Normalization of Bessel functions of the first kind

Join the discussion
Registration is free. Start your own thread to ask a follow-up.
1 reply · 8K views
Science Advisor
Insights Author
Messages
2,802
Reaction score
605
Before stating the main question,which section should the special functions' questions be asked?

Now consider the Bessel differential equation:

[itex] \rho \frac{d^2}{d\rho^2}J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})+\frac{d}{d\rho}J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})+(\frac{\alpha_{\nu m}^2 \rho}{a^2}-\frac{\nu^2}{\rho})J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})=0[/itex]

and a similar equation but with [itex]\alpha_{\nu m}[/itex] replaced by [itex]\alpha_{\nu n}[/itex] where [itex]\alpha_{\nu s}[/itex] is the [itex]s[/itex]th root of [itex]J_{\nu}(x)[/itex].

Now if one multiplies the first equation by [itex]J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})[/itex] and the second by [itex]J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})[/itex] and then subtracts the second from the first,the following will be found upon integration of the whole equation from 0 to a:

[itex] \int_0^a J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})\frac{d}{d\rho}[\rho\frac{d}{d\rho}J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})]d\rho-\int_0^a J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})\frac{d}{d\rho}[\rho\frac{d}{d\rho}J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})]d\rho=\frac{\alpha_{\nu n}^2-\alpha_{\nu m}^2}{a^2}\int_0^a J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})J_{\nu}(\alpha_{\nu m} \frac{\rho}{a}) \rho d\rho[/itex]

Integrating the LHS by part and cancelling gives:

[itex] J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})\rho\frac{d}{d\rho}J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})|_0^a-J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})\rho\frac{d}{d\rho}J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})|_0^a=\frac{\alpha_{\nu n}^2-\alpha_{\nu m}^2}{a^2}\int_0^a J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})J_{\nu}(\alpha_{\nu m} \frac{\rho}{a}) \rho d\rho[/itex]

Using [itex]\frac{d}{dx}J_n(x)=\frac{n}{x}J_n(x)-J_{n+1}(x)[/itex]:

[itex] J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})\rho[\frac{\nu a}{\alpha_{\nu m}\rho}J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})-J_{\nu+1}(\alpha_{\nu m}\frac{\rho}{a})]|_0^a-J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})\rho[\frac{\nu a}{\alpha_{\nu n}\rho}J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})-J_{\nu+1}(\alpha_{\nu n}\frac{\rho}{a})]|_0^a=\frac{\alpha_{\nu n}^2-\alpha_{\nu m}^2}{a^2}\int_0^a J_{\nu}(\alpha_{\nu n} \frac{\rho}{a})J_{\nu}(\alpha_{\nu m} \frac{\rho}{a}) \rho d\rho[/itex]

After placing [itex]\alpha_{\nu n}=\alpha_{\nu m}+\varepsilon[/itex] and taking the limit as [itex]\varepsilon\rightarrow 0[/itex] and using [itex]\frac{d}{dx}J_n(x)=\frac{n}{x}J_n(x)-J_{n+1}(x)[/itex] to replace terms involving Js with [itex]\varepsilon[/itex] in their arguments and calculating the terms in the boundaries:
[itex] -J_{\nu+1}(\alpha_{\nu m})\varepsilon[-aJ_{\nu+1}(\alpha_{\nu m})](\alpha_{\nu m})=\frac{2\alpha_{\nu m} \varepsilon}{a^2}\int_0^a J^2_{\nu}(\alpha_{\nu m} \frac{\rho}{a})\rho d\rho[/itex]

Which gives:

[itex] \int_0^a [J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})]^2\rho d\rho=\frac{a^3}{2\alpha_{\nu m}}[J_{\nu+1}(\alpha_{\nu m})]^2[/itex]

But the correct equation is:

[itex] \int_0^a [J_{\nu}(\alpha_{\nu m} \frac{\rho}{a})]^2\rho d\rho=\frac{a^2}{2}[J_{\nu+1}(\alpha_{\nu m})]^2[/itex]
(This is what you find about normalization of Bessel functions everywhere)
What's wrong in my calculations?
Thanks
 
Physics news on Phys.org
Hello,

the mistake is in the relationship where you change Jv for Jv+1. The x derivate changes to (d ro / dx)(d / d ro) and (d ro / dx) = alpha / a

I was stuck ages with this too! Can't believe there wasn't a reply for 5 years!