Related Experiment Video
Updated: Jan 8, 2026

11:10
Fabrication and Operation of a Nano-Optical Conveyor Belt
Published on: August 26, 2015
12.0K
Designing functional magnetic cloaks for real-world geometries.
Yusen Guo1, Alberto Paganini1, Harold S Ruiz2
1School of Computing and Mathematical Sciences, University of Leicester, Leicester LE1 7RH, UK.
Science Advances
|December 19, 2025
Summary
Researchers developed a new method for magnetic cloaking, making complex shapes undetectable to magnetic fields. This physics-based framework uses optimization to design custom magnetic shields for real-world applications.
Area of Science:
- Physics
- Materials Science
- Electromagnetism
Background:
- Magnetic cloaking allows objects to be invisible to external magnetic fields.
- Current methods are limited to simple shapes like spheres and cylinders, hindering practical use.
Purpose of the Study:
- To develop a physics-based framework for designing magnetic cloaks for arbitrarily shaped objects.
- To enable the creation of practical magnetic shields for complex geometries.
Main Methods:
- Solving Maxwell's equations with spatial material constraints.
- Utilizing a physics-based optimization framework.
- Designing continuous, spatially varying permeability profiles.
Main Results:
- Successfully designed magnetic cloaks for complex, non-ideal shapes.
- Demonstrated low-distortion cloaking performance using commercially available superconductors.
- Achieved permeability values within manufacturable ranges.
Conclusions:
- The developed framework enables customizable magnetic shields for real-world components.
- This approach paves the way for magnetic cloaking in extreme environments like fusion energy systems.
Related Concept Videos
Divergence and Curl of Magnetic Field
3.9K
The magnetic field due to a volume current distribution given by the Biot–Savart Law can be expressed as follows:
3.9K
Magnetic Field Of A Current Loop
6.2K
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.
6.2K
Potential Due to a Magnetized Object
752
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...
752
Magnetic Vector Potential
1.5K
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...
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...
1.5K
Magnetic Field Lines
5.4K
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:
5.4K
Electromagnetic Fields
2.7K
Electric fields generated by static charges, often referred to as electrostatic fields, are characteristically different from electric fields created by time-varying magnetic fields. While the former is a conservative field, implying that no net work is done on a test charge if it goes around in a complete loop in the field, the latter is, by definition, not a conservative field; net work is done, and it is proportional to the rate of change of magnetic flux.
However, the observation of...
However, the observation of...
2.7K

