Imagine a particle moving through space. Its position is not just a collection of coordinates $(x, y)$, but a story unfolding over time. While Cartesian equations like $y = f(x)$ provide a static 'snapshot' of a path, they are often handcuffed by the Vertical Line Test and cannot describe objects that double back on themselves or intersect.
Beyond the Cartesian Constraint, we introduce a third actor: the parameter $t$. By defining both $x$ and $y$ as functions of this third independent variable, we liberate the curve, allowing it to represent motion, velocity, and complex geometric forms like loops and spirals.
1. Fundamental Definitions
To define motion in the plane, we use a pair of equations where $x$ and $y$ are both dependent on a parameter (usually $t$ for time or $\theta$ for angles).
- Parameter: A third variable $t$ upon which $x$ and $y$ are dependent.
- Parametric Equations: Equations $x = f(t)$ and $y = g(t)$ that define $x$ and $y$ as functions of a parameter.
- Parametric Curve: The set of points $(x, y)$ traced out as the parameter varies over its domain.
A Cartesian equation in $x$ and $y$ describes where the particle has been, but it doesn't tell us when the particle was at a particular point. By contrast, parametric equations preserve the "history" of the motion.
In general, the curve with parametric equations $x = f(t), y = g(t), a \le t \le b$ has an initial point $(f(a), g(a))$ and a terminal point $(f(b), g(b))$.
2. The Trace and Orientation
It is vital to distinguish between a curve (the geometric set of points) and a parametric curve (the path as it is traced). Even if two sets of equations produce the same graph, they represent different physical realities if the speed or direction of the tracing differs.
Example: Representing a Parabolic Path
Consider a particle moving along $y = x^2$. We can parameterize this in multiple ways:
- Constant Speed: $x = t, y = t^2$. The particle moves horizontally at a constant rate.
- Acceleration: $x = t^3, y = t^6$. The particle starts slowly at the origin and accelerates rapidly as $|t|$ increases.
Both cover the same 'track,' but the second particle experiences much higher velocity and acceleration.