I general ALL power-lines exhibit resonances that vary with timeframes that are both long and short.
To see why all you have to do is realize that the power-line is subjected to many different loads, some of which are Inductive (motors), Capacitance (Fluorescent lights), resistive (heaters) to list just a few. Longer tem variations arise from people turning on loads, say a washing machine or lights and indeed even a change in the mechanical load seen by a motor will change what electrical load it presents to the power-lines. On shorter time frames, there is variation even on e a cycle to cycle basis as the sinusoidal waveform interacts with rectifiers, chopper circuits and switching power supplies.
You can see where a C load in parallel with a L load might form an easy resonance. This resonance might exist for long time frames, or the power-line may only see the C art of the resonance during part of the sinusoidal cycle. These L'and R' and C's are also distributed spatially thorough out a neighbourhood, so this ends up to be a seething complex time varying mess.
Buried cables, due primarily to the fact that the line and neutral wires are closer together tend to have higher capacitances than an air/pole mounted power-lines. That means that the resonances can be enhanced, depending upon the primary inductance that are present. Although it must be mentioned that it is possible that a buried cable can have fewer resonances also because of the increased capacitance. It all depends upon the mix of equipment and parasitic impedances.
They say a picture is worth a thousand words. And a handful of animated pictures...
All of these from Wikipedia. You can see these in context in the articles for Fourier transform, square wave, and Fourier series.
As it turns out, any periodic waveform can be represented by a Fourier series, although to represent it exactly may require an infinitely long series. In engineering practice, however, above a certain point continuing the series adds no additional useful precision, and we can call a finite series "good enough".
Direct answers to your questions:
How is it possible for something to generate a waveform across all frequencies by just looking at a waveform from one frequency?
I think your mental hangup here is "one frequency". The point of Fourier analysis is that a square wave (say, a 60 Hz square wave) is not just one frequency. I mean it is, in the sense that it's just a 60 Hz square wave. But we can also decompose that square wave into a number of sinusoidal waves, each with their own amplitude and phase.
Also, if harmonics are the changes in gain for other frequencies, why do I care about them if I'm running at a single constant frequency?
Because, through the lens of Fourier analysis, you aren't actually at a single constant frequency unless your waveform is a completely undistorted sine wave.
How can these changes from other frequencies affect something from another frequency?
In a linear and time invariant system, they can't. This is formally described in LTI system theory. Each frequency component passes through the system completely independently. We can consider what happens for one frequency, then separately consider what happens for another frequency. Adding the two together, we get the same result as if the two frequencies passed through the system simultaneously. This makes Fourier analysis a very useful analytical tool.
Also, is an RLC band-stop filter a good way of cleaning up the waveform by simply blocking out the frequency range where the harmonics are? How would you block out multiple frequency ranges since there's more than one bad harmonic?
If the problematic harmonics are in just one band, yes. In a power system, it's likely that you will be dealing with 60 or 50 Hz with some degree of harmonic distortion, meaning it will also contain frequency components at integer multiples of the fundamental. If you can design a filter that allows that fundamental frequency to pass, but attenuates all higher harmonics, then no matter how distorted the input, the output will be a pure, undistorted sine wave. In a power system you might also care about the phase of voltage and current (power factor), and there are filters to fix that too.
Best Answer
It's true because the voltage is sinusoidal and
sin(a).sin(b) = 1/2(cos(a-b)+cos(a+b))
And only in the case where a=b does the result have a mean value that is not zero.
so all harmonics give a result that has no effect on the real power