Representing higher order derivatives in terms of first derivatives problems:
\[\Large f'(x) = \lim_{h \to 0} \frac{f(x+\frac{h}{2})-f(x-\frac{h}{2})}{h}\] This is my derivative definition, so if we apply it again we get the second derivative like this: \[\small f''(x) = \lim_{h \to 0} \frac{1}{h}(\frac{f(x+\frac{h}{2}+\frac{h}{2})-f(x+\frac{h}{2}-\frac{h}{2})}{h}-\frac{f(x-\frac{h}{2}+\frac{h}{2})-f(x-\frac{h}{2}-\frac{h}{2})}{h})\] simplify a little we get: \[f''(x) = \lim_{h \to 0} \frac{1}{h^2}[f(x+h)+f(x-h)-2f(x)]\] So with a little rearranging we can show an interesting fact that the concavity is proportional the the difference between the function at a point and the average of the two adjacent points, but that's not really what I'm looking for, I want to take the third derivative now and get a result, so we continue on and we can simplify to something that looks like this: \[\ f'''(x) = \lim_{h \to 0} \frac{1}{h^2}\frac{f(x+\frac{3h}{2})-f(x-\frac{3h}{2})}{h}-\frac{3}{h^2}\frac{f(x+\frac{h}{2})-f(x-\frac{h}{2})}{h}\]
Can we write this final thing in terms of just ordinary derivatives? It is tempting to just rewrite it by a change of variables, but I don't know if it's possible or how I would do it.
If we apply the derivative a second time, I think we should end up with two limits.
They may be equivalent, but I'm not completely sure just yet.
So instead of combining the h's use separate variables, h, then k, etc? I am not sure either but it is an idea to play with.
Start like this, then use definition of derivatives:\[ \lim_{k\to 0}\frac{f'(x+k)-f'(x)}{k} \]
By changing variables and separating the limit into two parts we can have: \[\ f'''(x) = 216\lim_{h \to 0} \frac{1}{h^2}\frac{f(x+\frac{h}{2})-f(x-\frac{h}{2})}{h}-3\lim_{h \to 0}\frac{1}{h^2}\frac{f(x+\frac{h}{2})-f(x-\frac{h}{2})}{h}\] however I don't even know if I'm technically allowed to separate this limit or not.
I think that will just give essentially the same thing @wio I just kind of like looking from this perspective since I can sort of see symmetry a little easier.
Well for one, does the order of taking limits matter? You're assuming it doesn't when you merge them.
Order of taking limits? Is it even possible to take the second derivative before the first derivative?
I mean letting \(k\) goto \(0\) before \(h\) dies.
Well what is the difference between k and h?
If I switched them when you weren't looking you wouldn't tell. It's like if I have x and want to add 2. I can either add 1 first and then add 1 or I can add 1 then add 1 the other way around, and no one can tell the difference I think.
Start like this, then use definition of derivatives:\[ \lim_{k\to 0}\frac{f'(x+k)-f'(x)}{k} =\lim_{k\to 0}\lim_{h\to 0}\frac{f(x+h+k)-f(x+k)-f(x+h)+f(x)}{hk} \]
Sure, now replace h and k with each other, they are completely symmetric: \[ \lim_{k\to 0}\lim_{h\to 0}\frac{f(x+h+k)-f(x+k)-f(x+h)+f(x)}{hk} = \ \ \]\[ \lim_{h\to 0}\lim_{k\to 0}\frac{f(x+k+h)-f(x+h)-f(x+k)+f(x)}{kh} \]
So if they're symmetric then if follows that we can let \(h=k\) I suppose?
I think so, since I can imagine bringing h to 0 is the same as making k to 0 so in the hk-plane we should be able to just go straight to 0 in a single line |dw:1419023983100:dw|
I have seen it done before by a differential equations book I owned, but then again just because it works doesn't necessarily mean anything.
Were aren't taking them at the same time, we're taking them in order, which does make things easier.
We've already assumed that \(f'(x)\) exists.
Yeah this is all done based on the idea that all the higher derivatives we need exist, that's not important to worry about.
I think since we assume the derivatives exist, then we can use: \[ \lim_{x\to a}g(x) = b\land \lim_{x\to b}f(x) = L \implies \lim_{x\to a}f(g(x)) = L \]
In the case the function behaves relatively nicely, the two-limits of a second order derivative can be reduced to a single limit--but keep in mind this is the exception, not the rule. $$f''(x)=\frac{df'}{dx}=\lim_{\delta x\to0}\frac{f'(x+\delta x)-f'(x)}{\delta x}$$ ... is the general definition of the second derivative of a differentiable function \(f:\mathbb{R}\to\mathbb{R}\). If you're interested in similar limits for higher order derivatives then you should check out finite differences. http://en.wikipedia.org/wiki/Finite_difference
http://en.wikipedia.org/wiki/Finite_difference#Higher-order_differences In the limit as the step size or spacing goes to 0, the general formulae for the higher-order finite differences agree with the corresponding derivatives (for sufficiently well-behaved functions).
Okay, I'm curious as to what the exceptions are.
well behaved means \(C^1\)?
I think the exceptions would fall along the lines of \(f(x)\) is not differentiable and yet the higher order difference limit just so happens to exist.
I honestly didn't think too deeply about any particular conditions for 'well-behaved' but I figured I'd play it safe :-p I'll give it some thought.
but indeed, you can find more of these single-limit formulae using the n-th order finite differences and simply taking their limit as the step size goes to 0.
You're right. Proving anything complicated concerning limits ends but being a major battle.
Differentiable is a very high criterion, typically speaking.
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