Continuous Extension of Function at Origin: Can f=1?

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    Continuous Extension
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Discussion Overview

The discussion centers on the continuity of a function defined on ℝ², specifically how to extend the function at the origin (0,0) to achieve continuity. The focus includes mathematical reasoning and exploration of different coordinate systems.

Discussion Character

  • Exploratory, Mathematical reasoning

Main Points Raised

  • One participant proposes that the function can be defined at the origin as f(0,0)=1 based on evaluations along specific paths.
  • Another participant agrees that defining f(0,0)=1 allows for a continuous extension of the function.
  • Several participants suggest switching to polar coordinates to analyze the function's behavior as it approaches the origin, leading to a transformation that simplifies the expression.
  • One participant reiterates the polar coordinate transformation and expresses gratitude for the discussion, while also introducing a new question related to a different thread.

Areas of Agreement / Disagreement

Participants generally agree that defining f(0,0)=1 leads to a continuous function, but the discussion includes multiple approaches and perspectives on how to analyze the function's behavior.

Contextual Notes

The discussion does not resolve potential limitations in the assumptions made during the evaluation of the function, particularly regarding the paths taken to approach the origin and the implications of switching to polar coordinates.

Alexx1
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How can the function

f: ℝ² → ℝ : (x,y) |--> {{x^2+y^2-(x^3y^3)}\over{x^2+y^2}} if (x,y) ≠ (0,0)

be defined in the origin so that we get a continuous function?When I take 'x=y' (so (y,y)) and 'y=x' (so (x,x)) I get:

{{2-y^4}\over{2}}

and

{{2-x^4}\over{2}}

So for the first one I get '1' when y=0
and for the second one I get '1' when x=0

So can I say that if (x,y)=0 --> f=1 ??
 
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Yes, you can extend your function to a continuous one if you define f(0,0)=1.
 
Petr Mugver said:
Yes, you can extend your function to a continuous one if you define f(0,0)=1.

Thx!
 
In order to make this general, you should switch to polar coordinates.

Then, we can transforme the fraction to:
\frac{r^{2}-r^{6}\sin^{3}\theta\cos^{3}\theta}{r^{2}}=1-r^{4}\sin^{3}\theta\cos^{3}\theta, r\neq{0}
clearly, this is readily extendable for r=0.
 
arildno said:
In order to make this general, you should switch to polar coordinates.

Then, we can transforme the fraction to:
\frac{r^{2}-r^{6}\sin^{3}\theta\cos^{3}\theta}{r^{2}}=1-r^{4}\sin^{3}\theta\cos^{3}\theta, r\neq{0}
clearly, this is readily extendable for r=0.

Thank you very much!
And how about this one?

https://www.physicsforums.com/showthread.php?t=421612
 

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