329 Parameterization

A function that labels points of a curve by a real parameter that is used to write coordinates along the curve.

An implicit equation gives a constraint on points; parameterization instead gives a rule that generates each point on the curve.

For example:

\[ x^2+y^2=1 \]

versus \[ x=\cos t,\qquad y=\sin t.\]

The first describes which points belong to the circle. The second tells you how to move through those points.

definition [d] (Parameterization = Parametrization = Parametric Representation) A continuous vector-valued function that traces a curve \(C\) as the parameter varies over an interval \(I\):

  • \(\mathbf{r}(t) = \langle f(t),\, g(t),\, h(t) \rangle\) , \(t \in I\) .

where

  • \(\mathbf{r}(t)\) is the position vector of a point on \(C\).
  • \(C\) is the curve being traced.
  • \(f, g, h\) are continuous real-valued functions on \(I\).
  • \(t\) is the parameter.
  • \(I\) is the parameter interval.

Note:

  • a given curve admits many different parameterizations; speed and direction may differ.

definition [d] (Parameterization = Parametrization = Parametric Form) A description of a curve by expressing its coordinates as continuous functions of a single parameter \(t \in I\):

  • \(x = f(t)\), \(y = g(t)\), \(z = h(t)\) .

where

  • \(f, g, h\) are continuous real-valued functions on \(I\).
  • \(t\) is the parameter.
  • \(I\) is the parameter interval.
  • \(x, y, z\) are coordinates of a point on the curve.

Note:

  • as \(t\) increases, the point \((f(t), g(t), h(t))\) moves along the curve with a definite orientation.

329.1 Examples

329.1.1 Simple

A line in the plane labeled by three parameter values.

\[ \mathbf{r} : I \rightarrow \mathbb{R}^{2} \]

\[ I = \{ 0,\ 1,\ 2 \} \]

\[ \mathbf{r}(t) = \langle t,\ 2t \rangle \]

\[ \mathbf{r}(0) = \langle 0,\ 0 \rangle,\quad \mathbf{r}(1) = \langle 1,\ 2 \rangle,\quad \mathbf{r}(2) = \langle 2,\ 4 \rangle \]

where

  • \(\mathbf{r}\) is the parameterization.
  • \(I\) is the set of parameter values.
  • \(t\) is the parameter.

329.1.2 General

A unit circle in the plane labeled by a continuous parameter, with sample points and a second parameterization of the same curve.

\[ \phi : [0, 2\pi) \rightarrow \mathbb{R}^{2} \]

\[ \phi(t) = \langle \cos t,\ \sin t \rangle \]

\[ x = \cos t,\quad y = \sin t \]

\[ \phi(0) = \langle 1,\ 0 \rangle,\quad \phi\!\left(\dfrac{\pi}{2}\right) = \langle 0,\ 1 \rangle,\quad \phi(\pi) = \langle -1,\ 0 \rangle \]

Unit circle under \phi at t=0.
Unit circle under \(\phi\) at \(t=0\).
Unit circle under \phi at t=\pi/2.
Unit circle under \(\phi\) at \(t=\pi/2\).
Unit circle under \phi at t=\pi.
Unit circle under \(\phi\) at \(t=\pi\).

The same circle admits another parameterization that traverses it twice as fast. Every point on the unit circle still has the form \(\langle \cos\theta,\ \sin\theta \rangle\) for some angle \(\theta\).

\[ \psi : [0, \pi) \rightarrow \mathbb{R}^{2} \]

To finish one full lap while \(t\) runs only through \([0, \pi)\), the angle must advance twice as fast, so \(\theta = 2t\). Substituting that angle into the same cosine and sine form gives

\[ \psi(t) = \langle \cos 2t,\ \sin 2t \rangle \]

so \(\phi\) and \(\psi\) share the same image while differing in speed. At the same parameter value \(t=\pi/4\), the point \(\psi(t)\) has already advanced farther around the circle than \(\phi(t)\).

Comparison of \phi and \psi at t=\pi/4.
Comparison of \(\phi\) and \(\psi\) at \(t=\pi/4\).

where

  • \(\phi\) is a parameterization of the unit circle.
  • \(\psi\) is another parameterization of the same circle.
  • \(t\) is the parameter.
  • \(\theta\) is the angle used inside cosine and sine.
  • \([0, 2\pi)\) and \([0, \pi)\) are the parameter intervals.
  • \(x\) and \(y\) are coordinates of a point on the curve.
  • the image of \(\phi\) and of \(\psi\) is the circle of radius \(1\).

329.2 References

  1. Stewart, J. Calculus. — parametrization via \(\mathbf{r}(t)\) and parametric equations \(x=f(t)\), \(y=g(t)\), \(z=h(t)\).
  2. Bachman, D. A Geometric Approach to Differential Forms. Birkhäuser, 2012. — \(\phi(t)=(\cos t,\sin t)\) for \(0\leq t<2\pi\); also \(\psi(t)=(\cos 2t,\sin 2t)\) for the same circle at twice the speed.