JP4219826B2 - Rotation angle detector - Google Patents

Description

  The present invention relates to a rotation angle detection device that detects a rotation angle of a rotation shaft.

FIG. 11A shows an axial sectional view of the rotation angle detecting device, and FIG. 11B shows a top view thereof. As shown in the figure, the rotation angle detection device 100 includes a magnet 101, a yoke 102, and a Hall IC 103. The magnet 101 is mounted on the rotating shaft 104. The magnet 101 can rotate together with the rotating shaft 104. The yoke 102 is fixed to the inner peripheral surface of the housing (not shown). The yoke 102 and the magnet 101 are arranged coaxially. In the yoke 102, a pair of gaps 102a and 102b are disposed. The Hall IC 103 is disposed in the gap 102a. When the magnet 101 rotates together with the rotating shaft 104, the magnetic flux density in the gaps 102a and 102b changes. The Hall IC 103 outputs a voltage corresponding to the magnetic flux density. The rotation angle of the rotating shaft 104 is detected from this voltage.
Japanese Patent No. 2842482

  However, conventionally, the output of the Hall IC 103 differs depending on the rotation direction of the rotating shaft 104. In other words, hysteresis has occurred in the output of the Hall IC 103.

  FIG. 12 shows a change in magnetic flux density inside the yoke when the rotating shaft, that is, the magnet is reciprocally rotated within a range of ± 50 deg. For convenience of explanation, the angle of the magnet is expressed as “deg” and the angle of the yoke is expressed as “°”. In FIG. 12, the horizontal axis magnet rotation angle indicates an angle when the magnet 101 is reciprocally rotated with the position of the Hall IC 103 set to 0 deg, as shown in FIG. 11B. In FIG. 11B, the counterclockwise direction is the positive direction and the clockwise direction is the negative direction. In FIG. 12, solid line data indicates data when the magnet 101 is rotated in the plus direction. The dotted line data indicates data when the magnet 101 is rotated in the minus direction. As shown in FIG. 11 (b), the position of the Hall IC 103 is 0 °, and the yoke 102 circumferential direction is at 45 ° positions (that is, θ = 0 °, 45 °, 90 °, 135 °, 180 °, 225 °). 270 °, 315 °). In FIG. 12, regarding the direction of the magnetic flux density on the vertical axis, the clockwise direction is the positive direction and the counterclockwise direction is the negative direction on the paper surface of FIG.

  As an example, the magnetic flux density change at the position of θ = 0 ° in the yoke 102 will be described. When the magnet 101 is rotated from 0 deg to +50 deg, the magnetic flux density (solid line data) at the position of θ = 0 ° of the yoke 102 gradually increases as shown by the white arrow in FIG. The magnetic flux density is maximum at +50 deg.

  Subsequently, when the magnet 101 is restored and rotated from +50 deg to 0 deg, the magnetic flux density (dotted line data) at the position of θ = 0 ° of the yoke 102 gradually decreases as indicated by the white arrow in FIG. The magnetic flux density is minimum at 0 deg.

  However, even if the magnet 101 is restored and rotated, the magnetic flux density is not restored to the original state. That is, the magnetic flux density is increased by the arrow Y0. Similarly, at the position θ = 45 °, the magnetic flux density is increased by the arrow Y45. In addition, the magnetic flux density is increased by the amount of the arrow Y315 at the position θ = 315 °. On the other hand, at the positions θ = 135 °, 180 °, and 225 °, the magnetic flux densities are respectively reduced by the arrows Y135, Y180, and Y225. Note that the magnetic flux density does not change at the positions of θ = 90 ° and 270 °.

  FIG. 13 shows changes in the magnetic flux density at each angular position of these yokes. As shown in the figure, arrows Y45, Y0, and Y315 are directed in the plus direction, and Y135, Y180, and Y225 are directed in the minus direction. Changes in the magnetic flux density at each angular position of these yokes 102 affect each other magnetically. As a result, the magnetic flux density at the 0 ° position where the Hall IC 103 is disposed is in the positive direction. That is, the magnetic flux density at the 0 ° position increases when the magnet 101 is rotated forward / reversely from 0 deg → + 50 deg → 0 deg again. This means that even when the magnet 101 is at the same 0 deg position, the output of the Hall IC 103 during reverse rotation is larger than the output of the Hall IC 103 during forward rotation. That is, it means that hysteresis is generated in the output of the Hall IC 103.

