JP4455468B2 - Induction heating coil and high-frequency heating device - Google Patents

Description

  The present invention relates to an induction heating coil and a high-frequency heating device, and more particularly to an induction heating coil used in a magnetic anisotropy adding step in a method of manufacturing a magnetostrictive torque sensor and a high-frequency heating device including the induction heating coil.

  For example, in an electric power steering apparatus equipped as a steering system for an automobile, a steering torque applied to a steering shaft from a steering wheel by a driver's steering operation is generally detected by a steering torque detector. The steering torque detector is usually composed of a torsion bar type torque sensor, and recently a magnetostrictive type torque sensor has also been proposed. The steering shaft functions as a rotating shaft that rotates by receiving a rotational force generated by a steering operation, and is a rotating shaft of the steering torque detector. The electric power steering device drives and controls a motor for assisting steering force in accordance with the torque signal detected from the steering torque detector, thereby reducing the driver's steering force and providing a comfortable steering feeling.

  As described above, a magnetostrictive torque sensor is known as a steering torque detector used in the electric power steering apparatus. This magnetostrictive torque sensor includes magnetostrictive films having magnetic anisotropies opposite to each other at two predetermined positions on the surface of the steering shaft. The magnetostrictive torque sensor has a sensor configuration that detects, in a non-contact manner, a change in magnetostrictive characteristics of the magnetostrictive film in accordance with torsion that occurs on the steering shaft when torque is applied to the steering shaft from the steering wheel.

  In the process of manufacturing the magnetostrictive torque sensor as described above, a magnetostrictive film is formed on a predetermined surface of a part of the steering shaft, that is, a circumferential surface having a predetermined axial width on the rotating shaft, and the magnetostrictive film is magnetically anisotropic. A process of adding sex is necessary. A conventional method for adding magnetic anisotropy to a magnetostrictive film in the manufacture of a magnetostrictive torque sensor is to apply a torsional torque to a rotating shaft on which a magnetostrictive material plating part (magnetostrictive film) is formed by, for example, plating, thereby rotating the rotating shaft. This is a method in which stress is applied to the circumferential surface, and the rotating shaft is heated for a predetermined time by high-frequency induction heating in this stress-applied state (see, for example, Patent Document 1).

Further, there is a one-winding induction heating coil described in Patent Document 2 as a related conventional heating coil.
JP 2004-340744 A JP 2001-509633 A

  According to the conventional method of manufacturing a magnetostrictive torque sensor, in the step of adding magnetic anisotropy to the magnetostrictive film of the rotating shaft, an induction heating coil and an induction heating power source are used as heating means for heating the magnetostrictive material plating part. ing. In the conventional high-frequency heating device, the induction heating coil has a cylindrical one-turn coil portion, and the inner peripheral surface of the one-turn coil portion has a constant inner diameter over the entire inner peripheral surface and is free of irregularities. It was a smooth surface. When such a one-turn coil part is used, induction heating is not sufficient in the vicinity of the one-turn coil part corresponding to the high-frequency current introduction terminal part, so that the center deviation of the temperature distribution occurs in the magnetostrictive film, and the heating There was a problem that variations would occur.

  In view of the above problems, the object of the present invention is to heat the magnetostrictive film base portion (magnetostrictive material plating portion) of the rotating shaft at high frequency in the step of adding magnetic anisotropy to the magnetostrictive film of the rotating shaft of the magnetostrictive torque sensor. An object of the present invention is to provide an induction heating coil and a high-frequency heating device that can improve the sensitivity performance of the magnetostrictive film by matching the center of the heating coil with the temperature center.

  The induction heating coil and the high-frequency heating device according to the present invention are configured as follows in order to achieve the above object.

An induction heating coil according to the present invention (corresponding to claim 1) is a magnetostrictive film (magnetostrictive material plating portion) formed on the circumferential surface of a cylindrical bar-shaped workpiece (rotary shaft) of a magnetostrictive torque sensor to which a torsional torque is applied. An induction heating coil that heats the magnetostrictive film at a high frequency in the magnetic anisotropy adding step of the magnetostrictive torque sensor that adds the magnetic anisotropy to the magnetostrictive film by releasing the torsion torque of the rotating shaft after high-frequency heating, 2 the induction heating coil has one turn coil portion disposed to surround the magnetostrictive film (ring portion), first turn coil portion is La, which oppose each other through the cylindrical shape and a gap It has two plate-like high-frequency current introduction terminal portions, and at least one linear groove parallel to the axial direction is included in the inner peripheral surface of the one-turn coil portion on the inner peripheral surface due to the positional relationship included in the plane formed by the gap. Formed of one-turn coil part Dimension is greater than the axial width of the magnetostrictive film of the columnar bar-shaped workpiece, the protrusion is formed over the entire circumference on the inner peripheral surface of the upper opening and the lower opening, the protrusions relative to the magnetostrictive film that it is arranged so as to be positioned on the outside in the axial direction.

