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Slicing a Cone: Where Conics Come From

Tilt a plane through a cone and you carve out a circle, an ellipse, a parabola, or a hyperbola — one family of curves born from a single solid. This opening guide shows why these four belong together, and previews the three lenses (cone-sections, focus-and-directrix, and a single second-degree equation) the rest of the rung will sharpen.

One solid, four curves

By now you can place any figure on the Cartesian plane, read its slope, and write a line or a circle as an equation. The circle was the first curve whose equation was genuinely quadratic, (x - h)^2 + (y - k)^2 = r^2 — and it turns out the circle has three close cousins, all governed by second-degree equations. Together these four curves are the conic sections, and this rung is their story. The name is a promise: every one of them appears when you slice a cone with a flat plane.

Picture an ice-cream cone, but doubled: two cones tip-to-tip, sharing a single vertex and opening in opposite directions, stretching forever both up and down. This double cone is the surface we will slice. Now take an infinite flat plane and pass it through the cone at different tilts. As the plane's angle changes, the curve where it cuts the cone — the plane section — changes character, and four distinct shapes emerge. The whole family is generated by nothing more than one fixed cone and one rotating plane.

Watch the plane tilt

Start with the plane horizontal, perpendicular to the cone's axis. It cuts one nappe (one half of the double cone) in a perfect circle — every point the same distance from the axis. Now tilt the plane a little. The closed loop stretches into an ellipse, an oval that still closes on itself, longer one way than the other. Keep tilting and the oval grows more lopsided, but as long as the plane is less steep than the cone's own side, it always comes back around and closes.

Then comes the knife-edge moment. Tilt the plane until it is exactly parallel to one straight line lying on the cone's surface (one 'generator' of the cone). Now the section can no longer close — it runs off to infinity along that one direction, an open curve with a single branch. This is the parabola. It is the precise borderline between the closed ellipses and what comes next, the single special tilt where the curve is forever on the verge of escaping but never doubles back.

Tilt past that critical angle — steeper than the cone's side — and something new happens: the plane now cuts both nappes of the double cone, once above the vertex and once below. The section splits into two separate open branches, mirror images facing apart. This is the hyperbola. So the four shapes are not a random zoo; they are an ordered sequence keyed to a single number, the steepness of the plane, with the parabola standing guard at the boundary.

plane tilt vs. cone's side          section
--------------------------------    -----------
perpendicular to axis               circle
less steep than the cone's side     ellipse
exactly parallel to a generator     parabola   <- the borderline
steeper than the cone's side        hyperbola  (cuts both nappes)
How the tilt of the cutting plane decides which conic you get.

A flatlander's definition: focus and directrix

The cone picture is beautiful, but it lives in three dimensions, and the curves we want to study live in the flat plane. We need a definition that an inhabitant of the plane could state and use without ever leaving it — a definition as a locus, a set of points obeying a distance rule. Remember how a circle was defined: all points a fixed distance from one center. The conics generalize exactly this idea, by comparing distances instead of fixing just one.

Fix one point, called the focus, and one line, called the directrix. For a point P in the plane, measure two distances: its distance to the focus, and its perpendicular distance to the directrix. The focus-directrix property says a conic is the set of all P for which the ratio of these two distances is a fixed constant. That constant is the eccentricity, written e. One focus, one line, one ratio — and out of that single rule the entire family pours: change only the value of e and you walk through ellipse, parabola, and hyperbola in turn.

Here is the heart of it in one line: when e = 1, focus-distance equals directrix-distance, and the curve is a parabola. When e < 1 (the point hugs the focus more tightly than the line) the curve closes into an ellipse. When e > 1 the curve opens up into a hyperbola. So the mysterious borderline angle from the cone reappears here as the clean number e = 1. That a single dial sorts all three is the punchline guide 4 of this rung is named for — but you can already feel where it is heading.

Why the slice and the ratio agree: Dandelin's spheres

It is fair to be suspicious. Why should a curve carved by slicing a cone in three dimensions obey a tidy distance-ratio rule in two? The two stories sound unrelated. Yet they describe exactly the same curves, and the bridge between them is one of the most satisfying arguments in all of geometry: the Dandelin spheres. The full argument is the climax of guide 5 of this rung, so here we only sketch the idea honestly, without pretending the picture proves itself.

The trick is to wedge spheres inside the cone so that each one touches the cone all the way around in a circle and just kisses the cutting plane at a single point. For an ellipse, two such spheres fit — one above the slice, one below — and the points where they touch the plane turn out to be exactly the two foci of the ellipse. With the spheres in place, a short chain of equal-tangent-length facts converts the three-dimensional slicing into the flat distance rule, with no fudging. The spheres are the missing handshake between the cone and the locus.

All of them, in one equation

There is a third lens, and it is the most algebraic. Back on the coordinate plane, the line was first-degree (A*x + B*y + C = 0) and the circle was a special second-degree curve. If you write down the most general second-degree equation in two variables, you get the general second-degree equation: A*x^2 + B*x*y + C*y^2 + D*x + E*y + F = 0. The remarkable fact, which guide 5 makes precise, is that its graph is always a conic section — a circle, ellipse, parabola, hyperbola, or one of a few flattened 'degenerate' cases. Nothing else can appear.

Even better, you can read off which conic you have without graphing it, just from the coefficients of the squared and cross terms. The quantity B^2 - 4*A*C, the discriminant, sorts them: negative means an ellipse (or circle), zero means a parabola, positive means a hyperbola. Notice the pattern echoing through all three lenses — a single sign or a single number, e against 1, the discriminant against 0, deciding the same three outcomes. The conics keep telling the same story in three different languages.