JP2009031250A - Magnetostrictive torque sensor - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To improve detection accuracy of a magnetostrictive torque sensor. <P>SOLUTION: A plurality of first detection coils L1 for detecting magnetic permeability in a first direction in a shaft surface and a plurality of second detection coils L2 for detecting magnetic permeability in a second direction in the shaft surface are arranged along the same circumference of a rotating shaft S. Coils L1b and L2b of the first detection coils L1 and the second detection coils L2 are wound on a leg part on the same side in an axial direction among a pair of leg parts provided for cores L1a and L2a of the first detection coils L1 and the second detection coils L2 and arranged in one row in the same circumference of the rotating shaft S. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

  The present invention relates to a magnetostrictive torque sensor that detects the torque of a rotating shaft or a stationary shaft using the inverse effect of magnetostriction generated on the shaft surface.

  There is known a magnetostrictive torque sensor that detects the torque of a rotating shaft or a stationary shaft using the inverse effect of magnetostriction generated on the shaft surface. The inverse effect of magnetostriction is that when torque acts on the rotating shaft or stationary shaft, strain in the tensile direction (for example, + 45 ° direction) and compression direction (for example, −45 ° direction) occurs on the shaft surface. This is a magnetic strain phenomenon in which the permeability increases in the tension direction, while the permeability decreases in the compression direction. A first detection coil arranged to detect a change, and a second detection coil arranged to detect a change in permeability in a second direction (for example, −45 ° direction) on the shaft surface. Yes.

There are a plurality of types of magnetostrictive torque sensors due to differences in detection coils. For example, a method using a pair of U-shaped cores around which a detection coil is wound (see, for example, Patent Document 1), a method using a pair of detection coils formed in a shape of 8 (see, for example, Patent Document 2), a wave A method using a pair of detection coils formed in a shape (for example, see Patent Document 3), a method using a pair of detection coils formed in a hollow cylinder, and the like have been proposed. Are used, for example, a method of forming a magnetic anisotropic part made of slits, grooves, thin films, etc. on the shaft surface (for example, see Patent Documents 4 and 5), and a method of not forming a magnetic anisotropic part on the shaft surface (for example, And Patent Document 6).
JP 2001-133337 A JP-A-6-221940 JP-A-6-273247 JP 7-83769 A Japanese Patent Laid-Open No. 11-37863 JP 2005-208008 A

  However, in the conventional magnetostrictive torque sensor, a slight differential voltage generated between the detection coils is detected by using a bridge circuit or the like, and this differential voltage is amplified by the amplifier circuit. It was easy and the detection accuracy was limited.

  Incidentally, the magnetostrictive torque sensor of the method shown in Patent Documents 4 and 5 has been put into practical use in a torque assist system of an electrically assisted bicycle, but in order to ensure necessary detection accuracy, a groove, Since it is necessary to process a stripe pattern (magnetic anisotropic part) of ± 45 ° with a slit, a thin film, etc., it has been difficult to apply to a rotating shaft or a stationary shaft that does not allow such processing.

  In view of the above circumstances, the magnetostrictive torque sensor of the present invention created for the purpose of solving these problems is the torque of the rotating shaft and / or the stationary shaft using the inverse effect of magnetostriction generated on the shaft surface. A magnetostrictive torque sensor for detecting a change in permeability in a first direction on the shaft surface, a plurality of first detection coils for detecting the change in permeability as an inductance change, and the shaft A plurality of second detection coils arranged to detect a change in permeability in the second direction on the surface and detecting the change in permeability as a change in inductance, and a phase of an oscillation wave according to the change in inductance of the first detection coil A first oscillation circuit that causes a shift, a second oscillation circuit that generates a phase shift in an oscillation wave in accordance with a change in inductance of the second detection coil, and the first oscillation circuit A plurality of oscillating waves output from, and performing an oscillating wave counting process for determining whether or not the count number has reached a predetermined number N, and based on the time measurement required for the oscillating wave counting process, First direction permeability detection means for detecting a change in permeability in the first direction and a plurality of oscillation waves output from the second oscillation circuit are counted, and whether or not the count number has reached a predetermined number N is determined. Oscillation wave count processing to be determined, and based on the time measurement required for the oscillation wave count processing, second direction permeability detection means for detecting a change in permeability in the second direction, and permeability in the first direction And a torque detecting means for detecting the torque of the rotating shaft and / or the stationary shaft based on the difference between the magnetic permeability in the second direction and each of the plurality of first detecting coils is detected on the shaft surface. Area and detection direction For the purpose of limiting, an inverted U-shaped core that forms a closed magnetic circuit with the shaft surface and a coil wound around the core are provided, and the coils are connected in series or in parallel. Each of the plurality of second detection coils includes an inverted U-shaped core that forms a closed magnetic path with the shaft surface, and is wound around the core, in order to limit a detection region and a detection direction on the shaft surface. The coils are connected in series or in parallel, and the plurality of first detection coils and the plurality of second detection coils are arranged in the circumferential direction of the rotating shaft and / or the stationary shaft. Further, the coils of the first detection coil and the second detection coil are arranged on the same side in the axial direction of the pair of legs provided in the cores of the first detection coil and the second detection coil. Wound around the leg of the rotating shaft and / or Or it is arranged in a line on the same circumference of a stationary axis.

