| Magnetic Circuits |
|---|
|
Convetional Magnetic Circuits |
Magnetomotive force  |
| Magnetic flux Φ |
Magnetic reluctance  |
|
Phasor Magnetic Circuits |
| Complex reluctance Zμ |
|
Related Concepts |
| Magnetic permeability μ |
|
Gyrator-Capacitor Model variables |
| Magnetic impedance zM |
| Effective resistance rM |
| Magnetic inductivity LM |
| Magnetic capacitivity CM |
- Magnetic inductance is not to be confused with "Magnetic induction", which usually refers to Magnetic field.
Magnetic inductance (inductive magnetic reactance) (SI Unit: -Ω−1) is a component in the gyrator-capacitor model for magnetic systems.
For phasor analysis the magnetic inductive reactance is:
- xL = ωLM
Where:
- LM is the magnetic inductivity (SI Unit: -s·Ω-1)
- ω is the angular frequency of the magnetic circuit
In the complex form it is a positive imaginary number:
- jxL = jωLM
The magnetic potential energy sustained by magnetic inductivity varies with the frequency of oscillations in electric fields. The average power in a given period is equal to zero. Due to its dependence on frequency, magnetic inductance is mainly observable in magnetic circuits which operate at VHF and/or UHF frequencies.
The notion of magnetic inductivity is employed in analysis and computation of circuit behavior in the grator-capacitor model in a way analogous to inductance in electrical circuits.
References
- Pohl R. W. ELEKTRIZITÄTSLEHRE. – Berlin-Gottingen-Heidelberg: SPRINGER-VERLAG, 1960.
- Popov V. P. The Principles of Theory of Circuits. – M.: Higher School, 1985, 496 p. (In Russian).
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