We will study a special type of limit called a derivative. These arise when we are looking at an instantaneous rate of change, the slope of a tangent line, or a velocity.
In Section 1.4 we described the intuition behind creating a tangent line.
We saw it was a limit. Here's the definition:
The tangent line limit is an indeterminate form. Here is an animation of the previous example:
Notice how the expression $f(x) - f(a)$ approaches $0$ and $x - a$ also approaches 0.
Because this limit is an indeterminate form, we need to simplify the expression before applying the limit.
In practice, it's easier to simplify the following equivalent expression of the slope of the tangent line: \[m = \lim_{h \rightarrow 0} \dfrac{f(a + h) - f(a)}{h}\]
The tangent line is sometimes called the slope of the curve because if you zoom in far enough, the curve almost looks like a straight line.
In Section 1.4 we described dropping a ball from the CN tower and defined its velocity to be the "limit" of the average velocities over shorter and shorter time periods.
Recall that $s = f(t)$ gives the position of an object moving in a straight line $t$ seconds after rest, called the position function.
Over the time interval $[a, a+h]$, the change in position is $f(a + h) - f(a)$. Thus the average velocity is \[\text{average velocity} = \dfrac{\text{displacement}}{\text{time}} = \dfrac{f(a + h) - f(a)}{h}\]
But looking at shorter and shorter time periods of the average velocity requires $h \rightarrow 0$. Thus we have the following definition:
We now redo the problem in 1.4 but with this limit.
Notice how the same limit \[\lim_{h\rightarrow 0} \dfrac{f(a + h) - f(a)}{h}\] occurred when we wanted to calculate a "rate of change." This limit appears often enough so we give it a name:
The derivative can take on three interpretations:
The slope of the tangent line is the derivative.
Thus the tangent line to $y = f(x)$ at $(a, f(a))$ is the line through $(a, f(a))$ whose slope is $f'(a)$.
The general equation can be described with point-slope form.