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Magnetic Fields01:27

Magnetic Fields

7.3K
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...
7.3K
Magnetic Field of a Solenoid01:18

Magnetic Field of a Solenoid

5.8K
A solenoid is a conducting wire coated with an insulating material, wound tightly in the form of a helical coil. The magnetic field due to a solenoid is the vector sum of the magnetic fields due to its individual turns. Therefore, for an ideal solenoid, the magnetic field within the solenoid is directly proportional to the number of turns per unit length and the current. Conversely, the magnetic field outside the solenoid is zero.
Consider a solenoid with 100 turns wrapped around a cylinder of...
5.8K
Magnetic Field Lines01:19

Magnetic Field Lines

5.7K
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:
5.7K
Energy In A Magnetic Field01:24

Energy In A Magnetic Field

2.7K
If a magnetic field is sustained, there must be a current in a closed circuit or loop, implying some energy has been spent in creating the field. If this energy is not dissipated via the circuit's resistance, it is stored in the field.
Take an ideal inductor with zero resistance. Although it's practically impossible, assume that the coil's resistance is so small that it is practically negligible. The loss of the field's energy to dissipate thermal energy (or heat) is thus...
2.7K
Magnetic Field Of A Current Loop01:16

Magnetic Field Of A Current Loop

6.3K
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.
6.3K
Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

11.6K
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...
11.6K

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Updated: Jan 27, 2026

Fabrication and Characterization of Superconducting Resonators
10:26

Fabrication and Characterization of Superconducting Resonators

Published on: May 21, 2016

11.9K

Superconducting YBCO Foams as Trapped Field Magnets.

Michael R Koblischka1, Sugali Pavan Kumar Naik2, Anjela Koblischka-Veneva3

  • 1Superconducting Materials Laboratory, Department of Materials Science and Engineering, Shibaura Institute of Technology, Tokyo 135-8548, Japan. m.koblischka@gmail.com.

Materials (Basel, Switzerland)
|March 16, 2019
PubMed
Summary

Superconducting Yttrium Barium Copper Oxide (YBCO) foams demonstrate potential as powerful, lightweight trapped field magnets. These novel materials exhibit promising magnetic field trapping capabilities for advanced applications.

Keywords:
High-Tc superconductorsYBCOcurrent flowfoamtrapped fields

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Superconductivity

Background:

  • Superconducting foams made from Yttrium Barium Copper Oxide (YBCO) offer a unique combination of properties.
  • Their open-porous structure results in lightweight yet mechanically robust materials suitable for large-scale fabrication.
  • These properties make them candidates for advanced magnetic applications, including trapped field magnets.

Purpose of the Study:

  • To investigate the trapped magnetic field properties of YBCO superconducting foams.
  • To assess the feasibility of using these foams as supermagnets.
  • To explore potential applications in space, such as flux-pinning docking interfaces and debris collection.

Main Methods:

  • Field-cooling of YBCO foam samples in a 0.5 T magnetic field generated by a square Neodymium-Iron-Boron (Nd-Fe-B) permanent magnet.
  • Measurement of trapped field distributions using a scanning Hall probe.
  • Analysis of current flow and field distribution patterns.

Main Results:

  • A maximum trapped field (TF) of approximately 400 Gauss (G) was measured at 77 Kelvin (K) at the bottom of the YBCO foam sample.
  • Detailed mapping of the trapped field distribution across various sample surfaces was achieved.
  • The study provides insights into the current flow responsible for the trapped magnetic fields.

Conclusions:

  • YBCO superconducting foams exhibit significant potential as effective trapped field magnets.
  • The measured trapped fields support their consideration for demanding applications.
  • Potential space applications, including flux-pinning docking interfaces and portable strong magnets for debris management, are highlighted.