1.1: Changing in Tandem
- If we have two quantities that are changing in tandem, how can we connect the quantities and understand how change in one affects the other?
- When the amount of water in a tank is changing, what behaviors can we observe?
Mathematics is the art of making sense of patterns. One way that patterns arise is when two quantities are changing in tandem. In this setting, we may make sense of the situation by expressing the relationship between the changing quantities through words, through images, through data, or through a formula.
Suppose that a rectangular aquarium is being filled with water. The tank is 44 feet long by 22 feet wide by 33 feet high, and the hose that is filling the tank is delivering water at a rate of 0.50.5 cubic feet per minute.
- What are some different quantities that are changing in this scenario?
- After 11 minute has elapsed, how much water is in the tank? At this moment, how deep is the water?
- How much water is in the tank and how deep is the water after 22 minutes? After 33 minutes?
- How long will it take for the tank to be completely full? Why?
Using Graphs to Represent Relationships
In Preview Activity 1.1.1 , we saw how several changing quantities were related in the setting of an aquarium filling with water: time, the depth of the water, and the total amount of water in the tank are all changing, and any pair of these quantities changes in related ways. One way that we can make sense of the situation is to record some data in a table. For instance, observing that the tank is filling at a rate of 0.50.5 cubic feet per minute, this tells us that after 11 minute there will be 0.50.5 cubic feet of water in the tank, and after 22 minutes there will be 11 cubic foot of water in the tank, and so on. If we let tt denote the time in minutes and VV the amount of water in the tank at time t,t, we can represent the relationship between these quantities through Table 1.1.3.
| t | V |
| 0 | 0.0 |
| 1 | 0.5 |
| 2 | 1.0 |
| 3 | 1.5 |
| 4 | 2.0 |
| 5 | 2.5 |
Figure 1.1.4. A visual representation of the data in Table 1.1.3.
We can also represent this data in a graph by plotting ordered pairs \((t,V)\) on a system of coordinate axes, where \(t\) represents the horizontal distance of the point from the origin, \((0,0)\), and \(V\) represents the vertical distance from \((0,0)\). The visual representation of the table of values from Table 1.1.3 is seen in the graph in Figure 1.1.4 .
Sometimes it is possible to use variables and one or more equations to connect quantities that are changing in tandem. In the aquarium example from the preview activity, we can observe that the volume, \(V\), of a rectangular box that has length \(l\), width \(w\), and height hh is given by
\(V=l⋅w⋅h\),
and thus, since the water in the tank will always have length \(l=4\) feet and width \(w=2\) feet, the volume of water in the tank is directly related to the depth of water in the tank by the equation\(V=4⋅2⋅h=8h\).
Depending on which variable we solve for, we can either see how VV depends on hh through the equation \(V=8h\), or how hh depends on \(V\) via the equation \(h=\frac{1}{8}V\). From either perspective, we observe that as depth or volume increases, so must volume or depth correspondingly increase.Consider a tank in the shape of an inverted circular cone (point down) where the tank's radius is \(2\) feet and its depth is \(4\) feet. Suppose that the tank is being filled with water that is entering at a constant rate of \(0.75\) cubic feet per minute.
a. Sketch a labeled picture of the tank, including a snapshot of there being water in the tank prior to the tank being completely full.
b. What are some quantities that are changing in this scenario? What are some quantities that are not changing?
c. Fill in the following table of values to determine how much water, \(V\), is in the tank at a given time in minutes, \(t\), and thus generate a graph of the relationship between volume and time by plotting the data on the provided axes.
| t | V |
| 0 | |
| 1 | |
| 2 | |
| 3 | |
| 4 | |
| 5 |
Figure 1.1.6. How volume and time change in tandem in the conical tank.
d. Finally, think about how the height of the water changes in tandem with time. Without attempting to determine specific values of \(h\) at particular values of \(t\), how would you expect the data for the relationship between \(h\) and \(t\) to appear? Use the provided axes to sketch at least two possibilities; write at least one sentence to explain how you think the graph should appear.
Using Algebra to Add Perspective
One of the ways that we make sense of mathematical ideas is to view them from multiple perspectives. We may use different means to establish different points of view: words, numerical data, graphs, or symbols. In addition, sometimes by changing our perspective within a particular approach we gain deeper insight.
Figure 1.1.7. The empty conical tank
Figure 1.1.8. The conical tank, partially filled.
