somewhere near the beginning.

Today in complex analysis…

Filed under: Mathematics — Alex @ 10:31 pm 2/22/2005

I completed the proof that I’ve been working on for about two weeks— if a sequence s_0, s_1, \ldots is bounded, and z is such that |z|<1, then the series \sum_{k=0}^\infty s_k z^k converges. The proposition itself didn’t interest me too much, it was the tools necessary to prove it that I wanted: the triangle inequality, the existence of supremums and infimums, and the nested interval theorem. After having taken 2 other upper level courses with Dr. Johnson, those (except the triangle inequality) are topics that we spend a lot of time on— we managed to free up a significant amount of time this semester for new material by proving all that stuff early on.

Dr. Johnson made two important observations that added further tools to the kit: first, in the process, we had shown that any infinite bounded set has a limit point, and second, as a consequence, Cauchy sequences converge. At least, Cauchy sequences converge if in the concerned number system it is true that every set bounded above has a least upper bound.

He also defined the Stieljes integral today, and gave a nice introductory/motivatory talk on it. Here’s my paraphrasal of his definition:

Let f,g: \C \rightarrow \C be such that [a,b] is within the intial set of f,g. Then f is said to be g integrable on [a,b] iff there is a number M and a subdivision S of [a,b] such that given c>0, for all subdivisions R of S,
 \left| M - \sum_{t=1}^m f(r_{2t}) \left[ g(r_{2t+1}) - g(r_{2t-1}) \right] \right| < c.

I think that gets the gist of it. One sweet thing about this integral is that it makes some of the vague mathematical statements made in the sciences more precise; his example was  m = \int \rho\, dv . If we’re considering a rod whose volume v(x) and density p(x) vary along its length, how would we do that integration except via the Stieljes integral? I almost wished I hadn’t completed all my required mechanics classes, so I could bust out with that one on a homework assignment :).

Actually, since we’re dealing with a physical phenomena, I suspect all the concerned functions would be differentiable, and the Stieljes integral could be reduced to the form m = \int \rho\, dv = \int \rho \frac{\partial v}{\partial x} dx . I suspect this mainly because as that difference between the g(r_i) decreases, the difference term would approach g^\prime (r) \Delta r. We’ll see; supposedly he’s going to add derivatives to the toolbox sometime soon.

Moore’s method is such a neat way to learn math.

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