  In the induction heating coil, since the linear groove formed on the inner peripheral surface of the one-turn coil portion is provided, it becomes possible to enhance the circumferential symmetry of the heating when the magnetostrictive film is heated at a high frequency. It is possible to eliminate the temperature distribution at the point and improve the detection sensitivity.

  Another induction heating coil (corresponding to claim 2) is preferably characterized in that, in the above configuration, the linear groove is formed from the opening at one end to the opening at the other end.

Still another induction heating coil (corresponding to claim 3), in each of the above configurations, preferably, the one-turn coil portion has two plate-like high-frequency current introduction terminal portions arranged to face each other via a gap. And the linear groove is formed on the inner peripheral surface in a positional relationship included in a plane formed by the gap.

An induction heating coil according to the present invention (corresponding to claim 4 ) is configured to include any of the induction heating coils described above and a high-frequency power source that supplies a high frequency to the induction heating coil.

  The present invention has the following effects. According to the induction heating coil according to the present invention or the high-frequency heating device configured using the induction heating coil, the one-turn coil portion of the heating induction coil is formed with a predetermined linear groove on the inner peripheral surface thereof. When the magnetostrictive film (magnetostrictive material plating part) of the rotating shaft, such as a magnetostrictive torque sensor, is heated at a high frequency, the center of the rotating shaft and the temperature center can be made to coincide with each other. A direction can be added.

  Further, if the rotating shaft is used in a magnetostrictive torque sensor, the detection sensitivity of the magnetostrictive torque sensor can be improved.

  DESCRIPTION OF EMBODIMENTS Preferred embodiments (examples) of the present invention will be described below with reference to the accompanying drawings.

  First, the basic configuration of the magnetostrictive torque sensor will be described with reference to FIGS. 1 and 2 show an example of the structure of a magnetostrictive torque sensor. FIG. 1 is a partially sectional side view showing a basic structure of a magnetostrictive torque sensor, and FIG. 2 is a side view conceptually showing a basic structure of the magnetostrictive torque sensor.

  As shown in FIGS. 1 and 2, the magnetostrictive torque sensor 10 includes a rotation shaft 11, one excitation coil 12 and two detection coils 13 </ b> A and 13 </ b> B arranged around the rotation shaft 11. . In FIG. 1 and FIG. 2, the rotating shaft 11 is shown with its upper and lower parts cut away and omitted for convenience of explanation.

  The rotating shaft 11 is configured as a part of a steering shaft, for example. The rotating shaft 11 receives a rotational force (torque) of clockwise rotation (clockwise) or counterclockwise rotation (counterclockwise) as indicated by an arrow A around the axis 11a. The rotating shaft 11 is formed of a metal rod such as a chromium molybdenum steel material (SCM material). Magnetostrictive films 14 </ b> A and 14 </ b> B are provided on the rotary shaft 11 at two locations in the upper and lower directions in the axial direction. Each of the magnetostrictive films 14 </ b> A and 14 </ b> B has a constant width (axial width) in the axial direction of the rotating shaft 11 and is formed over the entire circumference of the rotating shaft 11 in the circumferential direction. The width dimension in the axial direction of each of the magnetostrictive films 14A and 14B and the distance between the two magnetostrictive films 14A and 14B are arbitrarily set according to conditions. The magnetostrictive films 14A and 14B are actually formed as magnetostrictive material plating portions on the surface of the rotating shaft 11 by electrolytic plating processing or the like. The magnetostrictive films 14A and 14B having magnetic anisotropy are formed by applying magnetic anisotropy processing to the magnetostrictive material plated portion.

  In the following description, for the convenience of explanation, “magnetostrictive films 14A and 14B” and “magnetostrictive material plating portions (14A and 14B)” indicate the same thing, but are used properly according to the stage and situation of manufacture. In principle, a stage completed by adding magnetic anisotropy is referred to as “magnetostrictive films 14A and 14B”, and in the previous stage, it is referred to as “magnetostrictive material plating portions (14A and 14B)”.

  The excitation coil 12 and the detection coils 13A and 13B are provided in correspondence with the two magnetostrictive films 14A and 14B formed on the surface of the rotating shaft 11, as shown in FIG. That is, as shown in FIG. 1, the detection coil 13A is disposed around the magnetostrictive film 14A with a gap interposed therebetween. The ring-shaped detection coil 13A surrounds the entire circumference of the magnetostrictive film 14A, and the axial width dimension of the detection coil 13A is substantially equal to the axial width dimension of the magnetostrictive film 14A. A detection coil 13B is disposed around the magnetostrictive film 14B with a gap interposed therebetween. Similarly, the ring-shaped detection coil 13B surrounds the entire circumference of the magnetostrictive film 14B, and the axial width dimension of the detection coil 13B is substantially equal to the axial width dimension of the magnetostrictive film 14B. Further, a ring-shaped excitation coil 12 is disposed around each of the two detection coils 13A and 13B. In FIG. 1, the exciting coils 12 are individually provided corresponding to the magnetostrictive films 14 </ b> A and 14 </ b> B, respectively, but actually, two portions of one exciting coil 12 are shown separately. is there. The detection coils 13A and 13B and the excitation coil 12 are provided in a space around the magnetostrictive films 14A and 14B using ring-shaped support frame bodies 15A and 15B provided around the rotation shaft 11 so as to surround the rotation shaft 11. It is wound.

