This application is a National Phase Entry of International Application No. PCT/FR2009/001151, filed on Sep. 28, 2009, which claims priority to French Patent Application Serial No. 08/05953, filed on Oct. 24, 2008, both of which are incorporated by reference herein.
The present invention relates to the field of analog, contactless, linear or rotary, position magnetic sensors. The analog sensors that detect the position from the direction of a magnetic field have several advantages:
For example, the contactless position sensors that measure the position by means of the magnetic field direction are insensitive to the temperature effect on the magnetic properties of the permanent magnets conversely to the sensors that measure the position by measuring the amplitude of a single component of the magnetic field. The measurement of a magnetic field direction is achieved through a ratio of at least two components of the magnetic field which vary identically in temperature. Therefore, the computation of the ratio makes it possible to overcome the variation caused by temperature.
In the field of rotary sensors that measure the magnetic field direction there are rotary sensors that use a permanent magnet at the tip of a rotating shaft of which position is to be measured and at least two magnetically-sensitive members that measure the magnetic field direction on the rotation axis of the moving shaft. However, these devices exhibit restrictions particularly when it comes up to measuring the rotary displacement of a shaft passing through the sensor itself because, in this case, it is impossible to place the magnetically-sensitive members on the rotation axis of the system. In the case of linear sensors, there are structures that use an axially magnetized disk magnet and at least two magnetically-sensitive members that measure the magnetic field direction but these sensors are limited to linear strokes as low as about 20 mm because the amplitude of both components used for the measurement of the field direction becomes too low when the stroke to be measured rises.
It is known from prior art, patent FR2893410 of the applicant, which uses two components of the magnetic induction, generated by a substantially diametrically magnetized ring magnet, measured in a single and same place located close to the median plan of the magnet. A computation of the arctangent of the ratio of both induction components (radial and tangential component) makes it possible to derive the angular position of the magnet. It is however necessary to apply beforehand a correction factor between these two components, in fact in this sensor, the amplitude of both components of the magnetic induction is substantially different.
Typically, this report varies in the range of 1.5 to 4 but the more the magnet diameter is large the more this ratio increases. The increase of the ratio is mainly due to the reduction in the tangential component. For the large diameter magnets, the amplitude of the tangential component is such that it becomes incompatible with the magnetically sensitive members that are conventionally used for this type of sensor and therefore the measurement of the angular position of the magnet is no longer satisfactorily guaranteed. Likewise, the weak amplitude of the tangential component makes the sensor sensitive to the magnetic disruptions that can apply on the sensor.
This correction factor can also lead to problems of measurement precision and the higher this factor is the greater the mistake will be. Furthermore, the necessity of having an amplification ratio between both components before the computation of the position (arctangent) leads to an incompatibility of these systems with certain types of magnetically sensitive members (e.g.: magneto-resistor). Furthermore, there are solutions of revolutions count, for applications of flywheel angle sensor, based on magneto-resistors as described for example in patent EPI 532425B1 which requires that the ratio between both components be lower than 1.5 and that the amplitudes of both components be close to 200 G.
It is also known from the related art, U.S. Pat. No. 0,208,727 illustrated by
It is also known from the related art, patent documents no. US 2002/0179825 and U.S. Pat. No. 5,942,895 describing respectively an angular position magnetic sensor with and a magnetic sensor provided with concentrators arranged to restrict the measurement to one of the components of the measured magnetic field. Meanwhile, the teaching of these documents does not carry out a reliable position detection from a magnet with a magnetization direction that is continuously variable along its displacement direction, nor even to respond to the technical problems that are previously mentioned.
The aim of the present invention is to solve all or part of the aforementioned problems by measuring two components of magnetic induction in a single and same point and by harmonizing the amplitude of both components of the magnetic induction, by means of flux collectors, in order to have an amplitude ratio between these two components of magnetic induction that is close to 1. Such an amplitude ratio makes it possible to use a larger choice of magnetically sensitive members (Hall effect probe, AMR . . . ).
In a first configuration, the sensor comprises a substantially diametrically magnetized ring magnet, a detection member capable of measuring two components of the magnetic induction in a single and same point and two flux collectors that are positioned on the exterior periphery of the magnet. Both components of the magnetic induction are measured in an axially offset plan with respect to the lower face of the collectors. The flux collectors can be molded directly in the sensor casing.
In another configuration, the flux collectors are folded and are directly fixed on the printed circuit supporting the detection elements. According to another alternative, the collectors will be combined to contactless, angular or linear position magnetic sensors as described in patent application FR2898189 of the applicant, whose content is incorporated herein by reference. The described alternatives are not limiting. For example, the collectors can be combined to a contactless, absolute revolution counter magnetic system.
In this regard, the invention relates to a contactless position sensor including at least a permanent magnet emitting a magnetic field, at least a detection member that is sensitive to the magnetic field direction and at least a pair of flux collectors, the permanent magnet being capable of moving in a displacement direction and having a continuously variable magnetization direction along the displacement direction. Each flux collector has at least one portion, provided with an end, extending substantially along the displacement direction of the magnet. The ends of a pair of flux collectors define an air gap oriented along the displacement direction of the magnet. The detection element is positioned outside said air gap and substantially equidistant from the ends.
