JP2015148627A - Angle measurement method and angle measurement system - Google Patents

Abstract

PROBLEM TO BE SOLVED: To measure a rotation angle with high accuracy and in a short time.SOLUTION: A angle measurement system comprises: a rotary encoder 2 that includes a rotating shaft 3 serving as a drive rotating body to be rotationally driven, and an encoder main body 2a serving as a support reference body supporting the rotating shaft 3, and detects a rotation angle of the rotating shaft 3 with respect to the encoder main body 2a as angle detection means; and contactless angle detection means 20 that does not contact with the encoder main body 2a to optically detect a position of the encoder main body 2a as optical position check means. Accordingly, the rotation angle detected by the rotary encoder 2 is enabled to be corrected on the basis of the position detected by the contactless angle detection means 20, and the rotation angle is enabled to be measured with high accuracy and in a short time.

Description

  The present invention relates to an angle measurement method and an angle measurement system that can be suitably used in a technical field that requires precise measurement of the rotation angle of a rotating body.

  Conventionally, in order to accurately measure the angle indexing accuracy of a rotating body in a machine tool or the like, an angle measuring method using a polygon mirror and an autocollimator (hereinafter referred to as “polyhedral mirror method”), a hearth coupling and a laser interferometer are used. An angle measurement method (hereinafter referred to as “Heas coupling method”) has been performed.

  In the polygon mirror method, the difference between the rotation angle of the object on which the polygon mirror is mounted and the angle of the polygon mirror is measured with a highly accurate autocollimator.

  In the hearth coupling method, the workpiece to which the hearth coupling is attached is rotated at a predetermined target angular displacement, the hearth coupling is reversely rotated by the amount corresponding to the target angular displacement after disconnecting the hearth coupling, The sum of the reverse angular displacement and the angular displacement from the reference position measured by the laser interferometer is compared with the target angular displacement of the object to be measured (see Patent Document 1).

Japanese Translation of National Publication No. 06-502727

  However, the conventional angle measurement technique has the drawbacks that it takes time to measure and it is difficult to improve measurement accuracy.

  In the polygon mirror method, the phase angle between the angle of the polygon mirror and the angle of the object to be measured is changed in various ways, and the measurement is repeated. Need to continue for hours. Further, since the resolution is coarse and it is difficult to keep the apparatus stable for a long time, there is a limit to the improvement of measurement accuracy.

  In the Hearth coupling method, after the object to be measured is rotated at the target angular displacement, a swing operation is required to reversely rotate the Hearth coupling by the amount of the target angular displacement and return the laser interferometer reflector to its original position. Therefore, the entire measurement time becomes long. In addition, the accuracy of angle measurement depends on the resolution of the hearth coupling teeth, and transmission errors occur in the teeth of the hearth coupling when the forward rotation and the reverse rotation are repeated, so that there is a limit to improving the measurement accuracy.

  In addition, a rotary encoder is known as a device for detecting the rotation angle, but when the rotary encoder is attached to the object to be measured, an eccentricity occurs between the rotating shaft of the object to be measured and the rotating shaft of the rotary encoder. Therefore, there is a problem that measurement error occurs.

  The present invention has been made in view of such circumstances, and an object thereof is to provide an angle measuring method and an angle measuring system capable of measuring a rotation angle with high accuracy and in a short time.

  In order to achieve the above object, the present invention provides a main body, a rotary shaft rotatable with respect to the main body, a cord attached to the rotary shaft, and a code fixed to the main body to read the code of the cord. An angle measurement method using a rotary encoder having a reading unit, wherein a rotary shaft of the rotary encoder is attached to a rotary shaft of a workpiece to be rotated, and the rotary shaft of the workpiece and the rotation of the rotary encoder are rotated. In order to allow eccentricity with respect to the shaft, the displacement of the main body of the rotary encoder within a plane orthogonal to the rotational axis of the rotary encoder is regulated within a certain play range, and the rotary with respect to the rotational shaft of the object to be measured is controlled. The eccentric amount of the rotary shaft of the encoder is detected in a non-contact manner, and the rotary encoder is based on the code read by the reading unit of the rotary encoder. The rotation angle of the rotation shaft of the encoder measures the rotation angle measured by using the rotary encoder, based on at least the detected eccentricity, to provide an angle measurement method and correcting. With this configuration, the measurement value of the rotary encoder is corrected with a non-contact measurement value, so that the rotation angle can be measured in a shorter time and with higher accuracy than conventional angle measuring techniques using a polygon mirror method or a hearth coupling method. be able to. Moreover, since the allowable range of the eccentric amount of the rotary shaft of the rotary encoder with respect to the rotary shaft of the object to be measured can be made larger than the specification of the rotary encoder, it is very easy to attach the rotary encoder to the object to be measured. That is, according to the present invention, the rotation angle can be measured with high accuracy and in a short time by using the rotary encoder, which greatly contributes to an increase in production capacity of machine tools and the like.

  In one embodiment of the present invention, a jig for locking the main body portion of the rotary encoder while allowing the displacement of the main body portion of the rotary encoder within the certain play range is used.

  In one embodiment of the present invention, a weight is attached to the main body of the rotary encoder, and the main body of the rotary encoder is biased in the direction of gravity.

