Hi, Element7k.
First, I consider you're talking about patch antenna
Any patch (consider lying in XY plane) supports only TM modes.
Imagine that under the patch you have only the z-component of electric field, Ez (simplified model). Patch is simplified to be only 2 dimensional. Magnetic fields you compute as follows:
H=(j*omega*mu0)^-1
z0 x grad(Ez)
z0 is unit vector in z direction and x is vector product
it results that
H under the patch have x,y compontents only and because XY is the transversal plane, modes are called
Transverse
Magnetic
Resonant freqs. of the TM modes you can calculate in general as
f_n=(c*k_n)/(2*pi*sqrt(epsreff))
epsreff is efective relative epsilon of substrate and k_n is the eigennumber which depends on geometry only!!!
If geometry is separable (circle, ellipse, ring, rectangle, triangle) you can separate eigennumbers in coordinates also.
Look in Microstrip antenna design handbook, you'll find there the eigennumbers and eigenmodes (together called eigenpars) for all separable geometries.
This approach coming from the idea patch antenna as resonator with magnetic walls around their boundary. PEC condition at patch itself and ground is fulfiled automaticaly, because we suppose only Ez (normal component).
Regards,
Eirp