  In order to suppress the occurrence of hysteresis, Patent Document 1 introduces the use of a material having a small hysteresis such as permalloy as the material of the yoke. However, materials with small hysteresis such as permalloy are generally expensive. Further, even if a material having a small hysteresis is used, it is difficult to completely eliminate the hysteresis.

  The rotation angle detection device of the present invention has been completed in view of the above problems. Accordingly, an object of the present invention is to provide a rotation angle detection device that can suppress the occurrence of hysteresis in the output of a magnetic detector regardless of the material of the yoke.

  (1) In order to solve the above-mentioned problem, a rotation angle detection device of the present invention is arranged in a magnetic field of a ring-shaped magnetism generating member connected to a rotating shaft to form a magnetic field, and the magnetism generating member. A ring-shaped yoke having a pair of gaps arranged so as to change the magnetic flux density when a relative angle with respect to the magnetism generating member is changed by rotation of the rotating shaft, and a magnetic circuit is formed between the pair of members A rotation angle detector that is disposed in one of the gaps and that detects the magnetic flux density, and when the rotation angle of the magnetism generating member is 0 degree, the magnetic flux density of the yoke The maximum density portion in the distribution is unevenly distributed on the region side of more than 270 degrees and less than 90 degrees with the magnetic detector position being 0 degrees.

In FIG. 13, the magnetic flux density distribution of the conventional yoke is shown by hatching. Note that the smaller the hatch pitch, the higher the magnetic flux density. As shown in the figure, when the magnet 101 is at the 0 deg position, the position of the magnetic detector (Hall IC 103 in FIG. 13) is 0 °, and the magnetic flux density distribution is relative to a straight line L connecting the 270 ° position and the 90 ° position. Is symmetrical. In other words, the arrangement of the maximum density portion B _max in the magnetic flux density distribution is symmetric with respect to the straight line L.

On the other hand, in the rotation angle detection device of the present invention, the arrangement of the maximum density portion B _max is closer to the magnetic detector side than the straight line L. That is, the density maximum portion B _max is unevenly distributed on the region side exceeding 270 ° and less than 90 ° with the magnetic detector position being 0 °.

  According to the rotation angle detection device of the present invention, it is possible to increase the magnetic flux density in the opposite direction with respect to the direction of the magnetic flux density in the gap where the magnetic detector is disposed (the positive direction in FIG. 13). For this reason, the hysteresis which generate | occur | produces in a magnetic detector can be suppressed. Further, it is not necessary to use an expensive permalloy or the like as a material for the yoke (which may of course be used). For this reason, hysteresis can be suppressed regardless of the material of the yoke.

  Further, by adjusting the amount of increase in the reverse magnetic flux density, the hysteresis can be finally reduced to zero. In this case, the magnetic detector can transmit the same output value regardless of the rotation direction of the rotating shaft.

  (2) Preferably, the magnetism generating member is a magnet, and the yoke is arranged on the outer peripheral side of the magnet. That is, this configuration uses the present invention for a rotation angle detection device (see FIG. 11) of a type in which a magnet is disposed on the inner peripheral side and a yoke is disposed on the outer peripheral side.

  (3) Preferably, in the configuration of (2), the magnet has a concentric ring shape, the yoke has a concentric ring shape, and the central axis of the magnet is relative to the central axis of the yoke Thus, it is better to have a configuration that is eccentric in the direction of the magnetic detector. That is, this configuration shifts the central axis of the magnet in the direction of the magnetic detector. According to this configuration, the hysteresis of the magnetic detector can be suppressed only by changing the relative position between the magnet and the yoke of the conventional magnetic detector.

  (4) Preferably, in the configuration of the above (2), the magnet has an eccentric ring shape, the yoke has a concentric ring shape, and the inner peripheral surface central axis of the magnet and the central axis of the yoke Is arranged coaxially, and when the rotation angle of the magnet is 0 degree, the outer peripheral surface central axis is decentered in the direction of the magnetic detector with respect to the central axis of the yoke Is good. According to this structure, the hysteresis of a magnetic detector can be suppressed by making the shape of a magnet into an eccentric ring shape.