  The present invention also provides a rotary having a main body, a rotary shaft that is rotatable with respect to the main body, a cord attached to the rotary shaft, and a reading unit that is fixed to the main body and reads the code of the code. An angle measurement method using an encoder, wherein the rotary encoder main body is attached to a rotary shaft of a device to be rotated, and eccentricity between the rotary shaft of the device to be measured and the rotary shaft of the rotary encoder is allowed. Thus, the displacement of the rotary shaft of the rotary encoder in a plane orthogonal to the rotary shaft of the rotary encoder is regulated within a certain play range, and the eccentricity of the rotary shaft of the rotary encoder with respect to the rotary shaft of the object to be measured Rotation of the main body of the rotary encoder based on the code read by the reading unit of the rotary encoder Degrees were measured, the rotation angle measured by using the rotary encoder, based on at least the detected eccentricity, to provide an angle measurement method and correcting. With this configuration, the measurement value of the rotary encoder is corrected with a non-contact measurement value, so that the rotation angle can be measured in a shorter time and with higher accuracy than conventional angle measuring techniques using a polygon mirror method or a hearth coupling method. be able to. Moreover, since the allowable range of the eccentric amount of the rotary shaft of the rotary encoder with respect to the rotary shaft of the object to be measured can be made larger than the specification of the rotary encoder, it is very easy to attach the rotary encoder to the object to be measured. That is, according to the present invention, the rotation angle can be measured with high accuracy and in a short time by using the rotary encoder, which greatly contributes to an increase in production capacity of machine tools and the like.

  In one embodiment of the present invention, a jig that locks the rotary shaft of the rotary encoder while allowing the displacement of the rotary shaft of the rotary encoder within the certain play range is used.

  In one embodiment of the present invention, a weight is attached to the rotary shaft of the rotary encoder, and the rotary shaft of the rotary encoder is biased in the direction of gravity.

  In addition, the present invention includes a main body, a rotating shaft that is rotatable with respect to the main body, a cord attached to the rotating shaft, and a reading unit that is fixed to the main body and reads the code of the code. A rotary encoder to which the rotary shaft is attached to a rotationally driven object to be measured, and an orthogonal to the rotational axis of the rotary encoder so as to allow eccentricity between the rotational axis of the object to be measured and the rotational axis of the rotary encoder. A non-contact detecting member that detects the eccentricity of the rotary shaft of the rotary encoder relative to the rotary shaft of the object to be measured in a non-contact manner, and a regulating member that restricts the displacement of the main body of the rotary encoder within a certain play range. The rotation angle corresponding to the code read by the contact eccentricity detecting means and the reading unit of the rotary encoder is detected by at least the non-contact eccentricity detecting means. Based on the amount of eccentricity, to provide an angle measurement system comprising: the correcting means, the correcting.

  In one embodiment of the present invention, the restricting member includes a jig for locking the main body portion of the rotary encoder while allowing the displacement of the main body portion of the rotary encoder within the certain play range. To do.

  In one embodiment of the present invention, the restricting member includes a weight attached to the main body of the rotary encoder and biasing the main body of the rotary encoder in the direction of gravity.

  In addition, the present invention includes a main body, a rotating shaft that is rotatable with respect to the main body, a cord attached to the rotating shaft, and a reading unit that is fixed to the main body and reads the code of the code. A rotary encoder in which the main body is attached to a rotationally driven object to be measured, and a rotation axis of the rotary encoder so as to allow eccentricity between the rotational axis of the object to be measured and the rotational axis of the rotary encoder. A non-contact detecting member for detecting the eccentricity of the rotary shaft of the rotary encoder with respect to the rotary shaft of the object to be measured in a non-contact manner. The rotation angle corresponding to the code read by the contact eccentricity detecting means and the reading unit of the rotary encoder is detected by at least the non-contact eccentricity detecting means. Based on the amount of eccentricity, to provide an angle measurement system comprising: the correcting means, the correcting.

  In one embodiment of the present invention, the restricting member includes a jig for locking the rotary shaft of the rotary encoder while allowing displacement of the rotary shaft of the rotary encoder within the certain play range. To do.

  In one embodiment of the present invention, the restriction member includes a weight attached to a rotary shaft of the rotary encoder and biasing the rotary shaft of the rotary encoder in a gravitational direction.

  In one embodiment of the present invention, static measurement for detecting a rotation angle at a timing when rotation of the rotation axis of the object to be measured stops, and detection of a rotation angle at a timing during rotation of the rotation axis of the object to be measured. It is characterized in that at least one of the dynamic measurements is performed.

  According to the present invention, it is possible to measure the rotation angle with high accuracy and in a short time as compared with the prior art. In addition, it is very easy to attach the rotary encoder to the object to be measured.

