Question:

An equilateral triangle $ABC$ is cut from a thin solid sheet of wood. (See figure) $D, \, E$ and $F$ are the mid-points of its sides as shown and $G$ is the centre of the triangle. The moment of inertia of the triangle about an axis passing through $G$ and perpendicular to the plane of the triangle is $I_{0}$ . If the smaller triangle $DEF$ is removed from $ABC,$ the moment of inertia of the remaining figure about the same axis is $I.$ Then:

Updated On: Jul 2, 2022
  • $I=\frac{3}{4}I_{0}$
  • $I=\frac{15}{16}I_{0}$
  • $I=\frac{9}{16}I_{0}$
  • $I=\frac{I_{0}}{4}$
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The Correct Option is B

Solution and Explanation

Dimension analysis $I_{o}=KMa^{2}$ Now for small lamina $I^{'}=K\frac{M}{4}\left(\frac{a}{2}\right)^{2}=\frac{k m a^{2}}{16}$ $I^{'}=\frac{I_{o}}{16}$ So moment of Inertia of remaining part $I_{L}=I_{o}-I^{'}$ $=I_{o}-\frac{I_{o}}{16}$ $I_{L}=\frac{15 I_{o}}{16}$
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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.