en>Spinningspark: /* References */ +cat

2014-10-16T22:00:15Z

References: +cat

← Older revision		Revision as of 00:00, 17 October 2014
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	~~'''Magnetic reactance''' is the parameter of a passive [[magnetic circuit]] or its element, which is equal~~ to the square root of the difference of squares of the full and effective magnetic resistance for a [[magnetic current]], taken with the sign plus, if the magnetic current lags behind the [[Magnetic tension force\|magnetic tension]] in phase, and with the sign minus, ~~if the magnetic current leads the magnetic tension in phase.~~		Nice to meet you, my title is Numbers Held although I don't really like being known as like that. Doing ceramics is what love performing. Hiring is his profession. South Dakota is exactly where me and my spouse reside.<br><br>my site :: std testing at home ([http://www.hard-ass-porn.com/blog/111007 see this here])

	~~Magnetic reactance <ref>{{Cite book\|~~
	~~author=Pohl, R. W.\|~~
	title~~=Elektrizitätslehre\|~~
	~~location=Berlin-Gottingen-Heidelberg\|~~
	~~publisher=Springer-Verlag\|~~
	~~year=1960\|~~
	~~language=German}}~~
	~~</ref><ref>{{Cite book\|~~
	~~author=Popov, V~~. P.\|
	~~title=The Principles of Theory of Circuits\|~~
	~~publisher=M.: Higher School\|~~
	~~year=1985\|~~
	~~language=Russian}}</ref><ref>{{Cite book\|~~
	~~author=Küpfmüller, K~~.\|
	~~title=Einführung in die theoretische Elektrotechnik\|~~
	~~location=Berlin-Gottingen-Heidelberg\|~~
	~~publisher=Springer-Verlag\|~~
	~~year=1959\|~~
	~~language=German}}</ref>~~ is ~~the component of [[complex magnetic impedance]] of the [[alternating current]] circuit, which produces the phase shift between a magnetic current~~ and ~~magnetic tension in the circuit~~. ~~It is measured in units of~~ <~~math~~>~~\tfrac{1}{\Omega}~~<~~/math> and is denoted by <math>x</math~~> (~~or <math>X</math>). It may be inductive <math>x_L = \omega L_M</math> or capacitive <math>x_C = \tfrac{1}{\omega C_M}</math>, where <math>\omega</math> is the~~ [~~[angular frequency]] of a magnetic current, <math>L_M<~~/~~math> is the [[magnetic inductivity]] of a circuit, <math>C_M<~~/~~math> is the [[magnetic capacitivity]] of a circuit~~. ~~The magnetic reactance of an undeveloped circuit with the inductivity and the capacitivity, which are connected in series, is equal: <math>x = x_L~~ - ~~x_C = \omega L_M~~ - ~~\frac{1}{\omega C_M}</math>~~ . ~~If <math>x_L = x_C<~~/~~math>, then the sum reactance <math>x = 0<~~/~~math> and [[resonance~~]~~] takes place in the circuit. In the general case <math>x = \sqrt{z^2 - r^2}</math>. When an [[energy loss]] is absent (<math>r = 0</math>~~) <math>x = z</math>. The angle of the phase shift in a magnetic circuit <math>\phi = \arctan{\frac{x}{r}}</math>. On a complex plane, the magnetic reactance appears as the side of the resistance triangle for circuit of an alternating current.

	~~==References==~~
	~~<references />~~

	~~{{DEFAULTSORT:Magnetic Reactance}}~~
	~~[[Category:Electromagnetism]]~~


	~~{{Physics-stub}}~~

en>Kmarinas86 at 11:08, 14 March 2011

2011-03-14T11:08:09Z

New page

'''Magnetic reactance''' is the parameter of a passive [[magnetic circuit]] or its element, which is equal to the square root of the difference of squares of the full and effective magnetic resistance for a [[magnetic current]], taken with the sign plus, if the magnetic current lags behind the [[Magnetic tension force|magnetic tension]] in phase, and with the sign minus, if the magnetic current leads the magnetic tension in phase.

