| 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 capacitivity (SI Unit: H) is a component used in the gyrator-capacitor model of magnetic systems.
This element, denoted as CM, is an extensive property and is defined as:

Where: μrμ0 = μ is the magnetic permeability, S, l is the cross-section and the length of the element.
For phasor analysis, the magnetic permeability[1] and the magnetic capacitivity are complex values[1, 2].
Magnetic capacitivity is also equal to magnetic flux divided by the difference of magnetic potential across the element.

Where:
- φM1 − φM2 is the difference of the magnetic potentials.
The notion of magnetic capacitivity is employed in the gyrator-capacitor model in a way analogous to capacitance in electrical circuits.
References
- Arkadiew W. Eine Theorie des elektromagnetischen Feldes in den ferromagnetischen Metallen. – Phys. Zs., H. 14, No 19, 1913, S. 928-934.
- Popov V. P. The Principles of Theory of Circuits. – M.: Higher School, 1985, 496 p. (In Russian).
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