Quote:
Originally Posted by Clem
1) Yes, but the convergence is only uniform when the original periodic function is continuous. Actually, the possible non-uniform convergence of Fourier series is an asset, because it allows them to expand a discontinuous function.
2) Even the first derivataive of the FS will be discontinuous.
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Yes indeed.. in fact I can see that my question (2) was a bit trite... in fact, not only is the first derivative not continuous, but the original function isn't even continuous(!).. LOL
Indeed, the derivative of a FS can be quite sensitive .. like you're saying the function whose derivative is being taken has to be continuous, and moreover the coefficients of the derived series tend to increase by a factor of (n) each time you take a derivative, which raises the risk of whether or not the derived series is going to converge of not.
Specifically, for the function f(x)=e^x defined on [0,2*pi] (2-pi periodic), the Fourier coefficients I arrived at are:
a(0) = (e^(2pi)-1)/(2pi)
a(n) = (e^(2pi)-1)/(pi*(1+n^2))
b(n) = (-n)*(e^(2pi)-1)/(pi*(1+n^2))
where a(n) is the coefficient for cos(n*x) and b(n) is the coefficient for sin(n*x). Plotting a couple sums for this series out, the series seems to converge to e^x (if slowly .. probably b/c of the b(n) coefficients which only tend to zero as 1/n). All of which is to say, differentiating this series term-by-term, we see that the "derivated" b(n) (which is actually going to be the coefficent for cos(n*x) in the derived series) has a n^2 in both the numerator and denominator.. In other words, its not clear that by taking the term-by-term derivative of the function will produce a series that even converges.
Conversely, though, integration is not nearly as sensitive an operation to perform on FS as differentiation is it? The function whose FS is being integrated does not need to be continuous, and the coefficients of the integrated series will be ~ (1/n) the size of the coefficients of the original series, so the terms will tend to zero (i.e., the series will converge) even faster than the series for the original function.
This raises a couple question for me:
1) Suppose we generate a "FS" for periodic function, but FS doesn't even converge. Can we "integrate" this function (and integrate the FS term-by-term), and arrive at a FS expression for the integrated function that *does* converge (perhaps uniformly, if the integrated function is continuous, even though the original function might not have been)?
2) I tried to apply this to the expression I derived above for e^x.. which is to say, integrate term-by-term the expression I obtained for the FS expansion of e^x on [0,2pi]. The FS converges, but it doesn't really seem to converge to anything that resembles e^x on [0,2pi]. Is the problem the same thing that was encountered going in the other direction? Namely that the integral of e^x on [0,2pi] is *not* e^x? Or is there something else preventing the term-by-term integration of this function? Or did I just do the calculation incorrectly?