The present invention relates to a geomagnetic sensor that measures the earth magnetism.
Conventionally, as a geomagnetic sensor that measures the earth magnetism, a flux gate type (FG type) geomagnetic sensor is known widely (for example, refer to Patent Literature 1).
Although being capable of high precision measurement of the earth magnetism, the flux gate type geomagnetic sensor has a problem in that, because a core with an exciting coil wound therearound has to be magnetically saturated with an AC current, namely an alternating current, the excitation current increases and power consumption is large.
Patent literature 1: Japanese Patent Application Laid Open No. 2009-92381
It is an object of the present invention is to provide a geomagnetic sensor being capable of reducing power consumption.
According to the present invention, a geomagnetic sensor includes: a core that constitutes a closed magnetic circuit; two coils that are wound around the core in positions facing each other and are connected in series to generate magnetic flux in the same circumferential direction in the core; an excitation power supply that applies an alternating current (AC) with a superimposed direct current (DC) to the two coils; and a detection circuit that is connected to a connection point of the two coils.
According to the present invention, unlike a conventional flux gate type geomagnetic sensor, it is not required to excite a core until the core is magnetically saturated, that is, without magnetically saturating the core, it is possible to measure the earth magnetism with high precision, and it is therefore possible to reduce power consumption compared with the conventional sensors.
Descriptions are given below to embodiments of the present invention.
A core 10 constituting a closed magnetic circuit is made of a highly permeable magnetic material, such as permalloy; the core is assumed to be a toroidal core in this case. Coils 21, 22 are wound around the core 10 in positions facing each other with the coil axial centers parallel to each other. The coils 21, 22 are wound around in the same direction viewed from the center of the core 10, and are connected in series to generate two pieces of magnetic flux in the same circumferential direction in the core 10 when a current is applied to the coils 21, 22.
To one end of the one coil 21, an excitation power supply 30 is connected. The excitation power supply 30 includes a DC (direct current) power supply 31 and an AC (alternating current) power supply 32, and is capable of applying an AC current with a superimposed DC current to the coils 21, 22. In
A DC current is applied to the coils 21, 22 by the DC power supply 31, which generates two pieces of DC magnetic flux in the core 10. In
The coils 21, 22 are assumed to have an identical number of turns, and an inductance L1 of the coil 21 and an inductance L2 of the coil 22 are equal. At a connection point P of the coil 21 and the coil 22, an AC voltage with a superimposed DC voltage is generated by the excitation power supply 30 including the DC power supply 31 and the AC power supply 32. An AC voltage Vd at the connection point P is expressed by the following, where Vac is an AC excitation voltage of the excitation power supply 30:
Vd=(L2/(L1+L2))·Vac (1)
and the inductances L1, L2 of the coil 21 and the coil 22 are equal when the external magnetic field is 0, so that the AC voltage Vd at the connection point P becomes ½ of the AC excitation voltage Vac.
In the meanwhile, when the earth magnetism M passes through the core 10 as illustrated in
When the magnetic flux density changes, as understood from
As seen from the above, the AC voltage Vd at the connection point P of the two coils 21, 22 changes depending on the input of the earth magnetism (external magnetic field), so that detection of the AC voltage Vd at the connection point P enables measurement of the earth magnetism.
A detection circuit 40 is connected to the connection point P of the coils 21, 22. The detection circuit 40 in this embodiment includes, as illustrated in
The detection circuit 40 is supposed to obtain the output Vo in such a manner. It is possible to measure the earth magnetism by the output Vo because the output Vo is responsive (proportional) to the magnitude of the earth magnetism.
As described above, in this embodiment, unlike the conventional flux gate type geomagnetic sensor, it is not required to excite the core 10 until the core is magnetically saturated, that is, the core 10 is not supposed to be magnetically saturated. Accordingly, the excitation current (DC current) may be small and the amplitude of the AC excitation voltage may also be small, thereby making it possible to reduce power consumption compared with the conventional flux gate type geomagnetic sensor.
Next, descriptions are given to a third embodiment of a geomagnetic sensor according to the present invention.
Relative to the configuration illustrated in
The feedback coil 23 is wound around the core 10 to make the core 10 magnetically-equilibrated. As illustrated in
The feedback circuit 50 is connected to a subsequent stage of the detection circuit 40. The feedback circuit 50 includes a reference voltage source 51 to generate a reference voltage, an adder 52 to add an output of the detection circuit 40 (output of the low pass filter 42) and the reference voltage, and an amplifier 53 to amplify the output of the adder 52 and flow a feedback current to the feedback coil 23.
The current sense resistor 60 converts the feedback current flowing through the feedback coil 23 to a voltage and outputs the voltage.
The reference voltage generated by the reference voltage source 51 is set up to cancel an output voltage output from the low pass filter 42 to 0 V when the external magnetic field is 0. Accordingly, the feedback current becomes 0 when the external magnetic field is 0, and a current does not flow through the feedback coil 23. An output of the current sense resistor 60 becomes 0 V.
In the meanwhile, when the earth magnetism M is input as illustrated in
Although embodiments of the present invention have been described above, the core 10 is not limited to a toroidal core and may also be in another shape, and for example, may also be a core in a quadrilateral shape. In addition, instead of the DC power supply 31, a DC constant current source may also be used.
Number | Date | Country | Kind |
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2011-262486 | Nov 2011 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2012/067709 | 7/11/2012 | WO | 00 | 4/8/2014 |
Publishing Document | Publishing Date | Country | Kind |
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WO2013/080601 | 6/6/2013 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
3260930 | Kawada | Jul 1966 | A |
3421074 | Geyger | Jan 1969 | A |
3731752 | Schad | May 1973 | A |
3829894 | Watanabe et al. | Aug 1974 | A |
5091697 | Roth et al. | Feb 1992 | A |
5530252 | Petric | Jun 1996 | A |
6194897 | Fukunaga | Feb 2001 | B1 |
6984979 | Edel | Jan 2006 | B1 |
Number | Date | Country |
---|---|---|
1208002 | Dec 1965 | DE |
1441177 | Sep 1969 | DE |
58-180964 | Oct 1983 | JP |
2000-028695 | Jan 2000 | JP |
2005-315812 | Nov 2005 | JP |
2009-092381 | Apr 2009 | JP |
Entry |
---|
Toshikatsu Sonoda et al. (“A Current Sensor of High Response and High Sensitivity”, Conference Record of the Industry Applications Society Annual Meeting. Seattle, Oct. 7 12, 1998; [Conference Record of the Industry Applications Society Annual Meeting], New York, IEEE, US, vol. Meeting 25, Oct. 7, 1998 (1998-18-87), pp. 626-631. |
Extended European Search Report, mailed Oct. 16, 2015, from the European Patent Office (E.P.O.) in the corresponding European Patent Application No. 12854399.8. |
Number | Date | Country | |
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20140253113 A1 | Sep 2014 | US |