{"title":"利用磁巴克豪森噪声构造能量环","authors":"Xiaoge Meng;Lin Li;Yanzhao Hou","doi":"10.1109/LMAG.2022.3191281","DOIUrl":null,"url":null,"abstract":"Magnetic Barkhausen noise (MBN), which contains microstructure information of materials, is widely used in nondestructive testing (NDT) of magnetic materials. MBN energy (MBN\n<sub>energy</sub>\n) is a time-independent indicator for NDT, but the initial MBN\n<sub>energy</sub>\n has no clear physical meaning and cannot be used to explain the relationship to the hysteresis loop. In this letter, based on the physical mechanism of MBN, a proportional relation is built between the MBN voltage signal \n<italic>V</i>\n<sub>B</sub>\n and energy loss, and the signal \n<italic>V</i>\n<sub>B</sub>\n is then related to the energy loss through wall pinning in the Jiles–Atherton hysteresis model. We define a novel magnetic Barkhausen noise energy eigenvalue (MBNE\n<italic>)</i>\n as the time integral of the product of the absolute value of \n<italic>V</i>\n<sub>B</sub>\n and the sign function sign(\n<italic>dH</i>\n/\n<italic>dt</i>\n). We prove that the MBNE is proportional to the irreversible magnetization \n<italic>M</i>\n<sub>irr</sub>\n. Since \n<italic>M</i>\n<sub>irr</sub>\n is equal to the saturation magnetization \n<italic>M</i>\n<sub>s</sub>\n when the magnetization of ferromagnetic material reaches saturation, we scaled the MBNE to make its maximum value equal to \n<italic>M</i>\n<sub>s</sub>\n and found that MBNE with respect to the magnetic field \n<italic>H</i>\n, MBNE(\n<italic>H</i>\n), coincides with the irreversible hysteresis loop \n<italic>M</i>\n<sub>irr</sub>\n(\n<italic>H</i>\n). We refer to MBNE(\n<italic>H</i>\n) as the MBN energy loop. The MBNE(\n<italic>H</i>\n) and \n<italic>M</i>\n<sub>irr</sub>\n(\n<italic>H</i>\n) for two kinds of electrical steel sheets are compared experimentally, which validates the adaptability of the MBNE(\n<italic>H</i>\n) construction method. The method to obtain \n<italic>M</i>\n<sub>irr</sub>\n(\n<italic>H</i>\n) from the MBN raw signal reveals the physical mechanism of MBN and the irreversible magnetization process of magnetic materials.","PeriodicalId":1,"journal":{"name":"Accounts of Chemical Research","volume":null,"pages":null},"PeriodicalIF":16.4000,"publicationDate":"2022-07-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Construction of Energy Loops Using Magnetic Barkhausen Noise\",\"authors\":\"Xiaoge Meng;Lin Li;Yanzhao Hou\",\"doi\":\"10.1109/LMAG.2022.3191281\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Magnetic Barkhausen noise (MBN), which contains microstructure information of materials, is widely used in nondestructive testing (NDT) of magnetic materials. MBN energy (MBN\\n<sub>energy</sub>\\n) is a time-independent indicator for NDT, but the initial MBN\\n<sub>energy</sub>\\n has no clear physical meaning and cannot be used to explain the relationship to the hysteresis loop. In this letter, based on the physical mechanism of MBN, a proportional relation is built between the MBN voltage signal \\n<italic>V</i>\\n<sub>B</sub>\\n and energy loss, and the signal \\n<italic>V</i>\\n<sub>B</sub>\\n is then related to the energy loss through wall pinning in the Jiles–Atherton hysteresis model. We define a novel magnetic Barkhausen noise energy eigenvalue (MBNE\\n<italic>)</i>\\n as the time integral of the product of the absolute value of \\n<italic>V</i>\\n<sub>B</sub>\\n and the sign function sign(\\n<italic>dH</i>\\n/\\n<italic>dt</i>\\n). We prove that the MBNE is proportional to the irreversible magnetization \\n<italic>M</i>\\n<sub>irr</sub>\\n. Since \\n<italic>M</i>\\n<sub>irr</sub>\\n is equal to the saturation magnetization \\n<italic>M</i>\\n<sub>s</sub>\\n when the magnetization of ferromagnetic material reaches saturation, we scaled the MBNE to make its maximum value equal to \\n<italic>M</i>\\n<sub>s</sub>\\n and found that MBNE with respect to the magnetic field \\n<italic>H</i>\\n, MBNE(\\n<italic>H</i>\\n), coincides with the irreversible hysteresis loop \\n<italic>M</i>\\n<sub>irr</sub>\\n(\\n<italic>H</i>\\n). We refer to MBNE(\\n<italic>H</i>\\n) as the MBN energy loop. The MBNE(\\n<italic>H</i>\\n) and \\n<italic>M</i>\\n<sub>irr</sub>\\n(\\n<italic>H</i>\\n) for two kinds of electrical steel sheets are compared experimentally, which validates the adaptability of the MBNE(\\n<italic>H</i>\\n) construction method. The method to obtain \\n<italic>M</i>\\n<sub>irr</sub>\\n(\\n<italic>H</i>\\n) from the MBN raw signal reveals the physical mechanism of MBN and the irreversible magnetization process of magnetic materials.\",\"PeriodicalId\":1,\"journal\":{\"name\":\"Accounts of Chemical Research\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":16.4000,\"publicationDate\":\"2022-07-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Accounts of Chemical Research\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://ieeexplore.ieee.org/document/9830868/\",\"RegionNum\":1,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"CHEMISTRY, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Accounts of Chemical Research","FirstCategoryId":"101","ListUrlMain":"https://ieeexplore.ieee.org/document/9830868/","RegionNum":1,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
Construction of Energy Loops Using Magnetic Barkhausen Noise
Magnetic Barkhausen noise (MBN), which contains microstructure information of materials, is widely used in nondestructive testing (NDT) of magnetic materials. MBN energy (MBN
energy
) is a time-independent indicator for NDT, but the initial MBN
energy
has no clear physical meaning and cannot be used to explain the relationship to the hysteresis loop. In this letter, based on the physical mechanism of MBN, a proportional relation is built between the MBN voltage signal
V
B
and energy loss, and the signal
V
B
is then related to the energy loss through wall pinning in the Jiles–Atherton hysteresis model. We define a novel magnetic Barkhausen noise energy eigenvalue (MBNE
)
as the time integral of the product of the absolute value of
V
B
and the sign function sign(
dH
/
dt
). We prove that the MBNE is proportional to the irreversible magnetization
M
irr
. Since
M
irr
is equal to the saturation magnetization
M
s
when the magnetization of ferromagnetic material reaches saturation, we scaled the MBNE to make its maximum value equal to
M
s
and found that MBNE with respect to the magnetic field
H
, MBNE(
H
), coincides with the irreversible hysteresis loop
M
irr
(
H
). We refer to MBNE(
H
) as the MBN energy loop. The MBNE(
H
) and
M
irr
(
H
) for two kinds of electrical steel sheets are compared experimentally, which validates the adaptability of the MBNE(
H
) construction method. The method to obtain
M
irr
(
H
) from the MBN raw signal reveals the physical mechanism of MBN and the irreversible magnetization process of magnetic materials.
期刊介绍:
Accounts of Chemical Research presents short, concise and critical articles offering easy-to-read overviews of basic research and applications in all areas of chemistry and biochemistry. These short reviews focus on research from the author’s own laboratory and are designed to teach the reader about a research project. In addition, Accounts of Chemical Research publishes commentaries that give an informed opinion on a current research problem. Special Issues online are devoted to a single topic of unusual activity and significance.
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