  According to such a magnetostrictive torque sensor, it is possible to improve torque detection accuracy. In other words, in the oscillation wave output from the first oscillation circuit and the second oscillation circuit configured as described above, the change in the magnetic permeability on the shaft surface clearly appears as a phase shift, and the phase shift in the oscillation wave occurs. Since the number of oscillating waves is accumulated, it is possible to detect the magnetic permeability change in the first direction and the second direction with high accuracy, and to detect the torque of the rotating shaft and stationary shaft with high accuracy from the difference. Become.

  In addition, the number of oscillation waves output from the oscillation circuit is counted, and an oscillation wave count process is performed to determine whether or not the count number has reached a predetermined number N. Based on the time required for the oscillation wave count process. Since the phase shift (permeability change) of the oscillation wave accumulated in this manner is measured, the phase shift component of the oscillation wave can be measured with high accuracy using an inexpensive digital circuit. Moreover, since the resolution is determined by the counter speed for time measurement and does not depend on the reference frequency of the oscillation circuit, high-resolution stress detection can be performed while optimizing the reference frequency of the oscillation circuit according to the detection target. .

  In addition, the first detection coil and the second detection coil form a closed magnetic circuit with the shaft surface in order to limit the detection region and / or detection direction on the shaft surface, and thus further improve the torque detection accuracy. be able to. That is, in the magnetostrictive torque sensor of the present invention, the phase shift of the oscillation wave corresponding to the torque is accumulated and detected by the number of oscillation waves, so that an error component included in the phase shift of the oscillation wave is also accumulated. However, by limiting the detection region and detection direction on the shaft surface, the SN ratio can be increased, so that accumulated error components can be suppressed and detection accuracy can be improved. Further, since the detection direction can be limited on the detection coil side, it is not necessary to process a striped pattern on the shaft surface with grooves, slits, thin films, or the like. As a result, the torque detection according to the present invention can be applied even to a rotating shaft or a stationary shaft that does not allow such processing.

  In addition to providing a plurality of first detection coils and a plurality of second detection coils, a plurality of first detection coils and a plurality of second detection coils are arranged so as to be aligned in the circumferential direction of the rotating shaft and / or the stationary shaft. Therefore, it is possible to average variations in temperature and material existing in the circumferential direction of the shaft surface, and fluctuations in the gap between the detection coil and the shaft surface, thereby avoiding a decrease in detection accuracy due to these error factors.

  Further, the coils of the first detection coil and the second detection coil are wound around the legs on the same side in the axial direction of the pair of legs included in the cores of the first detection coil and the second detection coil and rotate. Since they are arranged in a line on the same circumference of the shaft and / or the stationary shaft, it is possible to suppress the occurrence of detection errors due to the difference between the coil temperature of the first detection coil and the coil temperature of the second detection coil. That is, the inductances of the first detection coil and the second detection coil not only change according to the magnetic permeability change of the shaft surface, but also change according to the temperature change of the coil itself. If the position of the coil of the coil is shifted in the axial direction, there is a possibility that the detection accuracy is lowered due to the influence of the temperature gradient existing in the axial direction of the rotating shaft or the stationary shaft. Since the coils of the detection coil and the second detection coil are arranged in a line on the same circumference of the rotating shaft and stationary shaft, the influence of the temperature gradient existing in the axial direction of the rotating shaft and stationary shaft is eliminated, Detection accuracy can be improved. Further, when the coils of the first detection coil and the second detection coil are wound around the leg portion of the core, the coil approaches the shaft surface and is easily affected by the surface temperature of the shaft, but the torque detection target is the rotating shaft. In this case, since the temperature of the coil is averaged according to the rotation of the shaft, the temperature error can be further reduced.

