33 Years NEET-AIPMT Chapterwise Solutions - Physics 2020
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Telegram @unacademyplusdiscounts54 NEET-AIPMT Chapterwise Topicwise Solutions Physics53. The ratio of the radii of gyration of a circular discabout a tangential axis in the plane of the disc and ofa circular ring of the same radius and mass about atangential axis in the plane of the ring is(a) 2 : 3 (b) 2 : 1(c) 5: 6 (d) 1: 2 (2004)54. The moment of inertia of a disc of mass M and radius Rabout an axis, which is tangential to the circumferenceof the disc and parallel to its diameter is5 2(a) MR (b) 2 2MR433(c) 2MR (d) 4 2MR (1999)2555. Moment of inertia of a uniform circular disc abouta diameter is I. Its moment of inertia about an axisperpendicular to its plane and passing through apoint on its rim will be(a) 5I (b) 3I (c) 6I (d) 4I (1990)7.11 Kinematics of Rotational Motion abouta Fixed Axis56. A wheel has angular acceleration of 3.0 rad/sec 2 andan initial angular speed of 2.00 rad/sec. In a time of2 sec it has rotated through an angle (in radians) of(a) 10 (b) 12 (c) 4 (d) 6 (2007)7.12 Dynamics of Rotational Motion about aFixed Axis57. A solid cylinder of mass 2 kg and radius 4 cmis rotating about its axis at the rate of 3 rpm. Thetorque required to stop it after 2p revolutions is(a) 2 × 10 6 N m(c) 2 × 10 –3 N m(b) 2 × 10 –6 N m(d) 12 × 10 –4 N m(NEET 2019)58. Three objects, A : (a solid sphere), B : (a thin circulardisk) and C : (a circular ring), each have the samemass M and radius R. They all spin with the sameangular speed w about their own symmetry axes.The amounts of work (W) required to bring them torest, would satisfy the relation(a) W C > W B > W A(c) W B > W A > W C(b) W A > W B > W C(d) W A > W C > W B(NEET 2018)59. A rope is wound around a hollow cylinder of mass3 kg and radius 40 cm. What is the angularacceleration of the cylinder if the rope is pulled witha force of 30 N?(a) 0.25 rad s –2 (b) 25 rad s –2(c) 5 m s –2 (d) 25 m s –2 (NEET 2017)60. A uniform circular disc of radius 50 cm at rest is freeto turn about an axis which is perpendicular to itsplane and passes through its centre. It is subjectedto a torque which produces a constant angularacceleration of 2.0 rad s –2 . Its net acceleration inm s –2 at the end of 2.0 s is approximately(a) 6.0 (b) 3.0 (c) 8.0 (d) 7.0(NEET-I 2016)61. Point masses m 1 and m 2are placed at the oppositeends of a rigid rod oflength L, and negligiblePmass. The rod is to beset rotating about an axisperpendicular to it.The position of point P on this rod through whichthe axis should pass so that the work required to setthe rod rotating with angular velocity w 0 is minimum,is given bym(a) x = 2 m LmL 2(b) x =1m1+m2mL 1(c) x =(d) xm1+m= m 12m L (2015)262. An automobile moves on a road with a speed of54 km h –1 . The radius of its wheels is 0.45 m andthe moment of inertia of the wheel about its axis ofrotation is 3 kg m 2 . If the vehicle is brought to rest in15 s, the magnitude of average torque transmitted byits brakes to the wheel is(a) 10.86 kg m 2 s –2 (b) 2.86 kg m 2 s –2(c) 6.66 kg m 2 s –2 (d) 8.58 kg m 2 s –2 (2015)63. A solid cylinder of mass 50 kg and radius 0.5 m is freeto rotate about the horizontal axis. A massless stringis wound round the cylinder with one end attachedto it and other hanging freely. Tension in the stringrequired to produce an angular acceleration of2 revolutions s –2 is(a) 25 N(b) 50 N(c) 78.5 N (d) 157 N (2014)64. A rod PQ of mass M and length L is hinged at end P.The rod is kept horizontal by a massless string tiedto point Q as shown in figure. When string is cut, theinitial angular acceleration of the rod is(a)2gL(b) 2 g2L(c)3g2L(d)gL(NEET 2013)65. The instantaneous angular position of a point on arotating wheel is given by the equation q(t) = 2t 3 – 6t 2 .The torque on the wheel becomes zero at(a) t = 1 s(b) t = 0.5 s(c) t = 0.25 s (d) t = 2 s (2011)66. A uniform rod AB of length l and mass m is free torotate about point A. The rod is released from rest inthe horizontal position. Given that the moment ofinertia of the rod about A is ml 2 /3, the initial angularacceleration of the rod will be
