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Charge is usually thought of as a [[scalar]] or a [[quantum number]] while velocity is a [[vector]]. In fact, charge is a vector whose direction is determined by the [[spin]] of a particle, but [[macroscopic]] calculations are not concerned with this direction and define charge to be along an [[axis]] so that the direction of another vector is really its direction relative to charge. A vector pointing along an axis becomes one-dimensional, or identical to a scalar.
Charge is usually thought of as a [[scalar]] or a [[quantum number]] while velocity is a [[vector]]. In fact, charge is a vector whose direction is determined by the [[spin]] of a particle, but [[macroscopic]] calculations are not concerned with this direction and define charge to be along an [[axis]] so that the direction of another vector is really its direction relative to charge. A vector pointing along an axis becomes one-dimensional, or identical to a scalar.


The idea that magnetic forces act on moving charges is clear in an [[electromagnet]] but not obvious in a [[permanent magnet]]. In fact, all substances have charges moving in them all of the time, one of the difficulties in reaching [[absolute zero]]. In most substances, all of the magnetic fields produced by this motion cancel each other out, but magnetic substances have more proper alignment. At the microscopic level, many molecules are magnets - [[hydrogen fluoride|HF]] for example is a dipole. [[Polarity]] is most often expressed in terms of [[electronegativity]] but the strength of its poles could also be expressed in ampere-metres as well.
The idea that magnetic forces act on moving charges is clear in an [[electromagnet]] but not obvious in a [[permanent magnet]]. In fact, all substances have charges moving in them all of the time, one of the difficulties in reaching [[absolute zero]]. In most substances, all of the magnetic fields produced by this motion cancel each other out, but magnetic substances have more proper alignment. At the microscopic level, many molecules are magnets - [[hydrogen fluoride|HF]] for example is a dipole. [[Polarity]] is most often expressed in terms of [[electronegativity]] but the strength of its poles could be expressed in ampere-metres as well.


==References==
==References==

Revision as of 03:00, 13 May 2007

The ampere-metre which has the symbol A m or A-m is the SI unit for pole strength in a magnet. No abbreviation has been given to this unit.

Derivation

Einstein proved that a magnetic field is the relativistic part of an electric field. This means that while an electric field acts between charges, a magnetic field acts between moving charges (as a charge moves through space more quickly and through time more slowly, its electromagnetic force becomes more magnetic and less electric). Therefore, the pole strength is the product of charge and velocity.

Usefulness

Few calculations actually in involve the strength of a pole in ampere-metres because a single pole has never been isolated. Magnets are dipoles which require more complicated calculations than monopoles. However, the strength of a magnetic field is measured in teslas and one tesla is one newton per ampere-metre which confirms that the unit for pole strength is indeed the ampere-metre.

Misconceptions

Charge is usually thought of as a scalar or a quantum number while velocity is a vector. In fact, charge is a vector whose direction is determined by the spin of a particle, but macroscopic calculations are not concerned with this direction and define charge to be along an axis so that the direction of another vector is really its direction relative to charge. A vector pointing along an axis becomes one-dimensional, or identical to a scalar.

The idea that magnetic forces act on moving charges is clear in an electromagnet but not obvious in a permanent magnet. In fact, all substances have charges moving in them all of the time, one of the difficulties in reaching absolute zero. In most substances, all of the magnetic fields produced by this motion cancel each other out, but magnetic substances have more proper alignment. At the microscopic level, many molecules are magnets - HF for example is a dipole. Polarity is most often expressed in terms of electronegativity but the strength of its poles could be expressed in ampere-metres as well.

References