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The generalized version of Ptolemy's theorem, also known, as Casey's theorem states the following.

Theorem. Let OO be a circle of radius RR. Let O1,O2,O3,O4O_1,O_2,O_3,O_4 be (in that order) four non-intersecting circle that lie inside OO and tangent to it. Denote by tijt_{ij} the length of the exterior common tangent of the circles Oi,OjO_i,O_j. Then, t12⋅t34+t41⋅t23=t13⋅t24.t_{12} \cdot t_{34} + t_{41} \cdot t_{23} = t_{13} \cdot t_{24}.

Think about why this is a generalized case of Ptolemy's theorem. When is Ptolemy's Theorem a special case of this?

In the degenerate case, where all four circles reduce to points, this is exactly Ptolemy's theorem.

Proof, taken from Wikipedia. Use this diagram.

Denote the radius of circle OiO_i by RiR_i and its tangency point with the circle OO by KiK_i. We will use the notation OO, OiO_i for the centers of the circles. Note, from the Pythagorean Theorem, that tij2=(OiOj)2−(Ri−Rj)2.t_{ij}^2 = \left( O_i O_j \right)^2 - \left( R_i - R_j \right)^2. We will try to express this length in terms of the points Ki,KjK_i,K_j. By the law of cosines on triangle OiOOjO_iOO_j, we have (OiOj)2=(OOi)2+(OOj)2−2(OOi)⋅(OOj)⋅cos⁡∠OiOOj.\left( O_i O_j \right)^2 = \left( O O_i \right)^2 + \left( O O_j \right)^2 - 2 \left( O O_i \right) \cdot \left( O O_j \right) \cdot \cos \angle O_i O O_j.Since the circles OO and OiO_i are tangent to each other, we find that OOi=R−RiOO_i = R - R_i and ∠OiOOj=∠KiOKj\angle O_i O O_j = \angle K_i O K_j. Let CC be a point on the circle OO. According to the law of sines on triangles KiCKjK_i C K_j, we have KiKj=2R⋅sin⁡∠KiCKj=2R⋅sin⁡∠KiOKj2.K_i K_j = 2R \cdot \sin \angle K_i C K_j = 2R \cdot \sin \frac {\angle K_i O K_j}{2}. Therefore, cos⁡∠KiOKj=1−2sin⁡2∠KiOKj2=1−2⋅(KiKj2R)2=1−(KiKj)22R2.\cos \angle K_i O K_j = 1 - 2 \sin^2 \frac {\angle K_i O K_j}{2} = 1 - 2 \cdot \left( \frac {K_i K_j}{2R} \right)^2 = 1 - \frac {\left( K_i K_j \right)^2}{2R^2}. Substituting and simplifying, you should get (OiOj)2=((R−Ri)−(R−Rj))2+(R−Ri)(R−Rj)⋅(KiKj)2R2.\left( O_i O_j \right)^2 = \left( \left( R - R_i \right) - \left( R - R_j \right) \right)^2 + \left( R - R_i \right) \left( R - R_j \right) \cdot \frac {\left( K_i K_j \right)^2}{R^2}.And eventually, after much algebra, we find that tij=(OiOj)2−(Ri−Rj)2=R−Ri⋅R−Rj⋅(KiKj)Rt_{ij} = \sqrt {\left( O_i O_j \right)^2 - \left( R_i - R_j \right)^2} = \frac {\sqrt {R - R_i} \cdot \sqrt {R - R_j} \cdot \left( K_i K_j \right)}{R} and in fact, the left-hand-side in the original theorem becomes t12t34+t14t23=1R2⋅R−R1⋅R−R2⋅R−R3⋅R−R4⋅((K1K3)⋅(K2K4))=t13t24,\begin {align*} t_{12} t_{34} + t_{14} t_{23} &= \frac {1}{R^2} \cdot \sqrt {R-R_1} \cdot \sqrt {R - R_2} \cdot \sqrt {R - R_3} \cdot \sqrt {R - R_4} \cdot \left( \left( K_1 K_3 \right) \cdot \left( K_2 K_4 \right) \right) \\&= t_{13} t_{24}, \end {align*}as desired. ■\blacksquare

Exercise for the reader. Verify the steps we skipped and make sure you understand where everything comes from!

Type a concept, like “slope” or “photosynthesis”.

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