Telegram @unacademyplusdiscountsSystems of Particles and Rotational Motion55(a)mgl2 (b) 3 2 gl3g(c)(d) 2 g (2007, 2006)2l3l67. A wheel having moment of inertia 2 kg m 2 about itsvertical axis, rotates at the rate of 60 rpm about thisaxis. The torque which can stop the wheel’s rotationin one minute would be(a) 2 π πN m (b)1512 N mπ(c)15 N m π(d)18 N m (2004)68. The moment of inertia of a body about a given axisis 1.2 kg m 2 . Initially, the body is at rest. In orderto produce a rotational kinetic energy of 1500 joule,an angular acceleration of 25 radian/sec 2 must beapplied about that axis for a duration of(a) 4 s (b) 2 s (c) 8 s (d) 10 s (1990)7.13 Angular Momentum in case of Rotationabout a Fixed Axis69. A solid sphere is rotating freely about its symmetryaxis in free space. The radius of the sphere isincreased keeping its mass same. Which of thefollowing physical quantities would remain constantfor the sphere?(a) Angular velocity. (b) Moment of inertia.(c) Rotational kinetic energy.(d) Angular momentum. (NEET 2018)70. Two discs of same moment of inertia rotatingabout their regular axis passing through centreand perpendicular to the plane of disc has angularvelocities w 1 and w 2 . They are brought into contactface to face coinciding the axis of rotation. Theexpression for loss of energy during this process is1(a) I ( ω1 − ω2)2 (b) I (w 1 – w 2 ) 241(c) I ( ω1 − ω2)2 (d) 1 I ( ω1 + ω2)282(NEET 2017)71. Two rotating bodies A and B of masses m and 2mwith moments of inertia I A and I B (I B > I A ) haveequal kinetic energy of rotation. If L A and L B be theirangular momenta respectively, thenL(a)BL = (b) L A = 2L B2A(c) L B > L A (d) L A > L B (NEET-II 2016)72. Two discs are rotating about their axes, normal tothe discs and passing through the centres of thediscs. Disc D 1 has 2 kg mass and 0.2 m radius andinitial angular velocity of 50 rad s –1 . Disc D 2 has4 kg mass, 0.1 m radius and initial angular velocity of200 rad s –1 . The two discs are brought in contact faceto face, with their axes of rotation coincident. Thefinal angular velocity (in rad s –1 ) of the system is(a) 60 (b) 100 (c) 120 (d) 40(Karnataka NEET 2013)73. A circular platform is mounted on a frictionlessvertical axle. Its radius R = 2 m and its moment ofinertia about the axle is 200 kg m 2 . It is initially atrest. A 50 kg man stands on the edge of the platformand begins to walk along the edge at the speed of1 m s –1 relative to the ground. Time taken by theman to complete one revolution is(a) p s(b) 3p/2 s(c) 2p s (d) p/2 s (Mains 2012)74. A circular disk of moment of inertia I t is rotating ina horizontal plane, about its symmetry axis, with aconstant angular speed w i . Another disk of momentof inertia I b is dropped coaxially onto the rotatingdisk. Initially the second disk has zero angular speed.Eventually both the disks rotate with a constantangular speed w f . The energy lost by the initiallyrotating disc to friction is(a) 1 2Ib2ω i (b) 1 2It2ω2 ( I + I )i2 ( I + I )(c)tbIb− Iti( It+ Ib) ω2 (d) 1 IbIt2ω i2 ( It+ Ib)(2010)75. A thin circular ring of mass M and radius r isrotating about its axis with constant angular velocityw. Two objects each of mass m are attached gently tothe opposite ends of a diameter of the ring. The ringnow rotates with angular velocity given by(a) ( M + 2 m)ω2m(c) ( M + 2 m)ωM(b)(d)tb2MωM + 2mMωM + 2m(Mains 2010, 1998)76. A round disc of moment of inertia I 2 about its axisperpendicular to its plane and passing through itscentre is placed over another disc of moment ofinertia I 1 rotating with an angular velocity w aboutthe same axis. The final angular velocity of thecombination of discs isI2ω(a)(b) wI + I(c)1 2I1ωI1+I2(d) ( I 1+ I 2 ) ωI1(2004)
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Systems of Particles and Rotational Motion
55
(a)
mgl
2
(b) 3 2 gl
3g
(c)
(d) 2 g
(2007, 2006)
2l
3l
67. A wheel having moment of inertia 2 kg m 2 about its
vertical axis, rotates at the rate of 60 rpm about this
axis. The torque which can stop the wheel’s rotation
in one minute would be
(a) 2 π π
N m (b)
15
12 N m
π
(c)
15 N m π
(d)
18 N m (2004)
68. The moment of inertia of a body about a given axis
is 1.2 kg m 2 . Initially, the body is at rest. In order
to produce a rotational kinetic energy of 1500 joule,
an angular acceleration of 25 radian/sec 2 must be
applied about that axis for a duration of
(a) 4 s (b) 2 s (c) 8 s (d) 10 s (1990)
7.13 Angular Momentum in case of Rotation
about a Fixed Axis
69. A solid sphere is rotating freely about its symmetry
axis in free space. The radius of the sphere is
increased keeping its mass same. Which of the
following physical quantities would remain constant
for the sphere?
