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Related Concept Videos

Magnetic Field Of A Current Loop01:16

Magnetic Field Of A Current Loop

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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.
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Magnetic Vector Potential01:15

Magnetic Vector Potential

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In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
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Magnetic Field Due To A Thin Straight Wire01:28

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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.
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Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

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A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
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Torque On A Current Loop In A Magnetic Field01:13

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The most common application of magnetic force on current-carrying wires is in electric motors. These consist of loops of wire, which are placed between the magnets with a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate, thus converting electrical energy to mechanical energy.
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Magnetic Field of a Solenoid01:18

Magnetic Field of a Solenoid

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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.
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Related Experiment Video

Updated: Aug 9, 2025

Scanning SQUID Study of Vortex Manipulation by Local Contact
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A Superconducting Micro-Magnetometer for Quantum Vortex in Superconducting Nanoflakes.

Xiangyu Bi1, Feifan Tian1, Ganyu Chen1

  • 1National Laboratory of Solid State Microstructures, Collaborative Innovation Center of Advanced Microstructures, College of Engineering and Applied Sciences, Jiangsu Key Laboratory of Artificial Functional Materials, Nanjing University, Nanjing, 210000, P. R. China.

Advanced Materials (Deerfield Beach, Fla.)
|February 22, 2023
PubMed
Summary

A new superconducting nano-hole array enables contactless magnetic property detection in micro-sized superconducting nanoflakes. This method quantifies vortex pinning centers, overcoming limitations of conventional superconducting quantum interference device (SQUID) techniques for small samples.

Keywords:
Bi 2Sr 2CaCu 2O 8Little-Parks oscillationsuperconducting quantum interferometer devicessuperconductivityvortex pinning

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Fabrication of Magnetic Nanostructures on Silicon Nitride Membranes for Magnetic Vortex Studies Using Transmission Microscopy Techniques
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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Area of Science:

  • Condensed matter physics
  • Quantum materials science
  • Nanotechnology

Background:

  • Superconducting quantum interferometer devices (SQUIDs) are crucial for studying quantum materials but are limited to bulky samples.
  • Probing magnetic properties of micro-scale samples with weak magnetic signals is challenging with conventional methods.

Purpose of the Study:

  • To develop a contactless method for detecting magnetic properties of micro-sized superconducting nanoflakes.
  • To investigate quantized vortices and their pinning centers in these small-scale samples.

Main Methods:

  • Utilizing a specially designed superconducting nano-hole array for detection.
  • Measuring magnetoresistance signals from micro-sized superconducting nanoflakes.

Main Results:

  • Successfully realized contactless detection of magnetic properties and quantized vortices in micro-superconducting nanoflakes.
  • Observed anomalous hysteresis loops and suppressed Little-Parks oscillations due to disordered pinned vortices.
  • Quantitatively evaluated the density of pinning centers in Bi2 Sr2 CaCu2 O8+δ nanoflakes.

Conclusions:

  • The superconducting micro-magnetometer offers a novel approach for mesoscopic electromagnetic phenomena research.
  • This technique overcomes the limitations of conventional SQUID for analyzing micro-scale superconducting samples.
  • Enables quantitative evaluation of vortex pinning centers, previously inaccessible.