It is well known that each permanent magnet presents a magnetization of which direction is defined by a magnetization vector. This magnetization vector defines the magnetic field direction inside the magnet. This direction depends on the way the magnet is polarized when produced. For example, a non polarized magnet with the form of a “ring” placed in a sufficient homogenous unidirectional magnetic field will have its magnetization oriented direction along the direction of this magnetic field. In the case where the magnetic field is oriented along a direction perpendicular to the rotation axis of the magnet (a so called magnetization of diametric type) and if this magnet moves rotationally around its axis, the direction of magnetization as seen in a fixed point in the space inside the magnet will then be continuously variable along a linear function.
Preferably, the direction of magnetization of the permanent magnet varies in a linear way. It is the case when the direction of magnetization varies proportionally to the magnet displacement. Advantageously, the direction of magnetization of the permanent magnet varies periodically. It is the case when the direction of magnetization takes the same value when the magnet moves by a predetermined distance.
Preferably, the permanent magnet is substantially cylindrical. Advantageously, the permanent magnet is substantially parallelepiped. Preferably, the flux collectors also present a folding portion. Advantageously, the magnetic sensor includes two pairs of collectors, each pair of collectors defining an air gap, the detection element being positioned equidistant from the four ends of the collectors defining said air gaps. Preferably, the detection element is capable of counting in an absolute way the number of magnet revolutions.
According to an advantageous embodiment, the sensor includes at least a second detection element capable of measuring the angular position of the magnet over 360°. Preferably, the second detection element is combined to at least a pair of flux detectors. Each flux collector has at least a portion, provided with an end, extending substantially along the displacement direction of the magnet. The ends of the pair of flux collectors define an air gap oriented along the displacement direction of the magnet. The detection element is positioned outside said air gap and substantially equidistant from the ends.
Advantageously, the detection elements are positioned on either side of a printed circuit. Preferably, a magnetic shielding element is available in the vicinity of at least one of the detection elements.
Other characteristics and advantages of the invention will be more apparent from the reading of detailed exemplary embodiments, with reference to the figures which respectively represent:
a, is a cross-sectional view of a rotary sensor pertaining to the related art;
b, is a diagram representing the radial and tangential components of the magnetic induction measured by a device of prior art at a point located in the exterior periphery of a diametrically magnetized ring magnet;
a, is a diagram representing the direction of magnetization of the ring magnet for a configuration of a rotary sensor according to the present invention which is applied to the measurement of a high angular stroke;
b, is a diagram representing the direction of magnetization of a tile magnet for a configuration of a rotary sensor according to the present invention which is applied to the measurement of a small angular stroke;
c, is a diagram representing the direction of magnetization of a tile magnet for another configuration of the rotary sensor according to the present invention which is applied to the measurement of a small angular stroke;
a, is a diagram representing the radial and tangential components of the magnetic induction measured near the permanent magnet in two different positions of the sensor illustrated by
b, is a diagram representing the output signals of both detection elements of the sensor of
a represents a structure of a rotary sensor according to prior art. The magnetic flux generated by a substantially diametrically magnetized permanent magnet A1 is collected in the periphery thereof by 4 ferromagnetic pieces A10 that form 2 measurement air gaps. In these two measurement air gaps, two detection elements A4, A5 measure two components of the magnetic induction along two orthogonal axis.
b represents two, radial BR and tangential BT, components of a magnetic induction measured by a device of the prior art in the exterior periphery of a substantially diametrically magnetized ring magnet. The computation of the position is then made following the amplification of the tangential component and an arctangent computation of the ratio of both components of the magnetic induction.
a represents a rotary sensor for high angular stroke applications to be measured, that is to say, close to 360°, according to the present invention with a representation of the direction of magnetization which varies continuously over the 360° of the ring magnet 1. The rotation of the angle of magnetization along the periphery of the magnet is of 360° over the entirety of the periphery of the ring magnet.
b represents a rotary sensor for angular measurement applications over a restricted stroke, that is to say, much lower than 360°, according to the present invention. The angular width of the magnet 1 is adjusted to the useful stroke to be measured in order to reduce the necessary magnet volume to the minimum. The direction of magnetization is represented on the considered magnet sector for the useful stroke of the sensor. The rotation of the angle of magnetization along the periphery of the magnet 1 is substantially equal to the angular width of the considered magnet 1 for the stroke to be measured.
c represents a rotary sensor for angular measurement applications on a restricted stroke which is much lower than 360° according to the present invention. The direction of magnetization is also represented and varies by 360° over the entire periphery of the ring magnet 1.
