Reversed limit definition for monotonic functions

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The discussion centers on the validity of a reversed delta-epsilon definition for limits in monotonic functions. Participants explore whether this definition, which states that for each δ there exists an ε such that certain conditions hold, effectively describes limits. There is agreement that while this approach may work for monotonic functions, it is problematic for non-monotonic functions due to the potential for multiple values of f(x) satisfying the ε condition without adhering to the δ constraint. Concerns are raised about the clarity and purpose of the definition, as it appears to focus more on monotonic behavior than on limits themselves. Overall, the conversation highlights the need for precision in mathematical definitions and the implications of monotonicity on limit behavior.
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Homework Statement



Does the delta-epsilon limit definition in reverse work for describing limits in monotonic functions?

By reversed, one means for

lim (x -> a) f(x) = L

if for each δ there corresponds ε such that

0 < | x-a | < δ whenever | f(x) - L | < ε.

Homework Equations

The Attempt at a Solution



I am thinking that it works, because this definition means that the range interval must lie within the domain interval, and it can be seen that shrinking δ also shrinks ε, which is how the usual definition works but in reverse.

I don't think this would work for non-monotonic functions because there can be many f(x) that satisfy
| f(x) - L | < ε but not | f(x) - L | < ε. Hopefully someone can also confirm this part too.

Thanks
 
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You can define whatever you like, as long as it is well defined. For this reason it should be helpful to indicate which variable depends on which and to explicitly write the quantors. If I read it correctly, then ##\varepsilon = \varepsilon(\delta)##. But then I have difficulties with the next line. I read ##\forall \, \delta \, \exists \, \varepsilon(\delta)\, : \,\vert \, f(x)-L\,\vert \, < \varepsilon(\delta) \Longrightarrow \,\vert \,x-a\,\vert \,< \delta \,##. The order of the quantors don't seem to reflect to the order of the conclusion. And how do you specify ##L##\,?

The remaining question is in any case: What for?
 
fresh_42 said:
You can define whatever you like, as long as it is well defined. For this reason it should be helpful to indicate which variable depends on which and to explicitly write the quantors. If I read it correctly, then ##\varepsilon = \varepsilon(\delta)##. But then I have difficulties with the next line. I read ##\forall \, \delta \, \exists \, \varepsilon(\delta)\, : \,\vert \, f(x)-L\,\vert \, < \varepsilon(\delta) \Longrightarrow \,\vert \,x-a\,\vert \,< \delta \,##. The order of the quantors don't seem to reflect to the order of the conclusion. And how do you specify ##L##\,?

I forgot the part where δ > 0 and ε > 0, so I think it would be written like this:

##\forall \, \delta \ > 0, \exists \, \varepsilon(\delta)\ > 0, : \,\vert \, f(x)-L\,\vert \, < \varepsilon(\delta) \Longrightarrow \, 0 < \vert \,x-a\,\vert \,< \delta \,##

L is the supposed limit.

lim (x -> a) f(x) = L

fresh_42 said:
The remaining question is in any case: What for?

I'm not very experienced in this type of math, so it's just a random inquiry.
 
It doesn't really make sense. You can have ##f(x) = L## for several points ##x## which can be far away from ##x=a##. That's where "what for" is needed. The way it is written now, is only confusing (IMO). It is more a condition of monotone behavior than on limits, because it says, ##\lim_{x \to a}f(x)=L## can only happen in a neighborhood of ##x=a## and nowhere else.
 
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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