Analysis of the frequency dependence of the AC loss in MgB2 based on the eddy current model

The frequency dependence of the AC loss peak in x"(T) of MgB2 is analyzed using the eddy current model. In this model, eddy current loops are induced in the grain of a superconductor subject to small AC fields. This current, which generates lhe loss peak, is proportional to the area enclosed by...

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Main Authors: Olbinado, Margie P., Sarmago, Roland V.
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Published: Animo Repository 2001
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Online Access:https://animorepository.dlsu.edu.ph/faculty_research/9379
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spelling oai:animorepository.dlsu.edu.ph:faculty_research-94772023-05-30T23:50:49Z Analysis of the frequency dependence of the AC loss in MgB2 based on the eddy current model Olbinado, Margie P. Sarmago, Roland V. The frequency dependence of the AC loss peak in x"(T) of MgB2 is analyzed using the eddy current model. In this model, eddy current loops are induced in the grain of a superconductor subject to small AC fields. This current, which generates lhe loss peak, is proportional to the area enclosed by the loops and inversely proportional to the resislance of the loops. The AC loss peak is a result of the competition between the rapidly diminishing resistance of the material below Tc and the decreasing area where the hannonic field can thread as lhe penetralion depth λ decreases in the superconducting state [1]. Utilizing equations for temperature dependent penetration depth and electrical resistance, a fitting function for x"(T) which is proportional to i(T)/Bac is obtained. A circular grain of radius r is assumed. For a particular λ, the area where the field can penelrates is equal to A(T) =πr2 -(r -λ(T))2 (2) The temperature dependence of the penetration depth is chosen such that A(T) attains a zero value at low temperatures. The resulting eddy current equation is (2) At Tc, A.=lo and is very large compared to the grain radius; r. At temperatures 􀃎here r is less than λ, the penetrated area is maintained at A (T) = πr2 . lc is a fitting parameter that describes the rate of decrease of λ(T). R0 is the value of the electrical resistance at Tc. R0 is constant for all measurement since the material is in a region where the magnetization varies linearly with field. An increase in R0 indicates a nonlinear magnetization. b is a fitting parameter that describes the rale of decrease of R(T). The superimposed plots of the experimental data and the resulting curve employing the eddy current model are shown in the figure. The corresponding model fit show satisfactory agreement with the experimental X"(T) measurements. As the frequency is increased from 200 to 3200Hz, 1c decreases. This means that λ decreases faster at a higher frequency and the flux penetrated area attain the zero value faster. Thus. the penetration depth decreases with increasing frequency. On the other hand, the fitting parameter b, increases as the frequency is increased from 200 to 3200Hz. This equivalently means that the rate of change of R(T) is decreased with increased frequency. Thus, the resislance increases with frequency. This behavior is similar to the behavior of metals in the presence of AC field. Thus, indicating that MgB2 indeed a highly metallic material as previously observed. 2001-01-01T08:00:00Z text https://animorepository.dlsu.edu.ph/faculty_research/9379 Faculty Research Work Animo Repository Annealing of crystals Liquid phase epitaxy Superconductors Physics
institution De La Salle University
building De La Salle University Library
continent Asia
country Philippines
Philippines
content_provider De La Salle University Library
collection DLSU Institutional Repository
topic Annealing of crystals
Liquid phase epitaxy
Superconductors
Physics
spellingShingle Annealing of crystals
Liquid phase epitaxy
Superconductors
Physics
Olbinado, Margie P.
Sarmago, Roland V.
Analysis of the frequency dependence of the AC loss in MgB2 based on the eddy current model
description The frequency dependence of the AC loss peak in x"(T) of MgB2 is analyzed using the eddy current model. In this model, eddy current loops are induced in the grain of a superconductor subject to small AC fields. This current, which generates lhe loss peak, is proportional to the area enclosed by the loops and inversely proportional to the resislance of the loops. The AC loss peak is a result of the competition between the rapidly diminishing resistance of the material below Tc and the decreasing area where the hannonic field can thread as lhe penetralion depth λ decreases in the superconducting state [1]. Utilizing equations for temperature dependent penetration depth and electrical resistance, a fitting function for x"(T) which is proportional to i(T)/Bac is obtained. A circular grain of radius r is assumed. For a particular λ, the area where the field can penelrates is equal to A(T) =πr2 -(r -λ(T))2 (2) The temperature dependence of the penetration depth is chosen such that A(T) attains a zero value at low temperatures. The resulting eddy current equation is (2) At Tc, A.=lo and is very large compared to the grain radius; r. At temperatures 􀃎here r is less than λ, the penetrated area is maintained at A (T) = πr2 . lc is a fitting parameter that describes the rate of decrease of λ(T). R0 is the value of the electrical resistance at Tc. R0 is constant for all measurement since the material is in a region where the magnetization varies linearly with field. An increase in R0 indicates a nonlinear magnetization. b is a fitting parameter that describes the rale of decrease of R(T). The superimposed plots of the experimental data and the resulting curve employing the eddy current model are shown in the figure. The corresponding model fit show satisfactory agreement with the experimental X"(T) measurements. As the frequency is increased from 200 to 3200Hz, 1c decreases. This means that λ decreases faster at a higher frequency and the flux penetrated area attain the zero value faster. Thus. the penetration depth decreases with increasing frequency. On the other hand, the fitting parameter b, increases as the frequency is increased from 200 to 3200Hz. This equivalently means that the rate of change of R(T) is decreased with increased frequency. Thus, the resislance increases with frequency. This behavior is similar to the behavior of metals in the presence of AC field. Thus, indicating that MgB2 indeed a highly metallic material as previously observed.
format text
author Olbinado, Margie P.
Sarmago, Roland V.
author_facet Olbinado, Margie P.
Sarmago, Roland V.
author_sort Olbinado, Margie P.
title Analysis of the frequency dependence of the AC loss in MgB2 based on the eddy current model
title_short Analysis of the frequency dependence of the AC loss in MgB2 based on the eddy current model
title_full Analysis of the frequency dependence of the AC loss in MgB2 based on the eddy current model
title_fullStr Analysis of the frequency dependence of the AC loss in MgB2 based on the eddy current model
title_full_unstemmed Analysis of the frequency dependence of the AC loss in MgB2 based on the eddy current model
title_sort analysis of the frequency dependence of the ac loss in mgb2 based on the eddy current model
publisher Animo Repository
publishDate 2001
url https://animorepository.dlsu.edu.ph/faculty_research/9379
_version_ 1768028945829068800