A deuterium plasma ( ) has

PHYSICS · Multi-part · Fermi University Physics · Plasma Physics · Waves in plasmas · Waves in plasmas

Plasma Physics, Ch Waves that need pressure or tension: Langmuir, ion-acoustic, Alfven and magnetosonic

Problem

A deuterium plasma (mi=2mpm_i = 2m_p) has B=1.0 TB = 1.0\,\mathrm{T}, ne=ni=1.0×1019 m−3n_e = n_i = 1.0\times10^{19}\,\mathrm{m^{-3}} and Te=Ti=500 eVT_e = T_i = 500\,\mathrm{eV}. Take γad=5/3\gamma_{\rm ad} = 5/3. ((a)) Find the Alfven speed vA=B/(μ0ρ)1/2v_A = B/(\mu_0\rho)^{1/2} (with ρ=nimi\rho = n_im_i) and the sound speed cs=(γadp/ρ)1/2c_s = (\gamma_{\rm ad}p/\rho)^{1/2} with p=neTe+niTip = n_eT_e + n_iT_i. ((b)) Using ω2k2=12[vA2+cs2±((vA2+cs2)2−4vA2cs2cos⁡2θ)1/2]\dfrac{\omega^2}{k^2} = \tfrac{1}{2}\left[v_A^2+c_s^2 \pm \left((v_A^2+c_s^2)^2 - 4v_A^2c_s^2\cos^2\theta\right)^{1/2}\right], find the fast and slow magnetosonic speeds at θ=0∘\theta = 0^\circ, 45∘45^\circ and 90∘90^\circ, where θ\theta is the angle between k\mathbf{k} and B0\mathbf{B}_0.

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