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:Slicing a coneEllipses Hyperbolas Parabolas and directrices Completing the square Learning module LM 10.6: Conic Sections in Polar Coordinates:Chapter 12: Vectors and the Geometry of SpaceChapter 13: Vector FunctionsChapter 14: Partial DerivativesChapter 15: Multiple Integrals |
Completing the squareThe most general conic section has an equation of the form Ax2+By2+Cxy+Dx+Ey+F=0. So far we have taken C=D=E=0, except for parabolas. Here we'll see how to adjust for nonzero values of D and E. We'll still assume that C=0, which means that our curves will point in the direction of the coordinate axes. C≠0 describes rotated conic sections.
If A≠0, then we can always absorb the Dx term by completing the square: Ax2+Dx=A(x2+DAx)=A(x+D2A)2−D24A Likewise, if B≠0 then we can absorb the Ey term: By2+Ey=B(y+E2B)2−E24B. If B=0 then we cannot absorb the Ey term, and the equation of a parabola winds up looking like y−k=−AE(x−h)2.
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