Physical Meaning and Evaluation of Complex Integral in Heat Conduction Problems

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The integral presented relates to heat conduction problems, specifically involving the term \(\sqrt{-\sinh^{2}(bx)}\), which raises questions about its physical interpretation. The discussion highlights that the antiderivative of a real function cannot be complex, suggesting that the hypergeometric function may contain imaginary components that cancel out. Evaluating the integral at \(x=L\) requires understanding this cancellation process. The conversation emphasizes the importance of analytic continuation in resolving the complexities of the hypergeometric function. Overall, the evaluation and physical meaning of the integral are intricately linked to the behavior of hypergeometric functions in heat conduction contexts.
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Hello
In the following integral which I obtained from Wolfram, what is the physical meaning (e.g. in a heat conduction problem) of \sqrt{-\sinh^{2}(bx)}. Also how to evaluate this at x=L.
Thanks.

<br /> \int\frac{dx}{\cosh^{3n+1}(bx)}=\frac{\sinh(bx)\cosh^{-3n}(bx)}{3nb\sqrt{-\sinh^{2}(bx)}}\,_{2}F_{1}\left(\frac{1}{2},-\frac{3n}{2};\frac{2-3n}{2};\cosh^{2}(bx)\right)<br />
 
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The antiderivative of a real function can not possibly be complex, So perhaps the hypergeometric function has imaginary terms that cancel it out.
 
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That is indeed the case as the parameters to the Hypergeometric function force it into it's analytic continuation giving rise to a imaginary number which cancels the i in the denominator.
 
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