Shapiro–Wilk test: Difference between revisions

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{{MagneticCircuitSegments}}
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'''''Magnetic capacitance (capacitive magnetic reactance)''''' ([[SI Unit]]: -[[Omega|Ω]]<sup>−1</sup>) is a magnetic "reactance" which prevents magnetic "current" in oscillating magnetic circuits from rising. This is associated with high reluctance.
 
For harmonic regimes it is equal to:
 
:<math>x_C = \frac{1}{\omega C_M}</math>
 
Where:
:<math>C_M</math> is the [[magnetic capacitivity]] ([[SI Unit]]: -s·[[Omega|Ω]]<sup>-1</sup>)
:<math>\omega</math> is the [[angular frequency]] of the magnetic circuit
 
In complex form it is written as an imaginary number:
 
:<math>-jx_C = -j\frac{1}{\omega C_M} = \frac{1}{j\omega C_M}</math>
 
The electrical potential energy sustained by Magnetic capacitivity varies with the frequency of oscillations in magnetic fields. The average power in a given period is equal to zero. The magnetic capacitivity is a reactive part of the magnetic circuit[1, 2].<ref>Pohl R. W. ELEKTRIZITÄTSLEHRE. – Berlin-Gottingen-Heidelberg: SPRINGER-VERLAG, 1960.</ref><ref>Popov V. P.  The Principles of Theory of Circuits. – M.: Higher School, 1985, 496 p. (In Russian).</ref>
 
==References==
<references/>
 
[[Category:Magnetic circuits]]

Revision as of 23:06, 27 February 2014

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