Constraints on energy transfer and temperature gradients in magnetized plasma

1995 ◽  
Vol 52 (6) ◽  
pp. 699-707 ◽  
Author(s):  
Petro P Sosenko ◽  
Jan Weiland
1975 ◽  
Vol 12 (6) ◽  
pp. 1203-1203
Author(s):  
C. Ekdahl ◽  
M. Greenspan ◽  
J. Sethian ◽  
C. B. Wharton

1998 ◽  
Vol 60 (2) ◽  
pp. 209-214
Author(s):  
PETRO P. SOSENKO

Energy transfer from particles to low-frequency turbulent fields in the non-uniform magnetized plasma is studied. Sufficient conditions for plasma stability are derived taking account of magnetic field shear.


1997 ◽  
Vol 57 (2) ◽  
pp. 259-271 ◽  
Author(s):  
PETRO P. SOSENKO

The second-order approximation in a quasiparticle description of magnetized plasmas is studied. The second-order adiabatic invariant of quasiparticle motion is found. Global adiabatic invariants for a magnetized plasma are revealed, and their possible role in energy exchange between particles and fields, nonlinear mode cascades and global plasma stability is discussed.


Author(s):  
R.D. Leapman ◽  
P. Rez ◽  
D.F. Mayers

Microanalysis by EELS has been developing rapidly and though the general form of the spectrum is now understood there is a need to put the technique on a more quantitative basis (1,2). Certain aspects important for microanalysis include: (i) accurate determination of the partial cross sections, σx(α,ΔE) for core excitation when scattering lies inside collection angle a and energy range ΔE above the edge, (ii) behavior of the background intensity due to excitation of less strongly bound electrons, necessary for extrapolation beneath the signal of interest, (iii) departures from the simple hydrogenic K-edge seen in L and M losses, effecting σx and complicating microanalysis. Such problems might be approached empirically but here we describe how computation can elucidate the spectrum shape.The inelastic cross section differential with respect to energy transfer E and momentum transfer q for electrons of energy E0 and velocity v can be written as


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