Applicant hereby claims foreign priority under 35 U.S.C § 119 from European Patent Application No. 16196608.0 filed on Oct. 31, 2016, the disclosure of which is herein incorporated by reference.
The invention concerns a calibration tool for calibrating magnetic sensors.
The sensitivity of a magnetic sensor is defined by a sensitivity vector S. The sensitivity vector S needs to be calibrated in order to achieve the parallelism of its components Sx, Sy and Sz with the x, y and z axis of a reference coordinate system in which a magnetic field to be measured is present. Especially for a multi-axis magnetic field sensor, the calibration of the mutual orthogonality between the sensitivity vectors of individual sensor elements is required to achieve high accurate measurements of the magnetic field. The calibration of the sensitivity vector S requires a magnetic field source which produces a stable homogeneous magnetic field having a constant field intensity, i.e. a reference magnetic field source producing a defined magnetic field vector B. In order to fulfill this requirement, commonly a set-up with Helmholtz coils or electromagnets is used as magnetic field source.
Calibration also requires that the direction of the magnetic field vector B is aligned parallel to one of the axis of the sensor's coordinate system. However, perfect parallelism is very difficult to achieve in practice, mostly resulting in insufficient accuracy of the calibration.
The object of the invention is to provide a calibration tool for calibrating a magnetic sensor overcoming the above mentioned drawback.
A calibration tool for calibrating a magnetic sensor comprises a cuboid-shaped housing and one or more permanent magnets positioned in the housing. The housing is configured to provide six alignment planes. The alignment planes extend either parallel or at an angle of 90° with respect to each other. The one or more permanent magnets provide in a working volume a homogeneous magnetic field that has a constant field intensity. The housing has one or more holes allowing to position a magnetic sensor in the working volume. The one or more permanent magnets may also comprise such holes allowing to position the magnetic sensor in the working volume.
The one or more permanent magnets may comprise, for example, a predetermined number of two or four permanent magnets, namely a first permanent magnet and a second permanent magnet or a first permanent magnet, a second permanent magnet, a third permanent magnet and a fourth permanent magnet.
In a first embodiment, the calibration tool comprises a predetermined number of two permanent magnets, wherein
In a second embodiment, the calibration tool comprises a predetermined number of four permanent magnets, the four permanent magnets being a first permanent magnet, a second permanent magnet, a third permanent magnet and a fourth permanent magnet, wherein
In another embodiment, the one or more magnets may be hollow cylindrical, and given the case arranged concentrically and of different materials providing different temperature coefficients of their magnetic field, so that the temperature coefficient of the total magnetic field within the working volume is zero.
In yet another embodiment, the one or more permanent magnets may be arranged in a Halbach array.
A calibration setup for calibrating a magnetic sensor may include such a calibration tool, a reference member and a holder configured to hold the magnetic sensor. The reference member includes a reference wall for aligning the calibration tool and the holder is securable to the reference member in a fixed mechanical relationship.
The accompanying drawings, which are incorporated into and constitute a part of this specification, illustrate one or more embodiments of the present invention and, together with the detailed description, serve to explain the principles and implementations of the invention. The figures are not to scale. In the drawings:
The calibration of a magnetic sensor usually requires that the magnetic sensor is exposed to a magnetic field Bx pointing in the x-direction, then to a magnetic field By pointing in the y-direction and then to a magnetic field Bz pointing in the z-direction. The present invention concerns a calibration tool that can be used in a calibration setup to provide three magnetic field components Bx, By and Bz extending perfectly orthogonally to each other, with |Bx|=|By|=|Bz|.
The magnets 3 to 6 have a flat shape and they also have a symmetry center. Preferably, they are disc-shaped. They may also be ring-shaped. The magnets 3 to 6 are positioned in the housing 2 along an axis 7 and affixed to the housing 2. The two inner magnets 4 and 5 are each located at a first distance D1 from the geometric center of the housing 2 and, if present, the two outer magnets 3 and 6 are each located at a second distance D2 from the geometric center.
The housing 2 has one or more holes 8 and the magnets 3 to 6 have corresponding holes allowing to position a magnetic sensor in a working volume extending around the geometric center of the cuboid-shaped housing 2. The holes 8 of the housing 2 and the holes of the magnets 3 to 6 form one or more passageways from the outside of the housing 2 to the working volume. The holes 8 of the housing 2 are arranged in the center of the sidewalls and the corresponding holes of the magnets 3 to 6 are arranged in the symmetry centers of the magnets 3 to 6. The axis 7 runs through the geometric center of the housing 2 and through the symmetry centers of the magnets 3 to 6. If the magnets 3 to 6 have a hole 8 in their center, the axis 7 runs through the holes 8.
