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Area Electromagnetism / Electromagnetic concepts and quantities

IEV ref121-11-57

Symbol
Vm

en
magnetic tension
scalar quantity equal to the line integral of the magnetic field strength H along a specified path linking two points a and b:

V m,ab = r a r b Hdr MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabaabaiaafaaake aacaWGwbWaaSbaaSqaaiaab2gacaqGSaGaaeyyaiaabkgaaeqaaOGa eyypa0Zaa8qCaeaaiiWacaWFibGaeyyXICTaciizaiaa=jhaaSqaaG Gaciaa+jhadaWgaaadbaqcLbmacaqGHbaameqaaaWcbaGaamOCaWWa aSbaaeaajugWaiaabkgaaWqabaaaniabgUIiYdaaaa@4D08@

where ra and rb are the position vectors for a and b, respectively, and dr is the vector line element


fr
tension magnétique, f
grandeur scalaire égale à la circulation du champ magnétique H le long d’un chemin donné joignant deux points a et b:

V m,ab = r a r b Hdr MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgaruWqVvNCPvMCG4uz 3bqee0evGueE0jxyaibaieYdi9WrpeeC0lXdi9qqqj=hEeeu0lXdbb a9frFj0xb9Lqpepeea0xd9s8qiYRWxGi6xij=hbba9q8aq0=yq=He9 q8qiLsFr0=vr0=vr0db8meaabaGacmGadiWaaiWabaabaiaafaaake aacaWGwbWaaSbaaSqaaiaab2gacaqGSaGaaeyyaiaabkgaaeqaaOGa eyypa0Zaa8qCaeaaiiWacaWFibGaeyyXICTaciizaiaa=jhaaSqaaG Gaciaa+jhadaWgaaadbaqcLbmacaqGHbaameqaaaWcbaGaamOCaWWa aSbaaeaajugWaiaabkgaaWqabaaaniabgUIiYdaaaa@4D08@

ra et rb sont les rayons vecteurs de a et b respectivement et dr est l’élément vectoriel d’arc


ar
جهد مغناطيسي

de
magnetische Spannung, f

es
tensión magnética

fi
magneettijännite

it
tensione magnetica

ko
자기 장력

ja
磁位

no
nb magnetisk spenning

nn magnetisk spenning

pl
napięcie magnetyczne

pt
tensão magnética

ru
магнитное напряжение

sv
magnetisk spänning

Publication date: 1998-08
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