Magnetomotive force
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Conventional Magnetic Circuits
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Gyrator-capacitor model variables |
Magnetomotive force (MMF) (SI Unit: Ampere) is any physical driving (motive) force that produces magnetic flux. In this context, the expression "driving force" is used in a general sense of "work potential", and is analogous, but distinct from force measured in newtons. Magnetomotive force is so named because it plays a role in magnetic circuits analogous to that of electromotive force (voltage) in electric circuits.
[edit] SI versus CGS units
The SI unit of magnetomotive force is the ampere (A), represented by a steady, direct electric current of one ampere flowing in a single-turn loop of electrically conducting material in a vacuum.
The CGS unit of magnetomotive force is the gilbert (Gi), established by the IEC in 1930 [1]. The gilbert is defined differently, and is a slightly smaller unit than the ampere. The unit is named after William Gilbert (1544–1603) English physician, astronomer and natural philosopher.
The conversion factor between the SI and CGS units is
(≈ 0.795774715) ampere for every gilbert.
Between the CGS unit and SI unit, the MKS unit magnetomotive force was the ampere-turn At.
[edit] Equations
The magnetomotive force
in an inductor or electromagnet consisting of a coil of wire is given by:
where N is the number of turns of wire in the coil and I is the current in the wire.
The equation for the magnetic flux in a magnetic circuit, sometimes known as Hopkinson's law, is:
where Φ is the magnetic flux and
is the reluctance of the magnetic circuit. It can be seen that the magnetomotive force plays a role in this equation analogous to the voltage V in Ohm's law: V = IR.
[edit] References
- The Penguin Dictionary of Physics, 1977, ISBN 0-14-051071-0
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