In FIG. 2, the excitation coil 12 and the detection coils 13A and 13B arranged with respect to the magnetostrictive films 14A and 14B of the rotating shaft 11 are conceptually shown as electrical relationships. An AC power supply 16 that constantly supplies an AC current for excitation is connected to the excitation coil 12 that is arranged in common with respect to the magnetostrictive films 14A and 14B. Inductive voltages V _A and V _B corresponding to the torque to be detected are output from the output terminals of the detection coils 13A and 13B arranged corresponding to the magnetostrictive films 14A and 14B, respectively.

  The magnetostrictive films 14A and 14B formed on the surface of the rotating shaft 11 are magnetostrictive films having magnetic anisotropy made by, for example, electrolytic plating processing by Ni-Fe plating. Each of the two magnetostrictive films 14A and 14B is made to have magnetic anisotropies in opposite directions. When torque due to rotational force is applied to the rotating shaft 11, reverse magnetostrictive characteristics generated in the magnetostrictive films 14A and 14B are detected by using the detection coils 13A and 13B arranged around the magnetostrictive films 14A and 14B. To detect.

  The magnetostrictive torque sensor 10 is used by being incorporated as a steering torque detector on a steering shaft of an electric power steering device, for example.

  FIG. 3 will be further described in detail. FIG. 3 is a diagram showing the magnetostrictive characteristic curves 51A and 51B of the two magnetostrictive films 14A and 14B, respectively. In FIG. 3, the horizontal axis means the steering torque applied to the steering shaft 21, and the positive side (+) corresponds to the right rotation and the negative side (−) corresponds to the left rotation. The vertical axis in FIG. 3 means the voltage axis.

The magnetostrictive characteristic curves 51A and 51B for the magnetostrictive films 14A and 14B simultaneously represent the detection output characteristics of the detection coils 13A and 13B. That is, an exciting alternating current is supplied to the magnetostrictive films 14A and 14B having the magnetostrictive characteristic curves 51A and 51B by the common exciting coil 12, and the detecting coils 13A and 13B generate an induced voltage in response to the exciting alternating current. Since the voltage is output, the change characteristic of the induced voltage of the detection coils 13A and 13B corresponds to the magnetostriction characteristic curves 51A and 51B of the magnetostrictive films 14A and 14B. In other words, the magnetostrictive characteristic curve 51A shows the changing characteristics of the induced voltage V _A output from the sensor coil 13A, the magnetostrictive characteristic curve 51B shows the changing characteristics of the induced voltage V _B output from the detection coil 13B Yes.

According to the magnetostrictive characteristic curve 51A, the value of the induced voltage _VA output from the detection coil 13A is substantially linear as the steering torque value changes from the negative region to the positive region and further reaches the positive value T1 of the steering torque. It has a characteristic that it increases in the characteristic, reaches a peak value when the steering torque becomes a positive value T1, and gradually decreases when the steering torque further increases from T1. On the other hand, according to the magnetostrictive characteristic curve 51B, the value of the induced voltage V _B output from the detection coil 13B gradually increases until the steering torque reaches a negative value −T1, and the steering torque is negative. When the value is -T1, the peak value is obtained, and when the steering torque further increases from -T1 and changes from the negative region to the positive region, it has a characteristic of decreasing in a substantially linear characteristic.

  As shown in FIG. 3, the magnetostrictive characteristic curve 51A related to the detection coil 13A and the magnetostrictive characteristic curve 51B related to the detection coil 13B have magnetic anisotropies that are opposite to each other in the magnetostrictive films 14A and 14B. As a result, the relationship between the vertical axis and the vertical axis including the point where both magnetostrictive characteristic curves intersect is substantially symmetrical.

A line 52 shown in FIG. 3 represents a detection coil from each value of the magnetostrictive characteristic curve 51A obtained as an output voltage of the detection coil 13A in an area having a substantially linear characteristic, which is a common area of the magnetostrictive characteristic curves 51A and 51B. The graph produced based on the value which subtracted each corresponding value of the magnetostriction characteristic curve 51B obtained as an output voltage of 13B is shown. When the steering torque is zero, the induced voltages output from the detection coils 13A and 13B are equal, so the difference value is zero. The steering torque detector 20 uses the region regarded as a substantially constant gradient near the neutral point (zero point) of the steering torque in the magnetostrictive characteristic curves 51A and 51B, so that the line 52 has a substantially linear characteristic. It is formed as. Regarding the characteristic graph of the line 52, the vertical axis in FIG. 3 means the axis indicating the value of the differential voltage. A straight line 52 which is a characteristic graph is a straight line passing through the origin (0, 0), and exists on the positive and negative sides of the vertical axis and the horizontal axis. Since the detection output value of the steering torque detection unit 20 is obtained as the difference (V _A −V _B ) between the induction voltages output from the detection coils 13A and 13B as described above, based on the use of the straight line 52, The direction and magnitude of the steering torque applied to the rotating shaft 11 can be detected.

