2. 2
Example 1
Suppose that a ball is dropped from the upper observation
deck of the CN Tower in Toronto, 450 m above the ground.
Find the velocity of the ball after 5 seconds.
Solution:
Galileo discovered that the distance fallen by any freely
falling body is proportional to the square of the time it has
been falling. (This model for free fall neglects air
resistance.)
3. 3
Example 1 – Solution
If the distance fallen after t seconds is denoted by s(t) and
measured in meters, then Galileo’s law is expressed by the
equation
s(t) = 4.9t2
cont’d
4. 4
Example 1 – Solution cont’d
However, we can approximate the desired quantity by
computing the average velocity over the brief time interval
of a tenth of a second from t = 5 to t = 5.1:
5. 5
Example 1 – Solution
The table shows the results of similar calculations of the average
velocity over successively smaller time periods.
It appears that as we shorten the time period, the average velocity is
becoming closer to 49 m/s.
cont’d
6. 6
Example 1 – Solution
The instantaneous velocity when t = 5 is defined to be
the limiting value of these average velocities over shorter
and shorter time periods that start at t = 5.
Thus the (instantaneous) velocity after 5 s is
cont’d
9. 9
Intuitive Definition of a Limit
The values of f(x) tend to get closer and closer to the
number L as x gets closer and closer to the number a (from
either side of a) but x a.
Notice the phrase “but x a” in the definition of limit. This
means that in finding the limit of f(x) as x approaches, we
never consider x = a.
In fact, f(x) need not even be defined when x = a.
The only thing that matters is how f is defined near a.
10. 10
Example 2
Guess the value of
Solution:
Notice that the function is not
defined when x = 1, but that doesn’t matter because the
definition of says that we consider values of x
that are close to a but not equal to a.
11. 11
Example 2 – Solution
The tables below give values of f(x) (correct to six decimal
places) for values of x that approach 1
(but are not equal to 1).
cont’d
12. 12
Example 2 – Solution
On the basis of the values in the tables, we make the
guess that
cont’d
13. 13
Example 4
Guess the value of
Solution:
The function is not defined when x = 0.
Using a calculator (and remembering that, if , sin x
means the sine of the angle whose radian measure is ), we
construct the table of values correct to eight decimal
places.
14. 14
Example 4 – Solution
From the table below and the graph in Figure 6 we guess
that
cont’d
Figure 6
16. 16
Example 6
Its graph is shown in Figure 8.
As t approaches 0 from
the left, H(t) approaches 0.
As t approaches 0 from the right, H(t) approaches 1. There
is no single number that H(t) approaches as t approaches
0.
Therefore does not exist.
cont’d
Figure 8
18. 18
One-sided Limits
We noticed in Example 6 that H(t) approaches 0 as t
approaches 0 from the left and H(t) approaches 1 as t
approaches 0 from the right.
We indicate this situation symbolically by writing
The symbol indicates that we consider only
values of t <0. Likewise, indicates that we
consider only values of t > 0.
20. 20
One-sided Limits
Similarly, if we require that x be greater than a, we get “the
right-hand limit of f(x) as x approaches a is equal to L”
and we write
Thus the symbol means that we consider only
x > a.
23. 23
Example 7
The graph of a function g is shown in Figure 10. Use it to
state the values (if they exist) of the following:
(a) (b) (c)
(d) (e) (f)
Figure 10
24. 24
Example 7 – Solution
From the graph we see that the values of g(x) approach 3
as x approaches 2 from the left, but they approach 1 as x
approaches 2 from the right.
Therefore
(a) and (b)
(c) Since the left and right limits are different, we conclude
from that does not exist.
25. 25
Example 7 – Solution
The graph also shows that
(d) and (e)
(f) This time the left and right limits are the same and so,
by , we have
Despite this fact, notice that g(5) 2.
cont’d
27. 27
Precise Definition of a Limit
We want to express, in a quantitative manner, that f(x) can
be made arbitrarily close to L by taking x to be sufficiently
close to a (but x a).
This means that f(x) can be made to lie within any
preassigned distance from L (traditionally denoted by ε, the
Greek letter epsilon) by requiring that x be within a
specified distance (the Greek letter delta) from a.
That is, Notice
that we can stipulate that x a by writing
29. 29
Precise Definition of a Limit
Definition 4 is illustrated in Figures 12 –14.
If a number ε > 0 is given, then we draw the horizontal lines
and the graph of f. (See Figure
12.)
Figure 12
30. 30
Precise Definition of a Limit
If then we can find a number > 0 such
that if we restrict x to lie in the interval and
take
x a, then the curve y = f(x) lies between the lines
(See Figure 13.) You can see that
if such a has been found, then any smaller will also
work.
Figure 13
31. 31
Precise Definition of a Limit
It’s important to realize that the process illustrated in
Figures 12 and 13 must work for every positive number ε,
no matter how small it is chosen.
Figure 12 Figure 13
32. 32
Precise Definition of a Limit
Figure 14 shows that if a smaller ε is chosen, then a
smaller may be required.
Figure 14
33. 33
Example 9
Prove that
Solution:
Let ε be a given positive number. According to Definition 4
with a = 3 and L = 7, we need to find a number such that
Therefore we want:
34. 34
Example 9 – Solution
Note that
So let’s choose
We can then write the following:
Therefore, by the definition of a limit,
cont’d