BUTZMANN STEFAN (DE)
US6735062B1 | 2004-05-11 | |||
US6433973B1 | 2002-08-13 |
CLAIMS
1. Magnetoresistive sensor with a triangle made of magnetic sensitive material with three corners with two wiring connections, wherein the three sides of the triangle have different or at least substantially equal length.
2. Sensor according to claim 1, wherein the triangle is made of permalloy.
3. Sensor according to one of claims 1 or 2, wherein the triangle is a hollow triangle where the inner part of the triangle is left away, consisting of three side bars of different or at least substantially equal length.
4. Sensor according to one of the claims 1 to 3, wherein the corner is connectable to a current source while the other corners are connectable to a current or voltage detection system.
5. Method of measuring an angle of a magnetic field with a magnetoresistive sensor with a triangle made of magnetic sensitive material with three corners with two wiring connections on every corner, wherein the three sides of the triangle have different or at least substantially equal length, wherein a current has to be supplied to one contact at one corner acting as a source, while the other two contacts at two other corners acting as a sink are kept on a reference potential and measuring the current or the voltage on every of the two other corners. |
Sensor
FIELD OF THE INVENTION
The invention relates generally to a sensor, especially to a magnetoresistive sensor used for angular detection. Additionally the invention relates to a method of measuring an angle.
Magnetoresistive sensors are extensively used to detect angular positions or angular movements of elements. Such kinds of sensors are currently used in many automotive applications, e. g. for pedal positioning or throttle control.
BACKGROUND OF THE INVENTION
The sensors currently in use make use of Wheatstone bridges, which are rotated against each other by an angle of 45°. If an angle of an external magnetic field is changed, the two bridges deliver different signals with a phase difference of 45°. Thus the angular position can be determined. Such sensors are known from DE 198 39 450 Al.
DE 10 2004 019 238 Al discloses a device for measuring the direction of a magnetic field especially for use in a magnetoresistive sensor and a method for determining the direction of magnetic fields using voltage dividers, consisting of resistors that are configured from magnetoresistive thin layers, at least three voltage dividers being arranged in such a way that the signal voltages of the different voltage dividers, which occur in the central contacts during the rotation of the magnetic fields, have phases that are offset in relation to one another.
EP 0 411 971 Bl discloses a device using three magnetoresistive sensors arranged as a pyramid.
Disadvantages of the above mentioned types of sensor elements are its relatively high offset and the offset drift over temperature. Therefore the signals are not reproducible. These
drawbacks result in the need for a sophisticated offset compensation either by the customer or on the signal conditioning die.
SUMMARY OF THE INVENTION The aim of this invention is to mitigate the drawbacks of the prior art and to create a sensor, especially a magnetoresistive sensor with low offset, which can be located in the center of rotation of a magnet, e. g. a block magnet.
The invention relates generally to a sensor, especially to a magnetoresistive sensor used for angular detection according to claim 1. Additionally the invention relates to a method of measuring an angle according to claim 5.
Further inventive advantages are described in the claims 2 to 4.
BRIEF DESCRIPTION OF THE DRAWINGS
The above and other features and advantages of the invention will be apparent from the following description of an exemplary embodiment of the invention with reference to the accompanying drawings, in which:
Fig. 1 shows a schematic view of an inventive sensor;
Fig. 2 shows a schematic view of an inventive sensor;
Fig. 3 shows a schematic view of an inventive sensor; and
Fig 4 shows a diagram.
DETAILED DESCRIPTION OF THE DRAWINGS
Figure 1 show in a schematic view the principle layout of the new and inventive angle sensor 1. The structure of the sensor 1 consists of a triangle 2 with sides 3, 4, 5 of different or at least substantially equal length and with two wiring connections Ci, C 2 , C 3 , C 4 , C 5 , C 6 at each corner 6, 7, 8 in order to allow a signal conditioning with voltage sensing.
In order to determine the magnetic field angle, a current has to be supplied to one contact acting as a source, while the other two contacts acting as a sink are kept on a reference potential. As the angle of the externally applied magnetic field determines the resistances of the permalloy material of the triangle in different directions, different currents will flow to the two sink contacts. Subtraction of the two currents yields in a signal varying sinusoidally with rotation of the magnetic field. By applying this kind of stimulation alternatingly to all three contacts, three signals can be obtained with a phase offset to each other.
Figure 2 shows an alternative configuration of the inventive sensor 10, where the inner part 11 of the triangle 12 is left away. This configuration has the advantage, that the resistances of the sides increase thus yielding higher signal levels, however, possibly also at the cost of increased offset. The structure of the sensor 10 consists of a hollow triangle 12 and again with sides 13, 14, 15 of different or at least substantially equal length and with two wiring connections Ci, C 2 , C 3 , C 4 , C 5 and C 6 at each corner 16, 17, 18.
Figure 3 shows the realization of a possible signal conditioning circuit 20 of the above mentioned sensor 10 according to Figure 2. In the circuit 20, one of the current sources, e. g. II, is supplying a current to the triangular structure 10, while the other two current sources 12 and 13 are switched off. At the same time, the switch S 1 is open, thus ensuring that the complete current Il flows to the permalloy structure 10, while the switches S2 and S3 are closed. The operational amplifiers 21, 22, 23 connected to C4 and C6 keep the two remaining corners of the permalloy structure 10 at the potential of Uref. The relation of the currents flowing from C2 to C3 and from C2 to C5 then depends on the direction of the
external magnetic field applied. The difference of these currents is proportional to the difference of the resulting voltages U2 - U3.
In a similar way, the current source 12 is switched on, Il and 13 are switched off, the switch S2 is opened, while Sl and S3 are closed and the voltage difference Ul - U3 is measured. Ul - U2 is obtained similarly, when 13 is turned on and Sl and S2 are closed.
By this way, three signals DU12 (31) = Ul - U2, DU13 (32) = Ul - U3 and DU23 (33) = U2 - U3 are obtained, which are dependent on the direction of the external magnetic field as shown in Figure 4 with a periodicity of 180° . These three difference signals have a phase offset of 30° magnetic field angle to each other. Figure 4 shows in a diagram 30 the difference voltages DU12, DUl 3, DU23 as simulation data. It can be shown by trigonometric equations that the magnetic field angle α a can now be determined from these signals by the following equation:
\ a =
The sensor allows the determination of the magnetic field angle α with only one permalloy geometry of triangular shape and therefore promises better linearity behaviour than structures with two permalloy areas located next to each other. Additionally, the magnetic field angle can be determined by measuring the current distribution in the permalloy structures yielding in a robuster behaviour against external disturbances.
A sensor as above described may be used in angular sensing applications, such as throttle, pedal or windshield wipers.
REFERENCES
1 sensor
2 triangle
3 side
4 side
5 side
6 corner
7 corner
8 corner
10 sensor
11 inner part
12 triangle
13 side
14 side
15 side
16 corner
17 corner
18 corner
20 circuit
21 operational amplifiers
22 operational amplifiers
23 operational amplifiers
30 diagram
31 signal curve
32 signal curve
33 signal curve