Empirical distribution function: Difference between revisions

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{{MagneticCircuitSegments}}
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:'''''Magnetic inductance''' is not to be confused with "Magnetic induction", which usually refers to [[Magnetic field]].''
 
'''''Magnetic inductance (inductive magnetic reactance)''''' ([[SI Unit]]: -[[Omega|Ω]]<sup>−1</sup>) is a component in the [[gyrator-capacitor model]] for magnetic systems.
 
For phasor analysis the magnetic inductive reactance is:
 
:<math>x_L = \omega L_M</math>
 
Where:
:<math>L_M</math> is the [[magnetic inductivity]] ([[SI Unit]]: -s·[[Omega|Ω]]<sup>-1</sup>)
:<math>\omega</math> is the [[angular frequency]] of the magnetic circuit
 
In the complex form it is a positive imaginary number:
 
:<math>jx_L = j\omega L_M</math>
 
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 [[Very high frequency|VHF]] and/or [[Ultra high frequency|UHF]] frequencies.
 
The notion of magnetic inductivity is employed in analysis and computation of circuit behavior in the [[gyrator-capacitor model]] in a way analogous to [[inductance]] in electrical circuits.
 
==See also==
*[[Magnetic inductive coil]]
 
==References==
# Pohl R. W. ELEKTRIZITÄTSLEHRE. – Berlin-Göttingen-Heidelberg: SPRINGER-VERLAG, 1960.
# Popov V. P.  The Principles of Theory of Circuits. – M.: Higher School, 1985, 496 p. (In Russian).
 
[[Category:Magnetic circuits]]
 
 
{{electromagnetism-stub}}

Latest revision as of 20:31, 18 October 2014

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