Overall configuration diagram of an example of an angle measurement system in the first embodiment Side view showing a state where the rotary shaft of the rotary encoder is attached to the object to be measured Side view showing a state in which interference units of non-contact positioning means are arranged Explanatory drawing showing the positional relationship between the rotating shaft of the object to be measured, the rotating shaft of the rotary encoder, and the encoder body (A) is a plan view showing an example of the encoder, (B) is a plan view showing the encoder at the start of measurement, and (C) is used to explain the relationship among the actual rotation angle θr, eccentricity B, and reading angle θα. Plan view Plan view showing the displacement of the encoder read head corresponding to the displacement of the encoder body Front view showing an example when the displacement of the encoder body is regulated by a weight Side view showing the case where the device under test is placed along the horizontal direction The whole block diagram of an example of the angle measurement system in 2nd Embodiment Side view showing how the encoder body is attached to the device under test Schematic configuration diagram of an angle measurement system in the third embodiment The block diagram which shows an example of the inclination angle detection system of the angle measurement system in 3rd Embodiment Explanatory drawing used for explanation of angle detected by non-contact angle detection means The block diagram which shows an example of the inclination angle detection system of the angle measurement system in 4th Embodiment

  Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings.

  FIG. 1 is an overall configuration diagram of an example of an angle measurement system according to the first embodiment.

  The angle measuring system 100 shown in FIG. 1 measures the rotational angle of the rotating shaft 1a of the device under test 1 that is rotationally driven by using the rotary encoder 2. The rotary encoder 2 includes an encoder body 2a and a rotating shaft 3 that is rotatable with respect to the encoder body 2a.

  FIG. 2 is a side view showing a state in which the rotary shaft 3 of the rotary encoder 2 is attached to the rotary shaft 1 a of the DUT 1. FIG. 3 is a side view showing a state in which the interference unit 4 of the non-contact positioning means 20 is arranged.

  As shown in FIG. 2, a disk-shaped encoder 14 (code portion) is attached to the rotary shaft 3 inside the encoder body 2a. The encoder 14 has a scale (code) formed on the entire circumference around the rotation shaft 3. The encoder 14 may be an incremental type or an absolute type. An encoder reading head 13 (reading unit) that reads the scale of the encoder 14 is fixed to the encoder body 2a. The encoder reading head 13 outputs a pulse signal (rotation angle signal) in accordance with the scale reading of the encoder 14. That is, the rotary encoder 2 generates a pulse signal corresponding to the amount of change in the relative rotation angle between the encoder body 2 a and the rotary shaft 3. The encoder body 2a may be a coupling built-in type.

  A rotary shaft 3 of the rotary encoder 2 is attached to the encoder body 2a via a bearing 15 made of a ball bearing. In this embodiment, the rotary shaft 3 of the rotary encoder 2 is detachably attached to the rotary shaft 1a of the DUT 1. After attachment, the rotating shaft 3 is in a state of being freely rotatable with respect to the encoder body 2a via the bearing 15. For this reason, even if the rotating shaft 1a of the DUT 1 rotates, the cable (16 in FIG. 1) connected to the rotary encoder body 2a does not get entangled.

  The rotating shaft 3 of this example has an attachment portion 3 a for attaching to the rotating shaft 1 a of the DUT 1. You may attach to the rotating shaft 1a of the to-be-measured object 1 via a special attachment.

  As will be described later, the encoder body 2a has a surface orthogonal to the rotation shaft 3 (hereinafter referred to as an "orthogonal surface") so as to allow eccentricity between the rotation shaft 1a of the DUT 1 and the rotation shaft 3 of the rotary encoder 2. ) Are allowed to move within a certain play range (displacement). Even if there is an axial runout of the DUT 1, no measurement error occurs, but the surface runout becomes a measurement error, and is therefore kept within a specified value calculated in accordance with the target measurement accuracy.

  As shown in FIG. 1, the non-contact positioning means 20 includes a first corner cube prism 7a, an interference unit 4 (polarization beam splitter 6 and second corner cube prism 7b), laser light source 10, phase difference detection head 11, And the data processing device 12. The non-contact positioning means 20 detects a changed position of the first corner cube prism 7a fixed to the encoder body 2a (that is, displacement of the encoder body 2a) in a non-contact manner, and based on the detected displacement, The eccentric amount of the rotary shaft 3 of the rotary encoder 2 with respect to the rotary shaft 1a of the workpiece 1 is calculated.

  As shown in FIG. 1, a first corner cube prism 7a (reflective element) is installed on an orthogonal plane orthogonal to the rotation shaft 3 of the encoder body 2a. The interference unit 4 (interference optical system) is arranged to face the first corner cube prism 7a. The interference unit 4 includes a polarization beam splitter 6 and a second corner cube prism 7b. The interference unit 4 divides the laser light beam emitted from the laser light source 10 into a first laser light beam directed to the first corner cube prism 7a and a second laser light beam directed to the second corner cube prism 7b. To do. The first laser light beam (first reflected light beam) reflected by the first corner cube prism 7a and the second laser light beam (second reflected light beam) reflected by the second corner cube prism 7b are: Return to the polarizing beam splitter 6. As described above, the interference unit 4 causes the first and second laser light beams having different optical path lengths to interfere with each other. That is, interference fringes of the first and second reflected light beams are generated.

  In the polarization beam splitter 6, a part (first laser beam) of the laser beam emitted from the laser light source 10 passes through the polarization beam splitter 6 and enters the incident surface of the first corner cube prism 7a perpendicularly. Are arranged as follows. The second corner cube prism 7b is arranged so that the second laser beam returns to the polarization beam splitter 6 through the optical path of the reference length.

