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Related Concept Videos

Magnetostatic Boundary Conditions01:28

Magnetostatic Boundary Conditions

An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
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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.
Induction01:16

Induction

An emf is induced when the magnetic field in a coil is changed by pushing a bar magnet into or out of the coil. emfs of opposite signs are produced by motion in opposite directions, and the directions of emfs are also reversed by reversing poles. The same results are produced if the coil is moved rather than the magnet—it is the relative motion that is important. The faster the motion, the greater the emf. Additionally, there is no emf when the magnet is stationary relative to the coil.
A...
Lenz's Law01:15

Lenz's Law

The direction in which the induced emf drives the current around a wire loop can be found through the negative sign. However, it is usually easier to determine this direction with Lenz's law, named in honor of its discoverer, Heinrich Lenz (1804–1865). Lenz's law states that the direction of the induced emf drives the current around a wire loop always to oppose the change in magnetic flux that causes the emf.
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Optimized Setup and Protocol for Magnetic Domain Imaging with In Situ Hysteresis Measurement
09:43

Optimized Setup and Protocol for Magnetic Domain Imaging with In Situ Hysteresis Measurement

Published on: November 7, 2017

Minimizing crosstalk in three-axial induction magnetometers.

Asaf Grosz1, Eugene Paperno, Shai Amrusi

  • 1Department of Electrical and Computer Engineering, Ben-Gurion University of the Negev, 84105 Beer-Sheva, Israel.

The Review of Scientific Instruments
|January 5, 2011
PubMed
Summary

This study models and verifies crosstalk in three-axial induction magnetometers. Minimizing crosstalk is crucial for magnetometer accuracy, especially near resonance frequencies.

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Area of Science:

  • Physics
  • Electrical Engineering
  • Instrumentation

Background:

  • Crosstalk is an inherent issue in three-axial induction magnetometers.
  • Understanding crosstalk is vital for improving magnetometer accuracy.

Purpose of the Study:

  • To develop and experimentally verify a theoretical model for crosstalk in three-axial induction magnetometers.
  • To analyze the impact of crosstalk on magnetometer accuracy.

Main Methods:

  • Theoretical modeling of crosstalk in transverse coils.
  • Experimental verification of the developed model.
  • Analysis of crosstalk components and their frequency dependence.

Main Results:

  • Crosstalk has two components: applied magnetic flux and secondary flux.
  • Crosstalk magnitude and phase vary significantly with frequency, peaking at resonance.
  • Magnetic feedback can reduce crosstalk but increases the minimum crosstalk value.

Conclusions:

  • Crosstalk significantly affects magnetometer accuracy, particularly around resonance.
  • Magnetic feedback offers a method to manage crosstalk but has trade-offs.
  • Low crosstalk is beneficial for both narrow and wide-band magnetometer applications.