{"title":"磁感应层析成像中二次磁场成像的数值方面","authors":"B. Szuflitowska, M. Ziółkowski, K. Stawicki","doi":"10.5604/01.3001.0010.5206","DOIUrl":null,"url":null,"abstract":". Magnetic Induction Tomography (MIT) belongs to the noncontact electromagnetic imaging techniques. This paper focuses on determination of a secondary magnetic field map calculated with the help of the Biot-Savart law around the low-conductivity object. The inclusions of various shapes and different electrical conductivities values and two measurement planes are considered. In each case the objects’ single maximal cell volume with assumed uniform eddy current density has been determined. In order to keep the relative error below 1% the object should be divided in most cases into elements with maximal cell volume equal to 0.244 mm 3 for yz − plane, and 0.03 mm 3 for xy − plane.","PeriodicalId":142227,"journal":{"name":"Informatics, Control, Measurement in Economy and Environment Protection","volume":"3 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2017-09-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Numerical aspects of the secondary magnetic field mapping in Magnetic Induction Tomography\",\"authors\":\"B. Szuflitowska, M. Ziółkowski, K. Stawicki\",\"doi\":\"10.5604/01.3001.0010.5206\",\"DOIUrl\":null,\"url\":null,\"abstract\":\". Magnetic Induction Tomography (MIT) belongs to the noncontact electromagnetic imaging techniques. This paper focuses on determination of a secondary magnetic field map calculated with the help of the Biot-Savart law around the low-conductivity object. The inclusions of various shapes and different electrical conductivities values and two measurement planes are considered. In each case the objects’ single maximal cell volume with assumed uniform eddy current density has been determined. In order to keep the relative error below 1% the object should be divided in most cases into elements with maximal cell volume equal to 0.244 mm 3 for yz − plane, and 0.03 mm 3 for xy − plane.\",\"PeriodicalId\":142227,\"journal\":{\"name\":\"Informatics, Control, Measurement in Economy and Environment Protection\",\"volume\":\"3 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2017-09-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Informatics, Control, Measurement in Economy and Environment Protection\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.5604/01.3001.0010.5206\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Informatics, Control, Measurement in Economy and Environment Protection","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.5604/01.3001.0010.5206","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
. 磁感应层析成像(MIT)属于非接触式电磁成像技术。本文研究了利用比奥-萨瓦定律计算的低电导率物体周围的二次磁场图的确定。考虑了不同形状、不同电导率值的夹杂物和两种测量平面。在假设均匀涡流密度的情况下,确定了每一种情况下物体的最大单胞体积。为了使相对误差保持在1%以下,在大多数情况下,应将对象划分为最大单元体积为yz -面0.244 mm 3和xy -面0.03 mm 3的单元。
Numerical aspects of the secondary magnetic field mapping in Magnetic Induction Tomography
. Magnetic Induction Tomography (MIT) belongs to the noncontact electromagnetic imaging techniques. This paper focuses on determination of a secondary magnetic field map calculated with the help of the Biot-Savart law around the low-conductivity object. The inclusions of various shapes and different electrical conductivities values and two measurement planes are considered. In each case the objects’ single maximal cell volume with assumed uniform eddy current density has been determined. In order to keep the relative error below 1% the object should be divided in most cases into elements with maximal cell volume equal to 0.244 mm 3 for yz − plane, and 0.03 mm 3 for xy − plane.