  The phase difference detection head 11 (phase difference detection means) receives the interference light composed of the first reflected light beam and the second reflected light beam having different optical path lengths, and the first and second corner cube prisms 7a and 7b. The phase difference between the reflected light beams (first and second reflected light beams) is detected. In this example, the optical path length difference (phase difference) between the optical path of the first laser beam (solid line in FIG. 1) and the optical path of the second laser beam (dotted line in FIG. 1) is detected by counting the interference fringes. To do.

  As the laser light source 10, for example, a He—Ne laser is used. Even if wavelength stabilization is not performed, measurement accuracy is not greatly affected. When the laser light source 10 and the interference unit 4 are coupled by an optical fiber, the attachment becomes very easy. The phase difference detection head 11 may be a fringe count method using a Michelson interferometer or a heterodyne method. In the case of the heterodyne system, the laser light source 10 needs to have two orthogonal polarization frequencies, and for example, a Zeeman laser or an AOM (acousto-optic element) is used.

  The data processing device 12 is configured by a computer device. The computer device includes a storage unit including a memory, a control unit including a CPU (Central Processing Unit), a display unit, and an input unit including a keyboard.

  The rotating shaft 1a of the DUT 1 is rotationally driven using a driving means (not shown) (not shown).

  The pulse signal (rotation angle signal) output from the rotary encoder 2 is sent to the rotation angle detector 9 via the cable 16. In this example, an incremental encoder with a plurality of origin codes (for example, at an interval of 10 degrees) is used as the encoder 14, and a phase (hereinafter referred to as “θp”) is acquired from the encoder read head 13 together with a pulse signal. An origin signal for output is output. The rotation angle detection unit 9 of this example detects a rotation angle from the measurement start time (hereinafter referred to as “θr”) based on the pulse signal, and also detects the phase θp (“reading angle” based on the pulse signal and the origin signal. ) And θr and θp are sent to the data processor 12. The phase θp indicates the position on the circumference of the code of the encoder 14 read by the encoder reading head 13 as an angle.

  Further, the phase difference signal indicating the phase difference (optical path length difference) between the first laser beam and the second laser beam output from the phase difference detection head 11 of the non-contact positioning means 20 is sent to the data processing device 12. Sent. The data processing device 12 constitutes a part of the non-contact positioning means 20 (eccentricity calculation means), and based on the phase difference signal indicating the optical path difference output from the phase difference detection head 11, the DUT 1 The amount of eccentricity (hereinafter referred to as “B”) of the rotary shaft 3 of the rotary encoder 2 with respect to the rotary shaft 1a is calculated.

  The data processing device 12 corrects the rotation angle θr (measured value of the relative rotation angle between the encoder body 2a and the rotation shaft 3) measured using the rotary encoder 2 based on at least the eccentricity B. To do.

  Below, the example of the correction process performed by the control means of the data processor 12 is demonstrated.

  4A to 4D are explanatory views showing the positional relationship between the rotary shaft 1a of the DUT 1 and the rotary encoder 2 when the rotary shaft 1a of the DUT 1 is rotated. 4 (A) to 4 (D), the eccentricity B is exaggerated for the sake of understanding of the present invention. However, in practice, the eccentricity B is restricted to a level that can be measured by the non-contact positioning means 20 (for example, 1 mm or less). The data processing device 12 calculates the amount of eccentricity B based on the displacement of the encoder body 2a detected by the non-contact positioning means 20. At θp = 0 ° and 180 °, the rotation center 0 (the center of the rotating shaft 1a of the DUT 1) exists on the straight line connecting the reading position of the encoder reading head 13 and the center 3b of the rotating shaft 3. .

  5A shows an example of the encoder 14, FIG. 5B shows an example of the measurement start time, and FIG. 5C shows an example of the measurement end time. In this example, the phase θp = 0 at the measurement start time shown in FIG. At the end of measurement shown in FIG. 5C, the measured value θr = θp, and the measured value θr is expressed by the following equation.

[Equation 1]
θr = θp = tan ⁻¹ {(A / 2 × sin θ) / (A / 2 × cos θ + B)}
In Equation 1, A is the diameter of a circle indicating the reading position of the encoder 14 by the encoder reading head 13, B is the amount of eccentricity measured by the non-contact positioning means 20, and θ is the rotation angle of the rotating shaft 1a of the object 1 to be measured. It is.

  FIG. 6 shows the displacement L of the encoder reading head 13 measured by the non-contact positioning means 20 (corresponding to the displacement of the encoder main body 2a). The amount of eccentricity B is expressed by the following equation using the displacement L in FIG.

[Equation 2]
B = L / sinθ
As shown in FIG. 6, the eccentric amount B is obtained by measuring the displacement L from the start of measurement of the rotation angle to the end of measurement by the non-contact positioning means 20 as the displacement of the encoder body 2a. It is possible to calculate by For example, it is obtained as θ = θp.