  Next, with reference to FIGS. 4-7, the whole process of the manufacturing method of the magnetostrictive torque sensor 10 is demonstrated. The manufacturing method of the magnetostrictive torque sensor 10 shown in FIG. 4 is a manufacturing process of the rotating shaft 11 of the magnetostrictive torque sensor 10.

  In FIG. 4, the manufacturing process of the rotating shaft 11 is roughly divided into a magnetostrictive film forming process P1, a magnetic anisotropy adding process P2, a characteristic stabilizing process P3, and an inspection process P4. The characteristic stabilization process P3 includes an annealing process P31, and the inspection process P4 is a process of inspecting the quality of the manufactured rotating shaft 11 by sampling inspection. In order to complete the magnetostrictive torque sensor 10, a detector attaching step for attaching detectors such as the excitation coil 12 and the detection coils 13A and 13B to the rotating shaft 11 is provided after the inspection step P4. .

  First, the magnetostrictive film forming step P1 is executed. In the magnetostrictive film forming step P1, a magnetostrictive material plated portion is formed as a base portion of the magnetostrictive film at a predetermined location on the surface of the rotating shaft 11 by electrolytic plating.

  In the magnetostrictive film forming step P1, first, pretreatment such as cleaning of the rotating shaft 11 is performed (step S11). Thereafter, electrolytic plating is performed (step S12). In this electrolytic plating step, the magnetostrictive material is applied at a location above and below the rotating shaft 11 so as to have a predetermined film thickness. The upper and lower magnetostrictive plating portions are portions that become magnetostrictive films 14A and 14B having magnetic anisotropy by post-processing described later. Thereafter, drying is performed (step S13).

  In the magnetostrictive film forming step P1, the electroplating method is used to form the above-described magnetostrictive films 14A and 14B on the surface of the rotating shaft 11. However, the basic portion for forming the magnetostrictive films 14A and 14B on the rotating shaft 11 can also be formed by a method other than the electrolytic plating method, for example, a PVD method such as a sputtering method or an ion plating method, or a plasma spraying method. .

  Next, the magnetic anisotropy adding step P2 is performed. This magnetic anisotropy adding step P2 is a step of adding the magnetic anisotropy to the two upper and lower magnetostrictive material plated portions formed on the rotating shaft 11 to form the above-described magnetostrictive films 14A and 14B. The magnetic anisotropy adding process P2 includes a step S21 for performing high-frequency heating on the upper magnetostrictive material plating portion, and a step S22 for performing high-frequency heating on the lower magnetostrictive material plating portion.

  FIG. 5 shows a flowchart of processing steps performed in steps S21 and S22 of the magnetic anisotropy adding step P2. FIG. 6 is a diagram showing the temperature distribution in the axial radial direction and the strain distribution in the axial radial direction at the magnetostrictive material plating portion of the rotating shaft 11 in steps S21 and S22 of the magnetic anisotropy adding step P2.

  As shown in FIG. 5, step S21 of applying high-frequency heating to the upper magnetostrictive material plating portion in the magnetic anisotropy adding step P2 applies a predetermined torsion torque to the rotating shaft 11 by a torque application device, as shown in FIG. A heat treatment step S202 for supplying a high-frequency current to the upper magnetostrictive material plating portion of the rotating shaft 11 in an applied state for a predetermined time and performing a heat treatment by electromagnetic induction, a step S203 for naturally cooling the heated rotating shaft 11, and finally It comprises a torque release step S204 for forming the magnetostrictive film 14A by adding magnetic anisotropy to the upper magnetostrictive material plated portion by releasing the torsional torque.

  In the heat treatment step S202, an induction heating coil is disposed around the upper magnetostrictive material plating portion of the rotary shaft 11, and a high frequency is supplied to the induction heating coil from a high frequency oscillation circuit of an induction heating power source to thereby provide upper magnetostrictive material. Only the plated part is induction heated.

  Through the above steps S201 to S204, magnetic anisotropy is added to the upper magnetostrictive material plated portion of the rotating shaft 11, thereby forming a magnetostrictive film 14A having magnetic anisotropy.

  In the high-frequency heating step S22 for the lower magnetostrictive material plated portion of the rotary shaft 11, the above steps S201 to S204 are performed in the same manner, and magnetic anisotropy is added to the lower magnetostrictive material plated portion, thereby causing magnetic anomalies. An anisotropic magnetostrictive film 14B is formed. When magnetic anisotropy is added to the lower magnetostrictive material plating portion, the direction of application of torque applied to the rotating shaft 11 is reversed so as to be opposite to the magnetic anisotropy of the magnetostrictive film 14B.

  Next, with reference to FIG. 6 and FIG. 7, the mechanism for adding the magnetic anisotropy to the magnetostrictive material plating portion in the magnetic anisotropy adding step P2 to form the magnetostrictive film 14A will be described in detail.

