How to find the coefficients of this expansion?

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The discussion focuses on finding coefficients in the expansion of a solution to a differential equation involving Bessel functions. The user is uncertain about the orthogonality conditions necessary for the coefficients, particularly since the eigenvalues are linked to the derivative of the Bessel function rather than its zeros. The orthogonality condition typically used does not apply directly due to this distinction. However, it is noted that an alternative expansion using the roots of the derivative of the Bessel function can still satisfy the orthogonality requirements. The conversation emphasizes the importance of understanding the specific conditions under which these functions remain orthogonal for the problem at hand.
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I have solved a differential equation whose solutions is $$u = B + \sum_{n=1} C_{n }e^{-\lambda_{n}² q² t} J_{0}(\lambda_{n}r)$$

Where ##(\lambda_{n}r)## is such that ##J_{0}'(\lambda_{n}a) = 0##. So i should now try to satisfy the condition that, at t=0, u = ##f(r)##.

The problem is that i don't know what is the orthogonality here. If ##\lambda_{n}## were such that ##J_{0}(\lambda_{n}a)=0##, i would use the normal orthogonaltiy generally used, namely ##\int_{0}^{a} r J_{0}(\lambda_{n}r)J_{0}(\lambda_{q}r)##

But this dosen't work here, since ##\lambda_{q}a## is not a zero of J0, but it is a zero in fact of its derivative.

Not just it, what orthogornality i would use to find the B?
 
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Believe it or not, orthogonality, exactly the way you wrote it, is already guaranteed. My source is Jackson Classical Electrodynamics 3rd Edition, bottom of page 115:

But it will be noted that an alternative expansion is possible in a series of functions ##\sqrt{\rho} J_\nu (y_{\nu n}\rho / a)## where ##y_{\nu n}## is the ##n##th root of the equation ##[dJ_\nu(x)]/dx = 0##. The reason is that, in proving the orthogonality of functions, all that is demanded is that thte quantity ##[\rho J_\nu (k\rho) (d/d\rho) J_\nu (k' \rho) - \rho J_\nu (k' \rho) (d/d\rho) J_\nu (k\rho)]## vanish at the endpoints ##\rho = 0## and ##\rho = a##.
 
First, I tried to show that ##f_n## converges uniformly on ##[0,2\pi]##, which is true since ##f_n \rightarrow 0## for ##n \rightarrow \infty## and ##\sigma_n=\mathrm{sup}\left| \frac{\sin\left(\frac{n^2}{n+\frac 15}x\right)}{n^{x^2-3x+3}} \right| \leq \frac{1}{|n^{x^2-3x+3}|} \leq \frac{1}{n^{\frac 34}}\rightarrow 0##. I can't use neither Leibnitz's test nor Abel's test. For Dirichlet's test I would need to show, that ##\sin\left(\frac{n^2}{n+\frac 15}x \right)## has partialy bounded sums...