WO2001020349A1 - Detecteur magnetique et detecteur de courant - Google Patents
Detecteur magnetique et detecteur de courant Download PDFInfo
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- WO2001020349A1 WO2001020349A1 PCT/JP2000/003134 JP0003134W WO0120349A1 WO 2001020349 A1 WO2001020349 A1 WO 2001020349A1 JP 0003134 W JP0003134 W JP 0003134W WO 0120349 A1 WO0120349 A1 WO 0120349A1
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- current
- sensor device
- oscillation
- transistor
- magnetic
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R15/00—Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
- G01R15/14—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
- G01R15/18—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers
- G01R15/183—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers using transformers with a magnetic core
- G01R15/185—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers using transformers with a magnetic core with compensation or feedback windings or interacting coils, e.g. 0-flux sensors
Definitions
- the present invention relates to a magnetic sensor device for measuring a relatively large magnetic field and a current sensor device for measuring a large current in a non-contact manner using the magnetic sensor device.
- the Hall element has a problem in processing the offset voltage, which is an obstacle to the cost reduction of the current sensor device.
- the offset voltage is a residual output voltage when the magnetic field to be measured is zero.
- a magnetic sensor device or a current sensor device using a fluxgate element that uses the saturation phenomenon of the magnetic core as a magnetic sensor is expected to generate no offset voltage in principle, and thus attracts attention. ing.
- FIG. 12 is a characteristic diagram showing a relationship between an inductance of a coil wound around a magnetic core and a coil current. Since the magnetic core has magnetic saturation characteristics, when the coil current increases, the effective permeability of the magnetic core decreases, and the inductance of the coil decreases. Therefore, if a bias magnetic field B is applied to the magnetic core with a magnet or the like, an external magnetic field H is generated. When superimposed on the bias magnetic field, the external magnetic field H. The size of the coil inductance Can be measured. This is the simplest principle of operation of a fluxgate device. In FIG. 12, the bias magnetic field B and the external magnetic field H are shown. Are both expressed in terms of coil current.
- the position of the bias point B changes depending on the strength of the magnetic field generated by the magnet, the positional relationship between the magnet and the magnetic core, and so the inductance value when the external magnetic field is zero is adjusted to a constant value. Need to be kept. However, it is extremely difficult to compensate for the instability of this value against temperature changes and other disturbances. Therefore, the above method is not suitable for practical use.
- the effect of hysteresis is usually fairly small because the rod-shaped core has an open magnetic circuit. Therefore, if the hysteresis of the magnetic core is neglected, the saturation characteristics of the magnetic core do not depend on the direction of the coil current.Therefore, the inductance change characteristics when the coil current is made positive and when the coil current is made negative Are the same. For example, points P + and P. In FIG. 12 represent a positive coil current and a negative coil current having the same absolute value. In the vicinity of these points, the change characteristics of the inductance with respect to the change of the absolute value of the coil current are the same.
- the saturation region of the magnetic core refers to a region where the absolute value of the magnetic field is larger than the absolute value of the magnetic field when the magnetic permeability of the magnetic core becomes the maximum magnetic permeability.
- the inductance value decreases at the positive peak of the current (for example, the Q + point in Fig. 12), and the inductance value decreases at the negative peak (for example, the Q. point in Fig. 12).
- the inductance value increases, so the difference has a non-zero value. Since the difference between the inductance values depends on the external magnetic field, the external magnetic field can be measured by measuring the difference between the inductance values.
- the difference between the above-described inductance values is, for example, another inductance connected in series to the sensor coil It can be obtained from the signal obtained by differentiating the voltage generated at both ends of the inductance element, that is, the signal corresponding to the second derivative of the current flowing through the sensor coil.
- the present application describes a method of applying an AC current to the sensor coil such that the magnetic core enters the saturation region at the peak time and measuring the difference in the decrease in the inductance at each of the positive and negative peak values of the current. This is called the large amplitude excitation method.
- Japanese Patent Application Laid-Open No. Hei 4-257474 discloses an oscillation circuit using a sensor coil as a part of a resonance circuit as means for applying an alternating current to the sensor coil.
- the positive and negative waveforms of the excitation current in the sensor coil must be Must be symmetric.
- the positive and negative waveforms of the excitation current are not strictly symmetric.
- the positive and negative asymmetry of the excitation current waveform is quite large. For this reason, even in a sensor device using the large-amplitude excitation method, an offset voltage having a value that cannot be ignored is actually generated.
- the problems caused by this offset voltage are that the offset voltage causes a steady error in the output of the sensor device, and that the offset voltage fluctuates due to external disturbances such as temperature and power supply voltage. .
- the energy loss of the control input of the active element that constitutes the oscillation circuit that induces the positive and negative asymmetry of the excitation current waveform.
- the main cause of the external disturbance that fluctuates the asymmetry is a fluctuation in the operating temperature of the active element forming the oscillation circuit.
- FIG. 13 is a block diagram showing an example of a configuration of a magnetic sensor device using a flux gate element.
- This magnetic sensor device includes a magnetic core 201, a sensor coil 202 composed of at least one coil wound around the magnetic core 201, and one end connected to one end of the sensor coil 202. The end is grounded and core 201 reaches saturation region A change in the inductance value of the sensor coil 202 connected in series with the AC current supply unit 203 that supplies such an AC drive current to the sensor coil 202
- One end of the c- inductance element 204 including the inductance element 204 for detecting the voltage is connected to the other end of the sensor coil 202, and the other end is grounded.
- the magnetic sensor device shown in FIG. 13 is further connected to a connection point between the sensor coil 202 and the inductance element 204, and differentiates the voltage generated between both ends of the inductance element 204.
- the differentiator circuit 205, the positive peak hold circuit 206 that holds the positive peak value of the output signal of the differentiator circuit 205, and the negative peak value of the output signal of the differentiator circuit 205 A negative peak hold circuit 207 for holding; a summing circuit 209 for adding the value held by the positive peak hold circuit 207 to the value held by the negative peak hold circuit 207; An output terminal 209 for outputting an output signal of the adder circuit 208 is provided.
- the excitation current of the sensor coil 202 supplied from the alternating current supply unit 203 is differentiated twice by the inductance element 204 and the differentiation circuit 205,
- the spike-like voltage signals indicate the positive and negative peak values of the excitation current and have opposite polarities.
- the peak values of the positive and negative spike-shaped voltage signals are held by a positive peak hold circuit 206 and a negative peak hold circuit 207, added by an adder circuit 208, and output as an output signal as an output signal. Is output.
- the output signal is It becomes zero and no offset voltage is generated.
- the positive and negative waveforms of the excitation current are not strictly symmetric, especially when a self-excited oscillation circuit is used as the drive circuit.
- the asymmetry of the positive and negative waveforms in the excitation current is quite large. As a result, an offset voltage that cannot be ignored is generated.
- FIG. 14 is a circuit diagram showing an example of the configuration of a clap oscillation circuit for exciting the sensor coil 202. As shown in FIG.
- the clap oscillation circuit shown in FIG. 14 includes an NPN-type bipolar transistor 211, a sensor coil 202 also serving as a resonance coil, and a resonance coil connected in series to the sensor coil 202. Capacitors 2 1 and 2.
- the sensor coil 202 and the resonance capacitor 212 form a series resonance circuit.
- the base of the transistor 210 is connected to one end of the sensor coil 202 via the resonance capacitor 212, and the other end of the sensor coil 202 is grounded.
- One end of a feedback capacitor 2 13 is connected to the base of the transistor 2 1 1.
- the other end of the feedback capacitor 2 13 is connected to one end of the feedback capacitor 2 14 and the emitter of the transistor 2 11.
- the other end of the feedback capacitor 2 14 is grounded.
- the emitter of the transistor 211 is grounded via the emitter load coil 215.
- the collector of the transistor 211 is connected to the power input terminal 216 and to the base via the bias resistor 217.
- the oscillation waveform observed at the base of the transistor 211 is a waveform in which the vicinity of the positive peak value is clamped as shown in FIG.
- positive and negative asymmetry of the oscillation waveform that is, positive and negative asymmetry of the waveform of the excitation current occurs.
- the symbol V CL indicates a clamp potential. If the Q value of the resonant circuit is sufficiently large, the asymmetry of the oscillation waveform is corrected by the resonant circuit. However, in a magnetic sensor using a flux gate element, since the Q value of the sensor coil 102 is not so large, the above-described asymmetry remains, and this asymmetry causes generation of an offset voltage.
- the oscillation amplitude increases as the operating temperature of the transistor 211 increases, which promotes an increase in the offset voltage. This can be explained as follows.
- the excitation current supplied from the oscillation circuit does not include a DC component
- the area of the positive part and the area of the negative part of the excitation current waveform are equal.
- the excitation current waveform is positive / negative asymmetric, when the amplitude of the entire waveform is increased, the increase in the amplitude in the positive portion is not equal to the increase in the amplitude in the negative portion.
- the positive part of the excitation current waveform is a trapezoid
- the negative part is a triangle
- the base of the trapezoid and the triangle are equal.
- the amplitude increase is greater in the negative part than in the positive part.
- the energy consumed as the base current near the positive peak value of the oscillation waveform should be reduced as much as possible. It is necessary to reduce the clamping phenomenon between the base and the emitter, and to eliminate the fluctuation of the clamp potential due to temperature and the fluctuation of the oscillation amplitude due to temperature.
- a Darlington transistor a junction type field effect transistor
- a field effect transistor is also referred to as an FET
- MOS metal oxide semiconductor
- the energy consumed as base current can be reduced.
- the equivalent current gain becomes extremely large, the operation instability due to the temperature dependence of the collector leakage current is large, making it impractical.
- the junction type FET is adopted, the oscillation waveform is not clamped because the FET is voltage-controlled.
- the junction-type FET has no element with a large current capacity, and if used in an excitation circuit that requires a large excitation current, the power loss due to the internal resistance of the junction-type FET is too large to be practical.
- MOS FET If a MOS FET is used, it has the same disadvantages as a junction FET if the M ⁇ S FET is an element with high on-resistance, and a gate, if the MOS FET is an element with low on-resistance.
- the distortion of the oscillation waveform due to the capacitance between the sources is large, and the defect is greater than that of the bipolar transistor.
- the oscillation amplitude must not fluctuate at the operating temperature of the active element of the oscillation circuit.
- the above (1) reduces the absolute value of the offset voltage, (2) eliminates fluctuations in the offset voltage due to temperature, and (3) prevents the offset voltage from increasing due to temperature. Disclosure of the invention
- a first object of the present invention is to provide a magnetic sensor device and a current sensor device using a flux gate element, which provide a magnetic sensor device and a current sensor device capable of reducing the fluctuation of the offset voltage. It is in.
- a second object of the present invention is to reduce the offset voltage in addition to the first object. It is an object of the present invention to provide a magnetic sensor device and a current sensor device that can perform the above-described operations.
- the magnetic sensor device includes a magnetic core, a sensor coil wound around the magnetic core, for detecting an applied magnetic field to be measured, and an alternating current that causes the magnetic core to reach a saturation region. And driving means for driving the sensor coil by supplying the
- the driving means has a self-excited oscillation circuit including a sensor coil as a part of the resonance circuit, and each of the self-excited oscillation circuits independently includes two active elements that cause a change in an oscillation waveform according to a change in an operating temperature. Including, the fluctuation of the oscillation waveform due to the two active elements acts to suppress the fluctuation of the positive and negative asymmetry of the oscillation waveform.
- the current sensor device of the present invention measures a measured current by measuring a measured magnetic field generated by the measured current
- a magnetic core a sensor coil wound around the magnetic core for detecting an applied magnetic field to be measured, and an alternating current that causes the magnetic core to reach a saturation region to the sensor coil.
- the driving means has a self-excited oscillation circuit including a sensor coil as a part of the resonance circuit, and each of the self-excited oscillation circuits independently includes two active elements that cause a change in an oscillation waveform according to a change in an operating temperature. Including, the fluctuation of the oscillation waveform due to the two active elements acts to suppress the fluctuation of the positive and negative asymmetry of the oscillation waveform.
- the two active elements of the self-excited oscillation circuit individually cause fluctuations in the oscillation waveform in accordance with a change in the operating temperature.
- the fluctuation of the waveform acts to suppress the fluctuation of the positive and negative asymmetry of the oscillation waveform.
- the two active elements are an amplifying element used for continuation of oscillation, an NPN transistor that operates when the oscillation waveform is on the positive side, and an oscillation waveform. It may be a PNP-type transistor that operates on the negative side.
- the clamping phenomenon of the oscillation waveform occurs similarly on the positive side and the negative side. Therefore, the positive and negative asymmetry of the oscillation waveform is reduced.
- the NPN transistor The evening emitter and the emitter of the PNP transistor may be connected. Further, in the magnetic sensor device or the current sensor device of the present invention, it is preferable that the NPN transistor and the PNP transistor are formed on the same semiconductor substrate.
- the magnetic sensor device or the current sensor device of the present invention further comprises: a detecting means for detecting an alternating current flowing through the sensor coil; and Control means for controlling the amplitude of the signal.
- the control means may equivalently control the operating voltage of the driving means.
- the two active elements are a first active element having a characteristic of decreasing the oscillation amplitude as the operating temperature increases, and increasing the oscillation amplitude as the operating temperature increases It may be a second active element having characteristics. In this case, the fluctuation of the offset voltage due to the temperature fluctuation is suppressed.
- the first active element may be a field effect transistor
- the second active element may be a bipolar transistor
- the field effect transistor and the bipolar transistor may be cascaded.
- the self-excited oscillation circuit includes a field-effect transistor, converts a voltage having a waveform corresponding to the oscillation waveform into a current, and outputs the current.
- a current amplification element including a transistor and amplifying a current output from the voltage-current conversion element to generate a current for continuing oscillation may be provided. In this case, the clamp phenomenon does not occur, the positive and negative asymmetry of the oscillation waveform is suppressed, and the offset voltage decreases.
- the self-excited oscillation circuit may be a Colpits oscillation circuit or a clap oscillation circuit.
- FIG. 1 is a circuit diagram showing a configuration of a magnetic sensor device according to a first embodiment of the present invention.
- FIG. 2 is a waveform diagram showing an oscillation waveform in the magnetic sensor device according to the first embodiment of the present invention.
- FIG. 3 is a characteristic diagram showing an example of a temperature fluctuation rate of an offset voltage in the magnetic sensor device according to the first embodiment of the present invention.
- FIG. 4 is a circuit diagram showing a configuration of a magnetic sensor device according to a second embodiment of the present invention.
- FIG. 5 is a circuit diagram showing a configuration of a magnetic sensor device according to a third embodiment of the present invention.
- FIG. 6 is a circuit diagram showing a configuration of a current sensor device according to a fourth embodiment of the present invention.
- FIG. 7 is a block diagram showing a configuration of a magnetic sensor device according to a fifth embodiment of the present invention.
- FIG. 8 is a circuit diagram showing an active element portion of a self-excited oscillation circuit in a magnetic sensor device according to a fifth embodiment of the present invention.
- FIG. 9 is a circuit diagram showing a configuration of a magnetic sensor device according to a fifth embodiment of the present invention.
- FIG. 10 is a circuit diagram showing an active element portion of a self-excited oscillation circuit in a magnetic sensor device according to a sixth embodiment of the present invention.
- FIG. 11 is a circuit diagram showing a configuration of a current sensor device according to a seventh embodiment of the present invention.
- FIG. 12 is an explanatory diagram for explaining the operation principle of the flux gate element.
- FIG. 13 is a block diagram showing an example of a configuration of a magnetic sensor device using a flux gate element.
- FIG. 14 is a circuit diagram showing an example of a configuration of a clap oscillation circuit for exciting the sensor coil in FIG.
- FIG. 15 is a waveform diagram showing an oscillation waveform observed at the base of the transistor shown in FIG. BEST MODE FOR CARRYING OUT THE INVENTION
- FIG. 1 is a circuit diagram showing a configuration of a magnetic sensor device according to a first embodiment of the present invention.
- the magnetic sensor device according to the present embodiment includes a magnetic core 1 having magnetic saturation characteristics, a sensor coil 2 including at least one coil wound around the magnetic core 1, and a magnetic core 1 reaching a saturation region.
- a drive unit 10 that supplies a strong alternating current to the sensor coil 2 to drive the sensor coil 2, an inductance element 4 connected in series to the sensor coil 2, and a detection device for measuring the magnetic field to be measured.
- Unit 40 The sensor coil 2 is a coil for detecting an applied magnetic field to be measured.
- the inductance element 4 is an element for detecting a change in the inductance value of the sensor coil 2.
- the inductance element 4 is, for example, a coil having one end connected to the other end of the sensor coil 2 and the other end grounded.
- the drive unit 10 includes a sensor coil 2 and an inductance element 4.
- the detection section 40 is connected to a connection point between the sensor coil 2 and the inductance element 4.
- the drive unit 10 is a self-excited oscillation circuit configured as follows.
- the self-excited oscillation circuit is an NPN transistor 21 that operates when the oscillation waveform is on the positive side, and a PNP transistor that operates when the oscillation waveform is on the negative side. Has 3 and 1.
- the NPN transistor 21 and the PNP transistor 31 are preferably formed on the same semiconductor substrate (wafer).
- the base of the NPN transistor 21 is connected to one end of the resonance capacitor 22.
- the base of the PNP type transistor 31 is connected to one end of the common screw capacitor 32.
- the other ends of the resonance capacitors 22 and 32 are connected to one end of the sensor coil 2.
- the base of the NPN transistor 21 is connected to one end of the feedback capacitor 23. It is connected.
- the base of the PNP transistor 31 is connected to one end of the feedback capacitor 33.
- the other ends of the feedback capacitors 2 3 3 3 are connected to one end of the feedback capacitor 30.
- the other end of the feedback capacitor 30 is grounded.
- the emitter of the NPN transistor 21 and the emitter of the PNP transistor 31 are connected to each other and to the connection point of the feedback capacitors 23, 33.
- the base of the NPN transistor 21 is connected to the power input terminal 25 via the bias resistor 24.
- the collector of the NPN transistor 21 is connected to the power input terminal 25.
- the base of the PNP transistor 31 is grounded via a bias resistor 34.
- the collector of the PNP transistor 31 is grounded.
- the sensor coil 2, the inductance element 4, and the capacitors 22, 23, 33, 33, 33 constitute a series resonance circuit in a self-excited oscillation circuit. That is, the series resonance circuit partially includes the sensor coil 2.
- C S 1 C S2 «C E the self-excited oscillation circuit shown in Fig. 1 becomes a clap oscillation circuit.
- C S 1 C S2 » C B 1 C B2 and C S 1 C When S2 »C E , the self-excited oscillation circuit shown in Fig.
- the detection unit 40 is connected to the connection point between the sensor coil 2 and the inductance element 4, and the inductance element A differentiating circuit 41 for differentiating the voltage generated at both ends of 4, a positive peak-hold circuit 42 for holding the positive peak value of the output signal of the differentiating circuit 41, and an output signal of the differentiating circuit 41
- the negative peak hold circuit 43 holds the negative peak value of the negative peak value, and the value held by the positive peak hold circuit 42 and the negative peak hold circuit 43 Therefore, an addition circuit 44 for adding the held value is provided, and an output terminal of the addition circuit 44 is connected to the output terminal 45.
- an AC excitation current such that the magnetic core 1 reaches the saturation region is supplied to the sensor coil 2 by the driving unit 10 including a self-excited oscillation circuit, and the sensor coil 2 is driven.
- the excitation current is multiplied by the Q value of the series resonant circuit in the self-excited oscillation circuit with respect to the current value limited by the power supply voltage.
- the exciting current of the sensor coil 2 is differentiated twice by the inductance element 4 and the differentiating circuit 41, and becomes spike-like voltage signals having opposite polarities, representing the positive and negative peak values of the exciting current. .
- the peak values of the positive and negative spike-shaped voltage signals are held by the positive peak hold circuit 42 and the negative peak hold circuit 43 and added by the adder circuit 44 to obtain an output signal corresponding to the magnetic field to be measured. Output from the output terminals 45.
- NPN transistor 21 is turned on near the positive peak value of the oscillating voltage waveform applied to the base, and capacitor 30 is charged by the emitter current. .
- the energy stored in the capacitor 30 is used for continuation of oscillation.
- a part of the resonance energy is consumed as the base current of the NPN transistor 21 and a clamping phenomenon occurs.
- the PNP transistor 31 is turned on near the negative peak value of the oscillation voltage waveform applied to the base, and the capacitor 30 is discharged by its emitter current, that is, opposite to the case where the oscillation voltage waveform is positive. Is charged in the direction of. The energy charged in the capacitor 30 is used for continuation of oscillation.
- the negative peak value of the oscillation voltage waveform a part of the resonance energy is consumed as the base current of the PNP-type transistor 31 and a clamping phenomenon occurs.
- the clamping phenomenon of the oscillation waveform similarly occurs on the positive side and the negative side. Therefore, in the present embodiment, the oscillation waveform is positive / negative symmetric as shown in FIG. 2 or extremely small even if there is asymmetry. As a result, according to the present embodiment, the offset in the magnetic sensor device using the flux gate element is reduced. Can be reduced.
- the clamp potential fluctuates similarly on the positive side and the negative side of the oscillation waveform.
- the positive and negative symmetry of is maintained. Therefore, according to the present embodiment, in the magnetic sensor device using the flux gate element, the fluctuation of the offset voltage due to the temperature change can be reduced.
- the emitter of the NPN transistor 21 and the emitter of the PNP transistor 31 are connected, one transistor becomes a load of the emitter of the other transistor. The need for an independent emitter load for each of the transistors 21 and 31 is eliminated.
- the NPN transistor 21 and the PNP transistor 31 are formed on the same semiconductor substrate, compared to the case where the transistors 21 and 31 are independent. As a result, the characteristics of the transistors 21 and 31 with respect to the temperature change become more approximate, so that the fluctuation of the offset voltage with respect to the temperature change can be further reduced.
- FIG. 3 is a characteristic diagram showing an example of the temperature fluctuation rate of the offset voltage in the magnetic sensor device according to the present embodiment.
- the horizontal axis represents temperature
- the vertical axis represents the temperature fluctuation rate of the offset voltage.
- the temperature fluctuation rate of the offset voltage is a percentage of the fluctuation rate of the output voltage at different temperatures based on the output voltage of the magnetic sensor device at 25 ° C.
- the broken line shows the characteristics of the magnetic sensor device according to the present embodiment
- the solid line shows the characteristics of a magnetic sensor device using the oscillation circuit shown in FIG. 14 as a comparative example, for example.
- the value of the temperature fluctuation rate of the offset voltage shown in FIG. 3 is as follows. At a temperature of ⁇ 40 ° C., ⁇ 0.17% in the present embodiment, and 2.08% in the comparative example. When the temperature is 20 ° C., in the present embodiment, ⁇ 0.13%, and in the comparative example, 1.39%. At a temperature of 0 ° C., ⁇ 0.05% in the present embodiment, and 0.75% in the comparative example. At a temperature of 50 ° C., 0.06% in the present embodiment, and ⁇ 0.75% in the comparative example. At a temperature of 80 ° C., 0.12% in the present embodiment, and 1.187% in the comparative example.
- FIG. 3 also shows that, according to the present embodiment, the offset voltage changes with temperature. It can be seen that the movement can be reduced.
- FIG. 4 is a circuit diagram showing a configuration of the magnetic sensor device according to the present embodiment.
- the magnetic sensor device is different from the magnetic sensor device according to the first embodiment in that a detection unit that detects an alternating current flowing through the sensor coil 2 is provided based on a detection result of the detection unit.
- Control means for controlling the drive unit to control the amplitude of the current flowing through the sensor coil 2 is added.
- the detection means and the control means are configured as follows. That is, one end of the capacitor 51 is connected to the connection point between the sensor coil 2 and the inductance element 4, and one end of the capacitor 52 and one end of the resistor 53 are connected to the other end of the capacitor 51. It is connected.
- the other end of the capacitor 52 is connected to one end of a resistor 54, a force source of a diode 55, and a base of an NPN transistor 56.
- the other ends of the resistors 53, 54, the anode of the diode 55, and the emitter of the transistor 56 are grounded.
- the collector and the emitter of the transistor 56 are connected via the capacitor 58.
- the base of the NPN transistor 57 is connected to the collector of the transistor 56.
- connection point between the collector of the transistor 31 and the resistor 34 is not grounded, and this connection point is connected to the collector of the transistor 57 and is connected via the capacitor 59. Grounded.
- the emitter of transistor 57 is grounded.
- the collector of the transistor 56 and the base of the transistor 57 are connected to the power input terminal 25 via the resistor 60.
- the capacitor 51 and the resistor 53 constitute a differentiating circuit.
- the capacitor 52, the resistor 54, the diode 55, the transistor 56, and the capacitor 58 constitute a peak rectifier circuit which also serves as an amplification circuit. These differentiating circuit and peak rectifying circuit correspond to the detecting means in the present invention.
- the transistor 57 is equivalent to controlling the operating voltage of the driver, and corresponds to the control means in the present invention.
