Observations of Magnetotail Interchange Heads' Signatures at Later Stage of Development

Author(s):  
Evgeny V. Panov ◽  
San Lu ◽  
Philip L. Pritchett

<pre>The kinetic ballooning/interchange instability (BICI) was recently found to produce azimutally narrow interchange <br />heads extending from the near-Earth magnetotail into the dipole region. In their nonlinear evolution individual <br />heads were predicted to grow into transient earthward moving northward magnetic field intensifications <br />(dipolarization fronts; DFs). The distinguished signatures of such fronts would be their oblique propagation <br />and cross-tail localization due to the finite k$_y$ structure of the BICI modes. We compare DFs that were observed <br />by two THEMIS probes at 11 Earth's radii (R$_E$) downtail amidst previously identified interchange heads with a <br />simulated interchange head during later-stage BICI development. The comparison shows that the DFs propagated <br />dawnward at about 45$^{\circ}$ to the earthward direction. The leading edges and trailing tails of the DFs were <br />structured similarly to those of the simulated interchange head. The analysis evidences that BICI indeed releases <br />obliquely propagating azimuthally localized dipolarization fronts in the Earth's magnetotail. </pre>

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Minjun J. Choi ◽  
Lāszlo Bardōczi ◽  
Jae-Min Kwon ◽  
T. S. Hahm ◽  
Hyeon K. Park ◽  
...  

AbstractMagnetic islands (MIs), resulting from a magnetic field reconnection, are ubiquitous structures in magnetized plasmas. In tokamak plasmas, recent researches suggested that the interaction between an MI and ambient turbulence can be important for the nonlinear MI evolution, but a lack of detailed experimental observations and analyses has prevented further understanding. Here, we provide comprehensive observations such as turbulence spreading into an MI and turbulence enhancement at the reconnection site, elucidating intricate effects of plasma turbulence on the nonlinear MI evolution.


1987 ◽  
Vol 37 (1) ◽  
pp. 107-115
Author(s):  
B. Ghosh ◽  
K. P. Das

The method of multiple scales is used to derive a nonlinear Schrödinger equation, which describes the nonlinear evolution of electron plasma ‘slow waves’ propagating along a hot cylindrical plasma column, surrounded by a dielectric medium and immersed in an essentially infinite axial magnetic field. The temperature is included as well as mobile ion effects for ail possible modes of propagation along the magnetic field. From this equation the condition for modulational instability for a uniform plasma wave train is determined.


The influence of the earth’s magnetic field on the propagation of wireless waves in the ionosphere has stimulated interest in the problem of the propagation of electromagnetic waves through a non-isotropic medium which is stratified in planes. Although the differential equations of such a medium have been elegantly deduced by Hartree,f it appears that no solution of them has yet been published for a medium which is both non-isotropic and non-homogeneous. Thus the work of Gans and Hartree dealt only with a stratified isotropic medium, while in the mathematical theory of crystal-optics the non-isotropic medium is always assumed to be homogeneous. In the same way Appleton’s magneto-ionic theory of propagation in an ionized medium under the influence of a magnetic field is confined to consideration of the “ characteristic ”waves which can be propagated through a homogeneous medium without change of form. In applying to stratified non-isotropic media these investigations concerning homogeneous non-isotropic media difficulty arises from the fact that the polarizations of the characteristic waves in general vary with the constitution of the medium, and it is not at all obvious that there exist waves which are propagated independently through the stratified medium and which are approximately characteristic at each stratum. The existence of such waves has usually been taken for granted, although for the ionosphere doubt has been cast upon this assumption by Appleton and Naismith, who suggest that we might “ expect the components ( i. e ., characteristic waves) to be continually splitting and resplitting”, even if the increase of electron density “ takes place slowly with increase of height”. It is clear that, until the existence of independently propagated approximately characteristic waves has been established, at any rate for a slowly-varying non-isotropic medium, no mathematical justification exists for applying Appleton's magnetoionic theory to the ionosphere. It is with the provision of this justification that we are primarily concerned in the present paper. This problem has been previously considered by Försterling and Lassen,f but we feel that their work does not carry conviction because they did not base their calculations on the differential equations for a non-homo-geneous medium, and were apparently unable to deal with the general case in which the characteristic polarizations vary with the constitution of the medium.


2013 ◽  
Vol 8 (0) ◽  
pp. 2403157-2403157 ◽  
Author(s):  
Ryosuke UEDA ◽  
Masahiko SATO ◽  
Kiyomasa WATANABE ◽  
Yutaka MATSUMOTO ◽  
Yasuhiro SUZUKI ◽  
...  

Author(s):  
P. C. Clemmow ◽  
J. Heading

ABSTRACTIt is shown that the equations governing oblique propagation in a horizontally stratified ionosphere with an oblique magnetic field can be cast into a form suitable for solution by successive approximations. In the general case this ‘coupled’ form consists of four first order differential equations, each being associated with one characteristic wave. In the special cases (a) horizontal magnetic field, (b) plane of incidence perpendicular to the magnetic meridian, two second order coupled equations of a particular type can be derived, each of which is associated with a pair of corresponding upgoing and downgoing characteristic waves. These latter equations are similar to, and include, those already given by Försterling(7) for vertical incidence.The cases in which there is no coupling are briefly considered from the point of view of the first order equations.The general formulation provides a basis for assessing the validity of the standard ‘ray’ approximation, alternative to that developed by Booker (2), and brings out the nature of its breakdown in coupling and reflexion regions.Specific applications and extensions of the theory are left for later consideration.


2007 ◽  
Vol 26 (1-2) ◽  
pp. 139-144 ◽  
Author(s):  
E. E. Ortiz ◽  
A. C. Boxer ◽  
J. L. Ellsworth ◽  
D. T. Garnier ◽  
A. K. Hansen ◽  
...  

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