If we consider the conical tank discussed in Activity 1.1.2 , as seen in Figure 1.1.7 and Figure 1.1.8 , we can use algebra to better understand some of the relationships among changing quantities. The volume of a cone with radius rr and height hh is given by the formula\(V=\frac{1}{3}πr2h\).
Note that at any time while the tank is being filled, \(r\) (the radius of the surface of the water), \(h\) (the depth of the water), and \(V\) (the volume of the water) are all changing; moreover, all are connected to one another. Because of the constraints of the tank itself (with radius \(2\) feet and depth \(4\) feet), it follows that as the radius and height of the water change, they always do so in the proportion\(\frac{r}{h}=\frac{2}{4}\).
Solving this last equation for \(r\), we see that \(r=\frac{1}{2}h\); substituting this most recent result in the equation for volume, it follows that\(V=\frac{1}{3} \pi\left(\frac{1}{2} h\right)^{2} h=\frac{\pi}{12} h^{3}\).
This most recent equation helps us understand how \(V\) and \(h\) change in tandem. We know from our earlier work that the volume of water in the tank increases at a constant rate of \(0.75\) cubic feet per minute. This leads to the data shown in Table 1.1.9.
| t | 0 | 1 | 2 | 3 | 4 | 5 |
| V | 0.0 | 0.75 | 1.5 | 2.25 | 3.0 | 3.75 |
With the equation \(V=\frac{π}{12}h^{3}\), we can now also see how the height of the water changes in tandem with time. Solving the equation for \(h\), note that \(h^{3}=\frac{12}{π}V\), and therefore
\[h=\sqrt[3]{\frac{12}{\pi} V}\]
Thus, when \(V=0.75\), it follows that \(h=\sqrt[3]{\frac{12}{\pi} 0.75} \approx 1.42\). Executing similar computations with the other values of \(V\) in Table 1.1.9, we get the following updated data that now includes \(h\).| t | 0 | 1 | 2 | 3 | 4 | 5 |
| V | 0.0 | 0.75 | 1.5 | 2.25 | 3.0 | 3.75 |
| h |
0.0 |
1.42 | 1.79 | 2.05 | 2.25 | 2.43 |
Plotting this data on two different sets of axes, we see the different ways that \(V\) and \(h\) change with \(t\). Whereas volume increases at a constant rate, as seen by the straight line appearance of the points in Figure 1.1.11 , we observe that the water's height increases in a way that it rises more slowly as time goes on, as shown by the way the curve the points lie on in Figure 1.1.12 “bends down” as time passes.
Figure 1.1.11. Plotting \(V\) versus \(t\)
Figure 1.1.12 Plotting \(h\) versus \(t\).
These different behaviors make sense because of the shape of the tank. Since at first there is less volume relative to depth near the cone's point, as water flows in at a constant rate, the water's height will rise quickly. But as time goes on and more water is added at the same rate, there is more space for the water to fill in order to make the water level rise, and thus the water's height rises more and more slowly as time passes.
Consider a tank in the shape of a sphere where the tank's radius is \(3\) feet. Suppose that the tank is initially completely full and that it is being drained by a pump at a constant rate of \(1.2\) cubic feet per minute.
a. Sketch a labeled picture of the tank, including a snapshot of some water remaining in the tank prior to the tank being completely empty.
b. What are some quantities that are changing in this scenario? What are some quantities that are not changing?
c. Recall that the volume of a sphere of radius \(r\) is \(V=\frac{4}{3}πr^{3}\). When the tank is completely full at time \(t=0\) right before it starts being drained, how much water is present?
d. How long will it take for the tank to drain completely?
e. Fill in the following table of values to determine how much water, \(V\), is in the tank at a given time in minutes, \(t\), and thus generate a graph of the relationship between volume and time. Write a sentence to explain why the data's graph appears the way that it does.
| t | V |
| 0 | |
| 20 | |
| 40 | |
| 60 | |
| 80 | |
| 94.24 |
Figure 1.1.14. A plot of how volume and time change in tandem in a draining spherical tank.
f. Finally, think about how the height of the water changes in tandem with time. What is the height of the water when \(t=0\)? What is the height when the tank is empty? How would you expect the data for the relationship between \(h\) and \(t\) to appear? Use the provided axes to sketch at least two possibilities; write at least one sentence to explain how you think the graph should appear.