  Next, embodiments of the present invention will be described with reference to the drawings. However, the waveform shown in the drawing includes an actual detection waveform and a simulation waveform.

[Basic Configuration of Magnetostrictive Torque Sensor According to the Present Invention]
FIG. 1 is a block diagram showing a basic configuration of a magnetostrictive torque sensor according to the present invention. The magnetostrictive torque sensor 1 shown in this figure shows the basic configuration of the present invention, and detects the torque of the rotating shaft S (or stationary shaft) using the inverse effect of magnetostriction generated on the shaft surface. Therefore, the first detection coil L1, the second detection coil L2, the first oscillation circuit 2, the second oscillation circuit 3, and the detection circuit 4 are provided.

  The first detection coil L1 is arranged to detect a magnetic permeability change in the first direction (for example, + 45 ° direction) on the shaft surface, and detects the magnetic permeability change as a change in inductance. The second detection coil L2 is arranged to detect a change in permeability in the second direction (for example, −45 ° direction) on the shaft surface, and detects the change in permeability as a change in inductance.

  The detection coils L1 and L2 of this embodiment are formed using a high magnetic permeability material to limit the detection region and detection direction on the shaft surface, and are wound around the cores L1a and L2a and the cores L1a and L2a. Coils L1b and L2b are provided. Specifically, coils L1b and L2b are wound around inverted U-shaped cores L1a and L2a made of ferrite, and both ends of the cores L1a and L2a are brought close to the shaft surface. A closed magnetic circuit is formed between the two. This makes it possible to form magnetic paths in the first direction and the second direction in a limited region of the shaft surface, and to detect a change in permeability in the magnetic path. In addition, as long as the inverted U-shaped cores L1a and L2a include at least a pair of leg portions and a connecting portion that connects the upper end portions of the leg portions, the specific shape is not limited to the inverted U-shape. For example, a U-shaped or inverted V-shaped core can be applied to the present invention.

  The first oscillation circuit 2 is configured to autonomously oscillate at a predetermined reference frequency and to cause a phase shift in the oscillation wave in accordance with an inductance change of the first detection coil L1. Further, the second oscillation circuit 3 is configured to autonomously oscillate at a predetermined reference frequency and to cause a phase shift in the oscillation wave in accordance with an inductance change of the second detection coil L2. For example, if the detection coils L1 and L2 are arranged in the feedback circuit of the Schmitt oscillation circuit, it is possible to configure the oscillation circuits 2 and 3 in which a phase shift occurs in the oscillation wave according to the inductance change of the detection coils L1 and L2.

  The Schmitt oscillation circuit is an oscillation circuit that uses the hysteresis characteristics of the Schmitt inverter INV. The Schmitt inverter INV, the capacitor C connected to the input side of the Schmitt inverter INV, and the output of the Schmitt inverter INV are input to the Schmitt inverter INV. And a resistance element interposed in the feedback circuit.

In the Schmitt oscillation circuit in the initial state, since no charge is accumulated in the capacitor C, the voltage across the capacitor C is 0V. At this time, the Schmitt inverter INV has an output H level (5 V) because the input side voltage Vin is equal to or lower than _VL . When the output side voltage Vout of the Schmitt inverter INV is 5V, a current flows to the input side of the Schmitt inverter INV via the feedback circuit 2a, so that electric charges are gradually accumulated in the capacitor C, and the voltage at both ends thereof increases. When the input side voltage Vin of the Schmitt inverter INV reaches _VH , the output of the Schmitt inverter INV is switched to the L level (0 V). When the output side voltage Vout of the Schmitt inverter INV becomes 0V, the capacitor C is discharged, and the input side voltage Vin of the Schmitt inverter INV gradually decreases. When the input voltage Vin of the Schmitt inverter INV drops to _VL , the output of the Schmitt inverter INV is switched to the H level.

