As someone who has no prior experience with the \epsilon - \delta definition of limit, I
will teach myself about them with the help of my favourite math textbook and some creativity. This is what I gleaned so far.
In high school, we calculate limits. In university, we like to think that we are sophisticated thinkers. Knowing how to calculate is not enough for us. We must know why our calculation is correct. Then we need a definition to work with. This is where the the \epsilon - \delta definition
of limit comes in:
Let f:X \to R be a function, L \in R, a \in X and X \subseteq R. Then
\lim_{x \to a} f(x)
= L \iff
\forall \epsilon \in R^+, \exists \delta \in R^+, (\forall x \in R, |x - a| < \delta \implies |f(x) - L| < \epsilon).
After digesting this definition, we can prove or disprove
statements about the limits of functions.
For example, consider the following statement:
\lim_{x \to 2} x^2 = 4
By substituting two into x, we
discover that this statement should be true.
To show that our hunch is correct, we plug in a = 2 and L = 4 into
the \epsilon - \delta definition and prove it:
\forall \epsilon \in R^+,
\exists \delta \in R^+, (\forall x \in R, |x - 2| < \delta \implies |x^2 – 4|
< \epsilon)
Our value for \epsilon will be
arbitrary but our value for \delta must be concrete since \epsilon has a
\forall quantifier but \delta has a \exists quantifier. The hard part is choosing \delta. How do we do it?
Where to Start
Think
of \epsilon as a distance from L on the vertical axis and \delta as a
distance from 2 on the horizontal axis.
Once the distance of x from 2 is less than \delta on the
horizontal, then the \epsilon – \delta definition of limit guarantees
that the distance of x^2 from 4 is less than \epsilon on the vertical. Hence, our choice of \delta must satisfy
the definition for all \epsilon. To
achieve this, we express \delta in terms of \epsilon, which is done by working backwards from the definition.
How to Work Backwards
Since the definition is an implication, then working backwards begins with the
consequent:
|x^2 - 4| <
\epsilon
Since we operate in R, then we can manipulate
the left side of the inequality:
|x + 2||x - 2| =
|x^2 - 4| < \epsilon
We see that the |x - 2| in |x + 2||x - 2| < \epsilon will be useful in getting the antecedent of the definition, which is |x - 2| < \delta. However, there is still a bit of baggage to unload.
The Creative Step
Since we choose
our \delta, then we can give it an upper bound. For simplicity, we choose 1 as an upper
bound for \delta. So if |x - 2| < d, then |x - 2| < 1.
From |x - 2| < 1, the absolute value definition gives -1 < x - 2 < 1. By adding 4 to all sides of the inequality, then we have 3 < x + 2 < 5. Use the absolute value definition again, which gives us |x + 2| < 5.
From |x - 2| < 1, the absolute value definition gives -1 < x - 2 < 1. By adding 4 to all sides of the inequality, then we have 3 < x + 2 < 5. Use the absolute value definition again, which gives us |x + 2| < 5.
Now we can unload |x + 2| from |x
+ 2||x - 2| < \epsilon. Since |x + 2|
< 5, then |x + 2||x - 2| < 5|x - 2|.
Then 5|x - 2| < e is equivalent to |x - 2| < \frac{\epsilon}{5}.
Endgame
We can now chose \delta. If |x - 2| < \frac{\epsilon}{5} is true,
then its equivalent statement 5|x - 2| < e guarantees that |x - 2||x + 2|
= |x^2 - 4| < \epsilon since |x - 2| < 5. Yet we chose 1 as an upper bound for \delta. So if \frac{\epsilon}{5}>1,
then \delta = 1. Hence our choice of \delta
is min(1, \frac{\epsilon}{5}). The
proof follows naturally from the scratch work so it will be omitted.
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