Related Experiment Video
Updated: Jul 3, 2026

11:42
A Paired Bead and Magnet Array for Molding Microwells with Variable Concave Geometries
Published on: January 28, 2018
Magnetic flux array for spontaneous magnetic reconnection experiments.
1Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, MA 02139, USA.
The Review of Scientific Instruments
|July 8, 2008
Summary
Researchers developed a new magnetic flux array to measure the toroidal component of the magnetic vector potential. This tool enables detailed studies of spontaneous magnetic reconnection in plasmas, even when dynamics are not reproducible.
Area of Science:
- Plasma Physics
- Magnetic Reconnection Studies
Background:
- Accurate magnetic field characterization is crucial for studying magnetized plasma reconnection.
- Traditional methods struggle with non-reproducible plasma dynamics, requiring data from single discharges.
Purpose of the Study:
- To introduce a novel magnetic flux array for direct measurement of the toroidal magnetic vector potential, A(phi).
- To enable detailed 3D analysis of spontaneous magnetic reconnection in non-reproducible plasma experiments.
Main Methods:
- Development and implementation of a new magnetic flux array probe.
- Direct measurement of the toroidal magnetic vector potential, A(phi).
- Utilizing a small number of channels for multi-angle A(phi) profiling with minimal plasma disturbance.
Main Results:
- The array directly measures A(phi), allowing for straightforward calculation of magnetic field geometry, current density, and reconnection rate.
- The design facilitates accurate profiling of A(phi) at multiple toroidal angles.
Conclusions:
- The developed magnetic flux array is a key advancement for studying spontaneous magnetic reconnection in challenging experimental conditions.
- This technology enhances the ability to investigate the three-dimensional dynamics of magnetic reconnection in 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 Flux
The magnetic flux measures the number of magnetic field lines passing through a given surface area. The SI unit for magnetic flux is the weber (Wb). Magnetic flux is a scalar quantity. It depends on three factors: the strength of the magnetic field B, the area through which the field lines pass, and the relative orientation of the field with the surface area.
Suppose a surface is divided into elements of area dA. For each element, the component of the magnetic field that is normal to the...
Suppose a surface is divided into elements of area dA. For each element, the component of the magnetic field that is normal to the...
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.
Magnetic Field Due to Two Straight Wires
Consider two parallel straight wires carrying a current of 10 A and 20 A in the same direction and separated by a distance of 20 cm. Calculate the magnetic field at a point "P2", midway between the wires. Also, evaluate the magnetic field when the direction of the current is reversed in the second wire.
Magnetic Field Due To A Thin Straight Wire
Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
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...