  (5) Preferably, in the configuration of (2), the magnet has a concentric ring shape, the yoke has an eccentric ring shape, and the central axis of the magnet and the central axis of the inner peripheral surface of the yoke It is preferable that the central axis of the outer peripheral surface of the yoke is eccentric in the direction of the magnetic detector with respect to the central axis of the magnet. According to this configuration, the hysteresis of the magnetic detector can be suppressed by making the shape of the yoke an eccentric ring. Further, since the magnet has a concentric ring shape as compared with the configuration (4), it is easy to balance the rotation of the rotation shaft.

  (6) Preferably, in the configuration of (2) above, the magnet has a concentric ring shape, the yoke has a concentric ring shape, and the central axis of the magnet and the central axis of the yoke are coaxial. It is preferable that the thickness of the yoke in the axial direction is uneven in the direction of the magnetic detector. According to this configuration, the hysteresis of the magnetic detector is suppressed by increasing the axial thickness of the yoke from the gap where the magnetic detector is not arranged toward the gap where the magnetic detector is arranged. Can do.

  (7) Preferably, the magnetism generating member includes a ring-shaped magnetism generation side yoke having a pair of magnetism generation side gaps and a pair of the magnetism generation side gaps so that the directions of the magnetic poles are opposite to each other in the circumferential direction. It is preferable that the yoke is arranged on the inner peripheral side of the magnetism generating member. That is, this configuration uses the present invention for a rotation angle detection device of a type in which a yoke is disposed on the inner peripheral side and a magnetism generating member is disposed on the outer peripheral side.

  (8) Preferably, in the configuration of (7), the magnetism generating member has a concentric ring shape, the yoke has a concentric ring shape, and a central axis of the magnetism generating member is It is preferable that the center axis is decentered in a direction opposite to the magnetic detector direction. That is, in this configuration, the central axis of the magnetism generating member is shifted in the direction opposite to the magnetic detector direction. According to this configuration, the hysteresis of the magnetic detector can be suppressed relatively easily.

  (9) Preferably, in the configuration of (7), the magnetism generating member has a concentric ring shape, the yoke has a concentric ring shape, and the center axis of the magnetism generating member and the center of the yoke When the rotation angle of the magnetism generating member is 0 degree, the magnetism generation side gap of the magnetism generation side yoke is 270 degrees with the position of the magnetic detector as 0 degree. It is better to have a configuration in which it is arranged in an area exceeding 90 degrees. According to this configuration, the hysteresis of the magnetic detector can be suppressed by arranging the magnetic generation side gap, that is, the magnet, in the region of more than 270 degrees and less than 90 degrees with the magnetic detector position being 0 degrees.

  According to the present invention, it is possible to provide a rotation angle detection device that can suppress the occurrence of hysteresis in the output of the magnetic detector regardless of the material of the yoke.

  Hereinafter, an embodiment in which the rotation angle detection device of the present invention is used for detection of an operation amount of an accelerator pedal will be described.

<First embodiment>
First, the configuration of the rotation angle detection device of the present embodiment will be described. FIG. 1A shows an axial sectional view of the rotation angle detection device of the present embodiment, and FIG. As shown in the figure, the rotation angle detection device 1 includes a magnet 2, a yoke 3, and a Hall IC 4. The Hall IC 4 is included in the magnetic detector of the present invention.

  The magnet 2 is made of ferrite and has a concentric ring shape. The magnet 2 is fixed to the rotating shaft 5 made of SUS304. The rotating shaft 5 rotates forward / reversely within a predetermined angle range in response to depression of an accelerator pedal (not shown) and return. Therefore, the magnet 2 also rotates forward / reversely with the rotary shaft 5.

