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Cavity radiation says the number of modes in the cavity increases with frequency, or shorter wavelength, because more modes can fit in. But consider a square box with sides L with a small hole. EM radiation of wavelength 2L can fit a half wavelength in the cavity horizontally exactly with nodes at the walls. In all resources on black-body radiation I have seen, this lowest frequency is called "one" mode. But I can fit an almost infinite number of halfwavelengths inside the box just horizontally, let alone vertically and diagonally. What am I missing? Why can wavelength 2L only fit once?

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In a three-dimensional resonator the wave modes are usually characterized by three numbers: in a rectangular box these simply correspond to the numbers of wave lengths fitting along different directions parallel to the box edges. That is, we have something like $$ 2L_x=N_x\lambda, 2L_z=N_y\lambda, 2L_z=N_z\lambda. $$ This ultimately comes from solving the Maxwell equations by separation of variable technique.

Here are the first notes on rectangular cavities that popped-up in Google: Cavities with Rectangular Boundaries (there are likely a lot more.)

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  • $\begingroup$ Thanks for input, unfortunately my math skills are very limited (so wave functions are definitely out!), so should have mentioned I'm looking for a more "heuristic" explanation, if there is one! $\endgroup$ May 9 at 14:39
  • $\begingroup$ What exactly do you mean by "I can fit an almost infinite number of halfwavelengths inside the box just horizontally"? Just before that you state that only half a wave length can fit for a given wavelength. $\endgroup$ May 9 at 14:47
  • $\begingroup$ I mean that I could fit a halfwavelength horizontally at the vertical middle of the box (i.e. half way up). I could then move up a millimetre and fit another halfwavelength horizontally in the box. And then another millimetre up for another halfwavelength, and then another, and so on. If the amplitude of the wave was infinitessimally small, then I could fit an almost infinite number of halfwavelengths horizontally. Hope that helps. $\endgroup$ May 9 at 16:21

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