  In FIG. 6, regarding the temperature distribution (1) and strain distribution (2) in the radial direction of the rotating shaft 11 shown in the vertical direction, (a) torque application state, (b) induction heating state, (c) in the horizontal direction. Four states are shown: a plated portion strain release state, and (d) a torque release state. The torque application state (a) corresponds to step S201 shown in FIG. 5, the induction heating state (b) corresponds to step S202 in FIG. 5, and the plated portion strain release state (c) corresponds to step S203 in FIG. The torque release state (d) corresponds to step S204 in FIG. In FIG. 6 (1), the axis 61 indicates the temperature axis, and in (2) the axis 62 indicates the strain axis.

  In FIG. 6A, the torsion torque Tq is applied to the rotating shaft 11 to apply stress to the circumferential surface of the rotating shaft 11. Thereby, the torsion torque Tq acts. In this case, the radial strain distribution of the rotating shaft 11 is a distribution ST1 that increases from the axial center 11a located at the center of the rotating shaft 11 in the peripheral direction. However, in the distribution ST1, considering the strain distribution direction, the right and left sides of the axis 11a are opposite, so the right side strain distribution is shown on the positive side (+) and the left side strain distribution is on the negative side. (-). Furthermore, the temperature distribution in the radial direction of the rotating shaft 11 in FIG. 6A is as indicated by a broken line, and is a constant distribution T1 from the axis 11a of the rotating shaft 11 to the peripheral direction at room temperature. This room temperature becomes a reference temperature of the temperature of the rotating shaft 11.

  In FIG. 6B, the magnetostrictive material plated portion is surrounded by the induction heating coil while the torsion torque Tq is applied to the rotating shaft 11, and a high frequency current is passed through the induction heating coil to thereby generate the magnetostrictive material plated portion. Heat treatment. In FIG. 6B, the radial strain distribution of the rotating shaft 11 is the same as that in FIG. In addition, the temperature distribution in the radial direction of the rotating shaft 11 is a distribution T2 that increases rapidly from the vicinity of the outer peripheral edge of the rotating shaft 11 toward the outer peripheral edge.

  In FIG. 6C, cooling is performed. As a result, creep occurs in the magnetostrictive material plated portion, and the strain in the magnetostrictive material plated portion becomes zero. The strain distribution in the radial direction of the rotating shaft 11 at this time is indicated by reference ST2. The step showing the state of FIG. 6C is a step S203 for naturally cooling after the heat treatment. There is substantially no change in the shape of the temperature distribution T2 in the radial direction of the rotating shaft 11, and the temperature decreases as the cooling process progresses.

  In FIG. 6D, after cooling, the torsional torque Tq applied to the rotating shaft 11 is released, and the torque is released. As a result, as indicated by the strain distribution ST3, the radial strain distribution in the rotating shaft 11 becomes zero. On the other hand, as shown in the strain distribution ST3, a strain distribution is generated only in the magnetostrictive material plated portion. As a result, it is possible to add magnetic anisotropy to the magnetostrictive material plated portion by the strain distribution ST3, thereby forming the magnetostrictive film 14A having magnetic anisotropy. In FIG. 6 (d), the temperature distribution is reduced so as to be distributed gently as shown in T3.

  When forming the magnetostrictive film 14B, in order to add a magnetic anisotropy in the opposite direction compared to the magnetostrictive film 14A, a clockwise torsional torque in the direction opposite to the torsional torque Tq is applied to the process described above. Execute.

In Figure 7, the magnetostrictive films 14A and impedance characteristics Z ₀ of the magnetostrictive plating part which is provided at the upper portion and the lower portion, which is formed by adding a magnetic anisotropy in the magnetostrictive plating part of the rotating shaft 11, 14B of the impedance characteristics Z _a, it shows a _{Z B.} In FIG. 7, the horizontal axis represents torque (Nm) and the vertical axis represents impedance (Ω). Impedance characteristics Z ₀ of the magnetostrictive plating part of the stage before the magnetic anisotropy is added, by magnetic anisotropy is added, in the case of the magnetostrictive film 14A to the impedance characteristics Z _A, or magnetostrictive films changes in impedance characteristics _{Z B} in the case of 14B. Since the magnetostrictive film 14A is having impedance characteristics _{Z A,} the detection coils 13A corresponding to the magnetostrictive films 14A will have a magnetostrictive characteristic curve 51A described above. The magnetostrictive film 14B is for having an impedance _{Z B,} the sensor coil 13B corresponding to the magnetostrictive film 14B will have a magnetostrictive characteristic curve 51B described above.

In FIG. 7, a range 73 is a range in which a substantially linear change characteristic is obtained as an overlapping portion of the impedance characteristics Z _A and Z _B. This range 73 is used as the sensor use range of the magnetostrictive torque sensor 10.

  A characteristic stabilization step P3 is performed after the magnetic anisotropy addition step P2. In the characteristic stabilization process P3, an annealing process P31 is performed. In the annealing step P31, for example, the heat treatment is performed for a predetermined time at a temperature equal to or higher than the use temperature in the situation where the steering torque detector 20 is used.

