Not only is there an odd number of tricolor triangles, but they come in pairs according to their orientation (RGB clockwise/anticlockwise). Proof: define a continuously differentiable vector field on the plane, by letting the field at each vertex be 0, and the field in the center of each edge be a vector of magnitude 1 pointing in the direction R->G->B->R (or 0 if the two adjacent vertices are the same color). Extend the field to the complete edges, then the interiors of the triangles by some interpolation method with continuous derivative (eg. cosine interpolation).
Assume the line integral along one unit edge in the direction R->G or G->B or B->R to be 1⁄3. (Without loss of generality since we can rescale the graph/vectors to make this true). Then a similar parity argument to Sperner’s 1d lemma (or the FTC) shows that the clockwise line integral along each large edge is 1⁄3, hence the line integral around the large triangle is 1/3+1/3+1/3=1.
By green’s theorem, this is equal to the integrated curl of the field in the interior of the large triangle, and hence equal (by another invocation of green’s theorem) to the summed clockwise line integrals around each small triangle. The integrals around a unicolor or bicolor triangle are 0 and −1/3 + 1⁄3 + 0 = 0 respectively, leaving only tricolor triangles, whose integral is again 1 depending on orientation. Thus: (tricolor clockwise) - (tricolor anticlockwise) = 1. QED.
Proof of #4, but with unnecessary calculus:
Not only is there an odd number of tricolor triangles, but they come in pairs according to their orientation (RGB clockwise/anticlockwise). Proof: define a continuously differentiable vector field on the plane, by letting the field at each vertex be 0, and the field in the center of each edge be a vector of magnitude 1 pointing in the direction R->G->B->R (or 0 if the two adjacent vertices are the same color). Extend the field to the complete edges, then the interiors of the triangles by some interpolation method with continuous derivative (eg. cosine interpolation).
Assume the line integral along one unit edge in the direction R->G or G->B or B->R to be 1⁄3. (Without loss of generality since we can rescale the graph/vectors to make this true). Then a similar parity argument to Sperner’s 1d lemma (or the FTC) shows that the clockwise line integral along each large edge is 1⁄3, hence the line integral around the large triangle is 1/3+1/3+1/3=1.
By green’s theorem, this is equal to the integrated curl of the field in the interior of the large triangle, and hence equal (by another invocation of green’s theorem) to the summed clockwise line integrals around each small triangle. The integrals around a unicolor or bicolor triangle are 0 and −1/3 + 1⁄3 + 0 = 0 respectively, leaving only tricolor triangles, whose integral is again 1 depending on orientation. Thus: (tricolor clockwise) - (tricolor anticlockwise) = 1. QED.
As a physicist, this is my favorite one for obvious reasons :)
Generalized to n dimensions in my reply to Adele Lopez’s solution to #9 (without any unnecessary calculus :)