y=Jn(kr) is a solution of Bessel´s differential equation r2y″+ry′+(r2k2−n2)y=0, which can be rewritten as (ry′)′+(rk2−n2/r)y=0.
If u=Jn(ar) and v=Jn(br), then they fulfill the equations
(ru′)′+(ra2−n2/r)u=0
(rv′)′+(rb2−n2/r)v=0
Multiply the first by v, the second by u and substract them, and you get
(b2−a2)ruv=u(rv′)′−v(ru′)′=(vru′−urv′)′
Integrating this, you get that
(b2−a2)∫10ruvdr=(vru′−urv′)|10=v(1)u′(1)−u(1)v′(1)
So if you want the left hand side to be 0, then the right hand side must be 0 as well, so you must have aJn(b)J′n(a)=bJn(a)J′n(b).
This is fulfilled if Jn(a)=Jn(b)=0, or J′n(a)=J′n(b)=0, but also if aJ′n(a)/Jn(a)=bJ′n(b)/Jn(b). So the boundary condition y′=Cy at r=1 will also work.
This post imported from StackExchange Mathematics at 2014-06-02 20:22 (UCT), posted by SE-user Jaime