The center of gravity of a solid triangle is the point where its medians intersect (its centroid ).
Consider a hollow triangle, whose sides are made of uniformly dense, thin strings. Let be the triangle formed by connecting the midpoints of
Where is the center of gravity of
For reference, here are the other three common triangle centers: circumcenter , incenter , and orthocenter .
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The centre of mass G of the triangular frame A B C , with line density ρ , is equal to the centre of mass of three point masses ρ a , ρ b , ρ c at the points D , E , F respectively, where D , E , F are the midpoints of the lines B C , A C , A B respectively (here we are simply replacing each side of the triangle by a point particle of the same mass located at the midpoint of each side). Consider the centre of mass X of the point masses at E and F . This point lies on the line segment E F and the ratio E X : X F is equal to c : b . Since E D = 2 1 c and F D = 2 1 b , this is the same as the ratio E D : D F . By the Angle Bisector Theorem, we deduce that X lies on the angle bisector of ∠ E D F . Then G is the centre of mass of the system consisting of a particle of mass ρ a at D and a particle of mass ρ ( b + c ) at X . Thus G lies on the line segment D X , and hence lies on the angle bisector of ∠ E D F . Similar arguments tell us that G lies on the angle bisectors of ∠ D E F and ∠ D F E as well, and hence that G is the incentre of D E F .
The centre of mass of a triangular frame A B C is therefore the incentre of the medial triangle. This point is known as the Spieker centre for the triangle A B C .