The Parabola
Slice a cone with a flat plane and you get a family of curves called the
conic sections. Tilt the plane just so — parallel to the slope of the cone — and the
cut you expose is a parabola: the graceful open curve of a thrown ball, a
fountain's arc, or the cable of a suspension bridge. You have met one already as the graph of
a quadratic,
y = ax^2. This page reveals what that curve really is — and
why it hides inside every satellite dish and car headlight on Earth.
A circle is every
point a fixed distance from one point. A parabola swaps that single centre for a point
and a line, and balances between them:
A parabola is the set of all points that are the same distance from a fixed
point (the focus) as from a fixed line (the directrix).
\text{distance to the focus} \;=\; \text{distance to the directrix}.
Every point on the curve keeps this promise exactly; no point off the curve does. The focus sits
inside the bend of the curve, the directrix runs outside it, and the curve threads perfectly
between them.
The two equal distances, in a picture
Step through the figure below. A point P on the parabola sends one
segment straight to the focus and one straight down to the directrix. Drag your eye along the
curve in your mind: those two lengths grow and shrink together, staying equal at
every single point. That equality is the parabola.
The standard equations
Put the vertex at the origin and the equal-distance rule turns into tidy algebra. Let
p be the distance from the vertex to the focus (and, by symmetry, from
the vertex to the directrix). There are two orientations.
-
Opens up or down — axis vertical:
x^2 = 4py, focus (0, p), directrix
y = -p. Opens up if p > 0,
down if p < 0.
-
Opens right or left — axis horizontal:
y^2 = 4px, focus (p, 0), directrix
x = -p. Opens right if p > 0,
left if p < 0.
-
The axis of symmetry runs through the vertex and the focus; the curve is a
mirror image across it.
The number 4p is the whole personality of the parabola: a big
p means a far focus and a wide, lazy curve; a small
p means a near focus and a tight, narrow one.
The familiar y = ax^2, decoded
The school parabola y = ax^2 is exactly
x^2 = 4py in disguise. Rearrange:
x^2 = \tfrac{1}{a}\,y, so matching 4p = \tfrac{1}{a}
gives
a = \frac{1}{4p} \qquad\Longleftrightarrow\qquad p = \frac{1}{4a}.
So the plain graph y = x^2 (with a = 1) has
its focus a mere p = \tfrac14 above the vertex, at
\left(0, \tfrac14\right), and directrix
y = -\tfrac14. The steepness you already know and the focal distance are
two sides of the same coin.
Worked examples
1 · Read off the focus and directrix. Take
y^2 = 8x. This is the horizontal form
y^2 = 4px, so match the coefficients:
4p = 8 \;\Longrightarrow\; p = 2.
Therefore the focus is at (p, 0) = (2, 0) and the directrix is the line
x = -p, i.e. x = -2. The curve opens to the
right (because p > 0), wrapping around its focus.
2 · Build the equation from a focus and directrix. Find the parabola with
focus (0, 3) and directrix y = -3. The focus
is on the y-axis and the directrix is horizontal, so this is the
vertical form x^2 = 4py. Here the focus is
(0, p), so p = 3, and
x^2 = 4py = 4(3)y = 12y.
Check it against the definition: the point (6, 3) lies on
x^2 = 12y (since 36 = 12 \cdot 3). Its
distance to the focus (0,3) is 6; its distance
to the directrix y = -3 is 3 - (-3) = 6.
Equal — as promised.
Spin a parabola around its axis and you get a paraboloid — a dish. It has one magical
habit, the reflective property: every ray coming in parallel to the axis
bounces off the surface and passes through a single point — the focus. (And run it backwards: a
bulb at the focus throws out a perfectly parallel beam.)
That one fact powers a surprising amount of the world. A satellite dish gathers
faint parallel signals from space and concentrates them onto a receiver placed exactly at the
focus. A reflecting telescope does the same with starlight. Run the idea in
reverse and a car headlight or torch puts its bulb at the focus
to hurl a straight, bright beam down the road. Even a solar cooker uses it to pile sunlight onto
one blazing hot spot. The word "focus" is Latin for hearth — the fireplace — and now you
know why.
The tempting mistake is to read the steepness a as the distance to the
focus. It is not — in fact it is upside down. The focal distance is
p = \tfrac{1}{4a}, so a and
p pull in opposite directions:
-
A narrow parabola (large a, e.g.
y = 4x^2) has a close focus,
p = \tfrac{1}{16}.
-
A wide parabola (small a, e.g.
y = 0.1x^2) has a far focus,
p = 2.5.
And don't confuse the two constants across the forms: in y^2 = 4px the
coefficient is 4p (four times the focal distance), whereas in
y = ax^2 the coefficient a is its
reciprocal over four. Same curve, two different bookkeepers.
Once you have the parabola, its cousins are a short step away: the closed
ellipse and the
two-branched hyperbola
are the other slices of the same cone.