This application is based upon and claims the benefit of priority of the prior Japanese Patent Application No. 2021-022674, filed on Feb. 16, 2021 and the prior Japanese Patent Application No. 2022-006327, filed on Jan. 19, 2022, the entire contents of which are incorporated herein by reference.
A certain aspect of embodiments described herein relates to a scale and a manufacturing method of the scale.
There is disclosed a scale used for electromagnetic induction encodes (for example, see Japanese Patent Application Publication No. 2004-294225).
In one aspect of the present invention, it is an object to provide a scale and a manufacturing method that are capable of suppressing increasing in size and improving a signal detection accuracy.
According to an aspect of the present invention, there is provided a scale including: a scale including: a base material; an intermediate layer of soft magnetic material formed on one surface of the base material and roughened on face thereof opposite to the base material; and a scale pattern of a conductor formed on the intermediate layer.
According to another aspect of the present invention, there is provided a manufacturing method of a scale including: preparing an intermediate body in which an intermediate layer of a soft magnetic material having a roughened surface opposite to a base material is formed on one surface of the base material, and a conductor layer is provided on the intermediate layer; and forming a scale pattern by forming a patterning of the conductor layer.
According to another aspect of the present invention, there is provided a manufacturing method of a scale including: preparing an intermediate body in which an intermediate layer of a soft magnetic material and a conductor are laminated on a base material in this order; forming a scale pattern by forming a patterning of the conductor layer; and roughening an exposed portion of the intermediate layer.
The scale used in the electromagnetic induction encoder has a scale pattern of a conductor that generates an eddy current from the magnetic flux generated by the detector. As the base material of the scale, a steel tape, a glass epoxy substrate, or the like is used. When a conductive base material is used, the detection signal is reduced due to the eddy current loss caused by the base material. Even when a non-conductive base material such as glass epoxy is used, the generated magnetic flux passes through the base material, and if the mounting surface has conductivity, eddy current loss occurs there. Furthermore, if the mounting surface is not a uniform material over the entire scale (for example, electrically and magnetically different materials such as metal and air, such as when partially held by a metal material), it is detected by the position of the detector. The signal to be generated becomes uneven, and the accuracy deteriorates.
Therefore, for example, it is conceivable to reduce the influence of the mounting surface by thickening the base material or lining the back surface of the base material with a conductive material. However, the former cannot be miniaturized due to the increase in thickness, and the latter has a problem that the signal itself is attenuated by the backing material.
The following is a description of embodiments, with reference to the accompanying drawings.
(First embodiment)
The detection head 10 has a transceiver coil 50, a receiver coil 60 and so on. The transceiver coil 50 is a rectangular coil of which a longitudinal direction is the X-axis. As illustrated in
In the scale 20, a plurality of scale patterns 23 having a rectangular shape are arrayed in the fundamental period λ along the X-axis. Each of the scale patterns 23 is electromagnetically coupled with the transceiver coil 50 and is also electromagnetically coupled with the receiver coil 60.
The transmission signal generator 30 generates a transmission signal of a single phase AC and supplies the generated transmission signal to the transceiver coil 50. In this case, magnetic flux is generated in the transceiver coil 50. Thus, an electromotive current is generated in the plurality of scale patterns 23. The plurality of scale patterns 23 are electromagnetically coupled with the magnetic flux generated by the transceiver coil 50 and generate magnetic flux fluctuating in the X-axis direction in a predetermined spatial period. The magnetic flux generated by the scale patterns 23 generates an electromotive current in the receiver coil 60. The electromagnetic coupling among each coil fluctuates in accordance with the displacement amount of the detection head 10. Thereby, a sine wave signal of the same period as the fundamental period λ is obtained. Therefore, the receiver coil 60 detects a phase of the magnetic flux generated by the plurality of scale patterns 23. The displacement amount measurer 40 can use the sine wave signal as a digital amount of a minimum resolution by electrically interpolating the sine wave signal. Thereby, the displacement amount measurer 40 measures the displacement amount of the detection head 10.
In order to move the scale 20 relative to the measurement axis, the surface (back surface) on which the scale pattern is not formed is supported by a support member.