- a differentiating circuit including the capacitor 51 and the resistor 53 provides: The voltage generated at both ends of the inductance element 4 is differentiated to generate spike-like voltage signals having opposite polarities, representing the positive and negative peak values of the excitation current. Then, the peak rectifier circuit generates a control signal corresponding to the amplitude of the spike-like voltage signal and applied to the base of the transistor 57. This control signal decreases as the amplitude of the excitation current increases, and increases as the amplitude of the excitation current decreases, as described below.
- the base potential of the transistor 56 increases, and the collector potential of the transistor 56 decreases.
- the collector potential of transistor 56 is applied to the base of transistor 57 as a control signal.
- the control signal decreases, the current flowing between the collector and the emitter of the transistor 57 decreases, and the collector potential of the transistor 57 increases.
- the potential between the collector and the emitter of the transistors 21 and 31, ie, the operating voltage, is reduced, and the amplitude of the excitation current is controlled to decrease.
- the control signal increases, the operating voltage of transistors 21 and 31 increases, and the amplitude of the excitation current is controlled to increase.
- the amplitude of the excitation current is controlled based on the detection result of the amplitude of the excitation current so that the amplitude of the excitation current becomes constant. Therefore, according to the present embodiment, even if the excitation current waveform has a slight positive / negative asymmetry, the asymmetry is prevented from changing due to external disturbance, and the fluctuation of the offset voltage is further reduced. be able to.
- control signal may be subjected to signal processing such as amplification and phase complementation as needed.
- FIG. 5 is a circuit diagram showing a configuration of the magnetic sensor device according to the present embodiment.
- the present embodiment differs from the magnetic sensor device according to the first embodiment in that a detecting means for detecting an alternating current flowing through the sensor coil 2 and a detecting means Control means for controlling the drive unit based on the detection result of the above, and controlling the amplitude of the current flowing through the sensor coil 2.
- the configurations of the differentiating circuit and the peak rectifying circuit are the same as those of the second embodiment.
- an NPN transistor 61 is provided instead of the transistor 57 in the second embodiment.
- the transistor 61 is provided between the collector of the transistor 21 and the power input terminal 25 in the first embodiment.
- the base of transistor 61 is connected to the collector of transistor 56.
- the collector of the transistor 61 is connected to the power input terminal 25.
- the emitter of the transistor 61 is connected to the collector of the transistor 21 and grounded via the capacitor 62.
- the transistor 61 equivalently controls the operating voltage of the driving section, and corresponds to the control means in the present invention.
- the connection point between the collector of the transistor 31 and the resistor 34 is grounded.
- the base potential of the transistor 56 increases, and the collector potential of the transistor 56 decreases.
- the collector potential of the transistor 56 is applied to the base of the transistor 61 as a control signal.
- the control signal decreases, the emitter potential of the transistor 61 decreases.
- the potential between the collector and the emitter of the transistors 21 and 31, that is, the operating voltage decreases, and the amplitude of the excitation current is controlled to decrease.
- the control signal increases, the operating voltage of transistors 21 and 31 increases, and the amplitude of the excitation current is controlled to increase.
- control signal may be subjected to signal processing such as amplification and phase complementation as needed.
- FIG. 6 is a circuit diagram showing a configuration of the current sensor device according to the present embodiment.
- the current sensor device according to the present embodiment is configured using the magnetic sensor device according to the first embodiment.
- the current sensor device includes a magnetic yoke 72 provided so as to surround the conductive portion 71 through which the current to be measured passes, and having a gap in part.
- the magnetic core 1 and the sensor coil 2 of the magnetic sensor device according to the first embodiment are arranged in the gap of the magnetic yoke 72.
- the magnetic flux generated by the current (current to be measured) flowing through the conductive portion 71 in a direction perpendicular to the plane of FIG. 6 is converged by the magnetic yoke 72, Go through 2.
- the magnetic field (measured magnetic field) in the gap is measured by a magnetic sensor device including the magnetic core 1 and the sensor coil 2 arranged in the gear of the magnetic yoke 72, and the measured current is non-current. Measured by contact.
- the magnetic sensor device according to the second or third embodiment may be used as the magnetic sensor device.
- Other configurations, operations, and effects of the present embodiment are the same as those of the first to third embodiments.
- FIG. 7 is a block diagram showing a configuration of a magnetic sensor device according to a fifth embodiment of the present invention.
- the magnetic sensor device according to the present embodiment includes a magnetic core 101 having magnetic saturation characteristics, a sensor coil 102 composed of at least one coil wound around the magnetic core 101, and a magnetic core 1.
- a drive unit 110 that supplies an alternating current such that 01 reaches a saturation region to the sensor coil 102 to drive the sensor coil 102, and a sensor connected in series to the sensor coil 102. It comprises a conductance element 104 and a detecting section 140 for measuring a magnetic field to be measured.
- the sensor coil 102 is a coil for detecting an applied magnetic field to be measured.
- the inductance element 104 is an element for detecting a change in the inductance value of the sensor coil 102.
- the inductance element 104 is, for example, a coil having one end connected to the other end of the sensor coil 102 and the other end grounded.
- the driving unit 110 is a sensor coil And an inductance element 104.
- the detection section 140 is connected to a connection point between the sensor coil 102 and the inductance element 104.
- the drive unit 110 is a self-excited oscillation circuit configured as follows. That is, the driving unit 110 has a resonance capacitor 121, a feedback capacitor 122, and a feedback capacitor 123 connected in series to one end of the sensor coil 102 in this order. I have. The end of the feedback capacitor 1 2 3 opposite to the feedback capacitor 1 2 2 is grounded. The sensor coil 102, the inductance element 104, and the capacitors 121, 122, and 123 constitute a series resonance circuit in the self-excited oscillation circuit. That is, the series resonance circuit partially includes the sensor coil 102.
- the drive unit 110 further includes a voltage-current conversion element 1 11 and a current amplification element 1 12 which are connected in cascade at the connection point between the resonance capacitor 1 21 and the feedback capacitor 1 2 2.
- the current amplifying element 112 is connected to a connection point of the feedback capacitors 122, 123 and is connected to one end of a load inductance element 124 consisting of, for example, a coil. The other end of the inductance element 124 is grounded. Further, the voltage-current conversion element 111 and the current amplification element 112 are connected to the power input terminal 125.
- the voltage-current conversion element 111 converts a voltage having a waveform corresponding to the oscillation waveform into a current and outputs the current.
