Magnetomotive force

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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 \frac {10}{4\pi} (≈ 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 \mathcal{F} in an inductor or electromagnet consisting of a coil of wire is given by:

\mathcal{F} = N I

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:

\mathcal{F} = \Phi \mathcal{R}

where Φ is the magnetic flux and \mathcal{R} 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

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