Related Experiment Video
Updated: Jun 26, 2026

11:47
A 100 KW Class Applied-field Magnetoplasmadynamic Thruster
Published on: December 22, 2018
Magnetic reconnection by a self-retreating X line
M Oka1, M Fujimoto, T K M Nakamura
1Center for Space Plasma and Aeronomic Research, University of Alabama in Huntsville, Huntsville, Alabama 35805, USA. mitsuo.oka@uah.edu
Physical Review Letters
|December 31, 2008
Summary
Asymmetric magnetic reconnection simulations show an X-line retreat phenomenon. Despite this slow motion, the reconnection rate remains unaffected, offering new insights into plasma physics.
Area of Science:
- Plasma Physics
- Astrophysics
- Space Physics
Background:
- Collisionless magnetic reconnection is a fundamental process in plasma physics.
- Asymmetric reconnection, where outflows are uneven, presents unique challenges.
- Understanding X-line dynamics is crucial for astrophysical and space plasma phenomena.
Purpose of the Study:
- To investigate the effects of asymmetric magnetic reconnection with a blocked outflow.
- To analyze the phenomenon of X-line retreat in detail.
- To determine the impact of X-line retreat on the reconnection rate.
Main Methods:
- Particle-in-cell (PIC) simulations were employed.
- Simulations focused on asymmetric reconnection scenarios with a hard wall boundary.
- Analysis included ion flow patterns and X-line motion.
Main Results:
- A slow, constant X-line retreat was observed, moving away from the hard wall at approximately 0.1 Alfvén speed.
- Strong asymmetry in ion flow patterns was present within the diffusion region.
- The ion stagnation point and X-line were found to be spatially separated.
- Crucially, the reconnection rate was found to be independent of the X-line retreat.
Conclusions:
- X-line retreat is a significant feature of asymmetric reconnection under specific boundary conditions.
- Despite asymmetric flows and X-line motion, the global reconnection rate remains robust.
- These findings advance the understanding of magnetic reconnection dynamics in space and astrophysical plasmas.
Related Concept Videos
Magnetic Fields
A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
A magnetic field is defined by the force that a charged particle experiences...
Magnetic Field Lines
The representation of magnetic fields by magnetic field lines is very useful in visualizing the strength and direction of the magnetic field. Each of the magnetic field lines forms a closed loop. The field lines emerge from the north pole (N), loop around to the south pole (S), and continue through the bar magnet back to the north pole.
Magnetic field lines follow several hard-and-fast rules:
Magnetic field lines follow several hard-and-fast rules:
Magnetostatic Boundary Conditions
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
Magnetic Field due to Moving Charges
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
Magnetic Force Between Two Parallel Currents
Two long, straight, and parallel current-carrying conductors exert a force of equal magnitude on one another. The direction of the force depends on the current direction in the conductors.
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
Divergence and Curl of Magnetic Field
The magnetic field due to a volume current distribution given by the Biot–Savart Law can be expressed as follows:

