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Area Electromagnetism / Electromagnetic concepts and quantities

IEV ref 121-11-79

Symbol
Ul
Um

en
loop voltage
loop tension
scalar quantity equal to the time derivative of the line integral of the magnetic vector potential along a closed path C in which charge carriers can be displaced

U l = d dt C A dr = d dt S B e n dA = d dt Ψ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaciaabmqaamaabaabaaGcbaGaamyvamaaBa aaleaacaqGSbaabeaakiabg2da9iabgkHiTmaalaaabaGaaiizaaqa aiaacsgacaWG0baaamaapubabaGaaCyqaiacycOGKbGaaCOCaaWcba Gaae4qaaqab0GaeSyeUhTaey4kIipakiabg2da9iabgkHiTmaalaaa baGaaiizaaqaaiaacsgacaWG0baaamaapebabaGaaCOqaiabgwSixl aahwgadaWgaaWcbaGaaeOBaaqabaGccaGGKbGaamyqaaWcbaGaae4u aaqab0Gaey4kIipakiabg2da9iabgkHiTmaalaaabaGaaiizaaqaai aacsgacaWG0baaaiabfI6azbaa@5A98@

where A is the magnetic vector potential at a point of the path C, dr is a vector line element of C, B is the magnetic flux density at a point on a surface S delimited by the curve C, endA is a vector surface element of S, Ψ is the total flux through this surface, and t is time

Note 1 to entry: The loop voltage is often wrongly denoted as the induced voltage; this is only true when no current is flowing through the path C.

Note 2 to entry: The coherent SI unit of the loop voltage is volt, V = s−3 m2 kg A−1.


fr
tension de boucle, f
grandeur scalaire égale à la dérivée par rapport au temps de l'intégrale du potentiel vecteur magnétique le long d’un chemin C fermé dans lequel des porteurs de charge peuvent se déplacer

U l = d dt C A dr = d dt S B e n dA = d dt Ψ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaciaabmqaamaabaabaaGcbaGaamyvamaaBa aaleaacaqGSbaabeaakiabg2da9iabgkHiTmaalaaabaGaaiizaaqa aiaacsgacaWG0baaamaapubabaGaaCyqaiacycOGKbGaaCOCaaWcba Gaae4qaaqab0GaeSyeUhTaey4kIipakiabg2da9iabgkHiTmaalaaa baGaaiizaaqaaiaacsgacaWG0baaamaapebabaGaaCOqaiabgwSixl aahwgadaWgaaWcbaGaaeOBaaqabaGccaGGKbGaamyqaaWcbaGaae4u aaqab0Gaey4kIipakiabg2da9iabgkHiTmaalaaabaGaaiizaaqaai aacsgacaWG0baaaiabfI6azbaa@5A98@

A est le potentiel vecteur magnétique en un point du chemin C, dr est un élément vectoriel d’arc de C, B est l’induction magnétique en un point d’une surface S délimitée par la courbe C, endA est un élément vectoriel de surface S, Ψ est le flux total à travers cette surface, et t est le temps

Note 1 à l’article: La tension de boucle est souvent désignée à tort comme la tension induite; ceci est vrai uniquement en l’absence de courant circulant par le chemin C.

Note 2 à l’article: L’unité SI cohérente de la tension de boucle est le volt, V = s−3 m2 kg A−1.


ar
جهد حثي
جهد حلقى

de
Umlaufspannung, f

ko
원형전압

ja
ループ電圧

pl
napięcie w pętli, n
napięcie w obwodzie zamkniętym, n

zh
回路电压

Publication date: 2021-03
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