By repeating the above operation, a rectangular wave having a predetermined frequency is obtained from the output side of the Schmitt inverter INV. The Schmidt oscillation circuit of the oscillation frequency f (= 1 / T) is determined by the energy storage time period _{T H} discharge period _{T L,} the electric storage period _{T H} and the discharging period _{T L} is determined by the constants of the capacitor C and a resistor element. Therefore, if the detection coils L1 and L2 are arranged in the feedback circuit as resistance elements, it is possible to cause a phase shift in the oscillation wave of the Schmitt oscillation circuit according to the inductance change of the detection coils L1 and L2.

  Of course, the oscillation circuit of the present invention is not limited to the Schmitt oscillation circuit. If the oscillation circuit generates a phase shift in the oscillation wave in accordance with the inductance change of the detection coils L1, L2, the CR oscillation circuit, LC An oscillation circuit, a crystal oscillation circuit, or the like may be used.

  The detection circuit 4 is configured using, for example, a microcomputer (one-chip microcomputer) with a built-in CPU, ROM, RAM, I / O, comparator (comparator), etc., and torque detection described later according to a program written in the ROM. Process. Note that the detection circuit 4 may be configured by a plurality of microcomputers, or may be configured by one or a plurality of ICs.

  The detection circuit 4 counts a plurality of oscillation waves output from the first oscillation circuit 2, performs an oscillation wave count process for determining whether or not the count number has reached a predetermined number N, and performs the oscillation wave count process. The first direction permeability detection means for detecting the change in permeability in the first direction and the plurality of oscillation waves output from the second oscillation circuit 3 are counted based on the time required for the count, and the count number is a predetermined number. Oscillating wave counting processing for determining whether or not N has been reached, and based on the time required for the oscillating wave counting processing, second direction magnetic permeability detecting means for detecting a change in magnetic permeability in the second direction; Torque detecting means for detecting the torque of the rotating shaft S is provided based on the difference between the magnetic permeability in one direction and the magnetic permeability in the second direction.

  In this way, the torque detection accuracy of the magnetostrictive torque sensor 1 can be improved. That is, in the oscillating wave output from the first oscillating circuit 2 and the second oscillating circuit 3 configured as described above, the change in the magnetic permeability of the shaft surface clearly appears as a phase shift, Since the phase shift is accumulated by the number of oscillation waves, it is possible to detect the change in permeability in the first direction and the second direction with high accuracy, and to detect the torque of the rotating shaft S with high accuracy from the difference. Become. Also, the number of oscillation waves output from the oscillation circuits 2 and 3 is counted, and an oscillation wave count process is performed to determine whether or not the count number has reached a predetermined number N, which is necessary for the oscillation wave count process. Since the phase shift (permeability change) of the oscillation wave accumulated based on time is measured, the phase shift component of the oscillation wave can be measured with high accuracy using an inexpensive digital circuit. Moreover, since the resolution is determined by the counter speed for time measurement and does not depend on the reference frequency of the oscillation circuits 2 and 3, high-resolution stress can be achieved while optimizing the reference frequency of the oscillation circuits 2 and 3 according to the detection target. Detection can be performed.

  The first detection coil L1 and the second detection coil L2 form a closed magnetic circuit with the shaft surface in order to limit the detection region and the detection direction on the shaft surface. That is, in the magnetostrictive torque sensor 1 of the present invention, the phase shift of the oscillating wave corresponding to the torque is accumulated and detected by the number of oscillating waves, so that an error component included in the phase shift of the oscillating wave is also accumulated. However, by limiting the detection region and detection direction on the shaft surface, the SN ratio can be increased, so that accumulated error components can be suppressed and detection accuracy can be improved. Further, since the detection direction can be limited on the detection coils L1 and L2 side, it is not necessary to process a striped pattern with grooves, slits, thin films, or the like on the shaft surface. As a result, the torque detection according to the present invention can be applied even to the rotating shaft S in which these processes are not allowed.

  In addition, the first oscillation circuit 2 and the second oscillation circuit 3 are preferably driven alternately in order to avoid mutual interference. For example, after the oscillation driving of the first oscillation circuit 2 is stopped after the oscillation drive of the first oscillation circuit 2 is stopped after the oscillation wave count processing related to the first oscillation circuit 2 is executed in a state where the oscillation drive of the second oscillation circuit 3 is stopped, 3 is executed, and then the difference in measurement time required for each oscillation wave count process is obtained. In this way, it is possible to avoid a decrease in detection accuracy due to mutual interference. In addition, since the detection area of the first detection coil L1 and the detection area of the second detection coil L2 can be arbitrarily set without considering mutual interference, it is easy to optimize the detection area according to use conditions. It becomes.

