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In this section we are going to take a look at two fairly
important problems in the study of calculus.
There are two reasons for looking at these problems now.
First, both of these problems will lead us into the study of
limits, which is the topic of this chapter after all. Looking at these problems here will allow us
to start to understand just what a limit is and what it can tell us about a
function.
Secondly, the rate of change problem that we’re going to be
looking at is one of the most important concepts that we’ll encounter in the
second chapter of this course. In fact,
it’s probably one of the most important concepts that we’ll encounter in the
whole course. So looking at it now will
get us to start thinking about it from the very beginning.
Tangent Lines
The first problem that we’re going to take a look at is the
tangent line problem. Before getting
into this problem it would probably be best to define a tangent line.
A tangent line to the function f(x) at the point 
is a line that just touches the graph of the
function at the point in question and is “parallel” (in some way) to the graph
at that point. Take a look at the graph
below.

In this graph the line is a tangent line at the indicated
point because it just touches the graph at that point and is also “parallel” to
the graph at that point. Likewise, at
the second point shown, the line does just touch the graph at that point, but
it is not “parallel” to the graph at that point and so it’s not a tangent line
to the graph at that point.
At the second point shown (the point where the line isn’t a
tangent line) we will sometimes call the line a secant line.
We’ve used the word parallel a couple of times now and we
should probably be a little careful with it.
In general, we will think of a line and a graph as being parallel at a
point if they are both moving in the same direction at that point. So, in the first point above the graph and
the line are moving in the same direction and so we will say they are parallel
at that point. At the second point, on
the other hand, the line and the graph are not moving in the same direction and
so they aren’t parallel at that point.
Okay, now that we’ve gotten the definition of a tangent line
out of the way let’s move on to the tangent line problem. That’s probably best done with an example.
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Example 1 Find
the tangent line to  at x =
1.
Solution
We know from algebra that to find the equation of a line
we need either two points on the line or a single point on the line and the
slope of the line. Since we know that
we are after a tangent line we do have a point that is on the line. The tangent line and the graph of the
function must touch at x = 1 so the
point  must be on the line.
Now we reach the problem.
This is all that we know about the tangent line. In order to find the tangent line we need
either a second point or the slope of the tangent line. Since the only reason for needing a second
point is to allow us to find the slope of the tangent line let’s just
concentrate on seeing if we can determine the slope of the tangent line.
At this point in time all that we’re going to be able to
do is to get an estimate for the slope of the tangent line, but if we do it
correctly we should be able to get an estimate that is in fact the actual
slope of the tangent line. We’ll do
this by starting with the point that we’re after, let’s call it  . We will then pick another point that lies
on the graph of the function, let’s call that point  .
For the sake of argument let’s take choose  and so the second point will be  . Below is a graph of the function, the
tangent line and the secant line that connects P and Q.
We can see from this graph that the secant and tangent
lines are somewhat similar and so the slope of the secant line should be
somewhat close to the actual slope of the tangent line. So, as an estimate of the slope of the
tangent line we can use the slope of the secant line, let’s call it  ,
which is,


Now, if we weren’t too interested in accuracy we could say
this is good enough and use this as an estimate of the slope of the tangent
line. However, we would like an
estimate that is at least somewhat close the actual value. So, to get a better estimate we can take an
x that is closer to  and redo the work above to get a new
estimate on the slope. We could then
take a third value of x even closer
yet and get an even better estimate.
In other words, as we take Q closer and closer to P
the slope of the secant line connecting Q
and P should be getting closer and
closer to the slope of the tangent line.
If you are viewing this on the web, the image below shows this
process.

As you can see (if you’re reading this on the web) as we
moved Q in closer and closer to P the secant lines does start to look
more and more like the tangent line and so the approximate slopes (i.e. the slopes of the secant lines)
are getting closer and closer to the exact slope. Also, do now worry about how I got the
exact or approximate slopes. We’ll be
computing the approximate slopes shortly and we’ll be able to compute the
exact slope in a few sections.
In this figure we only looked at Q’s that were to the right of P, but we could have just as easily used Q’s that were to the left of P and we would have received the same
results. In fact, we should always
take a look at Q’s that are on both
sides of P. In this case the same thing is happening on
both sides of P. However, we will eventually see that
doesn’t have to happen. Therefore we
should always take a look at what is happening on both sides of the point in
question when doing this kind of process.
So, let’s see if we can come up with the approximate
slopes I showed above, and hence an estimation of the slope of the tangent
line. In order to simplify the process
a little let’s get a formula for the slope of the line between P and Q,  ,
that will work for any x that we
choose to work with. We can get a
formula by finding the slope between P
and Q using the “general” form of  .