The yoke 3 is formed by arranging a pair of half-ring members 30a and 30b to face each other. A pair of gaps 31 and 32 are disposed between the half ring-shaped members 30a and 30b so as to be separated from each other by 180 °. The yoke 3 is made of DSUS13A (heat-treated) and has a concentric ring shape as a whole. The yoke 3 is fixed to the inner peripheral surface of the housing (not shown). The yoke 3 is disposed on the outer peripheral side of the magnet 2. The yoke 3 is disposed in the magnetic field of the magnet 2. A magnetic circuit is formed between the yoke 3 and the magnet 2. The central axis A _M of the magnet 2 is eccentric in the direction of the gap 31 with respect to the central axis A _Y of the yoke 3.

  The Hall IC 4 is disposed only in the gap 31 of the pair of gaps 31 and 32. The Hall IC 4 includes a Hall element and an operational amplifier (not shown). The magnetic flux density is magnetoelectrically converted into a voltage by the Hall IC 4.

  Next, the movement of the rotation angle detection device of this embodiment will be described. When the rotation shaft 5 is rotated by the accelerator pedal operation, the magnet 2 fixed to the rotation shaft 5 is also rotated. For this reason, the magnetic flux density in the gaps 31 and 32 changes. The magnetic flux density is converted into a voltage by the Hall element of the Hall IC 4. The converted voltage is amplified by an operational amplifier. Based on the amplified voltage, the rotation angle of the rotating shaft 5, that is, the depression amount of the accelerator pedal is detected.

  Next, hysteresis in the Hall IC of the rotation angle detection device of the present embodiment will be described. FIG. 2 shows a change in magnetic flux density inside the yoke when the rotating shaft, that is, the magnet is reciprocally rotated within a range of ± 50 deg. FIG. 2 corresponds to FIG. For convenience of explanation, the angle of the magnet is expressed as “deg” and the angle of the yoke is expressed as “°”. In FIG. 2, the horizontal axis magnet rotation angle indicates an angle when the magnet 2 is reciprocally rotated with the position of the Hall IC 4 as 0 deg as shown in FIG. In FIG. 1B, the counterclockwise direction is the positive direction and the clockwise direction is the negative direction. In FIG. 2, solid line data indicates data when the magnet 2 is rotated in the plus direction. The dotted line data indicates data when the magnet 2 is rotated in the minus direction. As shown in FIG. 1 (b), the Hall IC 4 position is 0 °, and the yoke 3 circumferential direction is 45 ° position (that is, θ = 0 °, 45 °, 90 °, 135 °, 180 °, 225 °). 270 °, 315 °). In FIG. 2, regarding the direction of the magnetic flux density on the vertical axis, the clockwise direction is the plus direction and the counterclockwise direction is the minus direction on the paper surface of FIG.

  As an example, the magnetic flux density change at the position of θ = 0 ° in the yoke 3 will be described. When the magnet 2 is rotated from 0 deg to +50 deg, the magnetic flux density (solid line data) at the position of θ = 0 ° of the yoke 3 gradually increases as indicated by the white arrow in FIG. Subsequently, when the magnet 2 is restored and rotated from +50 deg to 0 deg, the magnetic flux density (dotted line data) at the position of θ = 0 ° of the yoke 3 gradually decreases as indicated by the white arrow in FIG.

  However, even if the magnet 2 is restored and rotated, the magnetic flux density is not restored to the original state. That is, the magnetic flux density is increased by the arrow y0. Similarly, at the position θ = 45 °, the magnetic flux density is increased by the arrow y45. In addition, at the position θ = 315 °, the magnetic flux density is increased by the amount of the arrow y315. On the other hand, at θ = 90 °, 135 °, 180 °, 225 °, and 270 °, the magnetic flux density is decreased by the amounts of arrows y90, y135, y180, y225, and y270, respectively.

  In FIG. 12, the magnetic flux density did not change at the positions of θ = 90 ° and 270 °. On the other hand, in FIG. 2, as described above, the magnetic flux density is decreased by y90 at the position θ = 90 °. In addition, the magnetic flux density is reduced by y270 at the position θ = 270 °.

  FIG. 3 shows changes in magnetic flux density at each angular position of the yoke. FIG. 3 corresponds to FIG. As shown in the figure, arrows y45, y0, and y315 are directed in the positive direction, and y90, y135, y180, y225, and y270 are directed in the negative direction. Changes in the magnetic flux density at each angular position of these yokes 3 affect each other magnetically. As a result, the magnetic flux density at the 0 ° position where the Hall IC 4 is arranged is in the plus direction, as in FIG.

