Osculating Circles of Conics in Cayley-Klein Planes

Osculating Circles of Conics in Cayley-Klein Planes

KoG•13 (2009), 7–12. G. Weiss, A. Sliepcevi´ˇ c: Osculating Circles of Conics in Cayley-Klein Planes Original scientific paper GUNTER WEISS Accepted 30. 06. 2009. ANA SLIEPCEVIˇ C´ Osculating Circles of Conics in Cayley-Klein Planes Osculating Circles of Conics in Cayley-Klein Oskulacijske kruˇznice konika u Cayley-Klein-ovim Planes ravninama ABSTRACT SAZETAKˇ In the Euclidean plane there are several well-known meth- U euklidskoj ravnini postoji nekoliko dobro poznatih ods of constructing an osculating (Euclidean) circle to a metoda konstrukcija oskulacijske kruˇznice konike. Cilj conic. We show that at least one of these methods can je te konstrukcije “translatirati” u neke od neeuklid- be “translated” into a construction scheme of finding the skih ravnina. U ˇclanku se daje op´ca konstrukcija osku- osculating non-Euclidean circle to a given conic in a hyper- lacijske kruˇznice konike zadane s pet elemenata u euklid- bolic or elliptic plane. As an example we will deal with the skoj ravnini. Pokazuje se da je konstruktivna metoda pri- Klein-model of these non-Euclidean planes, as the projec- mjenjiva u hiperboliˇckoj i eliptiˇckoj ravnini. Budu´ci da je tive geometric point of view is common to the Euclidean projektivno geometrijsko glediˇste zajedniˇcko euklidskom i as well as to the non-Euclidean cases. neeuklidskim sluˇcajevima, analogne se konstrukcije koriste na Klein-ovim modelima neeuklidskih ravnina. Key words: Cayley-Klein plane, elation, pencil of conics, osculating circle, curvature centre Kljuˇcne rijeˇci: Cayley-Klein-ova ravnina, elacija, pramen konika, oskulacijska kruˇznica, srediˇste zakrivljenosti MSC 2010: 51N30, 51M15, 53A35 1 Preliminary Remark Stachel, H. Havlicek) and Graz (J. Wallner, O. R¨oschel), where they still belong to the syllabus in teachers educa- Although the problem of constructing an osculating circle tion in Descriptive Geometry. at a point of a conic seems to be anachronistic in times of numerical approximation tools, knowledge about ex- act constructive methods is not at all obsolete, particularly 2 Euclidean Osculating Circles of Conics since these methods are uniformly applicable. Beyond that, with the following projective geometric constructions We start with “permissible standard givens” of a conic in of osculating circles, we place particular emphasis on syn- the Euclidean plane, i.e. from pair of conjugate diameters ( , ) thetic argumentation, which is typically for geometry. Un- AC , BD of an ellipse, from a pair of line elements A tA , ( , ) ( , ) fortunately Projective Geometry and Non-Euclidean Ge- B tB of a parabola and from a pair of asymptotes r s ometry in the sense of F. Klein does not have much space and a point A of a hyperbola. The problem is to find the in nowadays Mathematics education such that valuable Ge- osculating circle at the given point A. ometry culture is in danger of vanishing. Our article might In geometry courses for engineers one usually presents the perhaps help to counteract these facts. The paper is also construction recipe for the hyperosculating circles at the to be posed into the series of articles of classical Projec- vertex of the conic; in lectures on differential geometry tive and Non-Euclidean Geometry initiated by the second for Mathematicians this recipe is also presented and the author, see [5] - [8]. analytic equality of 4thorder is proved by calculation in It is hard to say, how “well-known” the presented consid- each of the three cases. But for all three cases there is a erations are; they could be for example exercise material to uniform projective geometric idea for the solution of this lectures on classical Projective Geometry and not consid- (more general) problem. This idea uses properties of oscu- ered to be valuable enough to be published. To our knowl- lating resp. hyperosculating pencils of conics. This unified edge lectures with related content still exist in Vienna (H. explanation of elementary construction of hyperosculating 7 KoG•13 (2009), 7–12. G. Weiss, A. Sliepcevi´ˇ c: Osculating Circles of Conics in Cayley-Klein Planes circles at vertices of a conic might be not new, but it is, Elliptic case (Figure 1) in our opinion, not at all so well-known as it is worthy to The point A is transformed into the vertex of an ellipse note. c by the shear σ1 : c → c (tangent tA at A is the axis of → In addition, the construction principle deduced from it can σ1). Furthermore, σ2 : c kA with the same axis, but be used for all Cayley-Klein geometries, as it is shown in with center A, transforms a “neighbouring” vertex B of c the following chapter only for the hyperbolic and the quasi- into the point B of kA. The line through the fixed point hyperbolic geometry (which is the dual geometry to the T = T = T on tA perpendicular to the chord AB = AB pseudo-Euclidean geometry) as an example. of the osculating circle kA intersects the normal n of the Specifically, the construction follows two steps: conic c given at the point A in the center MA of kA. Step 1: Transform the given conic c by the standard shear Parabolic case (Figure 2) → transformation σ1 : c → c into another conic c , which os- The shear σ1 : c c (axis is the tangent tA at A) transforms culates c at the point A, and has A as a vertex. The axis of the point A into the vertex of a parabola c , which osculates the shear therefore is the tangent tA in A. As all elations c. The midpoint H of the chord AB, together with the point with the center N on tA, this shear σ1 maps the given conic T := tA ∩tB,defines the diameter direction of the conic c, c into c which osculates the conic c at A. The osculating and therefore is mapped into the point H on the line nor- circle of one is also osculating circle for the other one. mal to tA at T .Forσ2 : c → kA (the center is A) the line = ( ) Step 2: Construct the hyperosculating circle kA of the conic AH is a fixed line; it contains the point B σ2 B of the c at A = A . For this one can use an additional elation σ2 hyperosculating conic kA. The line through the fixed point which also has tA as its axis, but the center A and it should T = T = T perpendicular to the chord AB = AH of kA map c into a hyperosculating conic c . By demanding passes through the sought-after curvature center M . A c → kA the transformation σ2 is uniquely defined; σ2 Hyperbolic case (Figure 3) transforms the point B of the osculating conic c (in the case of an ellipse this is a “neighbouring” vertex, in case At first we construct the tangent tA at the point A,(A is the of a hyperbola one of the asymptote’s ideal point “at infin- midpoint of the tangent segment between the asymptotes). ity”, in the case of a parabola it is the additionally given By a suitable shear σ1 one can transform the point A into point) into the point B of kA. The normal from the (fixed) the vertex of the hyperbola c whose asymptotes are r and = = ∈ = ∩ = ∩ → point T T T tA (T tA tB tB tB) to the chord s and the center is M . The elation σ2 : c kA with center = AB = AB of circle kA therewith passes through the center A transforms the ideal point R B of the asymptote r of MA of kA. the conic c into the point B of the hyperosculating conic kA. Therefore, the line through the fixed point T on the = The following figures (Figures 1-3) show the construction tangent tA perpendicular to AB AB passes through the costs, which in each of the three cases needs only a few common curvature center MA of the conics kA, c and c.As lines. AB is parallel to r , one only needs to draw the perpendic- ular line to the asymptote r = MT at the point T . M M N C A A kA B’’ s’ t B’ H H’ D A B B B’ M’ A n n tB n H MA N H’ t T=T’=T’’ tA A B M r r’ N s A tA T=T’=T’’ T=T’=T’’ R R’=B’ Figure1: Construction of the center Figure 2: Construction of the center Figure 3: Construction of the cur- MA of the osculating circle kA at the MA of the osculating circle kA at the vature center MA at the point A of endpoint A of one of the given con- point A of the parabola c given by the hyperbola cgiven by the pair of jugate diameters of the ellipse c. two line elements (A,tA), (B,tB). asymptotes (r,s) and the point A. 8 KoG•13 (2009), 7–12. G. Weiss, A. Sliepcevi´ˇ c: Osculating Circles of Conics in Cayley-Klein Planes Remark 1 Of course, there are other nice constructions visualise again the Euclidean case in Figure 4, i.e. “⊥ ”and of the Euclidean curvature circle at the point of a conic, “circles” allow an elementary geometric interpretation.) too. We want to mention the one found in [1], which is based on the differential geometric investigations and goes Step 1: determine the normal n of the conic c at the point A as follows: with respect to ⊥; i.e. one needs to construct the “absolute , conjugate line” n to the given tangent a of the conic c at A “Choose two points P Q on tangent tA symmetric to A, ⊥ draw the tangents from P and Q to the given conic c, re- with respect to π .

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