chernoshtanov i.s., tsidulko yu.a
DESCRIPTION
Outline Motivation Simple estimations Specifics of wave propagation and ion motion Integral equation for perturbations in non-uniform plasma Analytical solution for asymptotic case Summary picture ConclusionsTRANSCRIPT
Alfvén ion-cyclotron instability in a mirror trap with highly-
anisotropic plasmaChernoshtanov I.S., Tsidulko Yu.A.
Outline
• Motivation• Simple estimations• Specifics of wave propagation and ion motion • Integral equation for perturbations in non-uniform
plasma• Analytical solution for asymptotic case• Summary picture• Conclusions
Motivation• GDT end-cell:
• Traditional stability scaling:
•The purpose of this work: AIC instability in the highly-
anisotropic case.
Estimation• R.C. Davidson, J.M. Ogden. Phys. Fluids, 1975
unstable when
( : resonant ions move along isolines of distribution function)
• For plasma with finite scale stability
Reflection from turning points ( )
Specific of wave propagation
Reflection from plasma non-uniformity
Watson’s case:
kk
Our case:
WKB
Specific of ion motion• Bounce frequency:• Unstable perturbation frequency:
• Local dispersion relation• Resonances:
• Non-locality
Non-uniform plasma. Eigenmode equation. • The equations for the circularly polarized Fourier components:
Here • For , and
Analytical solution at• The equation isHere , • Wave vanishes at if
• Minimal asymptotic stability criterion
The AIC instability threshold ( )
GDT end-cell: the margin density:
Conclusions• A linear theory of AIC instability for highly
anisotropic mirror-confined bi-Maxwellian plasmas is presented.
• The asymptotic stability threshold and spatial distribution of the eigenmodes are found analytically in the limit of infinite anisotropy.
• The wave energy localization length as well as the unstable mode wavelength are of the order of anisotropic plasma scale length.
• Numerical results of the theory are in approximate agreement with preliminary results of GDT end-cell experiment.
• The mirror-confined highly anisotropic plasma can be much more stable than it follows from the traditional scaling.
Thank you for your attention.
References
• M.N. Rosenbluth, Bull. Am. Phys. Soc., Ser. II, 4 (197) 1959. (unpublished)
• R.Z. Sagdeev, V.D. Shafranov. JETP. 12, 1960.• R.C. Davidson, J.M. Ogden. Phys. Fluids. 18(8),
1975.• D.C. Watson. Phys. Fluids, 23(12), 1980• T.A. Casper, G.R. Smith. Physical Review
Letters 48(15), 1982• R.F. Post. Nuclear Fusion 27(10), 1987
Bi-Maxwellian plasma in the non-uniform magnetic field
• Axisymmetric magnetic field
• Distribution function:
plasma density:
• The criterion for absolute instability in the collisionless bi-maxwellian plasma with is
• The perturbation frequency and wave number are
The absolute instability in the uniform plasma
Numerical resultsEigenvalues of the equation at fixed
Eigenfunctions in z representation:
Simulation of non-linear saturation in uniform plasma R.C.Davidson, J.M.Ogeden, Phys.Fluids, 1975
P.Hellinger et al, Geophysical Research Letters, 2003
Plasma compression in the magnetosphere
Possible scenario: the instability modifies ion distribution function only near resonant orbits.
Nonlinear saturation in highly-anisotropic case
Nonlinear saturation does not lead to substantial anisotropy reducing
Estimations for highly-anisotropic uniform plasma
Цидулко, Черноштанов, препринт ИЯФ 2009-3Черноштанов, Цидулко, Вестник НГУ, 2010
- shape of resonant ions
?
Addition of cold plasma
Instability growth rate
Dielectric permeability for the non-uniform plasmas
Qualitative consideration• Resonant condition
• Existence of inverse population on resonant orbits instability
TMX, 2XIIB• TMX:
• 2XIIB:
The stability margin ( )