- Magnetomotive force
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Magnetic Circuits
Conventional Magnetic Circuits- Magnetomotive force
- Magnetic flux Φ
- Magnetic reluctance
Phasor Magnetic Circuits
Related Concepts
Gyrator-capacitor model variablesMagnetomotive 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. The name came about because in magnetic circuits it plays a role analogous to the role electromotive force (voltage) plays in electric circuits.
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.
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.
References
- The Penguin Dictionary of Physics, 1977, ISBN 0-14-051071-0
Categories:- Magnetism
- Physical quantities
- Physics stubs
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