Now, let’s pick some values of x getting closer and closer to  ,
plug in and get some slopes.
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x
|

|
x
|

|
|
2
|
-6
|
0
|
-2
|
|
1.5
|
-5
|
0.5
|
-3
|
|
1.1
|
-4.2
|
0.9
|
-3.8
|
|
1.01
|
-4.02
|
0.99
|
-3.98
|
|
1.001
|
-4.002
|
0.999
|
-3.998
|
|
1.0001
|
-4.0002
|
0.9999
|
-3.9998
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So, if we take x’s to
the right of 1 and move them in very close to 1 it appears that the slope of
the secant lines appears to be approaching -4. Likewise, if we take x’s to the left of 1 and move them in very
close to 1 the slope of the secant lines again appears to be approaching -4.
Based on this evidence it seems that the slopes of the
secant lines are approaching -4 as we move in towards  ,
so we will estimate that the slope of the tangent line is also -4. As noted above, this is the correct value
and we will be able to prove this eventually.
Now, the equation of the line that goes through  is given by

Therefore, the equation of the tangent line to  at x = 1
is

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There are a couple of important points to note about our
work above. First, we looked at points
that were on both sides of 
. In this kind of process it is important to
never assume that what is happening on one side of a point will also be
happening on the other side as well. We
should always look at what is happening on both sides of the point. In this example we could sketch a graph and
from that guess that what is happening on one side will also be happening on
the other, but we will usually not have the graphs in front of us or be able to
easily get them.
Next, notice that when we say we’re going to move in close
to the point in question we do mean that we’re going to move in very close and
we also used more than just a couple of points.
We should never try to determine a trend based on a couple of points
that aren’t really all that close to the point in question.
The next thing to notice is really a warning more than
anything. The values of 
in this example were fairly “nice” and it was
pretty clear what value they were approaching after a couple of
computations. In most cases this will
not be the case. Most values will be far
“messier” and you’ll often need quite a few computations to be able to get an
estimate.
Last, we were after something that was happening at 
and we couldn’t actually plug 
into our formula for the slope. Despite this limitation we were able to
determine some information about what was happening at 
simply by looking at what was happening around

. This is more important than you might at
first realize and we will be discussing this point in detail in later sections.
Before moving on let’s do a quick review of just what we did
in the above example. We wanted the
tangent line to 
at a point 
. First, we know that the point 
will be on the tangent line. Next, we’ll take a second point that is on
the graph of the function, call it 
and compute the slope of the line connecting P and Q as follows,
We then take values of x
that get closer and closer to 
(making sure to look at x’s on both sides of 
and use this list of values to estimate the
slope of the tangent line, m.
The tangent line will then be,
Rates of Change
The next problem that we need to look at is the rate of
change problem. This will turn out to be
one of the most important concepts that we will look at throughout this course.
Here we are going to consider a function, f(x), that represents some quantity that
varies as x varies. For instance, maybe f(x) represents the amount of water in a holding tank after x minutes. Or maybe f(x)
is the distance traveled by a car after x
hours. In both of these example we used x to represent time. Of course x
doesn’t have to represent time, but it makes for examples that are easy to
visualize.
What we want to do here is determine just how fast f(x) is changing at some point, say 
. This is called the instantaneous rate of change or sometimes just rate of change of f(x) at

.
As with the tangent line problem all that we’re going to be
able to do at this point is to estimate the rate of change. So let’s continue with the examples above and
think of f(x) as something that is
changing in time and x being the time
measurement. Again x doesn’t have to represent time but it will make the explanation a
little easier. While we can’t compute
the instantaneous rate of change at this point we can find the average rate of
change.
To compute the average rate of change of f(x) at 
all we need to do is to choose another point,
say x, and then the average rate of
change will be,
Then to estimate the instantaneous rate of change at 
all we need to do is to choose values
of x getting closer and closer to 
(don’t forget to chose them on both sides of 
) and compute values of A.R.C.
We can then estimate the instantaneous rate of change form that.
Let’s take a look at an example.
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Example 2 Suppose
that the amount of air in a balloon after t
hours is given by

Estimate the instantaneous rate of change of the volume
after 5 hours.
Solution
Okay. The first
thing that we need to do is get a formula for the average rate of change of
the volume. In this case this is,

To estimate the instantaneous rate of change of the volume
at  we just need to pick values of t that are getting closer and closer
to  . Here is a table of values of t and the average rate of change for
those values.
|
t
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A.R.C.
|
t
|
A.R.C.
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|
6
|
25.0
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4
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7.0
|
|
5.5
|
19.75
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4.5
|
10.75
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5.1
|
15.91
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4.9
|
14.11
|
|
5.01
|
15.0901
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4.99
|
14.9101
|
|
5.001
|
15.009001
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4 | |