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Cylindrical resonance cavity problem

  1. May 9, 2014 #1
    Hello all!
    1. The problem statement, all variables and given/known data
    Consider a cylindrical cavity with length "d" and radius "a". Find the corresponding electric field, and the dispersion relation therein.
    2. Relevant equations
    Maxwell's equations.
    3. The attempt at a solution
    I tried to solve the appropriate vector Helmholtz equation(obtained by assuming harmonic time-dependence of the waves in the cavity).
    Within the cylinder, one arrives at(where: [itex]\vec{E}=\vec{E_0}(r, \varphi, z)e^{-i \omega t}[/itex])
    [tex]
    \vec{\nabla}^2 \vec{E_0} = \frac{\omega^2}{c^2} \vec{E_0}
    [/tex]
    However, since [itex] \vec{E_0} = E_r \hat{r} + E_\varphi \hat{\varphi} + E_z \hat{z} [/itex], the Laplacian becomes far more convoluted in the cylindrical form.
    Solving for Ez is not that difficult(with appropriate separation of variables).
    However, how does one find E_r, E_phi?
    After all, solving for the wave equation for the r, phi components involves:
    [tex]
    (\vec{\nabla}^2 \vec{E_0})_r = \vec{\nabla}^2 E_r - \frac{1}{r^2}(E_r + 2\frac{\partial E_{\varphi}}{\partial \varphi})
    [/tex]
    However, this equation for E_r requires E_phi; and obviously, the components of E_r are not necessarily identical to E_phi, so substituting one for the other(through analogous separation of variables for both) is impossible here.
    Without making any other assumptions(or simplifications; for instance, I managed to simplify the problem greatly if I assumed complete azimuthal symmetry(i.e. E_phi = 0 & d/dphi =0)), is there any way to obtain an exact solution for this? Where should I turn to, next?
    Thank you for your attention,
    Reliant on your help,
    Daniel
     
  2. jcsd
  3. May 10, 2014 #2
    Going to have to bump this; is this at all solvable?
     
  4. May 14, 2014 #3
    Bump

    Bumping again.
     
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