@ RODAL
Can you generate a dispersion relation from the exact solution ?
@NotSoSureOfIt
I think that the relation between the wavenumber k and the angular frequency omega is perfectly linear for a truncated cone homogeneously filled with a medium having constant, isotropic, electric permittivity and constant magnetic permeability. It follows from the homogeneous electromagnetic wave equation, which for the truncated cone is solved in spherical coordinates via spherical waves (this involves an assumption of spherical ends, instead of flat ends).
Is your question what is the effective dispersion relation for a truncated cavity containing a dielectric (with constant properties) filling only a portion of the truncated cone?
Or is your question what is the dispersion relation for a truncated cavity containing a dielectric with nonlinear properties? Or anisotropic properties?
Or am I wrong, or missing something, ...
I was just thinking of the simplest case but based on your exact solution, rather than using that of the cylindrical cavity evaluated at both ends, which is what I have been using. The radii of both ends would presumably be already present in the single (presumably quadratic ?) expression.
1) The resonant cylindrical cavity is solved in terms of its natural coordinates: a cylindrical coordinate system rho(radius), phi(angle) and z (longitudinal coordinate).

1a)
The resonant cylindrical cavity (with a single medium inside it) has a linear dispersion relationship between frequency and wavenumber2a) the eigenvalue problem has a closed form solution (
http://en.wikipedia.org/wiki/Microwave_cavity#Cylindrical_cavity) expressing the frequency in terms of the SquareRoot of the sum of the square of the zero Bessel function m.n (
Xm,n and X'm,n are the eigenvalues ) divided by the Radius of the cylinder plus the Square of the longitudinal quantum number "p" divided by the cylinder's Length
3a) the only issue with the closed form solution (
http://en.wikipedia.org/wiki/Microwave_cavity#Cylindrical_cavity) is a side equation necessary to satisfy cut-off of mode shapes that cannot take place in the cylindrical cavity (
http://en.wikipedia.org/wiki/Cutoff_frequency#Waveguides )
2) The resonant truncated cone cavity is solved in terms of its natural coordinates: a spherical coordinate system r(radius), theta (polar angle), and phi(azimuthal angle). Please note that the radial coordinate "r" is entirely different in the spherical coordinate system than the radius "rho" in the cylindrical system.
In the spherical system the radius "r" defines the length of the walls of the truncated cone.
2a)
The resonant truncated cone cavity (with a single medium inside it) has a linear dispersion relationship between frequency and wavenumber2b) There are two eigenvalue problems to solve in the truncated cone: one eigenvalue problem deals with the spherical angle theta (polar angle) and another eigenvalue problem deals with the spherical radius "r".
Neither of these two eigenvalue problems has a closed-form solution. Hence the frequency for the truncated cone cannot be expressed as a closed-form solution (using classical functions). The two eigenvalue problems need to be solved numerically. . There is an exact solution, but it is not closed-form.
3c) while in the cylindrical cavity, the radius (or the diameter) of the cylindrical cavity appears, in the truncated cone this is not the case. In the truncated cone the
cylindrical coordinate radius "rho1" of the small base of the cone = r1*Sin[thetaw] and the
cylindrical coordinate radius "rho2" of the big base of the cone = r2*Sin[thetaw], where thetaw is the cone-half-angle and r1 is the radial distance from the origin of the spherical coordinate system to the small base and r2 is the radial distance from the origin of the spherical coordinate system to the big base. The cone-half-angle appears in the eigenvalue problem for the polar angle theta and the radial distances r1 and r2 appear in the eigenvalue problem for the spherical radius r.
Therefore the big and small diameter do not appear explicitly in the truncated cone solution. Instead the truncated cone solution parameters are the cone-half-angle thetaw and the spherical radii r1 and r2. And there is no closed-form solution: the frequency is the result of the numerical solution of two eigenvalue problems (which can be solved with numerical root finding procedures).
3d) The first eigenvalue problem contains Legendre functions (
http://en.wikipedia.org/wiki/Legendre_function) of the Cosine of the cone-half angle.
3e) The second eigenvalue problem contains Spherical Bessel functions (
http://mathworld.wolfram.com/SphericalBesselFunctionoftheFirstKind.html) in terms of the wavenumber K and the spherical radius.
3f)
No cut-off auxiliary equation is necessary for the solution of the truncated cone problem. Purely evanescent modes get cut-off automatically when solving the eigenvalue problem if one is seeking real solutions. There are also interesting degenerate modes in the truncated cone which are resonant within a portion of the cavity and evanescent on another portion of the cavity.