It is commonly presumed that an object moving on a straight line can be in only one place for a given time, so its position, $s$, is a function of time, $t$. Two points, $(a, s(a))$ and $(x, s(x))$, on the graph of this position function report information about two states or circumstances for the object.

See Figure I.B.6.

The first coordinate of the point gives the time value, $t$, for the state while the second coordinate gives its position value, $s$. The change in position between the two states, $\Delta s$, is the change in the second coordinates of the points, while the change in time, $\Delta t$, is the change in the first coordinates of the points.

Thus the average velocity determined by the two states, $\overline{v_a} (x) =\frac {\Delta s} {\Delta t}$ corresponds to the slope of the non-vertical line determined by the two points. On the graph of the position function, the slope of the secant line, $\overline {m_a(x)}$ , determined by the points $(a,s(a))$ and $(x,s(x))$ uses the same computations used to determine the average velocity over the time interval between $a$ and $x$. Thus we have $\overline{v_a} (x) =\frac {s(x)-s(a)} {x-a} =\overline {m_a(x)}$ .

Figure I.B.6

Now our analysis so far of average velocity and instantaneous velocity has suggested that as $x \rightarrow a$, the average velocity determined by $x$ and $a$ approaches the instantaneous velocity at time $a$, i.e., $\overline{v_a} (x) \rightarrow v(a)$. Meanwhile our work in Chapter I.A suggested that the slope of the secant lines determined by $x$ and $a$ approaches the slope of the line tangent to the curve that graphs the position function. i.e. $\overline{m_a} (x) \rightarrow m_{tan}(a)$.

Putting all this together gives us the conclusion that the numerical value of the instantaneous velocity at time $a$ is precisely the same as the slope of the line tangent to the graph of the position function at the point $(a, s(a))$.

Positive velocity is represented by a tangent line with positive slope, going "uphill" on the graph. while a negative velocity is seen as a tangent line with negative slope, going "downhill" on the graph. Greater speeds are seen as steeper lines. These relations can be reversed as well so that a tangent (or secant) line to the graph of the position function and its slope can be interpreted to give information about the velocity of a moving object. The following example and discussion shows more of the connection between the instantaneous velocity and the slope of a tangent to the position function graph.

Figure I.B.7 |

Discussion:

Looking at the point on the graph with first coordinate 1 and estimating the slope of a line tangent to the graph at that point gives an estimate of the instantaneous velocity at time 1.

If you draw the tangent line at the point with first coordinate 1, you will see a line that has a slope of about -2, so we estimate the cat's velocity as -2 meters per second.

Similarly we estimate the velocity at time 2 by estimating the slope of the tangent line at the point on the graph with first coordinate 2. This tangent line seems to be horizontal, so the slope would be 0, meaning a 0 velocity. So the cat appears to be stopped at time 2.

When the cat turned around its position function will change from increasing in value to decreasing or