Summary
- When two related quantities are changing in tandem, we can better understand how change in one affects the other by using data, graphs, words, or algebraic symbols to express the relationship between them. See, for instance, Table 1.1.9, Figure 1.1.11 , 1.1.12 , and Equation (1.1.1) that together help explain how the height and volume of water in a conical tank change in tandem as time changes.
- When the amount of water in a tank is changing, we can observe other quantities that change, depending on the shape of the tank. For instance, if the tank is conical, we can consider both the changing height of the water and the changing radius of the surface of the water. In addition, whenever we think about a quantity that is changing as time passes, we note that time itself is changing.
Exercises
Suppose we have an unusual tank whose base is a perfect sphere with radius \(3\) feet, and then atop the spherical base is a cylindrical “chimney” that is a circular cylinder of radius \(1\) foot and height \(2\) feet, as shown in Figure 1.1.15 . The tank is initially empty, but then a spigot is turned on that pumps water into the tank at a constant rate of \(1.25\) cubic feet per minute.
Figure 1.1.15. A spherical tank with a cylindrical chimney.
Let \(V\) denote the total volume of water (in cubic feet) in the tank at any time tt (in minutes), and hh the depth of the water (in feet) at time \(t\).
a. It is possible to use calculus to show that the total volume this tank can hold is \(V_{\text {full }}=\pi\left(22+\frac{38}{3} \sqrt{2}\right) \approx 119.12\) cubic feet. In addition, the actual height of the tank (from the bottom of the spherical base to the top of the chimney) is \(h_{\text {full }}=\sqrt{8}+5 \approx 7.83\) feet. How long does it take the tank to fill? Why?
b. On the blank axes provided below, sketch (by hand) possible graphs of how \(V\) and \(t\) change in tandem and how \(h\) and \(t\) change in tandem.
For each graph, label any ordered pairs on the graph that you know for certain, and write at least one sentence that explains why your graphs have the shape they do.
c. How would your graph(s) change (if at all) if the chimney was shaped like an inverted cone instead of a cylinder? Explain and discuss
Suppose we have a tank that is a perfect sphere with radius \(6\) feet. The tank is initially empty, but then a spigot is turned on that is pumping water into the tank in a very special way: the faucet is regulated so that the depth of water in the tank is increasing at a constant rate of \(0.4\) feet per minute.
Let \(V\) denote the total volume of water (in cubic feet) in the tank at any time \(t\) (in minutes), and hh the depth of the water (in feet) at given time \(t\).
a. How long does it take the tank to fill? What will the values of \(V\) and \(h\) be at the moment the tank is full? Why?
b. On the blank axes provided below, sketch (by hand) possible graphs of how \(V\) and \(t\) change in tandem and how hh and tt change in tandem.
For each graph, label any ordered pairs on the graph that you know for certain, and write at least one sentence that explains why your graphs have the shape they do.
c. How do your responses change if the tank stays the same but instead the tank is initially full and the tank drains in such a way that the height of the water is always decreasing at a constant rate of \(0.25\) feet per minute?
The relationship between the position, \(s\), of a car driving on a straight road at time \(t\) is given by the graph pictured at left in Figure 1.1.16 . The car's position 1 has units measured in thousands of feet while time is measured in minutes. For instance, the point \((4,6)\) on the graph indicates that after \(4\) minutes, the car has traveled \(6000\) feet from its starting location.
a. Write several sentences that explain the how the car is being driven and how you make these conclusions from the graph.
b. How far did the car travel between \(t=2\) and \(t=10\)?
c. Does the car ever travel in reverse? Why or why not? If not, how would the graph have to look to indicate such motion?
d. On the blank axes in Figure 1.1.16 , plot points or sketch a curve to describe the behavior of a car that is driven in the following way: from \(t=0\) to \(t=5\) the car travels straight down the road at a constant rate of \(1000\) feet per minute. At \(t=5\), the car pulls over and parks for \(2\) full minutes. Then, at \(t=7\), the car does an abrupt U-turn and returns in the opposite direction at a constant rate of \(800\) feet per minute for \(5\) additional minutes. As part of your work, determine (and label) the car's location at several additional points in time other than \(t=0,5,7,12\).
Figure 1.1.16. A graph of the relationship betwen a car's position \(s\) and time \(t\)