Fourier Series, what I'm trying to currently cram...
Really what it's doing is, say if we have a function
 & =\begin{cases}<br />1 & \text{if }-\frac{\pi}{2}<x<\frac{\pi}{2}<br />\\ -1 & \text{if }\frac{\pi}{2}<x<\frac{3\pi}{2}<br />\end{cases}\end{alignedat})
Then we can represent it as a single function, not a hybrid function by taking adding together a lot of functions and coefficients represented by a basis from the fourier series for it. So we're representing one a repeating function with another function. The more terms we take the closer it will be to the actual function.
e.g. Stolen from wiki.
Anyways, one of the main applications that we're looking at is, is applying it to find the solution to the Heat Equation (below is 1-D heat equation).

Now if we have some function that represents the distribution of temperatures at points along a 1-D rod, then our solution (not going to include the derivation, procrastinating but can't procrastinate for that long

) will be off the form:
 & =\underset{n=1}{\overset{\infty}{\sum}}D_{n}e^{-\left(\frac{n^{2}\pi^{2}\hat{\kappa}}{L^{2}}\right)t}\sin\left(\frac{n\pi x}{L}\right)\end{alignedat})
Which we get by using a separation of variables method for the PDE, in which we get a solution with just one of the terms in the sum of above, to get a more general solution we take a linear combination of all possible solutions, which results in the equation above.
Now lets say we have the Initial condition,
=f(x))
, then we get a Fourier Sine Series.
 & =\underset{n=1}{\overset{\infty}{\sum}}D_{n}\sin\left(\frac{n\pi x}{L}\right)\end{alignedat})
Which means we need to find the coefficients

, by applying our techniques for Fourier Series.
I'm not sure if that's how you'd be looking at it, or what the point of looking into it for what you're doing, but it's one motivation to use it anyways.
Sorry about being a bit vague though, really can't afford to procrastinate for too long.
EDIT: Added a bit, really crap explanation though....
* hands over to TrueTears/rife168