We use limits to compute instantaneous velocity.

When we compute average velocity, we look at

\[ \frac {\text {change in position}}{\text {change in time}}. \]

To obtain the (instantaneous) velocity, we want the change in time to “go to” zero. By this point we should know that “go to” is a buzz-word for a limit. The change in time is often given as the length of a time interval, and this length goes to zero.

Let’s put all of this together by working an example.

In our previous example, we computed average velocity on several different intervals. For example, the average velocity on the time interval \([2,t]\) is \(v_{\text {av}}=8-16t\). Note that the size or the length of that time interval is \(t-2\).

If we let \(t\to 2\), the size of the interval will go to \(0\). As \(t\) approaches \(2\), we are computing the average velocity on smaller and smaller time intervals, and the limit of these average velocities is called the instantaneous velocity at \(t=2\). Limits will allow us to compute instantaneous velocity.

The instantaneous velocity is given as a limit, \(v(a) = \lim _{t\to a}\dfrac {s(t)-s(a)}{t-a}\). What is the form of this limit? The numerator \(s(t)-s(a)\) approaches \(0\) as \(t\to a\) (since the displacement function \(s(t)\) is continuous) and the denominator \(t-a\) also approaches \(0\). This limit has form \(\relax \boldsymbol {\tfrac {0}{0}}\), an indeterminate form.

Let’s use the same setting as before to work with this definition.