Frequency dependence of the magnetostrictive phenomenon in Metglas® 2605SA1 ribbon: A minor-loop case

Frequency dependence of magnetostrictive phenomenon of as-cast 2605SA1 ribbon was studied. We applied a sinusoidal sweeping field (H), with a fixed frequency (f), along length (L) of the ribbon, and simultaneously recorded the longitudinal magnetostriction (λ∥) and the transverse magnetostriction (λ...

Full description

Bibliographic Details
Main Authors: S. U. Jen, C. C. Liu, H. R. Lin, S. H. Chou
Format: Article
Language:English
Published: AIP Publishing LLC 2014-12-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.4905264
_version_ 1811278611154468864
author S. U. Jen
C. C. Liu
H. R. Lin
S. H. Chou
author_facet S. U. Jen
C. C. Liu
H. R. Lin
S. H. Chou
author_sort S. U. Jen
collection DOAJ
description Frequency dependence of magnetostrictive phenomenon of as-cast 2605SA1 ribbon was studied. We applied a sinusoidal sweeping field (H), with a fixed frequency (f), along length (L) of the ribbon, and simultaneously recorded the longitudinal magnetostriction (λ∥) and the transverse magnetostriction (λ⊥) as a function of time (t), respectively. f was varied from 0.07 to 122 Hz. In the low-f case (f =0.07 Hz), we observed the frequency-doubling (FD) feature in λ∥(t) and λ⊥(t) curves; i.e., only even harmonic magnetostrictive signals showed up. In the high-f case (f = 122 Hz), we observed the no-frequency-doubling (NFD) feature; i.e., both odd and even harmonic magnetostrictive signals showed up. A theory, based on the balance among various torques acting on magnetization, is developed to explain the f dependence of the magnetostriction phenomenon observed. From this theory, we conclude that only when the reflection symmetry of the system is reserved, i.e., when the equivalent easy axis (EEA) is perpendicular to L, will λ∥(t) and λ⊥(t) have the true-frequency-doubling (TFD) feature. However, for the as-cast 2605SA1 ribbon, EEA is not perpendicular to L. Thus, strictly speaking, we should observe the NFD feature only. Nevertheless, in the low-f limit, we can show that the FD feature is somewhat allowed under the condition, b/α being close to 1, where b and α are the two parameters used in the theory. From experimental data, this condition is met for as-cast 2605SA1. To make a distinction from TFD, this low-f feature is called close-frequency-doubling (CFD) in this paper. In general, the theory explains all the experimental results fairly well.
first_indexed 2024-04-13T00:37:46Z
format Article
id doaj.art-733ce527e0924ca29f5440733c642ed5
institution Directory Open Access Journal
issn 2158-3226
language English
last_indexed 2024-04-13T00:37:46Z
publishDate 2014-12-01
publisher AIP Publishing LLC
record_format Article
series AIP Advances
spelling doaj.art-733ce527e0924ca29f5440733c642ed52022-12-22T03:10:16ZengAIP Publishing LLCAIP Advances2158-32262014-12-01412127140127140-1110.1063/1.4905264050412ADVFrequency dependence of the magnetostrictive phenomenon in Metglas® 2605SA1 ribbon: A minor-loop caseS. U. Jen0C. C. Liu1H. R. Lin2S. H. Chou3Institute of Physics, Academia Sinica, Taipei, Taiwan 11529, ROCInstitute of Physics, Academia Sinica, Taipei, Taiwan 11529, ROCInstitute of Physics, Academia Sinica, Taipei, Taiwan 11529, ROCDepartment of Mathematics & Statistics, Bowling Green State University, Bowling Green, OH, 43402-0221, USAFrequency dependence of magnetostrictive phenomenon of as-cast 2605SA1 ribbon was studied. We applied a sinusoidal sweeping field (H), with a fixed frequency (f), along length (L) of the ribbon, and simultaneously recorded the longitudinal magnetostriction (λ∥) and the transverse magnetostriction (λ⊥) as a function of time (t), respectively. f was varied from 0.07 to 122 Hz. In the low-f case (f =0.07 Hz), we observed the frequency-doubling (FD) feature in λ∥(t) and λ⊥(t) curves; i.e., only even harmonic magnetostrictive signals showed up. In the high-f case (f = 122 Hz), we observed the no-frequency-doubling (NFD) feature; i.e., both odd and even harmonic magnetostrictive signals showed up. A theory, based on the balance among various torques acting on magnetization, is developed to explain the f dependence of the magnetostriction phenomenon observed. From this theory, we conclude that only when the reflection symmetry of the system is reserved, i.e., when the equivalent easy axis (EEA) is perpendicular to L, will λ∥(t) and λ⊥(t) have the true-frequency-doubling (TFD) feature. However, for the as-cast 2605SA1 ribbon, EEA is not perpendicular to L. Thus, strictly speaking, we should observe the NFD feature only. Nevertheless, in the low-f limit, we can show that the FD feature is somewhat allowed under the condition, b/α being close to 1, where b and α are the two parameters used in the theory. From experimental data, this condition is met for as-cast 2605SA1. To make a distinction from TFD, this low-f feature is called close-frequency-doubling (CFD) in this paper. In general, the theory explains all the experimental results fairly well.http://dx.doi.org/10.1063/1.4905264
spellingShingle S. U. Jen
C. C. Liu
H. R. Lin
S. H. Chou
Frequency dependence of the magnetostrictive phenomenon in Metglas® 2605SA1 ribbon: A minor-loop case
AIP Advances
title Frequency dependence of the magnetostrictive phenomenon in Metglas® 2605SA1 ribbon: A minor-loop case
title_full Frequency dependence of the magnetostrictive phenomenon in Metglas® 2605SA1 ribbon: A minor-loop case
title_fullStr Frequency dependence of the magnetostrictive phenomenon in Metglas® 2605SA1 ribbon: A minor-loop case
title_full_unstemmed Frequency dependence of the magnetostrictive phenomenon in Metglas® 2605SA1 ribbon: A minor-loop case
title_short Frequency dependence of the magnetostrictive phenomenon in Metglas® 2605SA1 ribbon: A minor-loop case
title_sort frequency dependence of the magnetostrictive phenomenon in metglas r 2605sa1 ribbon a minor loop case
url http://dx.doi.org/10.1063/1.4905264
work_keys_str_mv AT sujen frequencydependenceofthemagnetostrictivephenomenoninmetglas2605sa1ribbonaminorloopcase
AT ccliu frequencydependenceofthemagnetostrictivephenomenoninmetglas2605sa1ribbonaminorloopcase
AT hrlin frequencydependenceofthemagnetostrictivephenomenoninmetglas2605sa1ribbonaminorloopcase
AT shchou frequencydependenceofthemagnetostrictivephenomenoninmetglas2605sa1ribbonaminorloopcase