  Next, the step (step S202) of high-frequency heating (induction heating) of the magnetostrictive material plating portion in the magnetic anisotropy adding step P2 will be described in detail.

  The configuration of a high-frequency heating apparatus that performs the high-frequency heating step will be described with reference to FIGS. FIG. 8 shows a side view of the main part of the induction heating coil, FIG. 9 shows the configuration of the induction heating power source, and FIG. 10 is a cross-sectional view of the main part showing the detailed shape and structure of the induction heating coil.

  In FIG. 8, the cylindrical rod-shaped rotating shaft 11 is disposed so as to be inserted through the ring portion 101 a at the tip of the induction heating coil 101. The rotating shaft 11 in FIG. 8 is the same as the rotating shaft 11 shown in FIG. The rotary shaft 11 is formed with the above-described upper magnetostrictive material plating portion 114A and lower magnetostrictive material plating portion 114B.

  The induction heating coil 101 has a ring portion 101a at its tip. The ring portion 101a forms a coil portion. The coil portion formed by the ring portion 101a is a one-turn coil portion formed by winding a plate-like object. The ring portion 101a has a predetermined width in the axial direction. In the illustrated example, the ring portion 101a is disposed so as to surround the upper magnetostrictive plating portion 114A. The width of the ring portion 101a is set to be larger than the width of the upper magnetostrictive material plating portion 114A. The induction heating coil 101 is a one-turn induction heating coil in which a sheet is formed as a whole so as to form a ring portion 101a at the tip. As shown in FIG. 9, the induction heating coil 101 includes two plate portions 101 b having the same shape and disposed in close proximity to each other through a narrow gap 102. The ring portion 101a is provided at the tip of the two plate portions 101b of the induction heating coil 101, and the two plate portions 101b are connected via the ring portion 101a.

  In FIG. 9, the rotating shaft 11 and the induction heating coil 101 are viewed from above. Each of the two plate portions 101 b of the induction heating coil 101 is connected to a one-port output terminal 104 of the induction heating power source 103. The high frequency current output from the output terminal 104 of the induction heating power source 103 which is a high frequency power source is supplied to the plate portion 101 b of the induction heating coil 101. In the induction heating coil 101, the two plate portions 101b function as high frequency current introduction terminal portions for introducing a high frequency current to the ring portion 101a.

On the input side of the induction heating power supply 121, a three-phase transformer 123 that transforms the three-phase AC 122 and a three-phase rectifier 124 that rectifies the three-phase AC output from the three-phase transformer 123 are provided. The direct current output from the three-phase rectifier 124 is input to the induction heating power supply 121 as input power. A high frequency oscillation circuit 125 is provided in the induction heating power supply 121. The high-frequency oscillation circuit 125 is an oscillation circuit that includes an oscillation triode vacuum tube and an LC circuit. The direct current supplied to the induction heating power supply 121 is supplied to the anode of the triode vacuum tube of the high-frequency oscillation circuit 125. The high frequency oscillating circuit 125 generates an oscillating action and outputs a high frequency current (I _H ) having a required frequency with the supplied direct current as an input. The high frequency current is supplied to the output terminal 104.

  The shape and structure of the ring portion (one-turn coil portion) 101a of the induction heating coil 101 will be described with reference to FIG. FIG. 10 shows an arrangement state when the upper magnetostrictive material plating portion 114 </ b> A of the cylindrical rod-shaped rotating shaft 11 is heated by the induction heating coil 101.

  In the arrangement state shown in FIG. 10, the axial width a of the ring portion 101 a is set to be longer than the axial width d of the upper magnetostrictive material plating portion 114 </ b> A of the rotating shaft 11. The upper end portion of the ring portion 101a is above the upper end portion of the upper magnetostrictive material plating portion 114A, and the lower end portion of the ring portion 101a is below the lower end portion of the upper magnetostrictive material plating portion 114A. Projections 131 are formed on the inner peripheral surfaces of the upper opening and the lower opening of the ring portion 101a over the entire circumference. The axial width of the protrusion 131 is c. In the ring portion 101a, the axial dimension of the portion excluding the width of the protruding portion 131 at both side openings is b. The axial dimension b is preferably larger than the axial width d of the upper magnetostrictive material plating portion 114A. Accordingly, the protrusions 131 formed at the opening portions at both the upper and lower ends of the ring portion 101a are arranged so as to be positioned outside the upper magnetostrictive material plating portion 114A in the axial direction as described above. Further, the inner diameter f of the protrusion 131 is smaller than the inner diameter e of the central portion in the axial direction of the ring portion 101a. The protrusion 131 formed on the inner peripheral surface of the ring portion 101a on the entire circumference of the inner peripheral portion of the opening at both ends forms a small inner diameter portion on the inner peripheral surface.

  Furthermore, with reference to FIGS. 11-14, the characteristic shape of the said induction heating coil and its effect are demonstrated. 11 shows a plan view of the induction heating coil 101, FIG. 12 shows a sectional view taken along line C1-C1 in FIG. 11, FIG. 13 shows a sectional view taken along line C2-C2 in FIG. 11, and FIG. The temperature distribution in the circumferential direction of the winding coil portion and the temperature center of the coil are shown.

