A laboratory argon plasma sits in a uniform field inside a vessel of radius

PHYSICS · Multi-part · Fermi University Physics · Plasma Physics · The plasma state and single-particle motion · The plasma state and single-particle motion

Plasma Physics, Ch What makes an ionised gas a plasma: shielding, the plasma parameter and the natural frequencies

Problem

A laboratory argon plasma sits in a uniform field B=0.10 TB = 0.10\,\mathrm{T} inside a vessel of radius 5.0 cm5.0\,\mathrm{cm}. Its electron density is ne=1.0×1016 m−3n_e = 1.0\times10^{16}\,\mathrm{m^{-3}}. The electrons have Te=3.0 eVT_e = 3.0\,\mathrm{eV}, and the singly charged ions (Ar+\mathrm{Ar^+}, mass 40×1.67×10−27 kg40\times1.67\times10^{-27}\,\mathrm{kg}) have Ti=0.030 eVT_i = 0.030\,\mathrm{eV}. Electrons collide with neutral atoms at a rate of 1.0×108 s−11.0\times10^{8}\,\mathrm{s^{-1}} and ions at a rate of 1.0×106 s−11.0\times10^{6}\,\mathrm{s^{-1}}. ((a)) Find the size of the gyrofrequency ∣Ωs∣|\Omega_s| and the thermal Larmor radius rLs=vts/∣Ωs∣r_{Ls} = v_{ts}/|\Omega_s|, with vts=(Ts/ms)1/2v_{ts} = (T_s/m_s)^{1/2}, for each species. ((b)) Decide which species is magnetised, testing both conditions. ((c)) Before using any of this, place the plasma on the density-temperature map (weakly coupled? classical? non-relativistic?) and check the three conditions for calling it a plasma, taking LL as the vessel radius and τ\tau as the electron-neutral collision time.

Browse the problem library