  The shaft surface of the rotating shaft S for detecting torque by the magnetostrictive torque sensor 1 is preferably a magnetostrictive film 5 formed by plating. For example, a magnetostrictive film 5 made of a nickel alloy is plated over the entire circumference of a part or the entire region of the rotating shaft S. In this way, not only can the torque be detected with high accuracy based on the inverse effect of magnetostriction in the magnetostrictive film 5 in accordance with the torque, but also hysteresis in torque detection can be suppressed. Moreover, in the magnetostrictive torque sensor 1 of the present invention, sufficient detection accuracy can be obtained even with the magnetostrictive film 5 formed by the plating method. Compared to the case of forming a magnetostrictive film, not only can the cost be reduced significantly, but also high-accuracy torque detection can be performed for existing members (including resin) that have been plated with nickel.

  Next, the phase shift accumulation action of the oscillation wave in the present invention will be described with reference to FIGS.

  FIG. 2 is an explanatory diagram showing the phase shift accumulation action of the oscillation wave (enlarged detection waveform start end), and FIG. 3 is an explanatory view showing the phase shift accumulation action of the oscillation wave (enlargement of the detection waveform end section). The waveforms shown in these figures are the output waveforms of the oscillation circuits 2 and 3 in one detection process. The number of oscillation waves output from the oscillation circuits 2 and 3 is counted, and the count number is set to a predetermined number N. The oscillation wave count process is performed to determine whether or not the oscillation wave has been reached, and the measurement of the phase difference of the accumulated oscillation wave is measured based on the time required for the oscillation wave count process. The waveform when the number N is 100 is shown. The upper waveform indicates a case where no torque is applied to the rotation axis S, and the lower waveform indicates a case where torque is applied to the rotation axis S. As is clear from these figures, since the phase shift is not accumulated so much at the beginning of the detected waveform, that is, at the stage where the number N of oscillation waves in the oscillation wave count processing is small, the difference is not clear ( It can be seen that when the count number N increases, the phase shift of the oscillation wave is accumulated and the difference becomes clear, so that the phase shift can be easily measured (see FIG. 3). Since the phase shift of the oscillation wave increases in proportion to the torque acting on the rotation axis S, the torque acting on the rotation axis S can be measured with high accuracy based on the phase shift of the oscillation wave. Become. Further, since the phase shift of the oscillation wave output from each oscillation circuit 2 and 3 appears in the contradictory direction based on the inverse effect of magnetostriction, it is only possible to detect the torque amount and torque polarity of the rotating shaft S based on the difference. Therefore, it is possible to obtain a detection value in which the temperature error and the displacement error are offset.

  Next, a specific detection processing procedure of the detection circuit 4 will be described with reference to FIGS.

  In the torque detection process (torque detection means) shown in FIG. 4, first, after initial setting (S11: including initial value setting of the oscillation wave count number N), the count number change process (S12), first direction transparent Magnetic permeability detection processing (S13: first direction magnetic permeability detection means) and second direction magnetic permeability detection processing (S14: second direction magnetic permeability detection means) are executed in order. Then, the difference between the first direction permeability detection value and the second direction permeability detection value obtained in the permeability detection process (S13, S14) is calculated (S15), and the calculated difference (torque detection value) is predetermined. Is converted into a detection signal format and output (S16), one torque detection process is completed.

  In the count number changing process shown in FIG. 5, first, the input of the count number change signal is determined (S21). If the determination result is YES, the oscillation wave count number N included in the count number change signal is read (S22). In accordance with this, the oscillation wave count number N is changed (S23).

  In the first direction magnetic permeability detection process shown in FIG. 6, after the drive of the first oscillation circuit 2 is started (S31), the counter clear process (S32), the oscillation wave count process (S33, S34), and the time measurement process (S35) is executed, and then the driving of the first oscillation circuit 2 is stopped (S36). The counter clear process is a process for clearing the oscillation wave counter and the time measurement counter (S32). The oscillation wave counting process is a process for counting the number of oscillation waves output from the first oscillation circuit 2 (S33) and determining whether the count number has reached a predetermined number N (S34). . The time measurement process is a process of reading a time measurement counter value (first-direction magnetic permeability detection value) when the count number of oscillation waves reaches N (S35).

