Understanding the solution to a calculus problem (removable discontinuities)

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    Calculus Spivak
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The discussion revolves around proving the continuity of the function g, defined as the limit of f at points of removable discontinuities. Participants clarify that since f(y) is bounded within g(a) ± ε for y near a, applying the limit as y approaches x leads to the conclusion that g(x) also remains within those bounds. This transition from strict inequalities to inclusive inequalities is emphasized as a key step in the proof. The conversation highlights the importance of understanding local behavior in limits and continuity. Overall, the problem illustrates the nuances of calculus related to limits and continuity at points of discontinuity.
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Homework Statement


The problem (Spivak's Calculus, chapter 6, problem 17):
"Let ##f## be a function with the property that every point of discontinuity is a removable discontinuity. This means that ##\underset {y \rightarrow x} {\lim} {f(y)}## exists for all ##x##, but ##f## may be discontinuous at some (even infinitely many) numbers ##x##. Define ##g(x)=\underset {y \rightarrow x} {\lim} {f(y)}##. Prove that ##g## is continuous."

After struggling with articulating a proof, I checked the answer, which I understood except for the last part:
"Since ##g(a)=\underset {y \rightarrow a} {\lim} {f(y)}##, by definition, it follows that for every ##\epsilon>0## there is a ##\delta>0## such that ##|f(y)-g(a)|<\epsilon## for ##|y-a|<\delta##. This means that
##g(a)-\epsilon<f(y)<g(a)+\epsilon## for ##|y-a|<\delta##."

I understand everything in this part, the next part is where I struggle:
"So if ##|x-a|<\delta##, we have
##g(a)-\epsilon≤\underset {y \rightarrow x} {\lim} f(y)≤g(a)+\epsilon##
which shows that ##|g(x)-g(a)|≤\epsilon## for all ##x## satisfying ##|x-a|<\delta##. Thus ##g## is continuous at ##a##."

I don't understand how he made the leap from ##g(a)-\epsilon<f(y)<g(a)+\epsilon## for ##|y-a|<\delta## to ##g(a)-\epsilon≤\underset {y \rightarrow x} {\lim} f(y)≤g(a)+\epsilon## for ##|x-a|<\delta##. It makes intuitive sense, if the values of ##f## in the interval are all bounded it's pretty obvious that the limit of ##f## at any given point will also be within the bounds (since the values of ##f## for ##x##'s arbitrarily close to it are within the bounds). But I can't find a reasonable mathematical proof of it.

Homework Equations


Continuity definiton: ##\underset {x \rightarrow a} {\lim} {f(x)} = f(x)##

The Attempt at a Solution


After racking my brain at this for several hours I eventually came up with a stupidly long proof, which is not even complete since it relies on the idea that a bounded function always has a point of least value ##f(x')## within an interval ##b_1≤x≤b_2## such that ##f(x')≤f(x)## for all ##x## in ##b_1≤x≤b_2##, an idea which I have not proven yet and probably can't at this point. Even if I did, I am pretty sure that there is a much simpler explanation considering the fact that Spivak allowed himself to skip it completely... It's important to note that at this point the book only covered up to limits and basic ideas of continuity, no derivatives, integrals, series or anything of the sort.
Help on the matter would be very appreciated.
 
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This is a great problem actually. I remember when I solved it the first time. You can't go wrong with Spivak. Well, let's get to the question.

We know:

##|y-a| < \delta \implies g(a)-\epsilon < f(y) < g(a) + \epsilon##

Thus, in some neighborhood of ##a##, this inequality is satisfied. Limits are something local. What happens when you apply ##\lim_{y \to x}## to these inequalities? Do you then see why we get ##\leq## instead of ##<##?

Assuming third edition, problem 12 of the limit chapter (chapter 5) is certainly relevant.
 
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Math_QED said:
This is a great problem actually. I remember when I solved it the first time. You can't go wrong with Spivak. Well, let's get to the question.

We know:

##|y-a| < \delta \implies g(a)-\epsilon < f(y) < g(a) + \epsilon##

Thus, in some neighborhood of ##a##, this inequality is satisfied. Limits are something local. What happens when you apply ##\lim_{y \to x}## to these inequalities? Do you then see why we get ##\leq## instead of ##<##?

Assuming third edition, problem 12 of the limit chapter (chapter 5) is certainly relevant.
Oh damn, I've done that question (I'm doing all of them in order) and it still went over my head. Since ##g(a)±\epsilon## is constant given a specific ##a## and ##\epsilon##, it's limit is that same constant, and by problen 12 your inequality arises.

Thanks for the help.
 
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Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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