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Destruction of cyclotron resonances in weakly collisional, inhomogeneous plasmas. Memorandum report

Technical Report ·
OSTI ID:5628170

It is shown, both analytically and numerically, that cyclotron resonances can be destroyed in dense (..omega../sub rho/ > ..cap omega.. where ..omega../sub rho/ is the plasma frequency and ..cap omega.. is the cyclotron frequency), weakly collisional, inhomogeneous plasmas when (..nu../..cap omega..) k/sup 2/ (r/sub L/)/sup 2/ is somewhat > 1, where ..nu.. is the collision frequency and r/sub L/ is the mean Larmor radius. The theory is based upon a model Fokker-Planck equation. It is found that the particles make a transition from magnetized to unmagnetized behavior. This is an important result since it indicates that the ion- and electron-cyclotron-drift instabilities transform into their unmagnetized counterparts, the lower-hybrid-drift instability and the ion acoustic instability, respectively. The ion-cyclotron-drift instability (or drift-cyclotron instability) is examined in detail and is found to become the lower-hybrid-drift-instability in the region of maximum growth when (..sqrt..(m/sub e//m/sub i/) ..omega../..cap omega../sub i/ somewhat > ..nu../sub ii//..cap omega../sub i/ somewhat > m/sub e//m/sub i/ for T/sub e/ approximately equal T/sub i/ plasmas. The first inequality is required to overcome electron viscous damping, while the second allows the ions to become unmagnetized. Applications to the equatorial F region of the ionosphere and the Tandem Mirror Experiment (TMX) are discussed.

Research Organization:
Naval Research Lab., Washington, DC (USA)
OSTI ID:
5628170
Report Number(s):
AD-A-067827
Country of Publication:
United States
Language:
English