CONIC SECTIONS. Our starting point is the following definition sketch-

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CONIC SECTIONS One of the most important areas of analtic geometr involves the concept of conic sections. These represent d curves formed b looking at the intersection of a transparent cone b a plane tilted at various angles with respect to the cone axis. The resultant intersections can produce circles, ellipses, parabolas, and hperbolas. Collectivel the are referred to as conic sections. We want here to review their properties. Our starting point is the following definition sketch- The construction of a conic section starts with drawing a horizontal x axis and a vertical axis termed the directrix. One next chooses a point Q(a,0] on the x axis termed the focus. If we then sketch a D curve represented b a heav thick curve in the x- plane and demand that this curve have the propert that an point P(x,) on it have the ratio r/x be a constant, we will have the definition of a conic section. Calling this ratio the eccentricit of the curve, we find- e r a r cos( ) ( x a) x On solving for r and x we get the polar coordinate and Cartesian versions of a conic section, namel,- ea r 1 e cos( ) and x (1 e ) ax a

Looking at the Cartesian version, one has an ellipse if e<1, a parabola if e=1, and a hperbola when e>1. A circle is a special form of an ellipse with zero eccentricit (e=0). We look at all three finite e cases starting with the ellipse. First one converts the Cartesian form of the conic section into the more recognizable form- ( x b) ( eb) ( e ab) 1 where a b (1 e ) Ellipse: Here e<1 so that b>1. This means we have a standard shifted ellipse of the form ( x b) A B 1 which is centered on [b,0] and has a semi-major axis A=eb=ea/(1-e ) and semiminor axis B =e sqrt(ab)= ea/sqrt(1-e ). If we take the quotient sqrt(a -B )/A, we find this ratio equals- B 1 ( ) A e the eccentricit of the ellipse Taking a=1 and e=1/sqrt(),we have A=sqrt(), B=1, and b= to ield the graph- The directrix remains the axis and the focus of the ellipse is located at [1,0]. The point on the ellipse closest to the focus is the perigee and the point furthest awa is termed the apogee. This ellipse has a second focus located at [3,0]. An

interesting propert of ellipses is that the total distance from the first focus to an point on the ellipse and then the reflection onto the second focus is a constant equal to twice the semi-major axis A The semi-minor axis is given b the above expression as B=A sqrt(1-e ). This equal time-travel propert has found important applications in whispering galleries, hdrogen bomb triggers, and kidne stone removal. Elliptical trajectories of this tpe also have a ver important application in connection with planetar trajectories about the sun. In that application one prefers the use of the following polar representation - ea r 1 e cos( ) with e 1 From it one sees at once that the distance from the focus to the left intersection is the length to the perigee r p =ea/(1+e) while the distance from the first focus to the right intersection at the apogee equals r a =ea/(1-e). The sum r p +r a =A. Parabola: Here e=1 so that the conic section takes on the form of the shifted parabola- a ( ) x a A graph of this parabola for a= looks like this-

An important propert of this conic is that all incoming light ras parallel to the x axis will focus at the focal point at [,0]. This focusing principle lies behind all parabolic reflectors be the used for receivers such as reflector telescopes or sending out a parallel beam of light such as in search lights. Hperbola: Here e>1 so that b<0. So the conic section has the form of the hperbola- ( x b ) ( e b ) e a b 1 A graph of this hperbola for the special case of a=3 and e= follows- Note here that the hperbola center is at x=-1 and =0 while the focus for the right branch lies at [3,0]. We can calculate the curves perpendicular to these branches b noting the must have the sloped dx 3( x 1) and thus form the orthogonal curves-

3 const. ( x 1), where the constant is adjusted to match a point on the hperbola. In certain incompressible and inviscid D fluid flows one encounters flows having hperbolic streamline shapes of this tpe.