An engineer designing electron cyclotron heating for a compact tokamak with at the…

PHYSICS · Subjective · Fermi University Physics · Plasma Physics · Waves in plasmas · Waves in plasmas

Plasma Physics, Ch Waves in a non-uniform plasma: rays, reflection, mode conversion and radiofrequency heating

Problem

An engineer designing electron cyclotron heating for a compact tokamak with B0=1.8 TB_0 = 1.8\,\mathrm{T} at the magnetic axis R0=0.9 mR_0 = 0.9\,\mathrm{m} (so B(R)=B0R0/RB(R) = B_0R_0/R) plans to launch a 50 GHz50\,\mathrm{GHz} fundamental X-mode beam from the low-field side (large RR, outboard midplane). The core electron plasma frequency is fpe=32 GHzf_{pe} = 32\,\mathrm{GHz}. The engineer argues: 'The X mode has a lower cutoff density than the O mode, so it will penetrate further into the plasma. Launched from the outboard side, it will cross the fundamental cyclotron resonance layer near the axis and be absorbed there.' Find the error in this reasoning, using the right-hand cutoff frequency ωR=12(∣Ωe∣+Ωe2+4ωpe2)\omega_R = \tfrac12\left(|\Omega_e| + \sqrt{\Omega_e^2+4\omega_{pe}^2}\right) (Chapter 9's cold-plasma dispersion, quoted here), evaluated with the axial values of B0B_0 and fpef_{pe}. State what the engineer should do instead.

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