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Question: A circular disc A of radius \(r\) is made from an iron plate of thickness t and another circular dis...

A circular disc A of radius rr is made from an iron plate of thickness t and another circular disc B of radius 4r4r is made from an iron plate of thickness t4\dfrac{t}{4}. The relation between the moments of inertia IA{I_A} and IB{I_B} is:
A. IA>IB{I_A} > {I_B}
B. IA=IB{I_A} = {I_B}
C. IA<IB{I_A} < {I_B}
D. the conditions are insufficient to predict the relation between IA{I_A} and IB{I_B} .

Explanation

Solution

Hint- By finding the value of moment of inertia of disc AA and BB about an axis passing through the centre perpendicular to the plane of the disc and on comparing these values we can arrive at the correct answer.

Complete step by step answer:
It is given that a circular disc A and B are made from an iron plate
Radius of disc A ,
RA=r{R_A} = r
Thickness of disc A,
tA=t{t_A} = t
Disc B has radius
RB=4r{R_B} = 4r
Thickness of disc B is
tB=t4{t_B} = \dfrac{t}{4}
We know that the moment of inertia of disc about an axis passing through the centre and perpendicular to the disc is given as,
I=12MR2I = \dfrac{1}{2}M{R^2}
Where, MM is the mass and RR is the radius,
Now we need to find the mass of disc AA and BB
We know that density is the ratio of mass to volume,
ρ=mV\rho = \dfrac{m}{V}
Where mm is the mass and VV is the volume.
Volume of disc will be area multiplied by thickness.
V=AtV = At
Thus, for disc A
MA=ρ×VA{M_A} = \rho \times {V_A}
MA=ρ×AA×tA\Rightarrow {M_A} = \rho \times {A_A} \times {t_A}
Area is the area of a circle πr2\pi {r^2}. Where, r is the radius.
MA=ρ×πr2×t\Rightarrow {M_A} = \rho \times \pi {r^2} \times t
Similarly, mass of disc B
MB=ρ×VB{M_B} = \rho \times {V_B}
Mb=ρ×AB×tB\Rightarrow {M_b} = \rho \times {A_B} \times {t_B}
MB=ρ×π(4r)2×(t4)\Rightarrow {M_B} = \rho \times \pi {\left( {4r} \right)^2} \times \left( {\dfrac{t}{4}} \right)
MB=ρ×4πr2t\Rightarrow {M_B} = \rho \times 4\pi {r^2}t
Now we can calculate the moment of inertia of disc A
IA=MARA22{I_A} = \dfrac{{{M_A}{R_A}^2}}{2}
On substituting the values, we get
IA=(ρπr2t)×r22\Rightarrow {I_A} = \dfrac{{\left( {\rho \pi {r^2}t} \right) \times {r^2}}}{2}
Moment of inertia of disc BB
IB=MBRB22{I_B} = \dfrac{{{M_B}{R_B}^2}}{2}
On substituting the values we get,
IB=(4ρπr2t)×(4r)22\Rightarrow {I_B} = \dfrac{{\left( {4\rho \pi {r^2}t} \right) \times {{\left( {4r} \right)}^2}}}{2}
IB=64×ρπr2t×r22\Rightarrow {I_B} = \dfrac{{64 \times \rho \pi {r^2}t \times {r^2}}}{2}
Let us divide equation 1 by equation 2. Then we get
IAIB=(ρπr2t)×r2264×ρπr2t×r22\Rightarrow \dfrac{{{I_A}}}{{{I_B}}} = \dfrac{{\dfrac{{\left( {\rho \pi {r^2}t} \right) \times {r^2}}}{2}}}{{\dfrac{{64 \times \rho \pi {r^2}t \times {r^2}}}{2}}}
IAIB=164\Rightarrow \dfrac{{{I_A}}}{{{I_B}}} = \dfrac{1}{{64}}
IB=64IA\Rightarrow {I_B} = 64{I_A}
We can see that moment of inertia of B is 64 times the moment of inertia of A.
Hence IB>IA{I_B} > {I_A}

So the correct answer is option C.

Note: The moment of inertia of the disc varies according to the axis of rotation. The moment of inertia about axis passing through centre and perpendicular to the plane of disc is given as
I=MR2I = \dfrac{{MR}}{2}
Where, MM is the mass and RR is the radius.
If any other axis of rotation is to be taken then the moment of inertia about that axis will be different from this equation.