Casey's theorem explained

In mathematics, Casey's theorem, also known as the generalized Ptolemy's theorem, is a theorem in Euclidean geometry named after the Irish mathematician John Casey.

Formulation of the theorem

Let

O

be a circle of radius

R

. Let

O1,O2,O3,O4

be (in that order) four non-intersecting circles that lie inside

O

and tangent to it. Denote by

tij

the length of the exterior common bitangent of the circles

Oi,Oj

. Then:

t12t34+t14t23=t13t24.

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

Proof

The following proof is attributable to Zacharias. Denote the radius of circle

Oi

by

Ri

and its tangency point with the circle

O

by

Ki

. We will use the notation

O,Oi

for the centers of the circles.Note that from Pythagorean theorem,
2=\overline{O
t
iO
2-(R
i-R
2.
j)

We will try to express this length in terms of the points

Ki,Kj

. By the law of cosines in triangle

OiOOj

,

\overline{OiO

2-2\overline{OO
i}

\overline{OOj}\cos\angleOiOOj

Since the circles

O,Oi

tangent to each other:

\overline{OOi}=R-Ri,\angleOiOOj=\angleKiOKj

Let

C

be a point on the circle

O

. According to the law of sines in triangle

KiCKj

:

\overline{KiKj}=2R\sin\angleKiCKj=2R\sin

\angleKiOKj
2

Therefore,

\cos\angleKiOKj=

2\angleKiOKj
2
1-2\sin

=1-2 ⋅ \left(

\overline{KiKj
}\right)^2 = 1 - \frac

and substituting these in the formula above:

\overline{OiO

2-2(R-R
i)(R-R
2}\right)
j)\left(1-\overline{KiKj
2}{2R

\overline{OiO

2-2(R-R
i)(R-R

j)+(R-Ri)(R-Rj)

\overline{KiKj
2}{R

2}

\overline{OiO

2=((R-R
i)-(R-R
2+(R-R
i)(R-R

j)

\overline{KiKj
2}{R

2}

And finally, the length we seek is

tij=\sqrt{\overline{OiO

2-(R
i-R
2}=\sqrt{R-Ri
j)

\sqrt{R-Rj}\overline{KiKj}}{R}

K1K2K3K4

:

\begin{align} &t12t34+t14t23\\[4pt] ={}&

1
R2

\sqrt{R-R1}\sqrt{R-R2}\sqrt{R-R3}\sqrt{R-R4}\left(\overline{K1K2}\overline{K3K4}+\overline{K1K4}\overline{K2K3}\right)\\[4pt] ={}&

1
R2

\sqrt{R-R1}\sqrt{R-R2}\sqrt{R-R3}\sqrt{R-R4}\left(\overline{K1K3}\overline{K2K4}\right)\\[4pt] ={}&t13t24\end{align}

Further generalizations

It can be seen that the four circles need not lie inside the big circle. In fact, they may be tangent to it from the outside as well. In that case, the following change should be made:

If

Oi,Oj

are both tangent from the same side of

O

(both in or both out),

tij

is the length of the exterior common tangent.

If

Oi,Oj

are tangent from different sides of

O

(one in and one out),

tij

is the length of the interior common tangent.

The converse of Casey's theorem is also true. That is, if equality holds, the circles are tangent to a common circle.

Applications

Casey's theorem and its converse can be used to prove a variety of statements in Euclidean geometry. For example, the shortest known proof of Feuerbach's theorem uses the converse theorem.

References

[1]

[2]

[3]

[4]

External links

Notes and References

  1. Casey . J. . John Casey (mathematician) . Proceedings of the Royal Irish Academy . 20488927 . 396–423 . On the Equations and Properties: (1) of the System of Circles Touching Three Circles in a Plane; (2) of the System of Spheres Touching Four Spheres in Space; (3) of the System of Circles Touching Three Circles on a Sphere; (4) of the System of Conics Inscribed to a Conic, and Touching Three Inscribed Conics in a Plane . 9 . 1866.
  2. M. . Zacharias . . 52 . 1942 . 79–89 . Der Caseysche Satz.
  3. Book: Bottema , O. . Hoofdstukken uit de Elementaire Meetkunde . (translation by Reinie Erné as Topics in Elementary Geometry, Springer 2008, of the second extended edition published by Epsilon-Uitgaven 1987) . 1944.
  4. Book: Johnson , Roger A. . Modern Geometry . Houghton Mifflin, Boston (republished facsimile by Dover 1960, 2007 as Advanced Euclidean Geometry) . 1929.