M408M Learning Module Pages
Main page Chapter 10: Parametric Equations and Polar CoordinatesLearning module LM 10.1: Parametrized Curves:Learning module LM 10.2: Calculus with Parametrized Curves:Learning module LM 10.3: Polar Coordinates:Learning module LM 10.4: Areas and Lengths of Polar Curves:Learning module LM 10.5: Conic Sections:Learning module LM 10.6: Conic Sections in Polar Coordinates:Foci and directricesVisualizing eccentricity Polar equations for conic sections Astronomy Chapter 12: Vectors and the Geometry of SpaceChapter 13: Vector FunctionsChapter 14: Partial DerivativesChapter 15: Multiple Integrals |
Foci and directricesEllipses and hyperbolas are usually defined using two foci, but they can also be defined using a focus and a directrix.
For instance, suppose that we have a conic section with focus at the origin, directrix at y=−1, and eccentricity e≠1. Then √x2+y2=e|y+1|x2+y2=e2(y2+2y+1)x2+(1−e2)y2−2e2y=e2. Notice that the coefficient of y2 in the last equation is positive if e<1, giving us an ellipse, and is negative when e>1, giving us a hyperbola. After completing the square and applying some more algebraic manipulations, we can put the equation in standard form: (1−e2e2)x2+((1−e2)2e2)(y−e21−e2)2=1. If e<1, this is an vertically aligned ("tall and skinny") ellipse with center at (0,e21−e2), with a=e1−e2, b=e√1−e2 and c=e21−e2 and eccentricity e=c/a. As e→1, the center and the size of the ellipse both go to infinity. If e>1 the situation is analogous. Our curve is then a hyperbola of with center at (0,−e2e2−1), with a=ee2−1, b=e√e2−1 and c=e2e2−1 and eccentricity e=c/a. As e→1, the center and the size of the hyperbola both go to infinity. |