Magnetic reactance <ref>{{Cite book|
author=Pohl, R. W.|
title=Elektrizitätslehre|
location=Berlin-Gottingen-Heidelberg|
publisher=Springer-Verlag|
year=1960|
language=German}}
</ref><ref>{{Cite book|
author=Popov, V. P.|
title=The Principles of Theory of Circuits|
publisher=M.: Higher School|
year=1985|
language=Russian}}</ref><ref>{{Cite book|
author=Küpfmüller, K.|
title=Einführung in die theoretische Elektrotechnik|
location=Berlin-Gottingen-Heidelberg|
publisher=Springer-Verlag|
year=1959|
language=German}}</ref> is the component of [[complex magnetic impedance]] of the [[alternating current]] circuit, which produces the phase shift between a magnetic current and magnetic tension in the circuit. It is measured in units of <math>\tfrac{1}{\Omega}</math> and is denoted by <math>x</math> (or <math>X</math>). It may be inductive <math>x_L = \omega L_M</math> or capacitive <math>x_C = \tfrac{1}{\omega C_M}</math>, where <math>\omega</math> is the [[angular frequency]] of a magnetic current, <math>L_M</math> is the [[magnetic inductivity]] of a circuit, <math>C_M</math> is the [[magnetic capacitivity]] of a circuit. The magnetic reactance of an undeveloped circuit with the inductivity and the capacitivity, which are connected in series, is equal: <math>x = x_L - x_C = \omega L_M - \frac{1}{\omega C_M}</math> . If <math>x_L = x_C</math>, then the sum reactance <math>x = 0</math> and [[resonance]] takes place in the circuit. In the general case <math>x = \sqrt{z^2 - r^2}</math>. When an [[energy loss]] is absent (<math>r = 0</math>) <math>x = z</math>. The angle of the phase shift in a magnetic circuit <math>\phi = \arctan{\frac{x}{r}}</math>. On a complex plane, the magnetic reactance appears as the side of the resistance triangle for circuit of an alternating current.

==References==
<references />

{{DEFAULTSORT:Magnetic Reactance}}
[[Category:Electromagnetism]]

{{Physics-stub}}

← Older revision		Revision as of 00:00, 17 October 2014
Line 1:		Line 1:
	~~'''Magnetic reactance''' is the parameter of a passive [[magnetic circuit]] or its element, which is equal~~ to the square root of the difference of squares of the full and effective magnetic resistance for a [[magnetic current]], taken with the sign plus, if the magnetic current lags behind the [[Magnetic tension force\|magnetic tension]] in phase, and with the sign minus, ~~if the magnetic current leads the magnetic tension in phase.~~		Nice to meet you, my title is Numbers Held although I don't really like being known as like that. Doing ceramics is what love performing. Hiring is his profession. South Dakota is exactly where me and my spouse reside.<br><br>my site :: std testing at home ([http://www.hard-ass-porn.com/blog/111007 see this here])

	~~Magnetic reactance <ref>{{Cite book\|~~
	~~author=Pohl, R. W.\|~~
	title~~=Elektrizitätslehre\|~~
	~~location=Berlin-Gottingen-Heidelberg\|~~
	~~publisher=Springer-Verlag\|~~
	~~year=1960\|~~
	~~language=German}}~~
	~~</ref><ref>{{Cite book\|~~
	~~author=Popov, V~~. P.\|
	~~title=The Principles of Theory of Circuits\|~~
	~~publisher=M.: Higher School\|~~
	~~year=1985\|~~
	~~language=Russian}}</ref><ref>{{Cite book\|~~
	~~author=Küpfmüller, K~~.\|
	~~title=Einführung in die theoretische Elektrotechnik\|~~
	~~location=Berlin-Gottingen-Heidelberg\|~~
	~~publisher=Springer-Verlag\|~~
	~~year=1959\|~~
	~~language=German}}</ref>~~ is ~~the component of [[complex magnetic impedance]] of the [[alternating current]] circuit, which produces the phase shift between a magnetic current~~ and ~~magnetic tension in the circuit~~. ~~It is measured in units of~~ <~~math~~>~~\tfrac{1}{\Omega}~~<~~/math> and is denoted by <math>x</math~~> (~~or <math>X</math>). It may be inductive <math>x_L = \omega L_M</math> or capacitive <math>x_C = \tfrac{1}{\omega C_M}</math>, where <math>\omega</math> is the~~ [~~[angular frequency]] of a magnetic current, <math>L_M<~~/~~math> is the [[magnetic inductivity]] of a circuit, <math>C_M<~~/~~math> is the [[magnetic capacitivity]] of a circuit~~. ~~The magnetic reactance of an undeveloped circuit with the inductivity and the capacitivity, which are connected in series, is equal: <math>x = x_L~~ - ~~x_C = \omega L_M~~ - ~~\frac{1}{\omega C_M}</math>~~ . ~~If <math>x_L = x_C<~~/~~math>, then the sum reactance <math>x = 0<~~/~~math> and [[resonance~~]~~] takes place in the circuit. In the general case <math>x = \sqrt{z^2 - r^2}</math>. When an [[energy loss]] is absent (<math>r = 0</math>~~) <math>x = z</math>. The angle of the phase shift in a magnetic circuit <math>\phi = \arctan{\frac{x}{r}}</math>. On a complex plane, the magnetic reactance appears as the side of the resistance triangle for circuit of an alternating current.

	~~==References==~~
	~~<references />~~

	~~{{DEFAULTSORT:Magnetic Reactance}}~~
	~~[[Category:Electromagnetism]]~~


	~~{{Physics-stub}}~~

Magnetic capacitivity - Revision history

en>Spinningspark: /* References */ +cat

en>Kmarinas86 at 11:08, 14 March 2011