frac{{v}_{1}}{{v}_{2}} * \frac{{m}_{1}}{{m}_{2}}[/latex]
[latex]\frac{1}{4} * 2 = 1 : 2[/latex]
8. If two bodies one light and other heavy have equal kinetic energies, which one has a greater momentum?
A. Heavy body
B. Light body
C. Both have equal momentum
D. It depends on the actual velocities.
Answer - Option B
Explanation -
Let light body be L and heavy body H
[latex]i.e, \frac{1}{2} {m}_{L} {{v}_{L}}^{2} = \frac{1}{2} {m}_{H} {{v}_{H}}^{2}[/latex]
or [latex] \frac{{m}_{L}}{{m}_{H}} = {\frac{{v}_{H}}{{v}_{L}}}^{2} < 1[/latex]
[latex] \frac{Momentum of light body}{Momentum of heavy body} = \frac{{m}_{L}}{{m}_{H}} \frac{{v}_{H}}{{v}_{L}} = \frac{{v}_{H}}{{v}_{L}}[/latex]
[latex] {\frac{{v}_{H}}{{v}_{L}}}^{2} = \frac{{v}_{H}}{{v}_{L}} < 1[/latex]
Hence momentum of light body is less than the momentum of heavy body or heavier body has greater momentum as compared to lighter body
9. The angular momentum of a system is conserved if there
A. are no forces present
B. are no magnetic forces present
C. is no net force on the system
D. are no torques present
Answer - Option D
Explanation -
Net torque on a system , [latex]\overrightarrow{{r}_{n}}[/latex] = time rate of change of the system’s angular momentum,
i.e.[latex]\overrightarrow{\frac{dl}{dt}}[/latex]
At constant [latex]\overrightarrow{L}[/latex], therefore, [latex]\overrightarrow{{r}_{n}}[/latex] = 0.
10. A body moves along a straight line and the variation of its kinetic energy with time is linear as depicted in the figure below
The force acting on the body is
A. directly proportional to velocity
B. inversely proportional to velocity
C. zero
D. constant
Answer - Option B
Explanation -
Kinetic energy = [latex]\frac{1}{2} m {(\frac{dx}{dt})}^{2} = kt[/latex]
where k is constant
Differentiating, we get
[latex]m \frac{dx}{dt} ({\frac{dx}{dt}}^{2}) = k[/latex]
Force = mass * acceleration
[latex]m {(\frac{dx}{dt})}^{2} = kt (\frac{dx}{dt}) = \frac{k}{v}[/latex]
11. For perfectly elastic bodies, the value of coefficient of restitution is
A. 1
B. 0.5 to 1
C. 0 to 0.5
D. zero
Answer - Option A
Explanation -
Value of coefficient of restitution is unity, if the collision is elastic, i.e. if no energy is dissipated during collision.
Minimum value of coefficient of restitution would be zero for plastic collision, i.e., if energy gets entirely dissipated.
12. A steel ball is dropped from a height [latex]{h}_{1}[/latex] onto a steel plate and rebounds to a height [latex]{h}_{2}[/latex]. The coefficient of restitution between the ball and plate will be
A. [latex]\frac{{h}_{1}}{{h}_{2}}[/latex]
B. [latex]\frac{{h}_{1}}{2{h}_{2}}[/latex]
C. [latex]\sqrt {\frac{{h}_{1}}{2{h}_{2}}}[/latex]
D. [latex]\sqrt {\frac{{h}_{2}}{{h}_{1}}}[/latex]
Answer - Option D
Explanation -
Velocity of ball just before impact, [latex]{v}_{1} = \sqrt {2g{h}_{1}}[/latex]
Its velocity as it rebound, [latex]{v}_{2} = \sqrt {2g{h}_{2}}[/latex]
By definition,
e = [latex]\frac{{v}_{2} - 0}{0 - {v}_{1}} = \frac {\sqrt {2g{h}_{2}}}{-(-\sqrt {2g{h}_{1}})} = \sqrt {\frac{{h}_{2}}{{h}_{1}}}[/latex]
13. Consider a one-dimensional elastic collision between an incoming body A of mass [latex]{m}_{1}[/latex] and a body B of mass [latex]{m}_{2}[/latex] initially at rest. For body B to move with greatest kinetic energy after collision
A. [latex]{m}_{1} > {m}_{2}[/latex]
B. [latex]{m}_{1} < {m}_{2}[/latex]
C. [latex]{m}_{1} = {m}_{2}[/latex]
D. None of these
Answer - Option A
Explanation -
After elastic collision, the velocity of stationary body,
[latex]{{m}_{2}}^{1} = \frac{2{m}_{1}}{{m}_{1} + {m}_{2}}{v}_{1}[/latex]
Kinetic energy = [latex] \frac{1}{2} {m}_{2}{(\frac{2{m}_{1}}{{m}_{1} + {m}_{2}}{v}_{1})}^{2}[/latex]
= [latex]{{v}_{1}}^{2} \frac{2{{m}_{1}}^{2}{m}_{2}}{{({m}_{1} + {m}_{2})}^{2}}[/latex]
Hence kinetic energy will have the greatest possible value when [latex]{m}_{1} > {m}_{2}[/latex]
14. Distance of the centroid of a semicircle of radius r from its base is
A. [latex]\frac{4r}{3\pi}[/latex]
B. [latex]\frac{3 \pi}{4r}[/latex]
C. [latex]\frac{4 \pi}{3r}[/latex]
D. [latex]\frac{2\pi}{3r}[/latex]
Answer - Option A
Explanation -
Area = [latex]\frac{1}{2}\pi {r}_{2}[/latex]
[latex]{x}_{c} = r, {y}_{c} = \frac{4r}{3\pi}[/latex]
15. For maximum horizontal range, the angle of projection of a projectile should be
A. 30º
B. 45º
C. 60º
D. 90º
Answer - Option B
Explanation -
Horizontal range, R = [latex]\frac{{{v}_{0}}^{2}sin 2 \alpha}{g}[/latex]
For maximum horizontal range,
sin 2[latex]\alpha[/latex] = 1
or 2[latex]\alpha[/latex] = 90º
or [latex]\alpha[/latex] = 45º