- the current amplification element 112 amplifies the current output from the voltage-current conversion element 111 to generate a current for continuation of oscillation.
- the detection unit 140 is connected to a connection point between the sensor coil 102 and the inductance element 104, and differentiates a voltage generated at both ends of the inductance element 104, and a differentiation circuit 1441, Circuit 14 1 Positive peak hold circuit 14 2 that holds the positive peak value of the output signal, and Differentiator circuit 14 4 1 Negative peak hold circuit 1 4 3 that holds the negative peak value of the output signal. And an adder circuit 144 for adding the value held by the positive peak hold circuit 144 and the value held by the negative peak hold circuit 144. The output terminal of the adder circuit 144 is connected to the output terminal 144.
- FIG. 8 is a circuit diagram showing an active element portion of a self-excited oscillation circuit in the magnetic sensor device according to the present embodiment.
- the active element portion is A portion including an active element and a passive element such as a resistor necessary for the operation of the active element.
- a portion indicated by reference numeral 120 is an active element portion.
- the inductance element 104 is omitted.
- the active element section 120 is composed of a junction field-effect transistor (junction FET) 13 1 as a voltage-current conversion element 1 11 and an NPN-type bipolar transistor 1 as a current amplification element 1 1 2 3 and 2.
- junction FET junction field-effect transistor
- the junction type FET 131 and the bipolar transistor 132 are connected in cascade as described below.
- the gate G of the junction type FET 13 1 is connected to the connection point between the resonance capacitor 1 21 and the feedback capacitor 1 2 2.
- the gate G of the junction type FET 13 1 is further connected to the connection point of the feedback capacitors 1 2 2 and 1 2 3 via the bias resistor 13 5, the emitter E of the bipolar transistor 13 2, and the inductance element. It is connected to one end of 24.
- the source S of the junction type FET 13 1 is connected to the connection point of the feedback capacitors 122, 123 via the resistor 133, the emitter E of the bipolar transistor 132, and one end of the inductance element 124. It is connected to the.
- the source S of the junction FET 131 is further connected to the base B of the bipolar transistor 132 via the resistor 134.
- the drain D of the junction type FET 13 and the collector C of the bipolar transistor 13 are connected to the power input terminal 125.
- the junction type FET 131 has a characteristic of decreasing the oscillation amplitude as the operating temperature rises, and corresponds to the first active element in the present invention. It has a characteristic of increasing the oscillation amplitude, and corresponds to the second active element of the present invention.
- the capacitances of the capacitors 122, 122, 123 in FIG. 8 are Cs, Cb, and Ce, respectively, when Cs ⁇ Cb and Cs ⁇ Ce, the capacitance shown in FIG.
- the excitation oscillation circuit becomes a clap oscillation circuit.
- Cs »Cb and Cs» Ce the self-excited oscillation circuit shown in FIG. 8 is a Colpitts oscillation circuit.
- FIG. 9 is a circuit diagram showing a configuration of the magnetic sensor device according to the present embodiment, including the active element portion 120 shown in FIG. The description of this figure is omitted because it is the same as the description of FIGS. 7 and 8.
- an AC excitation current such that the magnetic core 101 reaches the saturation region is supplied to the sensor coil 102 by the drive unit 110 constituted by a self-excited oscillation circuit.
- the sensor coil 102 is driven.
- the excitation current is multiplied by the Q value of the series resonant circuit in the self-excited oscillation circuit with respect to the current value limited by the power supply voltage.
- the exciting current of the sensor coil 102 is differentiated twice by the inductance element 104 and the differentiating circuit 141, and represents the positive and negative peak values of the exciting current. It becomes a spike-like voltage signal.
- the peak values of the positive and negative spike-shaped voltage signals are held by a positive peak hold circuit 144 and a negative peak hold circuit 144, added by an adder circuit 144, and output signals corresponding to the magnetic field to be measured. Output from the output terminals 1 4 5.
- the active element portion 120 of the self-excited oscillation circuit includes a junction type FET 131, which serves as a voltage-current conversion element 111, and a bipolar transistor 110, which serves as a current amplification element 112. 3 and 2.
- the input impedance of the gate G of F ET 13 1 is extremely large, and no clamping phenomenon of the input signal occurs. Therefore, if a junction type FET 131, which is a voltage driving element, is used as the voltage-to-current conversion element 111, there is no need for current to drive the voltage-to-current conversion element 111, and there is a portion that shunts energy Therefore, no clamping phenomenon occurs in the voltage waveform (oscillation waveform) applied to the input terminal of the voltage-to-current converter 111 (gate G of the junction type FET 1311).
- the current output from the voltage-current conversion element 111 is amplified by the current amplification element 112 and charged to the capacitor 123. The energy from this charging is used for continuation of oscillation.
- the positive and negative asymmetry of the oscillation waveform is very small. Also, since there is no clamping phenomenon, there is no fluctuation of asymmetry due to fluctuation of the clamp potential with temperature fluctuation. Therefore, according to the present embodiment, in the magnetic sensor device using the flux gate element, The offset voltage can be reduced.
- the current output of the active element portion 120 is obtained from the emitter E of the bipolar transistor 132 as the current amplification element 112.
- bipolar transistor 132 having a sufficiently small saturation voltage between the collector and the emitter can be employed as current amplifying element 112, so that power loss can be reduced.
- the voltage-current conversion element 111 may be a circuit such as a volt- age follower using an operational amplifier, an emitter follower using a bipolar transistor, or a source follower using a junction type or MOS type FET.
- operational amplifiers are costly.
- An emitter follower circuit using bipolar transistors has a characteristic that when the base voltage rises and the transistor saturates, a clamping phenomenon occurs, and the oscillation amplitude increases as the operating temperature rises. Therefore, when a bipolar transistor is used as the current amplifying element 112, both the voltage-current converting element 111 and the current amplifying element 112 increase the oscillation amplitude as the operating temperature increases. Absent.
- the output current of the voltage-current conversion element 111 may be sufficient to drive the current amplification element 112
- FET for small signals can be used. From the above, FET is preferable as the voltage-current conversion element used in the present invention.
- FET has a negative temperature coefficient of the transconductance between the gate voltage and the drain current in both the junction type and the M ⁇ S type. This means that when FET is used as the voltage-to-current conversion element 111, the conversion coefficient of the voltage-to-current conversion decreases as the operating temperature rises. Therefore, FET 131, as voltage-current conversion element 111 in the present embodiment, has a characteristic of decreasing the oscillation amplitude as the operating temperature increases.