  However, in order to detect the eccentricity B with high accuracy, for example, as shown in FIGS. 4A to 4D, the rotation shaft 1a of the DUT 1 is rotated in advance for one cycle (360 degrees) or more. However, it is preferable to detect the movement amplitude W in a straight line direction of a specific point on the encoder main body 2a using the non-contact positioning means 20 in a non-contact manner and convert the amplitude W into an eccentricity amount B.

  Since the diameter A is known from the specification, the correspondence between the measured value θr of the rotation angle and the actual rotation angle θ is known in advance.

  The angle error Δθr due to the eccentric amount B is expressed by the following equation.

[Equation 3]
Δθr = θr−θ
Therefore, by correcting the measured value θr of the rotation angle using the eccentricity B, Δθr is set to zero. The above equation 1 may be solved for θ.

  However, although the case where the measurement is started at the phase θp = 0 has been described with reference to FIG. 5, the measurement can be started at the phase θp ≠ 0. In this case, the data processing device 12 corrects the measured value θr using the eccentricity amount B output from the non-contact positioning means 20 and the phase θp output from the rotation angle detection unit 9.

  In the rotation angle measurement, even in the static measurement in which the rotation angle is detected at the timing when the rotation of the rotating shaft 1a of the device under test 1 is stopped, the rotation angle is measured at the timing when the rotating shaft 1a of the device under test 1 is rotating. It may be a dynamic measurement to detect. In static measurement, for example, the rotation start time is the rotation angle measurement start time. In the dynamic measurement, an arbitrary timing during rotation can be set as the rotation angle measurement start time.

  Next, a specific example of the regulating member will be described.

  In the example shown in FIG. 1, the movement of the encoder main body 2 a is regulated by the rotation preventing jig 8. The anti-rotation jig 8 locks the rod 2b extended to the encoder body 2a by the locking claws 8a and 8b. The width of the gap between the two locking claws 8a and 8b corresponds to the allowable range of the eccentricity. As a result, the movement of the encoder body 2 a is restricted at least within the measurable range of the non-contact angle detection means 40.

  In addition, when the performance of the bearing 15 is excellent and the encoder body 2a does not rotate in accordance with the rotation of the DUT 1, the anti-rotation jig 8 may be omitted. That is, depending on the performance of the bearing 15, the bearing 15 itself can function as a regulating member that regulates the movement of the encoder body 2a.

  FIG. 7 is a front view showing a case where the movement of the encoder body 2 a is restricted by the weight 17. As shown in FIG. 7, the weight 17 is attached to the encoder body 2a and lowered in the direction of gravity. The encoder body 2a is urged by the weight 17 in the direction of gravity, and the movement is restricted within a certain play range.

  In addition, although the case where the rotation stopping jig 8 is used is shown in FIG. 1 and the weight 17 is used in FIG. 7, both of these may be used as the regulating member. Other regulating members (for example, a magnetic body that regulates movement by magnetic force) may be used.

  FIG. 8 is a side view showing a case where the DUT 1 is arranged along the horizontal direction.

  Further, if the rotation prevention jig 8 has a weak magnetic force, the position of the encoder main body 2a is easily determined and is easy to measure, particularly in the case of the horizontal arrangement in FIG.

  In the first embodiment, the rotary shaft 3 of the rotary encoder 2 is attached to the rotary shaft 1a of the workpiece 1 to be rotated, and the eccentricity between the rotary shaft 1a of the workpiece 1 and the rotary shaft 3 of the rotary encoder 2 is set. In order to allow, the displacement of the encoder body 2a in a plane orthogonal to the rotary shaft 3 of the rotary encoder 2 is restricted within a certain play range, and the rotary shaft 3 of the rotary encoder 2 with respect to the rotary shaft 1a of the object 1 to be measured. The eccentric amount B is detected in a non-contact manner, the rotational angle of the rotary shaft 3 of the rotary encoder 2 is measured based on the code read by the encoder reading head 13 of the rotary encoder 2, and the rotational angle measured using the rotary encoder 2 θr is corrected based on at least the eccentricity B.

  With this configuration, the measured value of the rotary encoder 2 is corrected by the measured value B of the eccentricity, so that the rotation angle can be set in a short time and with high accuracy compared to the conventional angle measuring technique of the polygon mirror method or the hearth coupling method. Can be measured. In addition, since the allowable range of the eccentric amount of the rotary shaft 3 of the rotary encoder 2 with respect to the rotary shaft 1a of the device under test 1 can be made larger than the specification of the rotary encoder 2, the rotary encoder 2 can be attached to the device under test 1. It becomes very easy. That is, according to the present invention, the rotation angle can be measured with high accuracy and in a short time using the rotary encoder 2, which greatly contributes to an increase in production capacity of machine tools and the like.

Second Embodiment
FIG. 9 is an overall configuration diagram of an example of the angle measurement system 200 in the second embodiment. In FIG. 9, the same components as those in the first embodiment shown in FIGS. Below, description is abbreviate | omitted about the content demonstrated in 1st Embodiment, and a different point from 1st Embodiment is mainly demonstrated.

  In the first embodiment, the rotary shaft 3 of the rotary encoder 2 is attached to the rotary shaft 1a of the DUT 1 as shown in FIG. 2, whereas in the second embodiment, the DUT 1 is shown as shown in FIG. The encoder body 2a is attached to the rotary shaft 1a.