As illustrated in
The main body case 1 is integrally formed with a support collar 11 at substantially the center of the other end surface. A spindle protection cylinder 13 is located on the upper side of the main body case 1 in
The spindle 3 in which a head portion 31 at the upper end in
A plate-shaped holding member 41 is fixed to an inner peripheral wall 17 on one opened end side of the main body case 1 by a screw (not illustrated). As illustrated in
The electromagnetic induction encoder 100 includes the detection head 10 and the scale 20, and is configured to be able to detect an absolute displacement amount in the axial direction of the spindle 3. The detection head 10 is fitted in the notch 43 of the holding member 41 fixed to the main body case 1 in the vicinity of the spindle 3 and along the axial direction of the spindle 3. The scale 20 is arranged to face the detection head 10 with a predetermined gap, and is fixed to the spindle 3 via the support member 33.
On the front side (right side of
As the base material of the scale 20, for example, a steel tape, a glass epoxy substrate, a glass substrate, or the like is used. When a conductive base material is used, the detection signal is reduced due to the eddy current loss caused by the base material. Even when a non-conductive base material such as glass epoxy or glass is used, the generated magnetic flux passes through the base material, and if the mounting surface has conductivity, eddy current loss occurs there. Furthermore, if the mounting surface is not a uniform material over the entire scale (for example, electrically and magnetically different materials such as metal and air, such as when partially held by a metal material), it is detected by the position of the detector. The signal to be generated becomes uneven, and the accuracy deteriorates.
Therefore, for example, it is conceivable to reduce the influence of the mounting surface by thickening the base material or lining the back surface of the base material with a conductive material. However, the former cannot be miniaturized due to the increase in thickness, and the latter has a problem that the signal itself is attenuated by the backing material.
The scale 20 according to the present embodiment has a configuration capable of improving the signal detection accuracy while suppressing the increase in size. The details of the scale 20 will be described below.
The base material 21 is not particularly limited. The base material 21 is, for example, a self-standing plate made of a material other than metal. For example, metal oxides, organic substances, glass epoxy materials, glass and the like may be used as the base material 21. As the glass, a low expansion coefficient material such as quartz glass (synthetic fused silica) may be used.
The intermediate layer 22 is a soft magnetic material. As the intermediate layer 22, for example, iron, permalloy, silicon steel, sendust, soft ferrite, amorphous soft magnetic material, nanocrystalline soft magnetic material and the like can be used. The surface of the intermediate layer 22 opposite to the base material 21 is roughened.
The scale pattern 23 is made of a conductor such as a non-magnetic metal. As the scale pattern 23, for example, copper, aluminum, gold, silver, palladium, alloys containing them, austenitic stainless steel and the like can be used.
According to the present embodiment, since the scale pattern 23 is a conductor, an eddy current is generated in the scale pattern 23 when a magnetic flux that changes spatially and temporally is applied from the outside. Since the soft magnetic material has a high magnetic permeability, the intermediate layer 22 has a magnetic shielding property that does not allow magnetic flux to pass through. Therefore, leakage of the magnetic flux to the base material 21 can be suppressed. Next, an eddy current is also generated in the intermediate layer 22 which is a soft magnetic material, but since the surface of the intermediate layer 22 is roughened, the eddy current in the intermediate layer 22 becomes small, and the eddy current loss in the intermediate layer 22 becomes small. From the above, even if the scale 20 is not formed thick, leakage of magnetic flux is suppressed, eddy current loss is reduced, and signal detection accuracy is improved.
It is preferable to set a lower limit for the average thickness of the entire intermediate layer 22 from the viewpoint of forming a rough surface. The average thickness of the entire intermediate layer 22 is preferably 0.1 μm or more, more preferably 1 μm or more, and further preferably 2 μm or more.
It is preferable to set an upper limit on the average thickness of the entire intermediate layer 22 from the viewpoint of eddy current loss. The average thickness of the entire intermediate layer 22 is preferably 3 μm or less, more preferably 1 μm or less, and even more preferably 0.5 μm or less.
It is preferable to set a lower limit on the surface roughness Ra on the scale pattern 23 side of the intermediate layer 22 from the viewpoint of reducing the eddy current. The surface roughness Ra on the scale pattern 23 side of the intermediate layer 22 is preferably 10 nm or more, preferably 0.5 μm or more, and further preferably 1 μm or more. The surface roughness Ra is an arithmetic mean roughness.
It is preferable to set an upper limit on the surface roughness Ra on the scale pattern 23 side of the intermediate layer 22 from the viewpoint of grating pattern formation and signal strength gap characteristics. The surface roughness Ra on the scale pattern 23 side of the intermediate layer 22 is preferably 100 μm or less, preferably 50 μm or less, and further preferably 10 μm or less.