  In the second direction magnetic permeability detection process shown in FIG. 7, after the driving of the second oscillation circuit 3 is started (S41), the counter clear process (S42), the oscillation wave count process (S43, S44), and the time measurement process (S45) is executed, and then the driving of the second oscillation circuit 3 is stopped (S46). The counter clear process is a process for clearing the oscillation wave counter and the time measurement counter (S42). The oscillation wave counting process is a process for counting the number of oscillation waves output from the second oscillation circuit 3 (S43) and determining whether or not the count number has reached a predetermined number N (S44). . The time measurement process is a process of reading a time measurement counter value (second-direction magnetic permeability detection value) when the count number of oscillation waves reaches N (S45).

[Characteristic Configuration of Magnetostrictive Torque Sensor According to the Present Invention]
Next, a characteristic configuration of the magnetostrictive torque sensor according to the present invention will be described with reference to FIGS. However, the above description is incorporated by attaching the same reference numerals to the portions common to the magnetostrictive torque sensor 1 shown in FIGS.

  A magnetostrictive torque sensor 11 shown in FIGS. 8 to 10 shows a characteristic configuration of the present invention, and each of the oscillation circuits 2 and 3 includes a plurality of detection coils L1 and L2. More specifically, the first oscillation circuit 2 includes a plurality of (for example, four) first detection coils L1 connected in series (or parallel), and the second oscillation circuit 3 is in series (or parallel). A plurality of (for example, four) second detection coils L2 connected to each other. In this way, by arranging a plurality of first detection coils L1 and second detection coils L2 on the shaft surface, temperature and material variations existing on the shaft surface, and further, the detection coils L1, L2 and the shaft surface Variation in the gap between the two can be averaged, so that a decrease in detection accuracy due to these error factors can be avoided.

  As shown in FIGS. 9 and 10, the plurality of first detection coils L <b> 1 and the plurality of second detection coils L <b> 2 are arranged on the same circumference of the rotation axis S. In this way, not only can the temperature and material variations existing in the circumferential direction of the shaft surface, and also the gap fluctuation between the detection coils L1, L2 and the shaft surface, etc. be averaged, It is possible to minimize the influence of the temperature gradient existing in the axial direction and to avoid a decrease in detection accuracy due to these error factors. The plurality of first detection coils L1 and the plurality of second detection coils L2 are held at predetermined positions by the annular bobbin B. The bobbin B may be an integral type or a divided type.

  When the plurality of first detection coils L1 and the plurality of second detection coils L2 are arranged on the same circumference of the rotation axis S, as shown in FIG. An arrangement configuration in which the detection areas of the two detection coils L2 are alternated can be employed. In this way, it is possible not only to suppress the occurrence of an error due to the deviation between the detection region of the first detection coil L1 and the detection region of the second detection coil L2, but also to eliminate this error based on the rotation of the rotating shaft S. be able to.

  Further, when the plurality of first detection coils L1 and the plurality of second detection coils L2 are arranged on the same circumference of the rotation axis S, as shown in FIG. 10, the detection region of the first detection coil L1 Further, the arrangement may be such that the detection area of the second detection coil L2 overlaps. For example, the height dimensions of the first detection coil L1 and the second detection coil L2 are made different from each other and arranged so as to intersect in plan view. By doing so, it is possible to prevent the occurrence of an error due to the deviation between the detection region of the first detection coil L1 and the detection region of the second detection coil L2.

  Furthermore, in the magnetostrictive torque sensor 11 of the present invention, when the plurality of first detection coils L1 and the plurality of second detection coils L2 are arranged in the circumferential direction of the rotation axis S, the first detection coil L1 and the second detection coil L2 are arranged. Of the pair of legs provided in the cores L1a and L2a of the first detection coil L1 and the second detection coil L2, the coils L1b and L2b of the second detection coil L2 are wound around the same leg in the axial direction and rotated. They are arranged in a line on the same circumference of the axis S. If it does in this way, generation | occurrence | production of the detection error resulting from the difference of the coil temperature of the 1st detection coil L1 and the coil temperature of the 2nd detection coil L2 can be suppressed.

