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We discussed this in another thread a while back, but I was never quite satisfied, although I let it drop. Now I’m wondering about it again.
The usual definition of a differentiable function of variables is that there is a linear map such that
We know that this implies the existence of all directional derivatives, i.e. for any vector we have a number , namely , such that
And the converse doesn’t hold, though it does if the partial derivatives are continuous. However, suppose we assume that all the directional derivatives exist at a given point, and moreover depend linearly on . I.e. there is a linear map such that for any vector we have
Does it follow that is differentiable? The difference between this and the first equation is that the first requires for each a neighborhood of in which the quantity is , whereas the second would allow a different 1-dimensional neighborhood in each direction.
Actually, my calculus book has a third definition: it says that a 2-variable function is differentiable at if there are functions and and a linear map (actually, it assumes that is given by the partial derivatives) such that
and where . I see how this implies the usual definition, but I don’t see how it’s equivalent to it.
Quick answer, could it be connected to the divided differences? We connected some references in this paper.
I think the answer to #1 is no if the function is allowed to be discontinuous in a neighborhood of the point. For instance, consider
at . Along we have , whose derivative at 0 is 0; thus all directional derivatives at are zero (hence in particular are given by a linear map). But since along every line , every neighborhood of contains points where is arbitrarily large.
@spitters, what is a divided difference? There’s only one appearance that I can find in the paper, which doesn’t define the term.
wikipedia. Sorry, I’ll try to write more tomorrow.
I glanced at wikipedia, but I couldn’t figure out what it might have to do with the question.
The difference between this and the first equation is that the first requires for each a neighborhood of in which the quantity is , whereas the second would allow a different 1-dimensional neighborhood in each direction.
So we need a sort of uniform differentiability, but uniform in the direction rather than in the point (as is actually meant by the term ‘uniformly differentiable’).
That’s what I was trying to say by “simultaneously in all directions” here. Granted, the discussion there allowed us to consider arbitrary curves rather than just lines through the origin, but your argument for it a couple comments down seemed to use only tangent vectors, so now I don’t believe it. Am I confused?
There is an answer to #2 here.
your argument for it a couple comments down seemed to use only tangent vectors
You mean the argument in #63 there, currently the penultimate comment?
I agree with you now; you have a perfect example of something which has a linear differential but is still not differentiable.
I am actually thinking this term of bring up Taylor series fairly early and saying that a function is times differentiable if it has a Taylor polynomial of degree up to with the remainder satisfying as . (Officially we don’t cover Taylor series in higher dimensions, but we do cover Taylor polynomials of degree up to , only not under that name, and I’ve always made it a point to mention that the results used there are a special case of a higher-dimensional Taylor’s Theorem.) I have until late next week to decide!
I would like to record this observation somewhere on the nLab. However, I’m at a bit of a loss for where to put it. Any ideas?
Looking at it again, I think maybe I would rather put it at differentiation, which is currently lacking a “lowbrow” perspective.
Okay, I changed my mind again and put it at differentiable map as you suggested. I also changed the redirect for derivative to point there rather than differentiation.
Looks good.
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