Geospace Environment Modeling magnetic reconnection challenge: Simulations with a full particle electromagnetic code

被引:326
作者
Pritchett, PL [1 ]
机构
[1] Univ Calif Los Angeles, Dept Phys & Astron, Los Angeles, CA 90095 USA
关键词
D O I
10.1029/1999JA001006
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The objective of the Geospace Environment Modeling (GEM) magnetic reconnection challenge is to understand the collisionless physics that controls the rate of magnetic reconnection in a two-dimensional configuration. The challenge involves investigating a standard model problem based on a simple Harris sheet configuration by means of a variety of physical models in order to isolate the essential physics. In the present work the challenge problem is modeled using an electromagnetic particle-in-cell code in which full particle dynamics are retained for both electrons and ions and Maxwell's equations are solved without approximation. The timescale for reconnection is of the order of 10 Omega (-1)(i) (where Omega (i) is the ion cyclotron frequency based on the asymptotic field B-0), and the corresponding reconnection electric field is (c/nu (A))E-y/B-0 similar to 0.24. The diffusion region near the neutral line is observed to develop a multiscale structure based on the electron and ion inertial lengths c/omega (pe) and c/omega (pi). The difference between the ion and electron dynamics in the diffusion region gives rise to in-plane (Hall) currents which produce an out-of-plant: B-y field with a quadrupolar structure. In the diffusion region the magnetic field is no longer frozen-in to the electrons the inductive E-y field is supported primarily by the off-diagonal electron pressure terms in the generalized Ohm's law. The reconnection rate is found to be insensitive to electron inertia effects and to the presence of a moderate out-of-plane initial field component B-0y less than or similar to B-0. The results are consistent with the theory that the reconnection rate is independent of the mechanism which breaks the frozen-in condition and is controlled by dynamics at length scales much greater than the electron dissipation region.
引用
收藏
页码:3783 / 3798
页数:16
相关论文
共 53 条
[1]   Two-fluid theory of collisionless magnetic reconnection [J].
Biskamp, D ;
Schwarz, E ;
Drake, JF .
PHYSICS OF PLASMAS, 1997, 4 (04) :1002-1009
[2]   ON THE ENERGY PRINCIPLE AND ION TEARING IN THE MAGNETOTAIL [J].
BRITTNACHER, M ;
QUEST, KB ;
KARIMABADI, H .
GEOPHYSICAL RESEARCH LETTERS, 1994, 21 (15) :1591-1594
[3]   The generalized Ohm's law in collisionless magnetic reconnection [J].
Cai, HJ ;
Lee, LC .
PHYSICS OF PLASMAS, 1997, 4 (03) :509-520
[4]   Breakup of the electron current layer during 3-D collisionless magnetic reconnection [J].
Drake, JF ;
Biskamp, D ;
Zeiler, A .
GEOPHYSICAL RESEARCH LETTERS, 1997, 24 (22) :2921-2924
[5]   STRUCTURE OF THIN CURRENT LAYERS - IMPLICATIONS FOR MAGNETIC RECONNECTION [J].
DRAKE, JF ;
KLEVA, RG ;
MANDT, ME .
PHYSICAL REVIEW LETTERS, 1994, 73 (09) :1251-1254
[6]  
DRAKE JF, 1995, GEOPHYS MONOGR SER, V90, P155
[7]   Particle simulations of collisionless reconnection in magnetotail configuration including electron dynamics [J].
Dreher, J ;
Arendt, U ;
Schindler, K .
JOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICS, 1996, 101 (A12) :27375-27381
[8]   FINITE-RESISTIVITY INSTABILITIES OF A SHEET PINCH [J].
FURTH, HP ;
KILLEEN, J ;
ROSENBLUTH, MN .
PHYSICS OF FLUIDS, 1963, 6 (04) :459-484
[9]   Consequences of particle conservation along a flux surface for magnetotail tearing [J].
Guest, KB ;
Karimabadi, H ;
Brittnacher, M .
JOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICS, 1996, 101 (A1) :179-183
[10]   ON A PLASMA SHEATH SEPARATING REGIONS OF OPPOSITELY DIRECTED MAGNETIC FIELD [J].
HARRIS, EG .
NUOVO CIMENTO, 1962, 23 (01) :115-+