{"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":13040,"journal":{"name":"IEEE Magnetics Letters","volume":"13 ","pages":"1-5"},"PeriodicalIF":1.1000,"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\":13040,\"journal\":{\"name\":\"IEEE Magnetics Letters\",\"volume\":\"13 \",\"pages\":\"1-5\"},\"PeriodicalIF\":1.1000,\"publicationDate\":\"2022-07-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE Magnetics Letters\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://ieeexplore.ieee.org/document/9830868/\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Magnetics Letters","FirstCategoryId":"101","ListUrlMain":"https://ieeexplore.ieee.org/document/9830868/","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","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:
IEEE Magnetics Letters is a peer-reviewed, archival journal covering the physics and engineering of magnetism, magnetic materials, applied magnetics, design and application of magnetic devices, bio-magnetics, magneto-electronics, and spin electronics. IEEE Magnetics Letters publishes short, scholarly articles of substantial current interest.
IEEE Magnetics Letters is a hybrid Open Access (OA) journal. For a fee, authors have the option making their articles freely available to all, including non-subscribers. OA articles are identified as Open Access.