In a first embodiment, the calibration tool 1 only comprises the first magnet 3 and the second magnet 4. In a second embodiment, the calibration tool 1 comprises the four magnets 3 to 6 whereby the first magnet 3 and the second magnet 4 form a first, inner pair and the third magnet 5 and the fourth magnet 6 form a second, outer pair.
The magnets 3 and 4 are oriented in the same way, i.e. they have the same magnetization direction. Therefore, the magnets 3 and 4 produce magnetic fields which add up to a first magnetic field that points in a first direction and has a substantially constant field intensity B1 within a volume that is at least the size of the working volume. The field intensity B of the magnetic field in the working volume is then B=B1.
If present, the magnets 5 and 6 are oriented in the same way, i.e. they have the same magnetization direction which may be the same or opposite to the magnetization direction of the magnets 3 and 4. Therefore, the magnets 5 and 6 produce magnetic fields which add up to a second magnetic field that points in a second direction and has a substantially constant field intensity B2 within a volume that is at least the size of the working volume. From the described arrangement of the magnets 3 to 6 it follows that the first and second direction are either the same or opposite to each other. In the working volume, the field intensity B of the total magnetic field is then B=B1+B2.
In the first embodiment having only the first magnet 3 and the second magnet 4, the magnets 3 and 4 produce in the working volume the first magnetic field that points substantially along the axis 7 and has the constant field intensity B1. However, the field intensity B1 depends on the temperature.
In the second embodiment with the four magnets 3 to 6, the magnets 3 and 4 are made of a first magnetic material which has a first temperature coefficient k1. The magnets 5 and 6 are made of a second magnetic material which has a second temperature coefficient k2. The first and second material are selected such that the second temperature coefficient k2 is different from the first temperature coefficient k1. Furthermore, the distances D1 and D2 are selected such that the temperature dependence of the field intensity B=B1+B2 vanishes.
The magnetization direction of the magnets 3 and 4 and the magnetization direction of the magnets 5 and 6 are opposite to each other if the first temperature coefficient k1 and the second temperature coefficient k2 have the same sign and they are the same if the first temperature coefficient k1 and the second temperature coefficient k2 have different signs. Nowadays, commercially available permanent magnets all have a negative temperature coefficient. Therefore, in this case, the two magnetization directions are opposite to each other, as shown in
The working volume extends around the center of the cuboid-shaped housing 2 and is located in the middle between the magnets 3 and 4 and also in the middle between the magnets 5 and 6. The field intensity B1 of the magnetic field produced by the magnets 3 and 4 in the working volume is given by the equation:
B
1
=Br
1
C
1 (1)
while the field intensity B2 of the magnetic field produced by the magnets 5 and 6 in the working volume is given by the equation:
B
2
=−B
r2
C
2 (2)
C1 and C2 each denote a geometric form factor which depends on the geometry of the respective magnet pair and on the distance D1 or D2, respectively. Br1 denotes a temperature dependent factor of the magnetic field produced by the magnets 3 and 4 and Br2 denotes a temperature dependent factor of the magnetic field produced by the magnets 5 and 6. The negative sign in equation (2) results from the fact that the magnetization direction of the magnets 5 and 6 is opposite to the magnetization direction of the magnets 3 and 4.
The temperature dependence of Br1 and Ba is given by the equation:
B
r,i(T)=Br,i
where Br,i
The field intensity B of the magnetic field in the working volume of the calibration tool 1 shown in
B=B
r
C
1
−B
r
C
2
=B
r1
·(1+k1(T−20))·C1−Br2
The total magnetic field B is independent from the temperature T if the following equation is fulfilled:
B
r1
k
1
C
1
=B
r2
k
2
C
1 (5)
C1 depends on the distance between the magnets 3 and 4 which is 2D1 and C2 depends on the distance between the magnets 5 and 6 which is 2D2. Therefore, the distances D1 and D2 are selected such that equation (5) is fulfilled.
The field intensity B of the magnetic field in the working volume of the calibration tool 1 may be calibrated for example with a NMR Teslameter.
The calibration tool 1 of the present invention can be used in a calibration setup to produce three magnetic field components Bx, By and Bz extending perfectly orthogonally to each other, with |Bx|=|By|=|Bz|, as illustrated in
The reference member 18 is preferably in the form of a 3D corner as shown in
The calibration tool 1 and the reference member 18 make it possible—by 90° rotations of the calibration tool 1—to produce in the working volume a magnetic field pointing in anyone of the directions x, y, z, −x, −y and −z of a Cartesian coordinate system, i.e. to produce one of the magnetic field components Bx, By and Bz which extend perfectly orthogonally to each other as well as −By, −By and −Bz which are perfectly parallel to the respective component Bx, By or Bz.
In the embodiment illustrated in
During the calibration procedure, one of the sidewall of the calibration tool 1 touches the reference wall 19 of the reference member 18. Therefore, in this case the six sidewalls are alignment planes.
