For a general limit the ϵ−δ definition of a limit (the formal definition of a limit) states that
lim
However the \epsilon -\delta definition of a limit changes for limits as x \to +\infty and x \to -\infty, and it changes again for limits that evaluate to +\infty and -\infty
1. Limit as x \to +\infty
\lim_{x \ \to \ +\infty} f(x) = L \Leftrightarrow \forall \ \epsilon>0\; (\exists \ \delta : (\;x>\delta\implies |f(x) - L|\leq\epsilon))
2. Limit as x \to -\infty
\lim_{x \ \to \ -\infty} f(x) = L \Leftrightarrow \forall \ \epsilon>0\; (\exists \ \delta : (\;x<\delta\implies |f(x) - L|\leq\epsilon))
3. Limit evaluating to +\infty
\lim_{x \ \to \ a} f(x) = +\infty \Leftrightarrow \forall M > 0 \ (\exists \ \delta > 0 \ : \ (0<|x-a|<\delta \implies f(x) >M)
4. Limit evaluating to -\infty
\lim_{x \ \to \ a} f(x) = -\infty \Leftrightarrow \forall N < 0 \ (\exists \ \delta > 0 \ : \ (0<|x-a|<\delta \implies f(x) < N)
But why is that so? I understand that if you use the normal \epsilon-\delta definition of a limit in these cases, you get contradictions that pop up like 0 < |x-\infty| < \delta \implies \delta > \infty, which you cannot do anything further with.
While some of these differences might be subtle, it just seems counter-intuitive to change a formal and general definition.
I know that the fundamental idea behind the \epsilon - \delta definition remains the same throughout all of these examples (that no matter how small we want to make our "error distance" (\epsilon) we can always find a "distance to our limit point" (\delta) that satisfies the definition of a limit) , but to get to that fundamental idea, the \epsilon - \delta definition has to be subtly modified (and I'm not referring to modifications in notation) for each of these examples.
Or is it just a case that the \epsilon - \delta definition for the general limit I put at the very start of this post is not as general as I thought?
Furthermore, how does the \epsilon - \delta definition of a limit change for these cases, (the formal definitions of these don't seem to be covered in any introductory Calculus textbook).
5. Limit as x \to +\infty = +\infty
\lim_{x \ \to \ +\infty} f(x) = +\infty \Leftrightarrow \ ???
6. Limit as x \to -\infty = -\infty
\lim_{x \ \to \ -\infty} f(x) = -\infty \Leftrightarrow \ ???
7. Limit as x \to -\infty = +\infty
\lim_{x \ \to \ -\infty} f(x) = +\infty \Leftrightarrow \ ???
8. Limit as x \to +\infty = -\infty
\lim_{x \ \to \ +\infty} f(x) = -\infty \Leftrightarrow \ ???
Answer
To understand this, you need to think of the intuition behind the \epsilon-\delta definition. We want \lim_{x\to a}f(x)=L if we can make f(x) as close to L as we like by making x sufficiently close to a. Worded differently, we might say that:
\lim_{x\to a}f(x)=L if given any neighborhood U of L, there is a neighborhood V of a such that elements of V are mapped by f to elements of U (except possibly a itself).
In this context, a "neighborhood" of a point p should be understood to mean "points sufficiently close to p". Let's make that precise by defining what we mean by "close". For \epsilon>0 (assumed, but not required, to be very small) define
B(x,\epsilon):=\{y\,:\,|x-y|<\epsilon\},
the ball of radius \epsilon about x. For our purposes, we say U is a neighborhood of x if U=B(x,\epsilon) for some \epsilon>0. (The usual definition only requires that U contains such a ball.) Assuming \epsilon>0 is very small, this agrees with our intuition of what closeness should mean. Now if we go back to our neighborhood "definition" of a limit, you should be able to think about it for a bit and convince yourself that it is equivalent to the usual definition.
How does this relate to the problem with infinity? Given that infinity is not a real number (and things like distance from infinity do not make sense), we must revise what it means to be "close" to infinity. So for M>0 (assumed this time to be very large) define
B(+\infty,M):=\{y\,:\,y>M\},\quad B(-\infty,M):=\{y\,:\,y<-M\},
the neighborhoods of \pm\infty. Hopefully you can see why these make sense as definitions; a number should be close to infinity if it is very large (with the correct sign), so a neighborhood of infinity should contain all sufficiently large numbers.
Now we extend our neighborhood definition of limits to include the case where a or L can be \pm\infty. It is a similar exercise to before to verify now that the definition is still equivalent to the old one, only now we have in some sense unified somewhat.
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