  However, in FIG. 3, y90 and y270 are generated in the negative direction. Further, assuming that the magnetic flux density change before and after rotation at an arbitrary angular position θ in FIG. 3 is Bhybθ, and the magnetic flux density change before and after rotation at an arbitrary angular position θ in FIG. That is, the amount of hysteresis of the magnetic flux density changes in the negative direction.

  For this reason, the magnetic flux density in the minus direction of the gap 32 becomes larger than that in the case of FIG. On the other hand, the magnetic flux density in the positive direction of the gap 31 in which the Hall IC 4 is disposed becomes smaller by y90 and y270 that are directed in the negative direction.

Next, the function and effect of the rotation angle detection device of this embodiment will be described. FIG. 3 shows the magnetic flux density distribution of the yoke by hatching. Note that the smaller the hatch pitch, the higher the magnetic flux density. As shown in FIG. 1, the central axis A _M of the magnet 2 is eccentric in the direction of the gap 31 with respect to the central axis A _Y of the yoke 3. For this reason, when the rotation angle of the magnet 2 is 0 deg, the maximum density portion B _max of the magnetic flux density is unevenly distributed on the region side exceeding 270 ° and less than 90 ° with the position of the Hall IC 4 being 0 °. Due to this uneven distribution, negative magnetic flux densities y90 and y270 are generated at the θ = 90 ° position and the 270 ° position. For this reason, the positive direction magnetic flux density generated in the gap 31 can be offset. Therefore, according to the rotation angle detection device 1 of the present embodiment, hysteresis generated in the Hall IC 4 can be suppressed. Further, by adjusting the amount of eccentricity of the central axis A _M of the magnet 2 with respect to the central axis A _Y of the yoke 3, the hysteresis can be finally reduced to zero. In this way, the same output value can be transmitted regardless of the rotation direction of the rotating shaft 5. The relationship between the amount of eccentricity and hysteresis will be described in detail later.

  Further, the rotation angle detection device 1 of the present embodiment is completed only by shifting the central axis of the magnet 101 in the direction of the Hall IC 103 in the conventional rotation angle detection device 100 of FIG. For this reason, manufacturing cost can be reduced.

  Further, the yoke 3 of the rotation angle detection device 1 of the present embodiment is made of DSUS13A (heat treated). For this reason, compared with the case where expensive permalloy etc. are used, manufacturing cost can be reduced.

<Second embodiment>
The difference between the present embodiment and the first embodiment is that the magnet has an eccentric ring shape. Therefore, only the differences will be described here. FIG. 4A shows an axial sectional view of the rotation angle detection device of the present embodiment, and FIG. 4B shows a top view. In addition, about the site | part corresponding to FIG. 1, it shows with the same code | symbol.

As shown in the figure, the magnet 2 has an eccentric ring shape. That is, the inner peripheral surface central axis A1 _M and the outer peripheral surface central axis A2 _M of the magnet 2, are offset by a predetermined distance. Further, the central axis A _Y of the inner peripheral surface central axis A1 _M and the yoke 3, are arranged coaxially. Therefore, when the rotational angle of the magnet 2 is 0 deg, the outer peripheral surface central axis A2 _M, with respect to the central axis A _Y of the yoke 3 (inner peripheral surface central axis A1 _M), it is eccentric to the hole IC4 direction. The rotation angle detection device 1 of the present embodiment has the same effects as the rotation angle detection device of the first embodiment.

<Third embodiment>
The difference between the present embodiment and the first embodiment is that the yoke has an eccentric ring shape. Therefore, only the differences will be described here. FIG. 5A shows an axial sectional view of the rotation angle detection device of the present embodiment, and FIG. 5B shows a top view. In addition, about the site | part corresponding to FIG. 1, it shows with the same code | symbol.

