Casey's theorem

Casey's theorem 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.

Contenu 1 Formulation of the theorem 2 Preuve 3 Autres généralisations 4 Applications 5 Références 6 External links Formulation of the theorem {style d'affichage t_{12}cdot t_{34}+t_{14}cdot t_{23}-t_{13}cdot t_{24}=0} Laisser {style d'affichage ,O} be a circle of radius {style d'affichage ,R} . Laisser {style d'affichage ,O_{1},O_{2},O_{3},O_{4}} être (in that order) four non-intersecting circles that lie inside {style d'affichage ,O} and tangent to it. Denote by {style d'affichage ,t_{ij}} the length of the exterior common bitangent of the circles {style d'affichage ,O_{je},O_{j}} . Alors:[1] {style d'affichage ,t_{12}cdot t_{34}+t_{14}cdot t_{23}=t_{13}cdot t_{24}.} 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[2] to Zacharias.[3] Denote the radius of circle {style d'affichage ,O_{je}} par {style d'affichage ,R_{je}} and its tangency point with the circle {style d'affichage ,O} par {style d'affichage ,K_{je}} . We will use the notation {style d'affichage ,O,O_{je}} for the centers of the circles. Note that from Pythagorean theorem, {style d'affichage ,t_{ij}^{2}={surligner {O_{je}O_{j}}}^{2}-(R_{je}-R_{j})^{2}.} We will try to express this length in terms of the points {style d'affichage ,K_{je},K_{j}} . By the law of cosines in triangle {style d'affichage ,O_{je}OO_{j}} , {style d'affichage {surligner {O_{je}O_{j}}}^{2}={surligner {OO_{je}}}^{2}+{surligner {OO_{j}}}^{2}-2{surligner {OO_{je}}}cdot {surligner {OO_{j}}}cdot cos angle O_{je}OO_{j}} Since the circles {style d'affichage ,O,O_{je}} tangent to each other: {style d'affichage {surligner {OO_{je}}}=R-R_{je},,angle O_{je}OO_{j}=angle K_{je}OK_{j}} Laisser {style d'affichage ,C} be a point on the circle {style d'affichage ,O} . According to the law of sines in triangle {style d'affichage ,K_{je}CK_{j}} : {style d'affichage {surligner {K_{je}K_{j}}}=2Rcdot sin angle K_{je}CK_{j}=2Rcdot sin {frac {angle K_{je}OK_{j}}{2}}} Par conséquent, {displaystyle cos angle K_{je}OK_{j}=1-2sin ^{2}{frac {angle K_{je}OK_{j}}{2}}=1-2cdot left({frac {surligner {K_{je}K_{j}}}{2R}}droit)^{2}=1-{frac {{surligner {K_{je}K_{j}}}^{2}}{2R^{2}}}} and substituting these in the formula above: {style d'affichage {surligner {O_{je}O_{j}}}^{2}=(R-R_{je})^{2}+(R-R_{j})^{2}-2(R-R_{je})(R-R_{j})la gauche(1-{frac {{surligner {K_{je}K_{j}}}^{2}}{2R^{2}}}droit)} {style d'affichage {surligner {O_{je}O_{j}}}^{2}=(R-R_{je})^{2}+(R-R_{j})^{2}-2(R-R_{je})(R-R_{j})+(R-R_{je})(R-R_{j})cdot {frac {{surligner {K_{je}K_{j}}}^{2}}{R^{2}}}} {style d'affichage {surligner {O_{je}O_{j}}}^{2}=((R-R_{je})-(R-R_{j}))^{2}+(R-R_{je})(R-R_{j})cdot {frac {{surligner {K_{je}K_{j}}}^{2}}{R^{2}}}} And finally, the length we seek is {style d'affichage t_{ij}={sqrt {{surligner {O_{je}O_{j}}}^{2}-(R_{je}-R_{j})^{2}}}={frac {{sqrt {R-R_{je}}}cdot {sqrt {R-R_{j}}}cdot {surligner {K_{je}K_{j}}}}{R}}} We can now evaluate the left hand side, with the help of the original Ptolemy's theorem applied to the inscribed quadrilateral {style d'affichage ,K_{1}K_{2}K_{3}K_{4}} : {style d'affichage {commencer{aligné}&t_{12}t_{34}+t_{14}t_{23}\[4pt]={}&{frac {1}{R^{2}}}cdot {sqrt {R-R_{1}}}{sqrt {R-R_{2}}}{sqrt {R-R_{3}}}{sqrt {R-R_{4}}}la gauche({surligner {K_{1}K_{2}}}cdot {surligner {K_{3}K_{4}}}+{surligner {K_{1}K_{4}}}cdot {surligner {K_{2}K_{3}}}droit)\[4pt]={}&{frac {1}{R^{2}}}cdot {sqrt {R-R_{1}}}{sqrt {R-R_{2}}}{sqrt {R-R_{3}}}{sqrt {R-R_{4}}}la gauche({surligner {K_{1}K_{3}}}cdot {surligner {K_{2}K_{4}}}droit)\[4pt]={}&t_{13}t_{24}fin{aligné}}} Further generalizations It can be seen that the four circles need not lie inside the big circle. En réalité, they may be tangent to it from the outside as well. Dans ce cas, the following change should be made:[4] Si {style d'affichage ,O_{je},O_{j}} are both tangent from the same side of {style d'affichage ,O} (both in or both out), {style d'affichage ,t_{ij}} is the length of the exterior common tangent.

Si {style d'affichage ,O_{je},O_{j}} are tangent from different sides of {style d'affichage ,O} (one in and one out), {style d'affichage ,t_{ij}} is the length of the interior common tangent.

The converse of Casey's theorem is also true.[4] C'est-à-dire, 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. Par exemple, the shortest known proof[1]: 411  of Feuerbach's theorem uses the converse theorem.

Références ^ Aller à: a b Casey, J. (1866). "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". Actes de l'Académie royale d'Irlande. 9: 396–423. JSTOR 20488927. ^ Bottema, O. (1944). 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). ^ Zacharias, M. (1942). "Der Caseysche Satz". Rapport annuel de l'Association allemande des mathématiciens. 52: 79–89. ^ Sauter à: a b Johnson, Roger A.. (1929). Modern Geometry. Houghton Mifflin, Boston (republished facsimile by Dover 1960, 2007 as Advanced Euclidean Geometry). External links Wikimedia Commons has media related to Casey's theorem. Weisstein, Eric W. "Casey's theorem". MathWorld. Shailesh Shirali: "'On a generalized Ptolemy Theorem'". Dans: Crux Mathematicorum, Volume. 22, Non. 2, pp. 49-53 Catégories: Theorems about circlesEuclidean geometry