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Area Superconductivity / Electromagnetic phenomena and properties

IEV ref 815-22-18

en
scaling law of pinning force density
empirical law that describes the pinning force density as separable functions of temperature T, and magnetic flux density, B

Note 1 to entry: The pinning force density, F p MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOraOWaaSbaaK qaafaacaqGWbaabeaaaaa@3583@ , is typically given by F p B c2 (T) m f(b) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOraOWaaSbaaK qaafaacaqGWbaabeaajaaqcqGHDisTkmaadmaajaaqbaGaamOqaOWa aSbaaKqaafaacaqGJbGaaGOmaaqabaqcaaKaaeikaiaadsfacaqGPa aacaGLBbGaayzxaaGcdaahaaqcbauabeaacaaMi8UaamyBaaaajaaq caWGMbGaaeikaiaadkgacaqGPaaaaa@4553@ , where m is a real number, f(b) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaq Fn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpe WZqaaeaaciWacmGadaGadiaabaGaaqaaaOqaaiaadAgacaqGOaGaam OyaiaabMcaaaa@387A@ is a function of the reduced magnetic flux density b= B/B c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOyaiabg2da9O WaaSGbaKaaafaacaWGcbaabaGaamOqaaaakmaaBaaajeaqbaGaae4y aiaaikdaaeqaaaaa@394B@ and B c2 = μ 0 H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOqaOWaaSbaaK qaafaacaqGJbGaaGOmaaqabaqcaaKaeyypa0JaaqiVdOWaaSbaaKqa afaacaaIWaaabeaajaaqcaaMe8UaamisaOWaaSbaaKqaafaacaqGJb GaaeOmaaqabaaaaa@3EA4@ , where μ 0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaaqiVdOWaaSbaaK qaafaacaqGWaaabeaaaaa@35BD@ is the magnetic constant and H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaacaqGJbGaaeOmaaqabaaaaa@362D@ is the upper critical field strength.

Note 2 to entry: This entry was numbered 815-12-26 in IEC 60050-815:2015.


fr
loi d'échelle pour la densité de force d'ancrage, f
loi d’échelle pour la densité de la force de piégeage, f
loi empirique qui exprime la densité de force d'ancrage sous forme de fonctions distinctes de température T et d’induction magnétique, B

Note 1 à l’article: La densité de force d'ancrage, F p MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOraOWaaSbaaK qaafaacaqGWbaabeaaaaa@3583@ , est donnée généralement par F p B c2 (T) m f(b) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOraOWaaSbaaK qaafaacaqGWbaabeaajaaqcqGHDisTkmaadmaajaaqbaGaamOqaOWa aSbaaKqaafaacaqGJbGaaGOmaaqabaqcaaKaaeikaiaadsfacaqGPa aacaGLBbGaayzxaaGcdaahaaqcbauabeaacaaMi8UaamyBaaaajaaq caWGMbGaaeikaiaadkgacaqGPaaaaa@4553@ , où m est un nombre réel, f(b) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaq Fn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpe WZqaaeaaciWacmGadaGadiaabaGaaqaaaOqaaiaadAgacaqGOaGaam OyaiaabMcaaaa@387A@ dépend de l’induction magnétique réduite b= B/B c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOyaiabg2da9O WaaSGbaKaaafaacaWGcbaabaGaamOqaaaakmaaBaaajeaqbaGaae4y aiaaikdaaeqaaaaa@394B@ et B c2 = μ 0 H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOqaOWaaSbaaK qaafaacaqGJbGaaGOmaaqabaqcaaKaeyypa0JaaqiVdOWaaSbaaKqa afaacaaIWaaabeaajaaqcaaMe8UaamisaOWaaSbaaKqaafaacaqGJb GaaeOmaaqabaaaaa@3EA4@ , où μ 0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaaqiVdOWaaSbaaK qaafaacaqGWaaabeaaaaa@35BD@  est la constante magnétique et H c2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamisaOWaaSbaaK qaafaacaqGJbGaaeOmaaqabaaaaa@362D@  est le champ magnétique critique supérieur.

Note 2 à l’article: Cet article était numéroté 815-12-26 dans l’IEC 60050-815:2015.


ar
قانون سكالينج لكثافة قوة التثبيت

de
Skalierungsgesetz der Pinning-Kraftdichte, n

es
ley de escala de la densidad de fuerza de anclaje, f

it
legge di scala della densita' di forza d'ancoraggio

ja
ピン力密度のスケール則

pl
prawo skalowania gęstości siły zaczepienia, n

pt
lei de escala para a densidade de força de ancoramento

zh
钉扎力密度的标度律

Publication date: 2024-08
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