Curves Defined by Parametric Equations
What is a Parametric Curve?
A parametric curve is a set of points of the form:
where $f$ and $g$ are functions of a variable $t$, called the parameter (often representing time).
- As $t$ increases over an interval $[a, b]$, the point $(x(t), y(t))$ traces out a curve.
- Orientation: The curve has a natural direction of motion indicating increasing $t$.
- Vertical Line Test: Standard Cartesian functions $y = f(x)$ can only assign one $y$ to each $x$.
- Cannot naturally describe closed loops, circles, self-intersecting figures, or spirals without splitting equations.
- No velocity or direction: Cartesian graphs show the path, but cannot describe how fast or in what direction an object moves.
Method 1: Point Plotting & Orientation
| $t$ | $x = t^2 - 2t$ | $y = t + 1$ | Point $(x, y)$ |
|---|---|---|---|
| $-2$ | $8$ | $-1$ | $(8, -1)$ (Initial) |
| $-1$ | $3$ | $0$ | $(3, 0)$ |
| $0$ | $0$ | $1$ | $(0, 1)$ |
| $1$ | $-1$ | $2$ | $(-1, 2)$ (Vertex) |
| $2$ | $0$ | $3$ | $(0, 3)$ |
| $3$ | $3$ | $4$ | $(3, 4)$ |
| $4$ | $8$ | $5$ | $(8, 5)$ (Terminal) |
Method 2: Eliminating the Parameter
Given the parametric equations:
A Cartesian Equation is an equation containing only the variables in the Cartesian coordinate system (in a 2D plane, only $x$ and $y$). To find the Cartesian equation from $(x(t), y(t))$, we eliminate the parameter $t$ so that only $x$ and $y$ remain.
Eliminating $t$ yields the entire Cartesian curve, but the parametric curve may only trace a piece of it!
Identity $\sin^2\theta + \cos^2\theta = 1 \implies y = 1 - x^2$.
However: since $-1 \le \sin\theta \le 1$, the parametric curve is only the portion of the parabola for $x \in [-1, 1]$ and $y \in [0, 1]$!
Interactive Parametric Curve Visualizer
| $t$ | $x$ | $y$ | $(x, y)$ |
|---|
In-Class Practice Problems
Given the parametric equations:
(a) Eliminate the parameter $t$ to write this curve in Cartesian form: $$y = f(x)$$
(b) Identify the restricted domain of $x$ and describe the path traced out.
Consider the two parametric curves on $0 \le t \le \pi$:
(a) Find the Cartesian equations of both curves and explain the geometric difference between their graphs.
(b) Generalization: For any curve $x = t, y = f(t)$, what does the graph of the swapped curve $x = f(t), y = t$ look like?
Compare these three curves for $-\infty < t < \infty$:
(a) Show that eliminating $t$ gives the identical equation $y = x^2$ for all three.
(b) Explain how their domains, sketched paths, and particle motions actually differ.
Exercise 1: Cartesian Equation
Hint: Use the formula $\cos(2\theta) = \cos^2\theta - \sin^2\theta$.
Using the given double-angle formula and the Pythagorean identity $\cos^2 t + \sin^2 t = 1 \implies \cos^2 t = 1 - \sin^2 t$: $$\cos(2t) = \cos^2 t - \sin^2 t = (1 - \sin^2 t) - \sin^2 t = 1 - 2\sin^2 t$$
Substitute $x = \sin t$ directly into $y = 1 - 2\sin^2 t$: $$y = 1 - 2(\sin t)^2 \implies \mathbf{y = 1 - 2x^2}$$ Therefore, in the required form $y = f(x)$, we have: $$\mathbf{f(x) = 1 - 2x^2}$$
• Domain Restriction: Because $x = \sin t$, the domain is restricted to:
$$-1 \le x \le 1$$
• Range: As $x \in [-1, 1]$, $y = 1 - 2x^2$ ranges from $-1$ (when $x = \pm 1$) to $1$ (vertex at $x = 0$).
• Motion: The curve is the parabolic arc opening downward from $(-1, -1)$ to $(1, -1)$ with vertex at $(0, 1)$. As $t$ increases, a particle oscillates back and forth along this arc.
Exercise 2: Swapped Coordinates & Reflection Across $y = x$
2. Generalization: Given any curve $x(t) = t, \; y(t) = f(t)$, what does the graph of $x(t) = f(t), \; y(t) = t$ look like?
• Curve 1: Since $x = t$, substituting gives $\mathbf{y = \sin x}$ for $x \in [0, \pi]$ (horizontal arch peaking at $(\pi/2, 1)$).
• Curve 2: Since $y = t$, substituting gives $\mathbf{x = \sin y}$ for $y \in [0, \pi]$ (vertical arch bowing rightward to $(1, \pi/2)$).
Notice that every point $(x_1, y_1) = (t, \sin t)$ on Curve 1 corresponds directly to $(x_2, y_2) = (\sin t, t)$ on Curve 2.
In Cartesian geometry, the coordinate swap $\mathbf{(x, y) \longleftrightarrow (y, x)}$ is a reflection across the diagonal line $y = x$.
Therefore, Curve 2 is the exact reflection of Curve 1 across $y = x$!
For any $C_1: x = t, y = f(t) \implies y = f(x)$, the swapped curve $C_2: x = f(t), y = t \implies x = f(y)$ is always the reflection of $y = f(x)$ across the line $y = x$ (the geometric inverse relation).
Exercise 3: The "Same Cartesian Equation" Trap
In all three cases, substituting $x$ into $y$ yields: $$\mathbf{y = x^2}$$ However, their domains and physical motions are completely different!