  In FIG. 10, the attachment attachment 18 is an interposed member for attaching the encoder body 2 a to the rotating shaft 1 a of the device under test 1, and the rotating shaft 3 of the rotary encoder 2 rotates the rotating shaft 1 a of the device under test 1. The rotary shaft 3 of the rotary encoder 2 is protected so as not to be affected so much.

  The anti-rotation jig 8 in the present embodiment allows the rotary encoder 2 to move (displace) within the fixed play range while allowing the movement (displacement) of the rotary shaft 2 in a plane orthogonal to the rotary shaft 3 of the rotary encoder 2. The rotating shaft 3 of 2 is locked. A weight may be attached to the rotary shaft 3 of the rotary encoder 2 to bias the rotary shaft 3 in the direction of gravity.

  The first corner cube prism 7 a in this embodiment is attached to the rotary shaft 3 of the rotary encoder 2. Similar to the first embodiment, the first corner cube prism 7 a is arranged to face the interference unit 4. Using the interference unit 4 and the phase difference detection head 11, the displacement of the rotary shaft 3 of the rotary encoder 2 is detected without contact.

  In the present embodiment, unlike the first embodiment, the load of the encoder body 2a is not applied to the rotating shaft 3, and the load of the relatively lightweight corner cube prism 7a is sufficient, so the rotating shaft 3 and the bearing 15 can be small. Weight can be reduced. Therefore, this method is suitable depending on the loadable weight of the rotating shaft 1a of the DUT 1. On the other hand, care must be taken so that the cable connected to the encoder body 2a does not wind around the rotary encoder 2 as the encoder body 2a rotates.

  In the second embodiment, the encoder main body 2a is attached to the rotating shaft 1a of the object 1 to be rotated, and the eccentricity between the rotating shaft 1a of the object 1 to be measured and the rotating shaft 3 of the rotary encoder 2 is allowed. The movement (displacement) of the rotary shaft 2 of the rotary encoder 2 in a plane orthogonal to the rotary shaft 3 of the rotary encoder 2 is restricted within a certain play range, and the rotary encoder 2 rotates with respect to the rotary shaft 1a of the object 1 to be measured. The eccentric amount B of the shaft 3 is detected in a non-contact manner, the rotational angle θr of the encoder body 2a is measured based on the code read by the encoder reading head 13 of the rotary encoder 2, and the measured rotational angle θr is at least the eccentric amount. Based on B, correction is performed. Thereby, the effect similar to 1st Embodiment can be acquired.

<Third Embodiment>
As shown in FIG. 11, the angle measurement system 300 according to the third embodiment includes a non-contact positioning unit 20 and a non-contact angle detection unit 40. In FIG. 11, the rotation angle correction means 50 includes the eccentricity B detected by the non-contact positioning means 20 and the inclination detected by the non-contact angle detection means 40 with respect to the rotation angle θr measured using the rotary encoder 2. Correction is performed based on the angle (hereinafter referred to as “θ2”). The rotary encoder 2, the rotation angle detection unit 9, and the non-contact positioning means 20 are the same as those described in the first embodiment, and description thereof is omitted. The rotation angle correction means 50 is configured by the data processing device 12 shown in FIG.

  FIG. 12 is an overall configuration diagram mainly showing the non-contact angle detecting means 40, and the non-contact positioning means 20 shown in FIG. 1 is omitted for convenience of illustration. In FIGS. 11 and 12, the same components as those in the first embodiment shown in FIGS. Below, description is abbreviate | omitted about the content demonstrated in 1st Embodiment, and a different point from 1st Embodiment is mainly demonstrated.

  The non-contact angle detection means 40 includes the laser light source 10, the phase difference detection head 11, the interference unit 34 (the right-angle prism 35 and the polarization beam splitter 36), the pair of corner cube prisms 37 (37a, 37b), and the data processing device 12. It is configured to include. The non-contact angle detecting means 40 detects the changed tilt angle of the encoder body 2a from the start of the rotation angle measurement of the rotary shaft 3 using the rotary encoder 2 in a non-contact manner.

  As shown in FIG. 12, a pair of corner cube prisms 37a and 37b (reflective elements) are installed on the orthogonal surface of the encoder body 2a (the surface orthogonal to the rotation shaft 3). The interference unit 34 (interference optical system) is arranged to face the pair of corner cube prisms 37a and 37b.

  As shown in FIG. 12, the interference unit 34 includes a right-angle prism 35 and a polarization beam splitter 36. The interference unit 34 uses the laser beam emitted from the laser light source 30 as the first laser beam toward the first corner cube prism 37a of the non-contact angle detection means 40 and the second beam toward the second corner cube prism 37b. Are divided into laser beams. The first laser beam transmitted through the polarization beam splitter 36 is reflected by the first corner cube prism 37 a and returns to the polarization beam splitter 36. The second laser beam reflected by the polarization beam splitter 36 at a right angle is reflected by the second corner cube prism 37b via the right angle prism 35, and again reflected by the right angle prism 35 at a right angle, and is reflected by the polarization beam splitter 36. Come back. In other words, the interference unit 34 causes the first and second laser light beams parallel to each other to enter the first and second corner cube prisms 37a and 37b, respectively, and the first and second corner cube prisms 37a and 37b respectively. The first and second reflected light fluxes reflected and recursed are caused to interfere with each other. Therefore, the interference unit 34 generates interference fringes of the first and second reflected light beams having different optical path lengths.