During the calibration of a magnetic sensor, the ends of the screws 16 of one of the sidewalls of the calibration tool 1 touch the reference wall 19 of the reference member 18 and thus perfectly align the calibration tool 1 at the reference wall 19 of the reference member 18.
This embodiment also allows the adjustment of the alignment planes such that the direction of the magnetic field produced by the magnets 3 and 4 or by the magnets 3 to 6, respectively, also runs parallel or orthogonal, respectively, to the alignment planes.
Calibration of a Magnetic Sensor
The magnetic sensor may be a one, two or three axis magnetic sensor, i.e. a magnetic sensor delivering one, two or three output signals corresponding to the magnetic field component(s) extending along the one, two or three axes. The calibration of a magnetic sensor needs a number of different calibrations:
1. Offset Calibration
To calibrate the offset, the magnetic sensor is placed in a zero gauss chamber. The temperature dependence of the offset is determined by heating or cooling the zero gauss chamber and by measuring the temperature and the output signal(s) of the magnetic sensor.
2. Calibration of the Temperature Dependence of the Sensitivity
To determine the temperature dependence of the sensitivity of the magnetic sensor, the magnetic sensor is placed in the working volume of the calibration tool 1. Then the temperature is changed by heating or cooling the magnetic sensor and the temperature and the output signal(s) of the magnetic sensor are measured at different temperatures.
3. Calibration of the Sensitivity Vector
The sensitivity vector calibration of the magnetic sensor may be made as follows:
The magnetic field points in one of the directions x, y, z, −x, −y and −z.
The magnetic field points now in another one of the directions x, y, z, −x, −y and −z.
Steps 4 and 5 are repeated for any further direction of the magnetic field that is necessary for the calibration.
The reference member 18 and the calibration tool 1 define a Cartesian coordinate system with three orthogonal axes x, y and z.
The result of the calibration is a sensitivity matrix S, which for a 1-axis magnetic sensor has the dimensions 1×3, i.e.:
for a 2-axis magnetic sensor has the dimension 2×3, i.e.:
and for a 3-axis magnetic sensor has the dimension 3×3, i.e.:
Once the calibration has been completed, the calibrated magnetic sensor can be used to determine one, two or three components of a magnetic field. With a 1-axis magnetic sensor, the sensor has to be positioned in three mutually orthogonal orientations and a measurement has to be taken in each of the three orientations OA, OB and OC. The components Bx, By and Bz of the magnetic field can then be calculated from a system of three equations. The system of equations depends on the chosen orientations, it might be for example:
U
A
=S·B=S
x1
B
x
+S
y1
B
y
+S
z1
B
z
U
B
=S·B=S
x1
B
y
−S
y1
B
z
+S
z1
B
y
U
C
=S·B=−S
x1
B
y
−S
y1
B
z
+S
z1
B
x
where UA is the output signal of the 1-axis magnetic sensor in the first orientation OA, UB is the output signal of the 1-axis magnetic sensor in the second orientation OB and UC is the output signal of the 1-axis magnetic sensor in the third orientation OC. The quantities Sx1, Sy1 and Sz1 are known from the calibration.
With a 2-axis magnetic sensor two different orientations OA and OB of the magnetic sensor that are mutually orthogonal suffice to resolve the system of three equations with the three unknown components Bx, By and B7.
For instance, depending on the chosen orientations, the system of equations might be:
U
xA
=S·B=S
x1
B
x
+S
y1
B
y
+S
z1
B
z
U
yA
=S·B=S
x2
B
x
+S
y2
B
y
+S
z2
B
z
U
xB
=S·B=S
x1
B
x
−S
y1
B
z
+S
z1
B
y
where U, is the output signal of the X channel (first axis of the 2-axis magnetic sensor) in the first orientation OA, UyA is the output signal of the Y channel (second axis of the 2-axis magnetic sensor) in the first orientation OA and UxB is the output voltage of the X channel (first axis of the 2-axis magnetic sensor) in the second orientation OB, and Sx1, Sz1, Sy1, Sy2, Sz1 and Sz2 are known from the calibration. When choosing other orientations, the system of three equations is different. From the above system of equations the magnetic field components Bx, By and Bz can be calculated.
With a 3-axis magnetic sensor, the magnetic field components Bx, By and Bz can be calculated
where Ux, Uy and Uz are the output voltages of the 3-axis magnetic sensor and S−1 denotes the inverse matrix of the matrix S.
The calibration setup of the present invention provides the following advantages:
While embodiments and applications of this invention have been shown and described, it would be apparent to those skilled in the art having the benefit of this disclosure that many more modifications than mentioned above are possible without departing from the inventive concepts herein. The invention, therefore, is not to be restricted except in the spirit of the appended claims and their equivalents.
Number | Date | Country | Kind |
---|---|---|---|
16196608.0 | Oct 2016 | EP | regional |