Method and device for compensation in a measurement of a magnetic field, object-localizing method and system, recording medium for these methods

Patent metadata

Field	Value
Publication number	US-9354282-B2
Application number	US-201113085523-A
Country	US
Kind code	B2
Filing date	Apr 13, 2011
Priority date	Apr 14, 2010
Publication date	May 31, 2016
Grant date	May 31, 2016

Abstract

This method of compensation in the measurement of a magnetic field comprises: the determining of a position and of a magnetic moment of an image of the source situated on the other side of the magnetic disturber using one or more measurements of the emitted magnetic field, performed by at least one magnetic sensor whose position and orientation relatively to the source are known, and the subtraction of the magnetic field emitted by this image from the measurement of the magnetic field made by the sensor in the presence of the magnetic disturber to obtain compensation in this measurement.

First claim

The invention claimed is:

1. A method of compensating a measurement of a magnetic field, the method comprising:
emitting a magnetic field in the presence of a magnetic disturber, by means of a uniaxial source, situated on one side of the magnetic disturber, the magnetic moment of the source being known,
determining a position and a magnetic moment of an image of the source situated on the other side of the magnetic disturber using one or more measurements of the emitted magnetic field, the measurements being performed by at least one magnetic sensor whose position and orientation relative to the source are known, the position and the magnetic moment of the image minimizing the following relationship for each sensor:
{right arrow over (B)} me −({right arrow over (B)} S +{right arrow over (B)} I ),

where:
{right arrow over (B)} me is a magnetic field measured by the sensor in the presence of the magnetic disturber,
{right arrow over (B)} S is a magnetic field that would be measured by the sensor in the absence of the magnetic disturber, and
{right arrow over (B)} I is a fictitious magnetic field emitted by the image that would be measured by the sensor in the absence of the magnetic disturber,

subtracting the magnetic field emitted by the image, constructed from the position and the magnetic moment of the image, from the measurement of the magnetic field made by the sensor in the presence of the magnetic disturber to compensate the measurement,
determining the position and magnetic moment of several images of the same source from the same measurements of the magnetic field, the measurements being performed by several sensors whose positions and orientations are known relative to the source, and
subtracting the magnetic field emitted by the images from the measurement of the magnetic field performed by a sensor in the presence of the magnetic disturber, thereby compensating for the measurement.

2. The method of claim 1 , wherein determining the position and the magnetic moment of the image comprises using at least one supplementary relationship derived from electromagnetic image theory, the at least one supplementary relationship being chosen from the following set:

M
i

=

M
S

⁡

(

1
-

μ
r

1
+

μ
r

)

⁢

(

1
-
σ

1
+
σ

)

,

⁢

M
i

=

M
S

⁡

(

1
-

μ
r

1
+

μ
r

)

,
and

M
i

=

M
S

⁡

(

1
-
σ

1
+
σ

)

,

where:
M i and M S are magnetic moments of the image and of the source respectively, and
σ and μ r are the conductivity and relative permeability of the magnetic disturber respectively,

wherein the shortest distance between the source and the magnetic disturber is equal to the shortest distance between the image of the source and the magnetic disturber, and
wherein a normal component of the magnetic field at the crossing of one face of the magnetic disturber is kept on either side of the face.

3. The method of claim 1 , further comprising:
determining the position and the magnetic moment of an image of the source solely from the measurements of a magnetic field in quadrature relative to the magnetic field emitted by the source, the measurement being performed by the sensor or sensors whose position and orientation relative to the source are known, and
determining the position and the moment of an other image of the same source solely from the measurements of the magnetic field in phase with the magnetic field emitted by the source, the measurement being performed by the sensor or sensors whose position and orientation relative to the source are known.

4. The method of claim 1 , further comprising
computing an effective modulus of the magnetic field from measurements thereof, in phase and in quadrature relative to the magnetic field emitted by the source, the measurements being performed by the sensor or sensors whose position and orientation relative to the source are known;
determining the position and the magnetic moment of at least one image of the source from the modulus of the magnetic field.

5. The method of claim 1 , further comprising modeling each image of the source as a magnetic dipole.

6. A method for localizing an object, the method comprising:
emitting, in the presence of a magnetic disturber, a magnetic field provided by a uniaxial source situated on one side of the magnetic disturber, the magnetic moment of the source being known,
measuring a magnetic field emitted by a fixed sensor without any degree of freedom for the object,
localizing the object relative to the source by means of the measurement of the sensor,
during the localization, compensating the measurement of the sensor;
wherein compensating comprises determining a position and a magnetic moment of an image of the source situated on the other side of the magnetic disturber using one or more measuremen

Assignees

• Cattin Viviane
• Billeres Malvina
• Commissariat Energie Atomique

Inventors

• Cattin Viviane
• Billeres Malvina

Classifications

• G01R33/025 Primary

  Compensating stray fields {(G01R33/0017 takes precedence)} · CPC title