  The phase difference detection head 11 (phase difference detection means) receives the interference light composed of the first reflected light beam and the second reflected light beam having different optical path lengths, and the first and second corner cube prisms 37a and 37b. The phase difference between the reflected light beams (first and second reflected light beams) is detected. In this example, the optical path length difference (phase difference) between the optical path of the first laser beam (solid line in FIG. 12) and the optical path of the second laser beam (dotted line in FIG. 12) is detected by counting interference fringes. To do.

  When the interference unit 34 and the corner cube prisms 37a and 37b are facing each other, the corner cube prisms 37a and 37b are measured by the phase difference detection head 11 even if they move approximately 1 mm in all directions orthogonal to the laser beam. It is possible to keep the amplitude reduction of the interference signal within an allowable range. The allowable range of the positional deviation amount depends on the beam diameter of the laser light source 30 and the performance of the phase difference detection head 11 and the like. Since the allowable range of the misalignment amount of the corner cube prisms 37a and 37b is the allowable range of the eccentric amount between the rotary shafts 1a and 3, the rotary encoder 2 can be attached very easily.

  The laser light source 10 shown in FIG. 1 may be used as the laser light source 10 of the tilt angle detection system. Two laser light sources may be provided.

  The phase difference signal indicating the phase difference (optical path length difference) between the first laser beam and the second laser beam output from the phase difference detection head 31 is sent to the data processing device 12. The data processing device 12 constitutes a part of the non-contact angle detection means 40 (tilt angle calculation means), and the phase difference signal output from the phase difference detection head 11 and the apex of the first corner cube prism 37a. Based on the positional difference (interval) between the first corner cube prism 37b and the vertex of the second corner cube prism 37b, using a trigonometric function, as shown in FIG. 13, the vertex 70a of the first corner cube prism 7a and the second corner cube The inclination angle (θ2) of the straight line 70 connecting the apex 70b of the prism 7b is calculated. The resolution of θ2 by the non-contact angle detection means 40 is higher (the resolution pitch is smaller) than θ1 by the rotary encoder 2 and the rotation angle detector 9.

  Further, the data processing device 12 sets θr (which is a relative rotation angle between the encoder main body 2a and the rotation shaft 3) to at least the eccentric amount B and θ2 (the inclination angle of the portion of the rotary encoder 2 in which the movement is restricted). Is corrected). That is, θr measured using the rotary encoder 2 is based on the eccentric amount B detected by the non-contact positioning means 20 of FIG. 1 and the inclination angle θ2 of a straight line connecting the corresponding points of the corner cube prisms 7a and 7b. To correct.

  In the static measurement at the measurement point, it is required that variations in the measurement values of the rotary encoder 2 and the non-contact angle detection unit 40 are sufficiently reduced to be sufficiently smaller than the target measurement accuracy. The measurement of the angle indexing accuracy is often performed by static measurement. In this case, the measurement object 1 is repeatedly measured by rotating and stopping the measurement object 1 at a certain angle. In the measurement value capture, each measurement value is assumed to be sufficiently stable with respect to the target measurement accuracy. The rotation speed of the DUT 1 depends on the performance of the rotary encoder 2 and the non-contact angle detection means 40, and can generally be measured at a high speed. The measurement resolution is the same, and is generally superior to a method using a polygon mirror and an autocollimator (polyhedral mirror method), a method using a hearth coupling and a laser interferometer (hearth coupling method), and the like.

  As described above, in the angle measurement method according to the third embodiment, the rotary shaft 3 of the rotary encoder 2 is attached to the rotary shaft 1a of the workpiece 1 to be rotated, and the rotary shaft 1a and the rotary encoder of the workpiece 1 are measured. The movement (displacement) of the rotary encoder body 2a in the orthogonal plane orthogonal to the rotary shaft 3 of the rotary encoder 2 is restricted within a certain play range so as to allow eccentricity with the rotary shaft 3 of the encoder 2. The rotation angle θr of the rotary shaft 3 of the rotary encoder 2 is detected (measured) based on the code read by the encoder 13, and the encoder from the start of the measurement of the rotational angle of the rotary shaft 3 of the rotary encoder 2 by the non-contact angle detection means 40. The changed tilt angle θ2 of the main body 2a is detected, and θr is corrected based on θ2.

  With this configuration, the rotation angle can be measured accurately in a short time. That is, first, by performing angle measurement using the rotary encoder 2, the manual operation of the operator, which is necessary in the conventional polygon mirror system, can be omitted, and reverse rotation such as the Hearth coupling system is involved. Since the swing motion can be omitted, not only high-precision measurement is possible, but also the overall measurement time can be shortened. Secondly, since the measurement value of the rotary encoder 2 is corrected by the measurement value of the non-contact angle detection means 40, the measurement accuracy can be further improved. Thirdly, the allowable range of the eccentric amount of the rotary shaft 3 of the rotary encoder 2 relative to the rotary shaft 1a of the device under test 1 can be made larger than the specification of the rotary encoder 2 itself. The installation of the encoder 2 is very easy and takes a short time. For example, when the non-contact angle detecting means 40 is not used in combination, the mounting accuracy of about 100 μm is required. However, when the laser interference length measurement type non-contact positioning means 20 is used together, the mounting accuracy of about 1 mm is used. Accordingly, the allowable range of the eccentricity has been widened accordingly.

