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Faraday experimentally studied lines of magnetic force and electrostatic force, showing them not to fit action at a distance models. In 1852 Faraday wrote the paper "On the Physical Character of the Lines of Magnetic Force" [ 8 ] which examined gravity, radiation, and electricity, and their possible relationships with the transmission medium ...
Both of these are modeled quite well as tiny loops of current called magnetic dipoles that produce their own magnetic field and are affected by external magnetic fields. The most elementary force between magnets is the magnetic dipole–dipole interaction. If all magnetic dipoles for each magnet are known then the net force on both magnets can ...
[note 5] Magnetic field "lines" are also visually displayed in polar auroras, in which plasma particle dipole interactions create visible streaks of light that line up with the local direction of Earth's magnetic field. Field lines can be used as a qualitative tool to visualize magnetic forces. In ferromagnetic substances like iron and in ...
Magnetic lines of force of a bar magnet shown by iron filings on paper Detecting magnetic field with compass and with iron filings Main article: Magnetic field The phenomenon of magnetism is "mediated" by the magnetic field.
Michael Faraday developed the concept of lines of force to describe electric and magnetic phenomena. [13] In 1831, he writes [13] By magnetic curves, I mean the lines of magnetic forces, however modified by the juxtaposition of poles, which would be depicted by iron filings; or those to ·which a very small magnetic needle would form a tangent."
The magnetic equator is the line where the inclination is zero (the magnetic field is horizontal). The global definition of the Earth's field is based on a mathematical model. If a line is drawn through the center of the Earth, parallel to the moment of the best-fitting magnetic dipole, the two positions where it intersects the Earth's surface ...
The magnetic inductive current represents lines of force. In particular, it represents lines of inverse-square law force. The extension of the above considerations confirms that where B is to H , and where J is to ρ , then it necessarily follows from Gauss's law and from the equation of continuity of charge that E is to D i.e. B parallels with ...
This practical unit was previously called a line, [4] reflecting Faraday's conception of the magnetic field as curved lines of magnetic force, [5] which he designated as line of magnetic induction. [4] Kiloline (10 3 line) and megaline (10 6 line) were sometimes used because 1 line was very small relative to the phenomena that it was used to ...