首页> 外国专利> Dot matrix diagnosis of defects in geographical area using magnetic flux density/magnetic field strength/ electric field strength, includes forming Laplace derivative of measured variable at each measuring point in a horizontal dot matrix

Dot matrix diagnosis of defects in geographical area using magnetic flux density/magnetic field strength/ electric field strength, includes forming Laplace derivative of measured variable at each measuring point in a horizontal dot matrix

机译:使用磁通量密度/磁场强度/电场强度对地理区域中的缺陷进行点矩阵诊断,包括在水平点矩阵中的每个测量点处形成测量变量的拉普拉斯导数

摘要

The dot matrix diagnosis of defects in geographical area using magnetic flux density/magnetic field strength/ electric field strength, includes forming Laplace derivative of measured variable at each measuring point in a horizontal dot matrix. The Laplace derivation is applied for the labelling of the biologically effective attractive strength, which is indicated by the absolute value of Laplace derivative in millitesla per square meter or in microtesla per square meter. The dot matrix diagnosis of defects in geographical area using magnetic flux density/magnetic field strength/ electric field strength, includes forming Laplace derivative of measured variable at each measuring point in a horizontal dot matrix. The Laplace derivation is applied for the labelling of the biologically effective attractive strength, which is indicated by the absolute value of Laplace derivative in millitesla per square meter or in microtesla per square meter. The measurement in a horizontal dot matrix is carried on plains lying one above the other and included into the Laplace derivative with the second derivative of the measured variable in the direction perpendicularly to the planes of measurement. The difference between the two-dimensional and the three-dimensional Laplace derivation of the perpendicular magnetic flux density is applied to the distinction between natural and technically caused interferences, and this difference disappears in the natural magnetic field. A technical source such as mobile phone or electrically or electronically operated device or a magnetic object are brought into the center of the measuring field, in three-dimensional measurement on a plane of measurement of middle height, to determine the biological attractive strength. An object is placed alone or connected with the technical source for the improvement of the biological compatibility. A non-uniform background of the magnetic field such as a non-uniform field strength by Helmholtz-spool or a non-uniform gradient by two bar magnets with neighbouring dislike poles arranged at neighbouring sides of the measuring field, is created, during the measurement in order to increase the sensitivity of the detection of weak disturbing or compensatory effects on the magnetic field, i.e. an increase or an decrease of the attractive strength. A non-uniform background of the magnetic field by the bar magnets with neighbouring like poles, is created, in order to determine increase of the attraction strengths or improvement of the biological compatibility of the objects to prevent such increase or decrease the attraction strength.
机译:利用磁通密度/磁场强度/电场强度来诊断地理区域中的缺陷的点矩阵包括在水平点矩阵中的每个测量点处形成被测变量的拉普拉斯导数。拉普拉斯衍生物可用于标记生物有效的吸引力,该强度由拉普拉斯衍生物的绝对值表示,以每平方米毫特斯拉或每平方米微特斯拉表示。利用磁通密度/磁场强度/电场强度来诊断地理区域中的缺陷的点矩阵包括在水平点矩阵中的每个测量点处形成被测变量的拉普拉斯导数。拉普拉斯衍生物可用于标记生物有效的吸引力,该强度由拉普拉斯衍生物的绝对值表示,以每平方米毫特斯拉或每平方米微特斯拉表示。在水平点矩阵中的测量是在彼此叠置的平原上进行的,并在垂直于测量平面的方向上将测量变量的二阶导数包含在拉普拉斯导数中。垂直磁通密度的二维和三维拉普拉斯推导之间的差异适用于自然干扰和技术干扰之间的区别,并且该差异在自然磁场中消失。在中间高度的测量平面上进行三维测量时,将诸如移动电话或电动或电子操作设备或磁性物体之类的技术源带入测量场的中心,以确定生物吸引力。为了提高生物相容性,将物体单独放置或与技术来源连接。在测量过程中,会产生磁场的不均匀背景,例如亥姆霍兹线轴引起的磁场强度不均匀,或者两个棒状磁体产生的梯度不均匀,在相邻两个不对称磁极之间布置了测量场的相邻边为了提高检测对磁场的微弱干扰或补偿效应(即增加或减小吸引力)的灵敏度。为了确定吸引强度的增加或物体的生物相容性的改善,以防止这种增加或减小的吸引强度,产生具有相邻的类似磁极的条形磁体产生的磁场的不均匀背景。

著录项

  • 公开/公告号AT501845B1

    专利类型

  • 公开/公告日2008-08-15

    原文格式PDF

  • 申请/专利权人 MEDINGER WALTER MAG. DR.;HOMANN WOLFGANG;

    申请/专利号AT20050000433

  • 发明设计人 MEDINGER WALTER MAG. DR.;

    申请日2005-03-15

  • 分类号G01R33/10;A61B5/05;G06F19/00;

  • 国家 AT

  • 入库时间 2022-08-21 20:04:41

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