While solving a physical problem from Landau, Lifshitz "Mechanics" book, I came across an integral:
∫δ0du√(coshδcoshu)2−1.
In the book only the final answer for the problem is given, from which I deduce that this integral must be π2.
I've tried feeding it to Wolfram Mathematica, but it wasn't able to evaluate it, returning unevaluated result. Evaluating it numerically confirms that this is a likely answer, but I haven't been able to prove this.
I've tried making a substitution v=coshδcoshu and got this integral instead:
γ∫γ1dvv√(γ2−v2)(v2−1),
where γ=coshδ, but still this doesn't give me a clue how to proceed. Also, I can't seem to eliminate the parameter (δ or γ), which shouldn't affect the result at all.
So, the question is: how can one evaluate this integral or at least prove that it's equal π2?
Answer
It's actually a lot simpler than this. Rewrite the integral as
∫δ0ducoshu√cosh2δ−cosh2u=∫δ0ducoshu√sinh2δ−sinh2u
Sub y=sinhu and the integral becomes
∫sinhδ0dy√sinh2δ−y2
Now sub y=sinhδsint and the integral is
∫π/20dt=π2
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