Centroid locus

Geometry Level 5

Let C \mathscr{C} be a fixed circle with radius 4 4 , and A A a fixed point on its circumference.

Consider the set of all triangles Δ \Delta satisfying

  • A A is one of the vertices of Δ \Delta
  • C \mathscr{C} is the circumcircle of Δ \Delta
  • the inradius of Δ \Delta is 1 1

An example of one such triangle is below:

Find the locus L \mathscr{L} of the centroids of all such triangles.

What is the length of L \mathscr{L} ?

Bonus: find an equation for L \mathscr{L} , and a "nice" expression for its length

Bonus bonus: does this curve have a name?


Inspiration 1

Inspiration 2

(among others)


The answer is 15.55673.

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1 solution

Chris Lewis
Mar 5, 2021

As I did this numerically, this is just a sketch solution. First of all, here's a picture of the locus:

Some notation: O ( 0 , 0 ) O(0,0) is the circumcentre; I I is the incentre; d = O I d=OI is the distance between them; G G is the centroid; R = 4 R=4 and r = 1 r=1 are the circumradius and inradius. Let A ( R , 0 ) A(R,0) be the fixed vertex.

By Euler's theorem, O I 2 = R 2 2 R r OI^2=R^2-2Rr so d d is fixed and I I lies on a circle of radius d d centred at O O . So we can parameterise the point I I (and hence the triangles) by saying I ( d cos ( q ) , d sin ( q ) ) I(d \cos(q),d \sin(q)) .

The aim is to calculate the coordinates of B B and C C in terms of q q , so that we can find G G .

Since we can now work out A I AI , we also get B A C = 2 sin 1 r A I \angle BAC=2\sin^{-1} \frac{r}{AI} .

This is in fact enough; we know the gradient of the line A B AB , and that it goes through point A A ; since O B = R OB=R we can work out the coordinates of B B (and likewise C C ) from this.

By tabulating the position of G G for a high resolution of q q values, we can work out the path length to be approximately 15.55673 \boxed{15.55673\ldots} .


This is messy, and (to me) quite unsatisfactory. For a deeper dive into this, we can use some other triangle formulas to find G G .

We have G O 2 = 1 9 ( R 2 a 2 b 2 c 2 ) GO^2 = \frac19 \left(R^2-a^2-b^2-c^2 \right) and G A 2 = 1 9 ( 2 b 2 + 2 c 2 a 2 ) GA^2 = \frac19 \left(2b^2+2c^2-a^2 \right) , where a a is as usual the length of the side opposite A A , etc. We'll also use A A to denote the angle B A C \angle BAC . Note that these are symmetric in lengths b b and c c - this is to be expected from the way they're defined.

By the extended sine rule, a = 2 R sin A a=2R \sin A .

Now consider the triangle B I C BIC . By definition of the incentre, the altitude from I I has length r r . Also it's easy to show that B I C = A + π 2 \angle BIC = \frac{A+\pi}{2} . Using the fact the incentre lies on the angle bisectors, I B C = B 2 \angle IBC=\frac{B}{2} .

Combining all of this, B C = a = 2 R sin A = r ( cot B 2 + cot C 2 ) = r ( cot B 2 + tan A + B 2 ) BC=a=2R\sin A=r\left(\cot \frac{B}{2}+\cot \frac{C}{2}\right)=r\left(\cot \frac{B}{2}+\tan \frac{A+B}{2}\right)

This can be written as a quadratic in cot B 2 \cot\frac{B}{2} .

Ultimately, we can get expressions for b + c b+c and b c bc , and from these work out b 2 + c 2 b^2+c^2 to get G O GO and G A GA . This gives a slightly neater way to work out the position of G G ; but the expressions don't reduce very nicely. I'll post what I've found if anyone's interested, but I'd be really keen to see a less numerical solution.

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