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How can you prove that a function has no closed form integral?
(Forgive my crude lingo)
Why do some integrals seem to be unsolvable; that is to say the indefinite integral cannot be solved symbolically (or is it analytically(?)). For example, those with the form of a radial distribution function using the Lennard-Jones potential:
$$g(r) = \exp(-(r^{-12} - r^{-6}))$$
What prevents me from using my standard Calc II knowledge to come up with a continuous expression for $\int{g(r)dr}$?
I could've sworn I read something on here that referenced the theorem that developed in order to answer this question.
– 000 Apr 19 '12 at 16:28