  That is, the inductances of the first detection coil L1 and the second detection coil L2 not only change according to the magnetic permeability change of the shaft surface, but also change according to the temperature change of the coil itself. If the positions of the coils L1b and L2b of the second detection coil L2 are shifted in the axial direction, the detection accuracy may be lowered due to the influence of the temperature gradient existing in the axial direction of the rotating shaft S. Since the coils L1b and L2b of the first detection coil L1 and the second detection coil L2 are arranged in a line on the same circumference of the rotation axis S, the temperature gradient existing in the axial direction of the rotation axis S The detection accuracy can be improved. Further, when the coils L1b and L2b of the first detection coil L1 and the second detection coil L2 are wound around the legs of the cores L1a and L1a, the coils L1b and L2b approach the shaft surface and are easily affected by the surface temperature of the shaft. However, when the torque detection target is the rotary shaft S, the temperature of the coils L1b and L2b is averaged according to the rotation of the shaft, so that the temperature error can be further reduced.

1 is a block diagram showing a basic configuration of a magnetostrictive torque sensor according to the present invention. It is explanatory drawing which shows the phase shift accumulation effect | action (enlarged detection waveform start end part) of an oscillation wave. It is explanatory drawing which shows the phase shift accumulation effect | action (an enlarged detection waveform termination | terminus part) of an oscillation wave. It is a flowchart which shows the process sequence of the torque detection process in a detection circuit. It is a flowchart which shows the process sequence of the setting number change process in a detection circuit. It is a flowchart which shows the process sequence of the 1st direction magnetic permeability detection process in a detection circuit. It is a flowchart which shows the process sequence of the 2nd direction magnetic permeability detection process in a detection circuit. It is a block diagram which shows the characteristic structure of the magnetostrictive torque sensor which concerns on this invention. (A) is an expanded plan view showing a first arrangement example of detection coils, and (B) is a side view showing a first arrangement example of detection coils. (A) is a development top view showing the 2nd example of arrangement of a detection coil, and (B) is a side view showing the 2nd example of arrangement of a detection coil.

Explanation of symbols

1, 11 Magnetostrictive torque sensor 2 First oscillation circuit 3 Second oscillation circuit 4 Detection circuit L1 First detection coil L1a Core L1b Coil L2 Second detection coil L2a Core L2b Coil S Rotating shaft

Claims (1)

A magnetostrictive torque sensor that detects the torque of a rotating shaft and / or a stationary shaft using the inverse effect of magnetostriction generated on the shaft surface,
A plurality of first detection coils arranged to detect a change in permeability in a first direction on the shaft surface, and detecting the change in permeability as a change in inductance;
A plurality of second detection coils arranged to detect a change in permeability in the second direction on the shaft surface, and detecting the change in permeability as a change in inductance;
A first oscillation circuit that causes a phase shift in an oscillation wave in accordance with an inductance change of the first detection coil;
A second oscillation circuit that causes a phase shift in an oscillation wave in accordance with an inductance change of the second detection coil;
Counting a plurality of oscillating waves output from the first oscillating circuit, performing an oscillating wave counting process to determine whether or not the count number has reached a predetermined number N, and measuring the time required for the oscillating wave counting process Based on the first direction permeability detection means for detecting a change in permeability in the first direction,
Counts a plurality of oscillating waves output from the second oscillating circuit, performs an oscillating wave counting process for determining whether or not the counted number has reached a predetermined number N, and measures the time required for the oscillating wave counting process A second direction permeability detecting means for detecting a change in permeability in the second direction,
Torque detection means for detecting torque of the rotating shaft and / or stationary shaft based on the difference between the magnetic permeability in the first direction and the magnetic permeability in the second direction;
Each of the plurality of first detection coils is wound around an inverted U-shaped core that forms a closed magnetic path with the shaft surface in order to limit the detection region and the detection direction on the shaft surface. And the coils are connected in series or in parallel,
Each of the plurality of second detection coils is wound around an inverted U-shaped core that forms a closed magnetic path with the shaft surface in order to limit the detection region and the detection direction on the shaft surface. And the coils are connected in series or in parallel,
The plurality of first detection coils and the plurality of second detection coils are arranged so as to be aligned in the circumferential direction of the rotating shaft and / or the stationary shaft,
Furthermore, the coils of the first detection coil and the second detection coil are wound around the legs on the same side in the axial direction of the pair of legs provided in the cores of the first detection coil and the second detection coil. The magnetostrictive torque sensor is arranged in a line on the same circumference of the rotating shaft and / or the stationary shaft.

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