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Related Concept Videos

Magnetic Field Due To A Thin Straight Wire01:27

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 Field Due to Two Straight Wires01:18

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 Force Between Two Parallel Currents01:13

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...
Magnetic Field Of A Current Loop01:16

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 of a Solenoid01:18

Magnetic Field of a Solenoid

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...
Mutual Inductance01:24

Mutual Inductance

Inductance is the property of a device that tells us how effectively it induces an emf in another device. In other words, it is a physical quantity that expresses the effectiveness of a given device.
When two circuits carrying time-varying currents are close to one another, the magnetic flux through each circuit varies because of the changing current in the other circuit. Consequently, an emf is induced in each circuit by the changing current in the other. Therefore, this type of emf is called...

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MRM Microcoil Performance Calibration and Usage Demonstrated on Medicago truncatula Roots at 22 T
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PCB Coil Pairs for Small Magnetic Volumes.

Howard R Selden1, Rebecca Y Lai2, Ryan A Riskowski1

  • 1Department of Physics, University of Nebraska at Omaha, 6001 Dodge Street, Omaha, NE 68182, USA.

Nanomaterials (Basel, Switzerland)
|July 13, 2026
PubMed
Summary

A compact radiofrequency magnetic field generator using printed circuit board coils offers reduced size and power for localized applications. This device is suitable for magnetic nanoparticle heating and actuation, demonstrating consistent operating parameters.

Keywords:
iron oxide nanoparticlesmagnetic heatingmagnetic nanoparticlesradiofrequency heating

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Area of Science:

  • Electrical Engineering
  • Biomedical Engineering
  • Materials Science

Background:

  • Localized radiofrequency (RF) magnetic fields are crucial for applications like magnetic nanoparticle heating and actuation.
  • Conventional solenoidal systems often present limitations in terms of size, sample volume, and power consumption.

Purpose of the Study:

  • To describe a novel, compact RF magnetic field generator.
  • To enable field generation within millimeter-scale volumes.
  • To assess its suitability for applications requiring localized magnetic fields.

Main Methods:

  • Design and fabrication of a compact RF magnetic field generator using stacked, paired parallel printed multilayer circuit board (PCB) coils.
  • Characterization of RF response, including impedance and scattering parameters.
  • Electromagnetic modeling and experimental measurement of magnetic field amplitude and spatial homogeneity.

Main Results:

  • The PCB-based coil configuration significantly reduces device size, sample volume, and power requirements compared to solenoidal systems.
  • The system operates effectively near ~330 kHz, a frequency relevant for magnetic nanoparticle heating.
  • Electromagnetic modeling showed a maximum local deviation from the mean field of 5.5%.
  • Experimental measurements confirmed a mean Bz field of 6.3 ± 0.1 mT/A between paired PCBs.

Conclusions:

  • The developed compact RF magnetic field generator is a viable alternative to conventional systems for localized field generation.
  • The device's performance characteristics are consistent with the requirements for magnetic nanoparticle heating applications.
  • This PCB-based coil design offers a scalable and efficient solution for micro-scale magnetic field applications.