a represents the radial and tangential components of the magnetic induction measured at the detection elements 3 and 5 of the structure represented in
b represents the angular position signals which are provided by the detection element 5 of the sensor of
Number | Date | Country | Kind |
---|---|---|---|
08 05953 | Oct 2008 | FR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/FR2009/001151 | 9/28/2009 | WO | 00 | 7/8/2011 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2010/046550 | 4/29/2010 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
3061771 | Planer et al. | Oct 1962 | A |
4785242 | Vaidya et al. | Nov 1988 | A |
4966041 | Miyazaki | Oct 1990 | A |
5070298 | Honda et al. | Dec 1991 | A |
5159268 | Wu | Oct 1992 | A |
5164668 | Alfors | Nov 1992 | A |
5250925 | Shinkle | Oct 1993 | A |
5351387 | Iwata et al. | Oct 1994 | A |
5416410 | Kastler | May 1995 | A |
5444313 | Oudet | Aug 1995 | A |
5528139 | Oudet et al. | Jun 1996 | A |
5532585 | Oudet et al. | Jul 1996 | A |
5614668 | Ramirez-Soto | Mar 1997 | A |
5670876 | Dilger et al. | Sep 1997 | A |
5781005 | Vig et al. | Jul 1998 | A |
5814985 | Oudet | Sep 1998 | A |
5942895 | Popovic et al. | Aug 1999 | A |
6043645 | Oudet et al. | Mar 2000 | A |
6043646 | Jansseune | Mar 2000 | A |
6087827 | Oudet | Jul 2000 | A |
6184679 | Popovic et al. | Feb 2001 | B1 |
6219212 | Gill et al. | Apr 2001 | B1 |
6304078 | Jarrard et al. | Oct 2001 | B1 |
6326781 | Kunde et al. | Dec 2001 | B1 |
6518749 | Oudet et al. | Feb 2003 | B1 |
6545463 | Dettmann et al. | Apr 2003 | B1 |
6573709 | Gandel et al. | Jun 2003 | B1 |
6576890 | Lin et al. | Jun 2003 | B2 |
6593734 | Gandel et al. | Jul 2003 | B1 |
6922052 | Steinruecken et al. | Jul 2005 | B2 |
6992478 | Etherington et al. | Jan 2006 | B2 |
7028545 | Gandel et al. | Apr 2006 | B2 |
7030608 | Kawashima et al. | Apr 2006 | B2 |
7049808 | Martinez et al. | May 2006 | B2 |
7088096 | Etherington et al. | Aug 2006 | B2 |
7116210 | Lawrence et al. | Oct 2006 | B2 |
7221153 | Matsumoto et al. | May 2007 | B2 |
7239131 | Halder et al. | Jul 2007 | B2 |
7304450 | Prudham | Dec 2007 | B2 |
7501929 | Lawrence et al. | Mar 2009 | B2 |
7589445 | Gandel et al. | Sep 2009 | B2 |
7644635 | Prudham et al. | Jan 2010 | B2 |
7741839 | Jarrard | Jun 2010 | B2 |
7784365 | Masson et al. | Aug 2010 | B2 |
7898122 | Andrieux et al. | Mar 2011 | B2 |
7906959 | Frachon et al. | Mar 2011 | B2 |
8519700 | Jerance et al. | Aug 2013 | B2 |
20020113678 | Creighton | Aug 2002 | A1 |
20030137293 | Welsch et al. | Jul 2003 | A1 |
20030155909 | Steinruecken et al. | Aug 2003 | A1 |
20040130314 | Bossoli et al. | Jul 2004 | A1 |
20040164733 | Fukaya et al. | Aug 2004 | A1 |
20050218727 | Gandel et al. | Oct 2005 | A1 |
20060123903 | Gandel et al. | Jun 2006 | A1 |
20070008063 | Lawrence et al. | Jan 2007 | A1 |
20070090827 | Jarrard | Apr 2007 | A1 |
20080250873 | Prudham et al. | Oct 2008 | A1 |
20080284261 | Andrieux et al. | Nov 2008 | A1 |
20080314164 | Masson et al. | Dec 2008 | A1 |
20100045275 | Frachon | Feb 2010 | A1 |
20100194385 | Ronnat et al. | Aug 2010 | A1 |
20100231205 | Jerance et al. | Sep 2010 | A1 |
20100253324 | Jarrard | Oct 2010 | A1 |
20110043194 | Frachon et al. | Feb 2011 | A1 |
Number | Date | Country |
---|---|---|
101384883 | Mar 2009 | CN |
102 39 904 | Mar 2004 | DE |
102006051621 | May 2008 | DE |
0 273 481 | Jul 1988 | EP |
0 665 416 | Aug 1995 | EP |
1 014 039 | Jun 2000 | EP |
1 477 772 | Nov 2004 | EP |
1 532 425 | May 2005 | EP |
2 670 286 | Jun 1992 | FR |
2 724 722 | Mar 1996 | FR |
2 764 372 | Dec 1998 | FR |
2 790 549 | Sep 2000 | FR |
2 809 808 | Dec 2001 | FR |
2 845 469 | Apr 2004 | FR |
2 893 410 | May 2007 | FR |
2 898 189 | Sep 2007 | FR |
2 919 385 | Jan 2009 | FR |
2008-0077369 | Aug 2008 | KR |
2008-0104048 | Nov 2008 | KR |
WO 2007057563 | May 2007 | WO |
WO 2007099238 | Sep 2007 | WO |
WO 2009101270 | Aug 2009 | WO |
Number | Date | Country | |
---|---|---|---|
20110254543 A1 | Oct 2011 | US |