Related Experiment Video
Updated: Jun 29, 2026

04:35
Comparative Study of Simulation of Temperature Rise in Ring Main Unit
Published on: July 5, 2024
Quantitative, comprehensive, analytical model for magnetic reconnection in Hall magnetohydrodynamics
1Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
Physical Review Letters
|October 15, 2008
Summary
A new theory explains fast magnetic reconnection independent of dissipation, crucial for understanding plasma dynamics. It reveals reconnection rates strongly depend on ion inertial lengths.
Area of Science:
- Plasma physics
- Astrophysics
- Space physics
Background:
- Magnetic reconnection is a fundamental process in plasma physics, crucial for phenomena like solar flares and geomagnetic storms.
- Previous models often assumed dissipation-dependent reconnection, limiting their applicability.
- Hall magnetohydrodynamics (MHD) and electron MHD have suggested dissipation-independent reconnection, but lacked a comprehensive theory.
Purpose of the Study:
- To develop the first quantitative analytical theory for dissipation-independent magnetic reconnection.
- To provide expressions for reconnection rates applicable to arbitrary ion inertial lengths.
- To establish a formal criterion for fast reconnection.
Main Methods:
- Developed a two-dimensional analytical theory for the magnetic reconnection diffusion region.
- Derived expressions for reconnection rates based on dissipation parameters and ion inertial lengths.
- Formally derived a criterion for fast reconnection.
Main Results:
- The theory quantitatively describes dissipation-independent magnetic reconnection.
- Reconnection rates are shown to depend strongly on the ion inertial length (d{i}).
- Confirmed that both open and elongated diffusion regions support fast reconnection, consistent with electron MHD predictions.
Conclusions:
- The proposed theory offers a unified framework for understanding fast magnetic reconnection across various scales.
- The strong dependence of reconnection rates on d{i} highlights its importance in astrophysical and laboratory plasmas.
- This work bridges the gap between computational observations and analytical predictions of fast magnetic reconnection.
Related Concept Videos
The Hall Effect
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
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...
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...
Potential Due to a Magnetized Object
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
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:
Magnetic Field Of A Current Loop
Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.

