The Calculus of Explanations

Putting the fun in functionals


Moments of Inertia – Part V

A slightly impractical but fascinating use of the self-similarity method is finding the Moment of Inertia of certain famous fractals.

Example – The Sierpiński Triangle

Consider that the Sierpiński triangle of mass M and side length L is comprised of three smaller copies of itself.

The Sierpiński triangle, formed from iteratively removing the middle third of equilateral triangles.

If the triangle is being rotated about its centre, we simply need to calculate d between to the centre of one of the smaller constituent triangle.

So

I = 3I_{\text{small}}.

Using the Parallel Axis Theorem,

I_{\text{small}} = I_{\text{COM}} + \displaystyle \frac{M}{3} d^2,

where

I_{\text{COM}} = \gamma \displaystyle \frac{M}{3} \left(\frac{L}{2}\right)^2 = \frac{I}{12},

the contribution of each small triangle is the moment of inertia through its centre of mass (COM) plus its mass multiplied by the distance to the axis of rotation squared. This distance is d = L/2\sqrt{3}, so we find that

I = 3\left( \displaystyle \frac{I}{12} +  \displaystyle \frac{ML^2}{36} \right),

With which we reach the final result

\boxed{I = \displaystyle \frac{ML^2}{9}}

Note that the moment of inertia is larger than the MOI of an equilateral triangle with equivalent mass, which was ML^2/12, since in the fractal more of the mass is distributed far away from the axis of rotation!



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