- bipolar transistors generally have a positive current amplification temperature coefficient. Therefore, the bipolar transistor 132 as the current amplifying element 112 in the present embodiment has a characteristic that the oscillation amplitude increases as the operating temperature increases.
- the self-excited oscillation circuit The FET 131, which has the characteristic of reducing the oscillation amplitude by means of the circuit, and the bipolar transistor 132, which has the characteristic of increasing the oscillation amplitude as the operating temperature rises, are included.
- the fluctuation of the oscillation amplitude due to the temperature rise occurs in the opposite direction between the FET 13 1 and the bipolar transistor 13 2.
- the present embodiment since there is almost no positive or negative asymmetry of the oscillation waveform caused by the clamp phenomenon, there is almost no temperature fluctuation of the asymmetry accompanying the clamp phenomenon. Also, the temperature dependence of the oscillation amplitude is suppressed, so that the remaining slight asymmetry is not expanded by temperature changes. Therefore, according to the present embodiment, in the magnetic sensor device using the flux gate element, it is possible to solve all the following problems for solving the problem due to the offset voltage.
- the self-excited oscillation circuit according to the present embodiment is different from the conventional self-excited oscillation circuit shown in FIG. 14, for example, in that a small-signal FET 131 and two resistors for its source load are provided. It can be realized with a very simple configuration by adding 1 3 3 and 1 3 4. Therefore, according to the present embodiment, a very inexpensive magnetic sensor device having excellent characteristics can be realized. If this magnetic sensor device is applied to a current sensor device used in an electric vehicle, solar power generation, or the like, the industrial contribution is extremely large.
- FIG. 10 is a diagram of the magnetic sensor device according to the present embodiment.
- FIG. 3 is a circuit diagram showing an active element portion of the excitation oscillation circuit.
- a small-signal MOS type FET 13 6 is used as the voltage-current converter 111 of the self-excited oscillation circuit, instead of the junction type FET 13 1 in the fifth embodiment. It was what was.
- a bias resistor 1337 is provided between the gate of the FET 1336 and the power input terminal 125 instead of the bias resistor 135 in the fifth embodiment. It has been done.
- FIG. 11 is a circuit diagram showing a configuration of the current sensor device according to the present embodiment.
- the current sensor device according to the present embodiment is configured using the magnetic sensor device according to the fifth embodiment.
- the current sensor device is provided so as to surround conductive part 151 through which the current to be measured passes, and has magnetic yoke 152 having a gap in a part thereof.
- the magnetic core 101 and the sensor coil 102 in the magnetic sensor device according to the fifth embodiment are arranged in the gap between the magnetic yokes 152.
- the magnetic flux generated by the current (current to be measured) flowing through the conductive portion 151 in a direction perpendicular to the plane of FIG. 11 is converged by the magnetic yoke 152, Pass 1-5.
- the magnetic field (measured magnetic field) in the gap is measured by a magnetic sensor device including the magnetic core 101 and the sensor coil 102 arranged in the gap of the magnetic yoke 152.
- the measured current is measured in a non-contact manner.
- the magnetic sensor device according to the sixth embodiment may be used as the magnetic sensor device.
- Other configurations, operations, and effects of the present embodiment are the same as those of the fifth or sixth embodiment.
- each of the two active elements of the self-excited oscillation circuit causes a change in the oscillation waveform according to the change in the operating temperature. Since the fluctuation of the oscillation waveform caused by the two active elements acts in the direction of suppressing the fluctuation of the positive and negative asymmetry of the oscillation waveform, it is necessary to reduce the offset voltage in a magnetic sensor device or a current sensor device using a flux gate element. Can be.
- the two active elements are an NPN transistor that operates when the oscillation waveform is on the positive side and a PNP transistor that operates when the oscillation waveform is on the negative side.
- the oscillating waveform clamping phenomenon occurs on the positive side and the negative side in the same way, and the positive and negative asymmetry of the oscillating waveform decreases, so that in magnetic sensor devices or current sensor devices using flux gate elements, This makes it possible to reduce the offset voltage and the fluctuation of the offset voltage.
- the emitter of the NPN transistor and the emitter of the PNP transistor when the emitter of the NPN transistor and the emitter of the PNP transistor are connected, one transistor becomes a load of the emitter of the other transistor, The need for an independent emitter load for each transistor is eliminated.
- the fluctuation of the offset voltage with respect to the temperature change should be reduced. Can be. Further, in the magnetic sensor device or the current sensor device of the present invention, when the amplitude of the current flowing through the sensor coil is controlled, the fluctuation of the offset voltage can be further reduced.
- the two active elements include a first active element having a characteristic of decreasing the oscillation amplitude as the operating temperature increases, and an oscillation element as the operating temperature increases.
- the second active element having the characteristic of increasing the amplitude, the fluctuation of the offset voltage due to the temperature fluctuation can be suppressed, so that in the magnetic sensor device or the current sensor device using the flux gate element, Variations in offset voltage can be reduced.
- the self-excited oscillation circuit includes a field-effect transistor, converts a voltage having a waveform corresponding to an oscillation waveform into a current, and outputs the current.
