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In prior chapters we defined fumctions that gave information about the value of one quantity with respect to the value of another directly.
We asked, for example, how far an object has traveled after some number of seconds have elapsed when given the object's rate of change of distance with respect to time.
The accumulation function we defined in terms of the object's rate of change with respect to time allowed us to answer questions about the object's distance traveled at any moment in time.
There are other questions that arise naturally in such situations that cannot be answered so directly. For example:
We have a function for a car's velocity at each moment in time since it began moving. What was the car's velocity at every distance it traveled?
The difficulty we meet in answering this question is that we have distance as a function of time and velocity as a function of time, but we do not have velocity as a function of distance.
Cement is being poured into a building's foundation at the rate of $r_f(t)=t^4e^{-t/2}\text{ m$^3$/min}$ $t$ minutes after the pouring chute opened. At what rate is cement being poured when $V\text{ m$^3$}$ of cement has been poured?
The cement's rate of change of volume with respect to time after $t$ minutes is $r_f(t)=t^4e^{-t/2}\text{ m$^3$/min}$; its volume after $t$ minutes is $\displaystyle{f(t)=\int_0^t r_f(u)du}\text{ m$^3$}$.
At first thought it seems we must solve for $t$ in terms of $V$ in $\displaystyle{\int_0^t r_f(u)du=V}$ and then substitute that expression for $t$ in $r_f(t)$.
Using integration by parts repeatedly, we get $$\begin{align} f(t)&=\int_0^t u^4e^{-u/2}du\\[1ex]&=-2e^{-t/2}\left(t^4+8t^3+48t^2+192t+384\right)+768.\end{align}$$
Solving for $t$ in terms of $V$ in $-2e^{-t/2}\left(t^4+8t^3+48t^2+192t+384\right)+768=V$ will be daunting.
However, we can use GC to take a graphical approach. We can command GC to produce a graph of $r_f(t)$, the rate of change of poured concrete's volume with respect to time, in relation to $f(t)$, the concrete's volume with respect to time. The idea will be to put values of $f(t)$ on the horizontal axis and values of $r_f(t)$ on the vertical axis. We can then inspect the graph for values of $r_f(t)$ that correspond to values of $f(t)$.
Figures 12.0.1, 12.0.2, and 12.0.3 show three stages in envisioning a graph of values of one function in relation to values of another function when they share a common argument.
Figure 12.0.1 focuses on a way to imagine coordinating values of $r_f(t)$ and $f(t)$ to make points on the graph of $r_f$ in relation to $f$.
Figure 12.0.2 summarizes 12.0.1 by collecting values of both functions in a table and then plotting points from the table.
Figure 12.0.3 illustrates a way to think of coordinating values of $r_f(t)$ and $f(t)$ as the value of $t$ varies smoothly.
Coordinating values of $r_f(t)$ and $f(t)$
Figure 12.0.1. To sketch a graph of $r_f(t)$ in relation to $f(t)$, do this repeatedly:
(1) Select a value of $t$;
(2) Determine values of $r_f(t)$ and $f(t)$;
(3) Place the value of $f(t)$ on the horizontal axis;
(4) Place the value of $r_f(t)$ on the vertical axis;
(5) Plot the correspondence point $\left(f(t),r_f(t)\right)$.
Collecting values in a table
Figure 12.0.2. Collect corresponding values of $r_f(t)$ and $f(t)$ for values of $t$. Then plot the correspondence points $\left(f(t),r_f(t)\right)$.
Coordinating values of $r_f(t)$ and $f(t)$ as $t$ varies smoothly
Figure 12.0.3. Values of $r_f(t)$ and $f(t)$ vary as $t$ varies. We coordinate values of $r_f(t)$ and $f(t)$ by imagining the
value of $r_f(t)$ varying on the vertical axis as the value of $f(t)$ varies on the horizontal axis.
Reflection 12.0.1. Describe how Figures 12.0.1, 12.0.2, and 12.0.3 give complementary information.
Answering questions from graphs
The graph of $r(t)$ in relation to $f(t)$ allows us to approach the question of how fast concrete is being poured when $V$ $\text{ m$^3$}$ of concrete has been poured. Figure 12.0.4 shows the point $(547.187,51.7134)$ highlighted on the graph of $r_f$ in relation to $f$. This means that when the volume is 547.187 $\text{ m$^3$}$ the volume is changing at the rate of 51.7134 $\text{ m$^3$/min}$.
Figure 12.0.4. The concrete's volume is changing at 51.7134 $\text{ m$^3$/min}$ when its volume is 547.187 $\text{ m$^3$}$.
Using GC to graph values of one function in relation to values of another
Figure 12.0.5 shows the GC file that generated Figure 12.0.4.
Figure 12.0.5. The GC file that created Figure 12.0.4.
Define $r_f$ and $f$. Then press ctrl 2 to get a 2-row by 1-column array.
Then type = ctrl 2. In the second array, replace x by $f(30t)$ and y by $r_f(30t)$.
Note that, in GC, the value of t varies from 0 to 1 by default.
One aspect of GC's conventions is worth noticing. You can change the domain of $t$ (bottom right of equations pane in Figure 12.0.5) by typing new numbers for lower and upper values of its range.
Changing the range of values for $t$ is advisable only when you are graphing a single relationship, or when all relationships rely on $t$ having the same range of values. When different relationships rely on $t$ having different ranges of values it is better to leave the range of $t$ as $[0,1]$ and adjust the arguments of functions in the different relationships.
For example, in Figure 12.0.5 the arguments in $f(30t)$ and $r_f(30t)$ vary from 0 to 30 when the value of $t$ varies from 0 to 1. You could change the upper limit for $t$ to 30 (bottom right of equations pane) and use "$f(t)$" and "$r_f(t)$" in the statement that generates the graph.
It is well known in physics that horizontal motion and vertical motion are independent in a gravitational field.
This can be illustrated by an experiment where a bean bag is shot horizontally at the same moment that an object is released from the same height as the bean bag.
The two will collide if they don't hit the ground first -- regardless of the bean bag's horizontal speed and regardless of the distance between object and bean bag. (See animation below.)