The moment of inertia of a cube of mass \( m \) and side \( a \) about one of its edges is equal to:
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For any solid body, the moment of inertia about an edge can be found using the parallel axis theorem:
\[
I = I_C + m d^2
\]
where \( d \) is the perpendicular distance from the center to the edge.
Step 1: {Apply the perpendicular axis theorem} By the theorem of perpendicular axes, the moment of inertia about an edge is calculated as:\[I = I_C + m \left( \frac{a}{\sqrt{2}} \right)^2\]Step 2: {Moment of inertia of cube about its center} The moment of inertia of a cube about its central axis is given by:\[I_C = \frac{ma^2}{12} + \frac{ma^2}{12} = \frac{ma^2}{6}\]Step 3: {Adding the parallel axis contribution} \[I = \left[ \frac{ma^2}{12} + \frac{ma^2}{12} \right] + \frac{ma^2}{2}\]\[= \frac{2}{3} ma^2\]The final result is \( \frac{2}{3} ma^2 \).