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Mathematics · Ch 15 — Hyperbola

Standard Form of the Hyperbola

15.1

Standard Form of the Hyperbola

A hyperbola is defined the same way an ellipse is, except for one flipped inequality: it is the path traced by a point PP whose distance from a fixed point SS (the focus) stays a constant multiple ee of its distance from a fixed line (the directrix), where this time e>1e>1. Because the point is pulled disproportionately away from the line as it moves off to infinity, the locus splits into two mirror-image branches that never close up — that's the visual signature that separates a hyperbola from an ellipse at a glance.

To get a clean equation, place the centre of symmetry CC at the origin, and run the xx-axis straight through the focus, perpendicular to the directrix. Working through the focus-directrix condition SP=e (PM)SP = e\,(PM) algebraically (exactly the same style of computation used for the ellipse, just with e>1e>1 this time) collapses to the tidy standard form:

x2a2−y2b2=1\frac{x^2}{a^2} - \frac{y^2}{b^2} = 1

Here 2a2a is the length of the transverse axis — the segment AA′AA' joining the two points where the curve actually crosses the xx-axis — and bb is defined through the relation b2=a2(e2−1)b^2 = a^2(e^2-1), which is forced by the derivation. Unlike the ellipse, there's no requirement that b<ab<a; bb can be anything positive, because it no longer measures a semi-axis the curve touches. The segment BB′BB' of length 2b2b marked off on the (vertical) yy-axis is called the conjugate axis, and it's worth remembering that the curve itself never actually meets this axis — it's a construction axis, not a boundary the curve touches.

A quick feature-check on x2a2−y2b2=1\dfrac{x^2}{a^2}-\dfrac{y^2}{b^2}=1 tells you everything about its shape: setting y=0y=0 gives x=±ax=\pm a, so it crosses the xx-axis at (±a,0)(\pm a, 0); setting x=0x=0 gives y2=−b2y^2=-b^2, which has no real solution, confirming the curve never touches the yy-axis. Solving for yy gives y=±bax2−a2y = \pm\dfrac{b}{a}\sqrt{x^2-a^2}, which is only real when ∣x∣≥a|x|\ge a — so the entire strip −a<x<a-a<x<a is empty of the curve, and each branch stretches away to infinity as x→±∞x\to\pm\infty. The curve is symmetric about both axes, since replacing x→−xx\to -x or y→−yy\to -y leaves the equation unchanged. …