Note 1 to entry: The AC magnetization, M(t) , under the magnetic field strength of h0cosωt is expanded as: M(t)=h0∞∑n=0[κ'ncos(nωt)+κ"nsin(nωt)]
where κ'n and κ"n are the real and imaginary parts of the AC magnetic susceptibility for the order n .
Note 2 to entry: The fundamental components κ'1 and κ"1 are mostly observed for measurements of superconducting transition.
Note 3 to entry: The AC energy loss density W is given as:
W=πμ0h20κ"1.
Note 4 to entry: This entry was numbered 815-17-13 in IEC 60050-815:2015.
Note 1 to entry: The AC magnetization, M( t ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaq Fn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpe WZqaaeaaciWacmGadaGadiaabaGaaqaaaOqaaiaad2eadaqadaqaai aadshaaiaawIcacaGLPaaaaaa@38A5@ , under the magnetic field strength of h 0 cosωt MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaq Fn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpe WZqaaeaaciWacmGadaGadiaabaGaaqaaaOqaaiaadIgadaWgaaWcba GaaGimaaqabaGccaqGJbGaae4BaiaabohacqaHjpWDcaWG0baaaa@3CC2@ is expanded as: M t = h 0 ∑ n=0 ∞ κ n ' cos nωt + κ n " sin nωt MathType@MTEF@5@5@+= feaahCart1ev3aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabmqaamaabaabaaGcbaGaamytamaabm aabaGaamiDaaGaayjkaiaawMcaaiabg2da9iaadIgadaWgaaWcbaGa aGimaaqabaGcdaaeWbqaamaadmaabaGaeqOUdS2aa0baaSqaaiaad6 gaaeaacaGGNaaaaOGaae4yaiaab+gacaqGZbWaaeWaaeaacaWGUbGa eqyYdCNaamiDaaGaayjkaiaawMcaaiabgUcaRiabeQ7aRnaaDaaale aacaWGUbaabaGaaiOiaaaakiaabohacaqGPbGaaeOBamaabmaabaGa amOBaiabeM8a3jaadshaaiaawIcacaGLPaaaaiaawUfacaGLDbaaaS qaaiaad6gacqGH9aqpcaaIWaaabaGaeyOhIukaniabggHiLdaaaa@5C98@
where κ n ' MathType@MTEF@5@5@+= feaahCart1ev3aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabmqaamaabaabaaGcbaGaam4AamaaDa aaleaacaWGUbaabaGaai4jaaaaaaa@38B4@ and κ n " MathType@MTEF@5@5@+= feaahCart1ev3aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabmqaamaabaabaaGcbaGaam4AamaaDa aaleaacaWGUbaabaGaaiOiaaaaaaa@38AF@ are the real and imaginary parts of the AC magnetic susceptibility for the order n MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaq Fn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpe WZqaaeaaciWacmGadaGadiaabaGaaqaaaOqaaiaad6gaaaa@3644@ .
Note 2 to entry: The fundamental components κ 1 ' MathType@MTEF@5@5@+= feaahCart1ev3aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabmqaamaabaabaaGcbaGaam4AamaaDa aaleaacaaIXaaabaGaai4jaaaaaaa@387C@ and κ 1 " MathType@MTEF@5@5@+= feaahCart1ev3aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabmqaamaabaabaaGcbaGaam4AamaaDa aaleaacaaIXaaabaGaaiOiaaaaaaa@3877@ are mostly observed for measurements of superconducting transition.
Note 3 to entry: The AC energy loss density W MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHX garuavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGe aGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaq Fn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpe WZqaaeaaciWacmGadaGadiaabaGaaqaaaOqaaiaadEfaaaa@362D@ is given as:
W=π μ 0 h 0 2 κ 1 " MathType@MTEF@5@5@+= feaahCart1ev3aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabmqaamaabaabaaGcbaGaam4vaiabg2 da9iabec8aWjabeY7aTnaaBaaaleaacaaIWaaabeaakiaadIgadaqh aaWcbaGaaGimaaqaaiaaikdaaaGccaWGRbWaa0baaSqaaiaaigdaae aacaGGIaaaaaaa@4156@ .