As shown in the figure, the yoke 3 has an eccentric ring shape. That is, the inner peripheral surface central axis A1 _Y and the outer peripheral surface central axis A2 _{Y of} the yoke 3 are shifted by a predetermined distance. Further, the center axis A _M of the inner peripheral surface central axis A1 _Y and the magnet 2 is disposed on the same axis. For this reason, the outer peripheral surface central axis A2 _Y is eccentric in the Hall IC 4 direction with respect to the central axis A _M (inner peripheral surface central axis A1 _Y ) of the magnet 2. The rotation angle detection device 1 of the present embodiment has the same effects as the rotation angle detection device of the first embodiment.

<Fourth embodiment>
The difference between this embodiment and the first embodiment is that the axial thickness of the yoke is not constant. Therefore, only the differences will be described here. FIG. 6A shows a side view of the rotation angle detection device of the present embodiment, and FIG. 6B shows a top view thereof. In addition, about the site | part corresponding to FIG. 1, it shows with the same code | symbol.

As shown in the figure, the central axis A _M of the magnet 2 and the central axis A _{Y of} the yoke 3 are arranged coaxially, and the axial thickness of the yoke 3 is not constant. That is, the axial thickness L32 of the portion corresponding to the gap 32 is set to be the smallest, and the axial thickness L31 of the portion corresponding to the gap 31 is set to be the largest. That is, the axial thickness is uneven toward the Hall IC 4. The rotation angle detection device 1 of the present embodiment has the same effects as the rotation angle detection device of the first embodiment.

<Fifth embodiment>
The difference between the present embodiment and the first embodiment is that the internal / external relationship between the magnetism generating member (the magnet in the first embodiment) and the yoke is opposite. Therefore, only the differences will be described here. FIG. 7A shows an axial sectional view of the rotation angle detection device of the present embodiment, and FIG. 7B shows a top view thereof. In addition, about the site | part corresponding to FIG. 1, it shows with the same code | symbol.

As shown in the figure, the magnetic generation member 6 includes a magnetic generation side yoke 60 and a pair of magnets 7a and 7b. The magnetism generating member 6 is connected to a rotating shaft (not shown). The magnetic generation side yoke 60 includes a pair of magnetic generation side half ring-shaped members 60a and 60b. The pair of magnetic generation side half ring-shaped members 60a and 60b oppose each other with a predetermined magnetic generation side gap 61 and 62 therebetween. The magnetic generation side yoke 60 is made of DSUS13A (heat treated). The magnet 7 a is disposed in the magnetism generation side gap 61. The magnet 7 b is disposed in the magnetism generation side gap 62. Magnets 7a and 7b are both made of ferrite. The magnetism generating member 6 has a concentric ring shape as a whole. The yoke 3 and the Hall IC 4 are disposed on the inner peripheral side of the magnetism generating member 6. The central axis A ′ _M of the magnetism generating member 6 is eccentric in the direction opposite to the Hall IC 4 with respect to the central axis A _Y of the yoke 3. The rotation angle detection device 1 of the present embodiment has the same effects as the rotation angle detection device of the first embodiment.

<Sixth embodiment>
The difference between the present embodiment and the fifth embodiment is that the magnetism generating member and the yoke are arranged coaxially. Further, the magnet of the magnetism generating member is biased toward the Hall IC side. Therefore, only the differences will be described here. FIG. 8A shows an axial sectional view of the rotation angle detection device of the present embodiment, and FIG. 8B shows a top view. In addition, about the site | part corresponding to FIG. 7, it shows with the same code | symbol.

As shown in the figure, the central axis A ′ _M of the magnetic generating member 6 and the central axis A _{Y of the} yoke 3 are arranged coaxially. Both the magnetic generation side gaps 61 and 62 are disposed in a region of more than 270 ° and less than 90 ° with the position of the Hall IC 4 being 0 °. Therefore, the magnets 7a and 7b are also arranged in the region. The rotation angle detection device 1 of the present embodiment has the same effects as the rotation angle detection device of the first embodiment.

<Others>
The embodiment of the rotation angle detection device of the present invention has been described above. However, the embodiment is not particularly limited to the above embodiment. Various modifications and improvements that can be made by those skilled in the art are also possible.

