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for spheres each of mass m and radius r are placed
Question:
For spheres each of mass
M
M
M
and radius
R
R
R
are placed with their centres on the four comers
A
,
B
,
C
A, B, C
A
,
B
,
C
and
D
D
D
of a square of side
b
b
b
. The spheres
A
A
A
and
B
B
B
are hollow and
C
C
C
and
D
D
D
are solids. The moment of inertia of the system about side
A
D
AD
A
D
of square is
JKCET - 2005
JKCET
Updated On:
Jun 2, 2024
8
3
M
R
2
+
2
M
b
2
\frac{8}{3}MR^{2}+2Mb^{2}
3
8
M
R
2
+
2
M
b
2
8
5
M
R
2
+
2
M
b
2
\frac{8}{5}MR^{2}+2Mb^{2}
5
8
M
R
2
+
2
M
b
2
32
15
M
R
2
+
2
M
b
2
\frac{32}{15}MR^{2}+2Mb^{2}
15
32
M
R
2
+
2
M
b
2
32
M
R
2
+
4
M
b
2
32MR^{2}+4Mb^{2}
32
M
R
2
+
4
M
b
2
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The Correct Option is
C
Solution and Explanation
Moment of inertia of a hollow sphere of radius
R
R
R
about the diameter passing through
D
D
D
is
I
A
=
2
3
M
R
2
…
(
i
)
I_{A}=\frac{2}{3} M R^{2} \ldots(i)
I
A
=
3
2
M
R
2
…
(
i
)
Moment of inertia of sol id sphere about diameter
I
B
=
2
5
M
R
2
…
(
i
i
)
I_{B}=\frac{2}{5} M R^{2} \ldots(i i)
I
B
=
5
2
M
R
2
…
(
ii
)
∴
\therefore
∴
Moment of inertia of whole system about side
A
D
=
I
A
+
I
D
+
I
B
+
I
C
A D=I_{A}+I_{D}+I_{B}+I_{C}
A
D
=
I
A
+
I
D
+
I
B
+
I
C
=
2
3
M
R
2
+
2
5
M
R
2
+
(
M
b
2
+
2
3
M
R
2
)
+
(
M
b
2
+
2
5
M
R
2
)
=\frac{2}{3} M R^{2}+\frac{2}{5} M R^{2}+\left(M b^{2}+\frac{2}{3} M R^{2}\right)+\left(M b^{2}+\frac{2}{5} M R^{2}\right)
=
3
2
M
R
2
+
5
2
M
R
2
+
(
M
b
2
+
3
2
M
R
2
)
+
(
M
b
2
+
5
2
M
R
2
)
=
32
15
M
R
2
+
2
M
b
2
=\frac{32}{15} M R^{2}+2 M b^{2}
=
15
32
M
R
2
+
2
M
b
2
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Concepts Used:
System of Particles and Rotational Motion
The system of particles refers to the extended body which is considered a
rigid body
most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.