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Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2000620175A JP3366905B2 (ja) | 1999-09-10 | 2000-05-16 | 磁気センサ装置および電流センサ装置 |
EP00925684A EP1130404A1 (en) | 1999-09-10 | 2000-05-16 | Magnetic sensor and current sensor |
US09/648,460 US6316939B1 (en) | 1999-09-10 | 2000-08-28 | Magnetic sensor measuring apparatus and current sensor non-contact measuring apparatus |
Applications Claiming Priority (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP25683899 | 1999-09-10 | ||
JP11/256838 | 1999-09-10 | ||
JP25683999 | 1999-09-10 | ||
JP11/256839 | 1999-09-10 |
Related Child Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US09/648,460 Continuation US6316939B1 (en) | 1999-09-10 | 2000-08-28 | Magnetic sensor measuring apparatus and current sensor non-contact measuring apparatus |
Publications (1)
Publication Number | Publication Date |
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WO2001020349A1 true WO2001020349A1 (fr) | 2001-03-22 |
Family
ID=26542928
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/JP2000/003134 WO2001020349A1 (fr) | 1999-09-10 | 2000-05-16 | Detecteur magnetique et detecteur de courant |
Country Status (6)
Country | Link |
---|---|
US (1) | US6316939B1 (ja) |
EP (1) | EP1130404A1 (ja) |
JP (1) | JP3366905B2 (ja) |
CN (1) | CN1154851C (ja) |
TW (1) | TW498166B (ja) |
WO (1) | WO2001020349A1 (ja) |
Families Citing this family (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6823725B2 (en) * | 2000-01-13 | 2004-11-30 | Continental Teves Ag & Co., Ohg | Linear distance sensor and the use thereof as actuator for motor vehicles |
KR100451480B1 (ko) * | 2002-06-28 | 2004-10-08 | 주식회사 서미트 | 직류 및 교류의 측정이 가능한 클램프형 전류측정기 |
KR20050035251A (ko) * | 2002-08-01 | 2005-04-15 | 젠트론 아크티엔게젤샤프트 | 자기장 센서 및 자기장 센서의 작동 방법 |
EP2691782A1 (de) * | 2011-03-29 | 2014-02-05 | Continental Teves AG & Co. oHG | Stromsensor |
US8222898B1 (en) * | 2011-04-15 | 2012-07-17 | The United States Of America As Represented By The Secretary Of The Army | Method and apparatus for utilizing magnetic field modulation to increase the operating frequency of sensors |
CN102565723A (zh) * | 2012-01-17 | 2012-07-11 | 中国人民解放军91872部队上海研究室 | 磁通门式宽量程测磁仪 |
TWI451095B (zh) * | 2012-12-10 | 2014-09-01 | Ind Tech Res Inst | 電流偵測電路及其方法 |
TWI493208B (zh) * | 2013-07-22 | 2015-07-21 | 凱立自動化有限公司 | 交流電源感測裝置 |
ES2539399B2 (es) * | 2013-12-27 | 2015-11-06 | Instituto Nacional De Técnica Aeroespacial "Esteban Terradas" | Método de medida para un sensor saturable |
US20160003875A1 (en) * | 2014-07-01 | 2016-01-07 | K-Line Automation Co., Ltd. | Alternating current detector |
TWI561830B (en) | 2015-07-21 | 2016-12-11 | Ind Tech Res Inst | Non-contact type three-phase three-wire power cable measurement device and measurement method thereof |
CN105790716B (zh) * | 2016-05-03 | 2018-12-21 | 苏州泰思特电子科技有限公司 | 高频衰减振荡波电压发生器 |
JP6620796B2 (ja) * | 2017-07-28 | 2019-12-18 | Tdk株式会社 | オフセット推定装置および方法、磁気センサの補正装置ならびに電流センサ |
US11579172B2 (en) | 2018-09-26 | 2023-02-14 | Solaredge Technologies Ltd. | Flux gate sensor circuit |
CN109270325B (zh) * | 2018-11-12 | 2024-05-24 | 深圳市艾华迪技术有限公司 | 一种自激型开环磁通门电流传感器电路及其自激振荡方法 |
CN111751593A (zh) * | 2019-03-28 | 2020-10-09 | Tdk株式会社 | 电流传感器 |
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US5287059A (en) * | 1990-05-19 | 1994-02-15 | Nkk Corporation | Saturable core magnetometer with a parallel resonant circuit in which the W3 DC level changes with a change in an external magnetic field |
JPH08304481A (ja) * | 1995-05-08 | 1996-11-22 | Shimadzu Corp | 電力計 |
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JPS5660370A (en) | 1979-10-23 | 1981-05-25 | Nippon Telegr & Teleph Corp <Ntt> | Magnetometer |
US4384254A (en) | 1980-06-06 | 1983-05-17 | The United States Of America As Represented By The Secretary Of The Navy | Oscillator/driver circuit for fluxgate magnetometer |
JPS57194424A (en) | 1981-05-22 | 1982-11-30 | Mitsubishi Electric Corp | Exciting circuit |
DE3121234C1 (de) | 1981-05-27 | 1983-02-24 | Siemens AG, 1000 Berlin und 8000 München | Verfahren und Schaltungsanordnung zur Messung eines Magnetfeldes,insbesondere des Erdmagnetfeldes |
JPS6057277A (ja) | 1983-09-09 | 1985-04-03 | Mishima Kosan Co Ltd | 自励式磁気検出方法 |
WO1985001357A1 (en) | 1983-09-09 | 1985-03-28 | Mishima Kosan Company, Limited | Apparatus for detecting magnetism |
US4626782A (en) | 1983-09-26 | 1986-12-02 | The Boeing Company | Magnetometer operated at a self-resonant frequency by a sense winding |
JPH0223407A (ja) | 1988-07-12 | 1990-01-25 | Nec Corp | 磁気センサ及び磁場発生方法 |
US5537038A (en) * | 1988-12-15 | 1996-07-16 | Nkk Corporation | Magnetic flux measuring method and apparatus for detecting high frequency components of magnetic flux with high speed orientation |
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JPH05281312A (ja) | 1992-04-03 | 1993-10-29 | Nkk Corp | 磁気計測方法及び装置 |
JP3516780B2 (ja) | 1995-08-29 | 2004-04-05 | ジェコー株式会社 | 磁気センサ回路 |
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2000
- 2000-05-15 TW TW089109238A patent/TW498166B/zh not_active IP Right Cessation
- 2000-05-16 WO PCT/JP2000/003134 patent/WO2001020349A1/ja not_active Application Discontinuation
- 2000-05-16 CN CNB008006369A patent/CN1154851C/zh not_active Expired - Fee Related
- 2000-05-16 EP EP00925684A patent/EP1130404A1/en not_active Withdrawn
- 2000-05-16 JP JP2000620175A patent/JP3366905B2/ja not_active Expired - Fee Related
- 2000-08-28 US US09/648,460 patent/US6316939B1/en not_active Expired - Fee Related
Patent Citations (3)
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JPS418372B1 (ja) * | 1962-09-20 | 1966-04-30 | ||
US5287059A (en) * | 1990-05-19 | 1994-02-15 | Nkk Corporation | Saturable core magnetometer with a parallel resonant circuit in which the W3 DC level changes with a change in an external magnetic field |
JPH08304481A (ja) * | 1995-05-08 | 1996-11-22 | Shimadzu Corp | 電力計 |
Also Published As
Publication number | Publication date |
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EP1130404A1 (en) | 2001-09-05 |
JP3366905B2 (ja) | 2003-01-14 |
CN1310801A (zh) | 2001-08-29 |
US6316939B1 (en) | 2001-11-13 |
TW498166B (en) | 2002-08-11 |
CN1154851C (zh) | 2004-06-23 |
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