  For example, although the magnet 2 is made of ferrite in the first to fourth embodiments and the magnets 7a and 7b are made of ferrite in the fifth and sixth embodiments, they may be made of other hard magnetic materials. Further, in the first to fourth embodiments, the yoke 3 is made of DSUS13A (heat-treated), and in the fifth and sixth embodiments, the yoke 3 and the magnetic generation side yoke 60 are both made of DSUS13A (heat treated). It may be made. In the first to fourth embodiments, a combination of the magnet 2 and a soft magnetic auxiliary yoke may be used as the magnetism generating member.

  In the above embodiment, the Hall IC is used as the magnetic detector. However, for example, a magnetic detector having a magnetoresistive element whose resistance value changes according to the strength of the magnetic field may be used.

  Hereinafter, an experiment performed on the relationship between the amount of eccentricity and hysteresis will be described. This experiment was performed on the rotation angle detection device of the first embodiment. FIG. 9 shows the dimensions of the rotation angle detection device used in this experiment. In addition, about the site | part corresponding to FIG. 1, it shows with the same code | symbol.

As shown in the figure, the diameter D1 of the rotating shaft 5 is 4 mm, the outer diameter D2 of the magnet 2 is 10 mm, the thickness L1 of the magnet 2 is 6 mm, the inner diameter D3 of the yoke 3 is 13 mm, the outer diameter D4 of the yoke 3 is 16 mm, The thickness L2 of the yoke 3 was set to 5 mm, and the gap G between the gaps 31 and 32 was set to 1.5 mm. The distance between the central axis A _Y of the yoke 3 and the central axis A _M of the magnet 2, that is, the eccentricity A is set to 0 mm, 0.5 mm, and 1.0 mm, and the magnet 2 is ± 50 deg forward / reverse around 0 deg. Changes in the magnetic flux density in the gaps 31 and 32 when rotating were measured.

  FIG. 10 is a graph showing the measurement results. As shown in the figure, it can be seen that the hysteresis loop of the gap 32 gradually increases as the amount of eccentricity A increases from 0 mm → 0.5 mm → 1.0 mm. That is, it can be seen that the hysteresis increases as the eccentricity A increases.

  On the other hand, it can be seen that the hysteresis loop of the gap 31 in which the Hall IC 4 is arranged gradually decreases as the eccentricity A increases from 0 mm to 0.5 mm. It can be seen that when the eccentricity A = 0.5 mm, the hysteresis loop is crushed to a substantially straight line. At this time, it is understood that the hysteresis loop is inverted as indicated by an arrow in the figure. It can also be seen that the hysteresis loop gradually increases as the eccentricity A increases from 0.5 mm to 1.0 mm.

  From the above experiment, it can be seen that the hysteresis of the gap 31 becomes substantially zero when the eccentricity A = 0.5 mm. In addition, in the rotation angle detection device of another embodiment, there is a point where the hysteresis loop is reversed. Therefore, the hysteresis can be reduced to 0 by performing the experiment as described above in each rotation angle detection device and searching for the point.

(A) is an axial sectional view of the rotation angle detection device of the first embodiment, and (b) is a top view of the rotation angle detection device. It is a graph which shows the change of the magnetic flux density in the yoke when a magnet is reciprocatingly rotated in the range of ± 50 deg in the same rotation angle detection device. It is a schematic diagram which shows the change of the magnetic flux density in each angular position of the yoke of the same rotation angle detection apparatus. (A) is an axial sectional view of the rotation angle detection device of the second embodiment, and (b) is a top view of the rotation angle detection device. (A) is an axial sectional view of the rotation angle detection device of the third embodiment, and (b) is a top view of the rotation angle detection device. (A) is a side view of the rotation angle detection device of the fourth embodiment, and (b) is a top view of the rotation angle detection device. (A) is an axial sectional view of the rotation angle detection device of the fifth embodiment, and (b) is a top view of the rotation angle detection device. (A) is an axial sectional view of the rotation angle detection device of the sixth embodiment, and (b) is a top view of the rotation angle detection device. It is (a) axial direction sectional drawing and (b) top view which show the dimension in the experiment of the rotation angle detection apparatus of 1st embodiment. It is a graph which shows the experimental result with respect to the same rotation angle detection apparatus. (A) is an axial sectional view of a conventional rotation angle detection device, and (b) is a top view of the rotation angle detection device. It is a graph which shows the change of the magnetic flux density in the yoke when a magnet is reciprocatingly rotated in the range of ± 50 deg in the same rotation angle detection device. It is a schematic diagram which shows the change of the magnetic flux density in each angular position of the yoke of the same rotation angle detection apparatus.