(a) Angular velocity. (b) Moment of inertia.
(c) Rotational kinetic energy.
(d) Angular momentum. (NEET 2018)
70. Two discs of same moment of inertia rotating
about their regular axis passing through centre
and perpendicular to the plane of disc has angular
velocities w 1 and w 2 . They are brought into contact
face to face coinciding the axis of rotation. The
expression for loss of energy during this process is
1
(a) I ( ω1 − ω2)
2 (b) I (w 1 – w 2 ) 2
4
1
(c) I ( ω1 − ω2)
2 (d) 1 I ( ω1 + ω2)
2
8
2
(NEET 2017)
71. Two rotating bodies A and B of masses m and 2m
with moments of inertia I A and I B (I B > I A ) have
equal kinetic energy of rotation. If L A and L B be their
angular momenta respectively, then
L
(a)
B
L = (b) L A = 2L B
2
A
(c) L B > L A (d) L A > L B (NEET-II 2016)
72. Two discs are rotating about their axes, normal to
the discs and passing through the centres of the
discs. Disc D 1 has 2 kg mass and 0.2 m radius and
initial angular velocity of 50 rad s –1 . Disc D 2 has
4 kg mass, 0.1 m radius and initial angular velocity of
200 rad s –1 . The two discs are brought in contact face
to face, with their axes of rotation coincident. The
final angular velocity (in rad s –1 ) of the system is
(a) 60 (b) 100 (c) 120 (d) 40
(Karnataka NEET 2013)
73. A circular platform is mounted on a frictionless
vertical axle. Its radius R = 2 m and its moment of
inertia about the axle is 200 kg m 2 . It is initially at
rest. A 50 kg man stands on the edge of the platform
and begins to walk along the edge at the speed of
1 m s –1 relative to the ground. Time taken by the
man to complete one revolution is
(a) p s
(b) 3p/2 s
(c) 2p s (d) p/2 s (Mains 2012)
74. A circular disk of moment of inertia I t is rotating in
a horizontal plane, about its symmetry axis, with a
constant angular speed w i . Another disk of moment
of inertia I b is dropped coaxially onto the rotating
disk. Initially the second disk has zero angular speed.
Eventually both the disks rotate with a constant
angular speed w f . The energy lost by the initially
rotating disc to friction is
(a) 1 2
Ib
2
ω i (b) 1 2
It
2
ω
2 ( I + I )
i
2 ( I + I )
(c)
t
b
Ib
− It
i
( It
+ Ib) ω2 (d) 1 IbIt
2
ω i
2 ( It
+ Ib)
(2010)
75. A thin circular ring of mass M and radius r is
rotating about its axis with constant angular velocity
w. Two objects each of mass m are attached gently to
the opposite ends of a diameter of the ring. The ring
now rotates with angular velocity given by
(a) ( M + 2 m)
ω
2m
(c) ( M + 2 m)
ω
M
(b)
(d)
t
b
2Mω
M + 2m
Mω
M + 2m
(Mains 2010, 1998)
76. A round disc of moment of inertia I 2 about its axis
perpendicular to its plane and passing through its
centre is placed over another disc of moment of
inertia I 1 rotating with an angular velocity w about
the same axis. The final angular velocity of the
combination of discs is
I2ω
(a)
(b) w
I + I
(c)
1 2
I1ω
I1+
I2
(d) ( I 1+ I 2 ) ω
I1
(2004)