Question:

For the given uniform square lamina $ABCD$, whose centre is $O$,

Updated On: Jul 28, 2022
  • $\sqrt 2I_{AC}=I_{EF}$
  • $I_{AD}=3I_{EF}$
  • $I_{AD}=4I_{EF}$
  • $I_{AC}=\sqrt 2I_{EF}$
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The Correct Option is C

Solution and Explanation

Let the each side of square lamina is d. So, $\hspace5mm I_{EF}=I_{GH} \hspace10mm (due \, to \, symmetry) $ and $\hspace5mm I_{AC}=I_{BD} \hspace10mm (due \, to \, symmetry) $ Now, according to theorem of perpendicular axis $\hspace10mm I_{AC}+I_{BD}=I_0$ or $\hspace10mm 2I_{AC}=I_0 \hspace5mm ...(i) $ and $\hspace10mm I_{EF}+I_{GH}=I_0$ or $\hspace10mm 2I_{EF}=I_0 \hspace5mm ...(ii) $ From Eqs. (i) and (ii), we get $I_{AC}=I_{EF}$ $\therefore \hspace5mm I_{AD}=I_{EF}+ \frac {md^2}{4}$ $\hspace5mm =\frac {md^2}{12}+ \frac {md^2}{4} \hspace5mm \bigg (as \, I_{EF}= \frac {md^2}{12}\bigg ) $ So, $\hspace5mm I_{AD}= \frac {md^2}{3}=4I_{EF}$
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Concepts Used:

System of Particles and Rotational Motion

  1. 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.
  2. 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.
  3. The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.