<Fourth embodiment>
The outline of the angle measurement system in the fourth embodiment is the same as that of the angle measurement system 300 in the third embodiment shown in FIG.

  FIG. 14 is an overall configuration diagram showing the non-contact angle detecting means 40 in the fourth embodiment.

  In the third embodiment, the rotary shaft 3 of the rotary encoder 2 is attached to the rotary shaft 1a of the device under test 1, whereas in the fourth embodiment, the encoder body 2a is attached to the rotary shaft 1a of the device under test 1. The detent jig 8 is the same as in the second embodiment.

  In the angle measuring method according to the fourth embodiment, the encoder body 2a is attached to the rotating shaft 1a of the device 1 to be rotated, and the eccentricity between the rotating shaft 1a of the device 1 to be measured and the rotating shaft 3 of the rotary encoder 2 is adjusted. In order to allow, the movement (displacement) of the rotary shaft 3 of the rotary encoder 2 in the orthogonal plane orthogonal to the rotary shaft 3 of the rotary encoder 2 is restricted within a certain play range, and the code read by the encoder read head 13 is changed. Based on this, the rotation angle θr of the encoder main body 2a is detected (measured), and the non-contact angle detecting means 40 detects the changed tilt angle θ2 of the rotary shaft 3 from the start of the measurement of the rotation angle of the encoder main body 2a. Correction is performed based on the eccentricity B and θ2.

  In the first to fourth embodiments described above, the case where an optical rotary encoder is used as the rotary encoder has been described as an example. However, it goes without saying that another rotary encoder such as a magnetic encoder may be used. .

  In the first to fourth embodiments described above, the case where a so-called laser interference length measuring device is used as the non-contact positioning means and the non-contact angle detection means has been described as an example. Any other detection means can be used. For example, an autocollimator or a level may be used.

  The measurement of the rotation angle may be a dynamic measurement. In the angle measuring method and the angle measuring system according to the present invention, static measurement for detecting the rotation angle at the timing when the rotation of the rotating shaft 1a of the device under test 1 stops, and during the rotation of the rotating shaft 1a of the device under test 1 At least one of the dynamic measurements for detecting the rotation angle at the timing is performed. In the dynamic measurement, the output of the non-contact positioning means 20 used with the rotary encoder 2 needs to be real time.

  Further, in order to briefly explain the present invention, the case where the rotation angle θr is corrected using the eccentricity B and the inclination angle θ2 has been described as an example. However, the rotation angle θr may be corrected based on other measured values. Needless to say. That is, in the present invention, the rotational angle θr is corrected based on at least the eccentricity B. As described in the first and second embodiments, it is preferable to correct based on the phase θp of the angle error Δθr. Further, as described in the third and fourth embodiments, it is preferable to correct based on the inclination angle θ2.

  Further, the object to be measured is not limited to the shape shown in the figure. For example, a disk shape may be sufficient. Further, the rotation axis of the object to be measured to which the rotary encoder 2 is attached need not have a specially formed shaft shape. For example, the rotation center of the object to be measured is the rotation axis of the object to be measured. What is necessary is just to attach a rotary encoder to.

  The present invention is not limited to the examples described in the present specification and the examples illustrated in the drawings, and various design changes and improvements may be made without departing from the scope of the present invention.

  DESCRIPTION OF SYMBOLS 1 ... Measured object, 1a ... Rotating shaft of measured object, 2 ... Rotary encoder, 2a ... Encoder main body, 3 ... Rotating shaft of rotary encoder, 4 ... Interference unit, 6, 36 ... Polarizing beam splitter, 7 (7a, 7b), 37 (37a, 37b) ... Corner cube prism (reflective element), 8 ... Anti-rotation jig, 9 ... Rotation angle detector, 10 ... Laser light source, 11 ... Phase difference detection head, 12 ... Data processing device, DESCRIPTION OF SYMBOLS 13 ... Encoder reading head (reading part), 14 ... Encoder (code part), 15 ... Bearing, 17 ... Weight, 18 ... Mounting attachment, 20 ... Non-contact positioning means, 35 ... Right angle prism, 40 ... Non-contact angle detection means 50 ... Rotation angle correction means

Claims (2)

An angle detection means for detecting a rotation angle of the drive rotator with respect to the support reference body, the drive rotator for rotationally driving; and a support reference body for supporting the drive rotator.
Optical position confirmation means for optically detecting the position of the support reference body without contacting the support reference body;
An angle measurement system comprising: An angle detection step of detecting a rotation angle of the driving rotating body supported by the supporting reference body and driven to rotate with respect to the supporting reference body;
An optical position confirmation step for optically detecting the position of the support reference body without contacting the support reference body;
An angle measurement method comprising:

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