sutupidmath said:
THis looks cute, although i do not understand a damn thing what u did! I mean i haven't yet dealt with double integrals!
EDIT: Note: Read the article D H posted, and not the gibberish below.
Honestly, I can't believe I remembered how to do it. I've seen it a couple of times in class. To me it is, a trick.
But here's the jist of it. That x^2 looks like a beast, and integrating from -infinity to infinity seems like a problem.
We know that if we multiply two exponentials e^u*e^y we get e^(u+y). So when we multiply the two integrals together and get x^2+y^2 this should be screaming, convert me into polar coordinates.
So we multiply the two integrals together, and convert the x^2+y^2 into r^2.
First though, why is that even possible? Well remember that when you integrate with "numbers" you get a number. What I mean by this is the following.
If we integrate \int_0^1 x dx we get a number right? What about when we integrate \int_0^u x dx? Well the second case returns a function dependent on u.
So in the first case, \int_0^1 x dx, why not just call this a number, how about I. So this makes sense to be able to multiply two numbers together, eg. I\timesI = \int_0^1 x dx \times \int_0^1 x dx [/tex]. Think about why we can "push" them together. <br />
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I think the most interesting part about it, was changing to polar coordinates. The part where we change from sweeping out -infinity to infinity in the x and y direction in rectangular coordinates to sweeping out all values by rotating from 0 to 2pi and extending the "arm" from 0 to infinity.