Explanation of symbols

  1: rotation angle detector, 2: magnet, 3: yoke, 30a: semi-ring member, 30b: semi-ring member, 31: gap, 32: gap, 4: Hall IC (magnetic detector), 5: rotation Axis, 6: magnetism generating member, 60: magnetism generating side yoke, 60a: magnetism generating side semi-ring shaped member, 60b: magnetism generating side half ring shaped member, 61: magnetism generating side gap, 62: magnetism generating side gap, 7a : Magnet, 7b: Magnet.

Claims (9)

A ring-shaped magnetism generating member connected to the rotating shaft to form a magnetic field;
Arranged in the magnetic field of the magnetism generating member, forming a magnetic circuit between the magnetism generating member and arranging the magnetic flux density to change when the relative angle to the magnetism generating member changes due to rotation of the rotating shaft A ring-shaped yoke having a pair of gaps,
A magnetic detector disposed in one of the pair of gaps for detecting the magnetic flux density;
A rotation angle detection device comprising:
When the rotation angle of the magnetism generating member is 0 degree, the maximum density portion in the magnetic flux density distribution of the yoke is unevenly distributed on the region side of more than 270 degrees and less than 90 degrees with the magnetic detector position being 0 degrees. A rotation angle detection device characterized by that.   The rotation angle detection device according to claim 1, wherein the magnetism generating member is a magnet, and the yoke is disposed on an outer peripheral side of the magnet. The magnet has a concentric ring shape, and the yoke has a concentric ring shape;
The rotation angle detection device according to claim 2, wherein the central axis of the magnet is eccentric in the direction of the magnetic detector with respect to the central axis of the yoke. The magnet has an eccentric ring shape, and the yoke has a concentric ring shape;
The central axis of the inner peripheral surface of the magnet and the central axis of the yoke are arranged coaxially,
The rotation angle detection device according to claim 2, wherein when the rotation angle of the magnet is 0 degree, the outer peripheral surface central axis is decentered in the direction of the magnetic detector with respect to the central axis of the yoke. The magnet has a concentric ring shape, and the yoke has an eccentric ring shape;
The central axis of the magnet and the central axis of the inner peripheral surface of the yoke are arranged coaxially,
The rotation angle detection device according to claim 2, wherein the central axis of the outer peripheral surface of the yoke is eccentric in the direction of the magnetic detector with respect to the central axis of the magnet. The magnet has a concentric ring shape, and the yoke has a concentric ring shape;
The central axis of the magnet and the central axis of the yoke are arranged coaxially,
The rotation angle detection device according to claim 2, wherein an axial thickness of the yoke is uneven in a direction of the magnetic detector. The magnetism generating member includes a pair of magnets arranged in the pair of magnetism generation side gaps so that the directions of magnetic poles are opposite to each other in the circumferential direction, and a ring-shaped magnetism generation side yoke having a pair of magnetism generation side gaps And consists of
The rotation angle detection device according to claim 1, wherein the yoke is disposed on an inner peripheral side of the magnetism generating member. The magnetism generating member has a concentric ring shape, and the yoke has a concentric ring shape;
The rotation angle detection device according to claim 7, wherein a central axis of the magnetism generating member is decentered in a direction opposite to the magnetic detector direction with respect to the central axis of the yoke. The magnetism generating member has a concentric ring shape, and the yoke has a concentric ring shape;
The central axis of the magnetism generating member and the central axis of the yoke are arranged coaxially,
When the rotation angle of the magnetism generating member is 0 degree, the magnetism generating side gap of the magnetism generating side yoke is arranged in an area of more than 270 degrees and less than 90 degrees with the magnetic detector position being 0 degrees. The rotation angle detection device according to claim 7.

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