I have been asked the following question. Take a circle, and three arcs of magnitude $\dfrac{\pi}{3}$ (or you could say the corresponding centered angles are of $60$ degrees) each, that do not intersect with each other, say arc $AB$, arc $CD$ and arc $EF$.
For each of the three remaining arcs take the corresponding chords $BC$, $DE$ and $FA$. Let $M, N, P$ respectively be the middles of these three line segments. Is the triangle $MNP$ equilateral?
The person that asked me this question (a mathematician) did not know if the statement is true. I asked him where did he find it and he told me that his barber asked him. I tried to solve it using Euclidean geometry and I failed. I found a positive solution using trigonometry (I may present it here later). I tried repeatedly to solve it again only using Euclidean geometry and I failed. Any idea? (I mean no analytic geometry or complex numbers, just to prove $MN=NP=PM$ using Euclidean geometry)
Edit : I will present the solution that I have, that is based on trigonometry. Let $O$ be the center of the circle, $R$ its radius and a,b,c respectively the magnitudes of the angles BOC, DOE and FOA respectively. Then $OM=R\cos\frac{a}{2}$, $ON=R\cos\frac{b}{2}$, $OP=R\cos\frac{c}{2}$.
The angle $MON$ is equal to $MON=\frac{a}{2}+\frac{\pi}{3}+\frac{b}{2}$ and taking into account that $a+b+c=\pi$ we get that $MON=\frac{5\pi}{6}-\frac{c}{2}$.
Thus $\cos(MON)=\cos(\frac{5\pi}{6}-\frac{c}{2})= \cos\frac{5\pi}{6}\cos\frac{c}{2}+\sin\frac{5\pi}{6}\sin\frac{c}{2}$ from which we deduce that $$ \cos(MON)= -\frac{\sqrt{3}}{2}\cos\frac{c}{2}+\frac{1}{2}\sin\frac{c}{2}$$
Since $\frac{c}{2}=\frac{\pi}{2}-(\frac{a}{2}+\frac{b}{2})$ we have that $\sin\frac{c}{2}=cos(\frac{a}{2}+\frac{b}{2}) =\cos\frac{a}{2}\cos\frac{b}{2}-\sin\frac{a}{2}\sin\frac{b}{2}$. We get $$ \sin\frac{c}{2}-\cos\frac{a}{2}\cos\frac{b}{2}=-\sin\frac{a}{2}\sin\frac{b}{2}. $$
Apply now the law of cosines in the triangle $MON$, in order to compute $MN^2$. Our main concern is to find a formula that is symmetric to any permutation of $a,b,c$, which will imlpy that the same formula is valid for $NP^2$ and $PM^2$.
$$ MN^2 = OM^2+ON^2-2 OM\cdot ON \cos(MON) \\ = R^2 \cos^2\frac{a}{2}+ R^2 \cos^2\frac{b}{2} -2 R\cos \frac{a}{2}R\cos\frac{b}{2} \cos(MON)\\ =R^2\Big(\cos^2\frac{a}{2}+ \cos^2\frac{b}{2} -2 \cos \frac{a}{2} \cos\frac{b}{2} \cos(MON)\Big)\\ =R^2\Big[\cos^2\frac{a}{2}+ \cos^2\frac{b}{2} -2 \cos \frac{a}{2} \cos\frac{b}{2}\big (-\frac{\sqrt{3}}{2}\cos\frac{c}{2}+\frac{1}{2}\sin\frac{c}{2}\big) \Big]\\ = R^2 \Big( \sqrt{3} \cos\frac{a}{2}\cos\frac{b}{2}\cos\frac{c}{2} +\cos^2\frac{a}{2} + \cos^2\frac{b}{2} -\cos \frac{a}{2}\cos\frac{b}{2}\sin\frac{c}{2}\Big)\\ =R^2 \Big( \sqrt{3} \cos\frac{a}{2}\cos\frac{b}{2}\cos\frac{c}{2} +\cos^2\frac{a}{2} + \cos^2\frac{b}{2} +\cos^2\frac{c}{2}-1 +\sin^2\frac{c}{2}- \cos \frac{a}{2}\cos\frac{b}{2}\sin\frac{c}{2}\Big)\\ =R^2[-1+\sqrt{3} \cos\frac{a}{2}\cos\frac{b}{2}\cos\frac{c}{2} +\cos^2\frac{a}{2} + \cos^2\frac{b}{2} +\cos^2\frac{c}{2}\\ \qquad\qquad\qquad\qquad\qquad\qquad +\sin\frac{c}{2}(\sin\frac{c}{2}-\cos \frac{a}{2}\cos\frac{b}{2})\Big]\\ =R^2\Big[-1+\sqrt{3} \cos\frac{a}{2}\cos\frac{b}{2}\cos\frac{c}{2} +\cos^2\frac{a}{2} + \cos^2\frac{b}{2} +\cos^2\frac{c}{2} -\sin\frac{a}{2}\sin\frac{b}{2}\sin\frac{c}{2}\Big] $$
It seems to me impossible to translate this trigonometric proof to a pure euclidean geometry proof. This is the reason that I made the post, for someone to suggest a pure proof based on euclidean geometry.
Edit3: As pointed out by @Blue the formula is simlpified to $$MN^2= R^2(1+\sqrt{3}\cos\frac{a}{2} \cos\frac{b}{2}\cos \frac{c}{2}+ \sin \frac{a}{2} \sin \frac{b}{2} \sin \frac{c}{2}).$$