Loading...
Some curves cannot be written as at all — a full circle fails immediately, because most values have two values. Parametric equations solve this by defining and separately in terms of a third variable, the , so the curve is described by where a point is at each value of that parameter.
The big picture
The change of viewpoint is worth dwelling on. Cartesian form describes a curve as a relationship between coordinates; parametric form describes it as a — first this point, then that one. That is why parametric equations are the natural language for anything moving: projectile motion in Mechanics is exactly and given separately in terms of time. It is also why they unlock curves that fail the vertical line test: a parameter can revisit the same with a different because it has moved on. Later you will differentiate parametrically to find gradients on such curves without ever eliminating the parameter.
What you'll be able to do
A parametric definition gives and . Each value of produces one point, and as runs through its range the point traces the curve.
Take , . At the point is ; at it is ; at it is . Note that give the same but different — impossible for a function , and completely unremarkable parametrically.
The parameter is usually or . It often has no physical meaning at all; it is simply the variable doing the bookkeeping.
The parameter carries information the Cartesian equation throws away — the order in which points are visited, and how fast. Two different parametrisations can trace the same curve in opposite directions.
To convert to Cartesian form, make the subject of the simpler equation and substitute into the other. Choose the equation where is easiest to isolate — usually the linear one.
The result is a single relationship between and . Sometimes it is a familiar curve in disguise, which is exactly the point of the exercise.
Tip — State any restriction the parametrisation imposes. For the Cartesian curve only exists for , because a square is never negative.
When the parameter appears inside sine and cosine, isolating it means using inverse functions and that gets messy fast. The better route is to rearrange so that and stand alone, then use to eliminate in one move.
This is why the circle is the standard example. , gives , which rearranges to — the circle equation from the previous lesson, arrived at from a completely different direction.
Squaring and adding is the whole technique whenever both and of the same angle appear. Look for it as soon as you see a trigonometric parameter — it converts the problem to algebra immediately.
You do not always need the Cartesian equation. To find where a curve crosses the -axis, set , solve for the parameter, and substitute back into . Crossing the -axis works the same way with .
For an intersection with a line, substitute both parametric expressions into the line equation and solve for the parameter. Each solution gives one intersection point.
Tip — When two parameter values give the same point, the curve crosses itself there. That self-intersection is invisible in the Cartesian equation and is one of the things parametric form is genuinely better at showing.
Think like an examiner
Common misconceptions
Parametric essentials
Stretch yourself
A curve is given by , . Find its Cartesian equation, and determine the coordinates of the point where the curve is furthest to the left.
Hint — The second equation is linear — make the subject there. For the leftmost point, think about what value minimises .
Questions students ask
Key takeaways
How this fits the course
Build on
Related
Leads to
Test yourself
Ready to lock in Parametric Equations? Pick a mode and earn XP & Dobloons.
Real past-paper questions on Parametric Equations, marked mark-by-mark. How you do feeds straight into your weak-topic list, so your revision keeps targeting what actually needs work.