# US 8,148,976 B2 · Method and arrangement for the contactless inspection of moving electrically conductive substances > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 8,148,976 B2 - Document ID: US8148976B2 - Status: Granted - Kind: B2 - Application number: 12/067,794 - Filed: 2006-09-21 - Published: 2008-10-16 - Granted: 2012-04-03 - Earliest claimed: 2006-09-21 - Assignees: Technische Universitat Ilmenau - Inventors: André Thess; Yuri Kolesnikov; Christian Karcher - Web page: https://patentgrep.com/patent/US8148976B2 ## CPC - G01N 27/9026: {by moving the material} - G01F 1/56: by using electric or magnetic effects (G01F1/66 takes precedence) - G01N: INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES (measuring or testing apparatus or processes other than immunoassay, involving enzymes or microorganisms C12M, C12Q) - G01F: MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME ## Abstract The invention relates to a method and arrangement for the contactless determination of conductivity-influencing properties and their spatial distribution over the entire cross section of an electrically conductive substance moving in a primary magnetic field (B). The substance may be a liquid or a solid. A simultaneous measurement of a number of mechanical state parameters of the magnetic system is performed (three-dimensional components of the force and the torque), said parameters being variable by the effect of a secondary field on the magnetic system, the secondary field being produced on the basis of eddy currents induced in the substance by the primary field (B). To determine the spatial distribution of the property that is sought, the primary field is changed in intensity or form a number of times and a measurement of the state parameters is carried out for each change. The determination of the properties sought or their distribution takes place by solving an inverse problem using the method of least squares. ## Claims ### Claim 1 A method for the contactless determination of properties influencing the conductance of an electrically conductive substance moving in a primary magnetic field (B), comprising the following steps: coupling a primary magnetic field (B) into a substance being inspected using a magnetic system with at least two poles, wherein lines of force of the primary field (B) running in an air gap between the at least two poles penetrate the substance and run substantially transverse to a direction of movement of the substance; measuring at least one mechanical state parameter of the magnetic system, the at least one mechanical state parameter changing due to an action of a secondary field on the magnetic system, the secondary field being formed by eddy currents induced in the substance by the primary field (B); calculating at least one property influencing a conductance of the substance method of least error squares, wherein a function being minimized is a mean square deviation of the at least one state parameter as calculated by an assumed spatial distribution of the at least one property of the substance being inspected from the respective measured state parameters. ### Claim 2 (depends on 1) The method of claim 1, wherein the following steps are additionally carried out to determine the spatial distribution of the properties of the substance which influence the conductance: changing the shape and/or strength of the primary magnetic field (B) passing through the substance; measuring the mechanical state parameters of the magnetic system for every change in the primary field (B); calculating the spatial distribution of the properties influencing the conductance of the substance being inspected across its entire cross section, using the method of least error squares, wherein the function being minimized is the mean square deviation of the state parameters as calculated by the assumed spatial distribution of these properties of the substance being inspected from the respective measured state parameters. ### Claim 3 (depends on 2) The method of claim 2, wherein a determination of the spatial distribution of the properties is also done along a given length of the substance in its axial direction of movement by carrying out the mentioned steps of the method for at least two axially separated points of the substance. ### Claim 4 (depends on 1) The method of claim 1, wherein the primary magnetic field (B) is a direct field or an alternating field. ### Claim 5 (depends on 1) The method of claim 1, wherein the state parameters of the magnetic system are three-dimensional components of the force (F) and/or the torque (M), acting on the magnetic system by virtue of the secondary field caused by eddy currents induced in the substance. ### Claim 6 (depends on 5) The method of claim 5, wherein the state parameters of the magnetic system are determined with a compensation measurement method. ### Claim 7 (depends on 1) The method of claim 1, wherein the state parameters of the magnetic system are determined from mechanical stresses occurring in the magnetic system. ### Claim 8 (depends on 2) The method of claim 2, wherein the shape and/or the strength of the primary magnetic field (B) is changed by a changing of position of the magnetic system relative to the substance being inspected. ### Claim 9 (depends on 2) The method of claim 2, wherein the strength of the primary magnetic field (B) is changed by varying a current flowing through a coil surrounding at least part of the magnetic system. ### Claim 10 (depends on 1) The method of claim 1, wherein the primary magnetic field (B) is inhomogeneous in configuration. ### Claim 11 (depends on 1) The method of claim 1, wherein the substance is an electrically conductive solid and the property being determined is the position and/or form of an inhomogeneity in the solid. ### Claim 12 (depends on 1) The method of claim 1, wherein the properties of a fluid substance are determined, which is moving in a channel or the like, which extends transversely to the lines of force running in the air gap. ### Claim 13 A Lorentz force anemometer for contactless determination of properties influencing the conductance of a moving electrically conductive substance, comprising: a magnetic system for generating a primary field (B), including a yoke and at least two magnetic poles, wherein a substance can be moved in an air gap between the poles transverse to a direction of the primary field; a measurement system to detect at least two mechanical state parameters of the magnetic system, the state parameters characterizing a mechanical action of a secondary field on the magnetic system, wherein the secondary field arises by virtue of eddy currents induced in the substance moving in the primary field; and an evaluation unit to determine at least one property influencing a conductance of the substance from the measured state parameters. ### Claim 14 (depends on 13) The Lorentz force anemometer of claim 13, further comprising an actuator system, which is coupled to the magnetic system in such a way as to allow a changing of position of the magnetic system relative to the substance, thereby achieving a change in the form and/or strength of the primary magnetic field (B) in the cross section of the substance. ### Claim 15 (depends on 13) The Lorentz force anemometer of claim 13, wherein the poles are formed by permanent magnets. ### Claim 16 (depends on 15) The Lorentz force anemometer of claim 15, wherein the permanent magnets are of different strength and/or size, so that an inhomogeneous primary field (B) is formed. ### Claim 17 (depends on 13) The Lorentz force anemometer of claim 13, wherein the poles of the magnetic system are formed by normally conducting or superconducting coils or by a combination of such coils with permanent magnets. ### Claim 18 (depends on 13) The Lorentz force anemometer of claim 13, wherein the poles of the magnetic system are formed by two oppositely arranged disks with permanent magnets arranged on them with alternating polarity, and the disks are joined by a yoke and can be driven centrally. ### Claim 19 (depends on 18) The Lorentz force anemometer of claim 18, wherein the disks rotate with a speed ω which can be adjusted and varied by a drive unit. ### Claim 20 (depends on 13) The Lorentz force anemometer of claim 13, wherein the magnetic system comprises magnetically conductive material and ferrofluids to form the primary magnetic field ### Claim 21 (depends on 13) The Lorentz force anemometer of claim 13, wherein a channel runs in the air gap between the poles, in which a liquid flows as the substance being inspected.