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Area Superconductivity / Electromagnetic phenomena and properties

IEV ref 815-22-19

en
Kramer's law
specific scaling law of the pinning force density in which the pinning force density F p MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOraOWaaSbaaK qaafaacaqGWbaabeaaaaa@3583@ is given as F p b 1/2 ( 1b ) 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOraOWaaSbaaK qaafaacaqGWbaabeaajaaqcqGHDisTjugabiaadkgakmaaCaaajeaq beqaaiaaigdacaGGVaGaaGOmaaaakmaabmaajaaqbaacbaGaa8xmai abgkHiTiaadkgaaiaawIcacaGLPaaakmaaCaaajeaqbeqaaiaaikda aaaaaa@40DF@ , where 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 1 to entry: This entry was numbered 815-12-27 in IEC 60050-815:2015.


fr
loi de Kramer, f
loi d'échelle pour la densité de force d'ancrage dans laquelle 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 par F p b 1/2 ( 1b ) 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm 0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9ad baqaaiGaciGacmaaceqaaeaacaabaaGcbaqcaaKaamOraOWaaSbaaK qaafaacaqGWbaabeaajaaqcqGHDisTjugabiaadkgakmaaCaaajeaq beqaaiaaigdacaGGVaGaaGOmaaaakmaabmaajaaqbaacbaGaa8xmai abgkHiTiaadkgaaiaawIcacaGLPaaakmaaCaaajeaqbeqaaiaaikda aaaaaa@40DF@ , avec 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 1 à l’article: Cet article était numéroté 815-12-27 dans l’IEC 60050-815:2015.


ar
قانون كرامر

de
Kramersches Gesetz, n

es
ley de Kramer, f

it
legge di Kramer

ja
クレーマ則

pl
prawo Kramera, n

pt
lei de Kramer

zh
克拉默定律

Publication date: 2024-08
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