| I can't resist not showing this clever derivation of the e Maclaurin series. I referenced the fact that e^x = 1 + x/1 + x^2/(2!) + x^3/(3!) + ... Now, one of the many equivalent definitions of e is that it is the only real number for which this holds: d/dt (e^t) = e^t This means that e^t is a real function which is so smooth, that no matter how many times you differentiate it, you always get the same function (it turns out that it is the only such real function) Now, we know that e^0 = 1 (since x^0 = 1, where x != 0). Therefore, in its Maclaurin series, the only term not depending on x should therefore be 1 (otherwise e^0 wouldn't be 1). So know we know that e^x looks something like this: e^x = 1 + (something) Now we can ask ourselves which this question: since d/dx e^x = e^x, what must also be in the e^x series, if 1 belongs to it? Well, whatever differentiates to 1, so now we know that e^x = 1 + x + (something) (because d/dx (1 + x + something) = 1 + x + d/dx something) Now we can again ask this question for our current form; what must we differentiate in order to obtain 1 + x? And thus we get e^x = 1 + x + x^2/2 + something This way, if we write the two (equivalent) series this way: e^x = 1 + x + x^2/2 +
d/dx e^x = 1 + x + x^2/2 + x^3/(2*3) + And we can complete it with the infinite Maclaurin series. Now this is less formal than it should be and it would probably make the formalists cringe, but I hope you get the idea. You can actually apply the same principle for sin x and cos x, except in their case, they're actually mutually derived from each other. I'll leave that as an exercise for the reader (oh how fun it is to say that after reading this phrase countless times) |
[Edit: Ah yes. The formalism goes like this: Consider the above series. By the above argument, it differentiates to itself. QED. ]