- #1
pellman
- 684
- 5
One the things which always bugged me about the definition of the integral is that limit of a Reimann sums consists of a countably infinite number of terms, yet it is supposed to be giving the under area under a curve which varies in a continuous manner. Has anyone else thought seriously about this?
I suspect it is closely related to the fact some functions on a finite interval can be represented by a Fourier series.
[tex]f(x) =\frac{a_0}{2}+\sum_{n=1}^\infty\left[a_n cos(nx)+ b_n sin(nx)\right][/tex]
Here we see that a function f consisting of a continuum of points [tex]f(x)[/tex] is represented entirely by a countably infinite set of numbers [tex]\{a_0,a_1,...,b_1,b_2,...\}[/tex].
I'm not able to pose a coherent question about this. There is something interesting here but I can't get my head around putting it into words.
I'm interested in thoughts anyone cares to share on continuum vs countable. Is there a relation between integrable and able to be represented by a Fourier series?
I suspect it is closely related to the fact some functions on a finite interval can be represented by a Fourier series.
[tex]f(x) =\frac{a_0}{2}+\sum_{n=1}^\infty\left[a_n cos(nx)+ b_n sin(nx)\right][/tex]
Here we see that a function f consisting of a continuum of points [tex]f(x)[/tex] is represented entirely by a countably infinite set of numbers [tex]\{a_0,a_1,...,b_1,b_2,...\}[/tex].
I'm not able to pose a coherent question about this. There is something interesting here but I can't get my head around putting it into words.
I'm interested in thoughts anyone cares to share on continuum vs countable. Is there a relation between integrable and able to be represented by a Fourier series?