  As shown in FIG. 11, the induction heating coil 101 includes the two plate portions 101 b and the cylindrical ring portion (one-turn coil portion) 101 a as described above, and is made based on one plate-like object as a whole. It has been. The two plate portions 101b have a gap 102 interposed therebetween. In the induction heating coil 101, the plate portion 101b is connected to the output terminal 104 of the induction heating power source 121, and introduces a high-frequency current supplied from the output terminal 104 into the ring portion 101a. The high-frequency current introduced from one plate portion 101b flows through the ring portion 101a in the circumferential direction and further flows to the other plate portion 101b. The two plate portions 101b are portions for introducing a high-frequency current to the ring portion 101a that performs induction heating. Accordingly, in the ring portion 101a, the portion D of the plate portion 101b in the circumferential direction serves as a terminal portion for introducing a high-frequency current.

  In the above, the thickness of the plate portion 101b is, for example, 4 mm, and the width of the gap 102 is, for example, 1 mm. A plane is defined by a gap 102 formed between the two plate portions 101b. The plane defined by the gap 102 matches the cross-sectional line of the C1-C1 line cross section in FIG.

  Next, a linear groove 141 parallel to the axial direction is formed on the inner peripheral surface of the ring portion 101a. The groove 141 is included in the plane defined by the gap 102 and is formed so as to face the gap 102. The depth direction of the groove 141 is a plane direction defined by the gap 102. In other words, the linear groove 141 is formed at the center symmetrical position of the high-frequency current introducing terminal portion of the ring portion (one-turn coil portion) 101 a of the induction heating coil 101. The width of the groove 141 is preferably 1 mm, and the depth is preferably 1.5 mm. Further, the groove 141 is preferably formed from the upper opening to the lower opening of the ring portion 101a. The number, location, and shape of the grooves 141 are not limited to those shown in FIG. For example, a plurality of slits may be used.

  Next, by using the induction heating coil 101 provided with the ring portion 101a, the upper magnetostrictive material plating portion 114A of the rotating shaft 11 and the like are subjected to high-frequency heating, thereby producing the following effects.

  Since the linear groove 141 is formed at the center symmetrical position of the high-frequency current introduction terminal portion on the inner peripheral surface of the ring portion (one-turn coil portion) 101a of the induction heating coil 101, that is, as shown in FIG. Since the linear groove 141 is formed at a position on the extended line of the gap 102 between the plate portions 101b, the heating distribution (temperature distribution) in the circumferential direction of electromagnetic induction heating in the upper magnetostrictive material plating portion 114A is changed. It can be made uniform without causing bias. This will be described with reference to FIG.

  In FIG. 14, the characteristic comparison of the induction heating coil 101 which concerns on this embodiment, and the conventional coil is shown. FIG. 14 shows an induction heating coil 101 having the coil portion 101a (hereinafter referred to as “coil 101”) and a conventional induction heating coil having a coil portion in which the groove 141 is not formed (hereinafter referred to as “conventional coil”). The graph for comparing the temperature distribution of the circumferential direction is shown. The shape and dimensions of the coil 101 and the conventional coil are the same, and are the same except for the presence or absence of the groove 141. In FIG. 14, the horizontal axis indicates the distance (mm) from the geometric center (0.0) of the coil, and the vertical axis indicates the temperature (° C.). As shown in FIG. 11, the horizontal axis is defined by a point P1 representing the position of the high-frequency current introduction terminal portion, a point P2 representing the position of the groove 141, and points P1 and P2 in the coil portion 101a. With respect to the coil center point P3 on the diameter, the geometric center of the coil means the coil center point P3. In the case of a conventional coil, the geometric center of the coil is the same as the geometric center of the coil 101.

  In the comparison between the coil 101 based on FIG. 14 and the conventional coil, the conclusion will be described first. In the case of the conventional coil, the coil temperature center O2 is deviated from the geometric center of the coil. The coil temperature center O1 coincides with the geometric center of the coil. As a result, in the case of the conventional coil, when the rotary shaft is installed in the coil in the induction heating process, the rotary shaft is offset to the high-frequency current introduction terminal portion side from the geometric center of the coil. On the other hand, when the coil 101 is used, the geometric center of the coil coincides with the coil temperature center, so that position adjustment is not required, and the position adjustment process is greatly simplified.

  The coil temperature center O1 of the coil 101 is determined as an intersection of the circumferential temperature distribution characteristic N1 on the high frequency current introduction terminal portion side of the coil 101 and the circumferential temperature distribution characteristic N2 on the groove side. The coil temperature center O2 of the conventional coil is determined as an intersection of the circumferential temperature distribution characteristic M1 on the high frequency current introduction terminal portion side of the conventional coil and the circumferential temperature distribution characteristic M2 on the groove side. As is apparent from the circumferential temperature distribution characteristics N1, N2, M1, and M2, the circumferential temperature distribution characteristics N1 and N2 of the coil 101 substantially coincide with the geometric center of the coil.

