# Parametric Equations

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Parametric Equations – HMC Calculus Tutorial

Think of a curve being traced out over time, sometimes doubling back on itself or crossing itself. Such a curve cannot be described by a function $y=f(x)$. Instead, we will describe our position along the curve at time $t$ by \begin{eqnarray*} x&=&x(t)\\ y&=&y(t). \end{eqnarray*} Then $x$ and $y$ are related to each other through their dependence on the parameter $t$.

###### Example

Suppose we trace out a curve according to \begin{eqnarray*} x&=&t^2-4t\\ y&=&3t \end{eqnarray*} where $t\geq 0$. The arrow on the curve indicates the direction of increasing time or orientation of the curve. Drag the box along the curve and notice how $x$ and $y$ vary with $t$.

The parameter does not always represent time:

###### Example

Consider the parametric equation \begin{eqnarray*} x&=&3\cos\theta\\ y&=&3\sin\theta. \end{eqnarray*} Here, the parameter $\theta$ represents the polar angle of the position on a circle of radius $3$ centered at the origin and oriented counterclockwise.

#### Differentiating Parametric Equations

Let $x=x(t)$ and $y=y(t)$. Suppose for the moment that we are able to re-write this as $y(t)=f(x(t))$. Then $\displaystyle \frac{dy}{dt}=\frac{dy}{dx}\cdot \frac{dx}{dt}$ by the Chain Rule. Solving for $\displaystyle \frac{dy}{dx}$ and assuming $\displaystyle \frac{dx}{dt}\neq 0$, $\frac{dy}{dx}=\frac{~\frac{dy}{dt}~}{~\frac{dx}{dt}~}$ a formula that holds in general.

###### Example

If $x=t^2-3$ and $y=t^8$, then $\displaystyle \frac{dx}{dt}=2t$ and $\displaystyle \frac{dy}{dt}=8t^7$. So \begin{eqnarray*} \frac{dy}{dx}&=&\frac{\frac{dy}{dt}}{\frac{dx}{dt}}=\frac{8t^7}{2t}=4t^6\\ \frac{d^2y}{dx^2}&=&\frac{d}{dx}\left[\frac{dy}{dx}\right]= \frac{~\frac{d[\frac{dy}{dx}] \strut}{dt}~}{~\frac{dx}{dt}~}=\frac{24t^5}{2t}=12t^4. \end{eqnarray*}

#### Notes

• It is often possible to re-write the parametric equations without the parameter. In the second example, $\displaystyle \frac{x}{3}=\cos\theta$, $\displaystyle \frac{y}{3}=\sin\theta$. Since $\cos^2 \theta +\sin^2 \theta =1$, $\displaystyle \left(\frac{x}{3}\right)^2+\left(\frac{x}{3}\right)^2=1$. Then $x^2+y^2=9$, which is the equation of a circle as expected. When you do eliminate the parameter, always check that you have not introduced extraneous portions of the curve.

• Every curve has infinitely many parametrizations, amounting to different scales for the parameter. For example, \begin{eqnarray*} x&=&3\cos 2\theta\\ y&=&3\sin 2\theta \end{eqnarray*} traces out the circle from the second example twice as “quickly,” completing a full revolution in $\pi$ rather than $2\pi$ units of $\theta$.

• Every equation $y=f(x)$ may be re-written in parametric form by letting $x=t$, $y=f(t)$.

#### Key Concepts

A curve in the $xy$-plane may be described by a pair of parametric equations $$x = x(t)$$ $$y = y(t)$$ where $x$ and $y$ are related through their dependence on $t$. This is particularly useful when neither $x$ nor $y$ is a function of the other.

The derivative of $y$ with respect to $x$, in terms of the parameter $t$, is given by $$\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}.$$