2016: Problem 24

Topic: Rigid Bodies
Concepts: Moments of inertia, Parallel-axis theorem


Solution:

We are given that the moment of inertia I1I_1 of an equilateral triangle (axis through side) is

I1=18ma2I_1=\frac{1}{8}ma^2

Let’s first find the moment of inertia I2I_2 of an equilateral triangle (axis through vertex). We use the parallel axis theorem:

I1=ICM+m(a36)2=ICM+ma212I_1=I_{\text{CM}}+m\left(\frac{a\sqrt{3}}{6}\right)^2=I_{\text{CM}}+\frac{ma^2}{12}
I2=ICM+m(a33)2=ICM+ma23I_2=I_{\text{CM}}+m\left(\frac{a\sqrt{3}}{3}\right)^2=I_{\text{CM}}+\frac{ma^2}{3}

Subtracting these two equations,

I2I1=ma2(13112)=ma24I_2-I_1=ma^2\left(\frac{1}{3}-\frac{1}{12}\right)=\frac{ma^2}{4}
I2=I1+14ma2=(18+14)ma2=38ma2I_2=I_1+\frac{1}{4}ma^2=\left(\frac{1}{8}+\frac{1}{4}\right)ma^2=\frac{3}{8}ma^2

The hexagon can be broken down into 6 smaller equilateral triangles. Thus, the moment of inertia about an axis through opposite vertices of a hexagon is equivalent to the moment of inertia of 4 triangles (axis through side) and 2 triangles (axis through vertex). If mm is the mass of the hexagon, then each triangle has mass m/6m/6 so

Ihex=4(I16)+2(I26)=23(18ma2)+13(38ma2)=524ma2I_{\text{hex}}=4\left(\frac{I_1}{6}\right)+2\left(\frac{I_2}{6}\right)=\frac{2}{3}\left(\frac{1}{8}ma^2\right)+\frac{1}{3}\left(\frac{3}{8}ma^2\right)=\frac{5}{24}ma^2

Hence, the answer is B.

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