  As described above, in the induction heating coil 101 according to the present embodiment, since the groove 141 having a predetermined shape is formed at a predetermined position on the inner peripheral surface of the coil portion 101a, the temperature distribution in the circumferential direction due to the coil heating is improved. It is possible to make the coil geometric center coincide with the coil temperature center.

  The configurations, shapes, sizes, and arrangement relationships described in the above embodiments are merely shown to the extent that the present invention can be understood and implemented, and the numerical values and the compositions (materials) of the respective configurations are as follows. It is only an example. Therefore, the present invention is not limited to the described embodiments, and can be variously modified without departing from the scope of the technical idea shown in the claims.

  The present invention is used as an induction heating coil of a high-frequency heating device used in a process of manufacturing a magnetostrictive torque sensor that detects steering torque with an electric power steering device or the like.

It is a partial cross section side view which shows the basic structure of the magnetostrictive torque sensor in which this invention is utilized. It is a side view which shows notionally the basic composition of a magnetostriction type torque sensor. It is a graph which shows the magnetostriction characteristic curve and sensor detection characteristic regarding each detection coil in a magnetostriction type torque sensor. It is a manufacturing method of a magnetostrictive torque sensor, and is a process diagram showing a manufacturing process of a rotating shaft. It is a flowchart of a magnetic anisotropy addition process. It is a figure which shows temperature distribution (1) and distortion distribution (2) of the radial direction in the rotating shaft in each step (a)-(d) of a magnetic anisotropy addition process. It is a figure which shows the impedance characteristic of the magnetostriction type torque sensor using the magnetostriction film | membrane after the magnetostriction type torque sensor after the magnetostriction type torque sensor manufacturing method in the manufacturing method of a magnetostriction type torque sensor formation part and magnetic anisotropy addition. It is a principal part side view of an induction heating coil. It is a block diagram which shows the structure of an induction heating power supply. It is principal part sectional drawing which shows the characteristic shape of the ring part (one-turn coil part) of an induction heating coil. It is a top view which shows the actual shape of the induction heating coil which concerns on this embodiment. It is the C1-C1 sectional view taken on the line in FIG. It is the C2-C2 sectional view taken on the line in FIG. It is a graph which shows the temperature distribution of the circumferential direction in the ring part (one-turn coil part) of the induction heating coil which concerns on this invention, and the coil part of the conventional induction heating coil, and the temperature center of a coil.

Explanation of symbols

DESCRIPTION OF SYMBOLS 10 Magnetostrictive torque sensor 11 Rotating shaft 12 Excitation coil 13A, 13B Detection coil 14A, 14B Magnetostrictive film 51A, 51B Magnetostrictive characteristic curve (impedance characteristic curve)
101 Induction heating coil 101a Ring part (one-turn coil part)
121 Induction heating power supply 125 High frequency oscillation circuit 131 Projection (inner diameter small diameter part)
141 Linear groove P1 Magnetic film formation process P2 Magnetic anisotropy addition process P3 Characteristic stabilization process

Claims (4)

The magnetostrictive film is magnetically anisotropic by releasing the torsional torque of the rotating shaft after high-frequency heating of the magnetostrictive film formed on the circumferential surface of the cylindrical rod-shaped rotating shaft of the magnetostrictive torque sensor to which the torsional torque is applied. In the magnetic anisotropy adding step of the magnetostrictive torque sensor to be added, an induction heating coil for heating the magnetostrictive film at a high frequency,
This induction heating coil has a one-turn coil portion arranged so as to surround the magnetostrictive film,
The one-turn coil portion has two plate-shaped high-frequency current introduction terminal portions arranged to face each other with a cylindrical shape and a gap, and is at least parallel to the axial direction on the inner peripheral surface of the one-turn coil portion. One linear groove is formed on the inner peripheral surface in a positional relationship included in a plane formed by the gap,
The axial dimension of the one-turn coil part is larger than the axial width of the magnetostrictive film of the cylindrical rod-shaped rotary shaft , and a protrusion is formed on the inner peripheral surface of the upper opening and the lower opening over the entire circumference .
The protrusions induction heating coil, wherein that you have been arranged so as to be positioned on the outside in the axial direction with respect to the magnetostrictive film. The induction used in the magnetic anisotropy adding step in the method of manufacturing a magnetostrictive torque sensor according to claim 1, wherein the linear groove is formed from an opening at one end to an opening at the other end. Heating coil. The one-turn coil portion has two plate-shaped high-frequency current introduction terminal portions arranged to face each other with a gap therebetween, and the linear groove is positioned in a positional relationship included in a plane formed by the gap. The induction heating coil used in the magnetic anisotropy adding step in the method of manufacturing a magnetostrictive torque sensor according to claim 1 or 2, wherein the induction heating coil is formed on a peripheral surface. The induction heating coil according to any one of claims 1 to 3 ,
A high frequency power source for supplying a high frequency to the induction heating coil;
A high-frequency heating device comprising:

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