The above shows the general upper limit and lower limit, but as a preferable combination, when Cu is used as the metal gratings of the scale pattern 23, the height of the gratings is 8 μm or more and 18 μm or less. When the soft magnetic permalloy is used as the intermediate layer 22, a continuous film having a surface roughness Ra of 0.5 μm or more is required to reduce the influence of the eddy current. It is therefore preferable that the average thickness of the intermediate layer 22 is 1 to 3 μm.
Next, as illustrated in
Next, as illustrated in
Next, as illustrated in
(Second Embodiment) Next, a scale 20a according to a second embodiment will be described. The scale 20a can be used in place of the scale 20.
The metal tape material 21a is not particularly limited. The metal tape material 21a is, for example, a flexible metal film that is not self-standing. The metal tape material 21a is, for example, stainless steel, copper, Inconel, Invar, Super Invar, aluminum, or the like.
The intermediate layer 22a is a soft magnetic material. As the intermediate layer 22a, for example, iron, permalloy, silicon steel, sendust, soft ferrite, amorphous soft magnetic material, nanocrystalline soft magnetic material and the like can be used. The surface of the intermediate layer 22a opposite to the metal tape material 21a is roughened.
The scale pattern 23a is made of a conductor such as a non-magnetic metal. As the scale pattern 23a, for example, copper, aluminum, gold, silver, palladium, alloys containing them, austenitic stainless steel and the like can be used.
According to the present embodiment, since the scale pattern 23a is a conductor, an eddy current is generated in the scale pattern 23a when a magnetic flux that changes spatially and temporally is applied from the outside. Since the soft magnetic material has a high magnetic permeability, the intermediate layer 22a has a magnetic shielding property that does not allow magnetic flux to pass through. Therefore, leakage of the magnetic flux to the metal tape material 21a can be suppressed. Next, an eddy current is also generated in the intermediate layer 22a, which is a soft magnetic material, but since the surface of the intermediate layer 22a is roughened, the eddy current in the intermediate layer 22a becomes small, and the eddy current loss in the intermediate layer 22a becomes small. From the above, even if the scale 20a is not formed thick, leakage of magnetic flux is suppressed, eddy current loss is reduced, and signal detection accuracy is improved.
It is preferable to set a lower limit for the average thickness of the entire intermediate layer 22a from the viewpoint of forming a rough surface. The average thickness of the entire intermediate layer 22a is preferably 0.1 μm or more, more preferably 1 μm or more, and further preferably 2 μm or more.
It is preferable to set an upper limit on the average thickness of the entire intermediate layer 22a from the viewpoint of eddy current loss. The average thickness of the entire intermediate layer 22a is preferably 100 μm or less, more preferably 10 μm or less, and even more preferably 0.5 μm or less.
It is preferable to set a lower limit on the surface roughness Ra on the scale pattern 23a side of the intermediate layer 22a from the viewpoint of reducing the eddy current. The surface roughness Ra on the scale pattern 23a side of the intermediate layer 22a is preferably 10 nm or more, preferably 0.5 μm or more, and further preferably 1 μm or more.
It is preferable to set an upper limit on the surface roughness Ra on the scale pattern 23a side of the intermediate layer 22a from the viewpoint of grating pattern formation and signal strength gap characteristics. The surface roughness Ra on the scale pattern 23a side of the intermediate layer 22a is preferably 100 μm or less, preferably 50 μm or less, and even more preferably 10 μm or less.
The above shows the general upper and lower limits, but as a preferable combination, when Cu is used as the metal gratings of the scale pattern 23a, the height of the gratings is 8 μm or more and 18 μm or less. When soft magnetic permalloy is used as the intermediate layer 22a, a continuous film having a surface roughness Ra of 0.5 μm or more is required to reduce the influence of eddy current, and therefore the average thickness of the intermediate layer 22a is preferably 1 to 3 μm. However, when the intermediate layer 22a is used as the clad material, the average thickness of the intermediate layer 22a is preferably 0.1 mm or less.
Next, as illustrated in
Since the manufacturing method of
(Modified Embodiment 1) The intermediate layer under the scale pattern does not have to be roughened.
(Modified Embodiment 2)
The present invention is not limited to the specifically disclosed embodiments and variations but may include other embodiments and variations without departing from the scope of the present invention.
Number | Date | Country | Kind |
---|---|---|---|
2021-022674 | Feb 2021 | JP | national |
2022-006327 | Jan 2022 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
7358724 | Taylor | Apr 2008 | B2 |
20070031705 | Hattori | Feb 2007 | A1 |
20120266478 | Frank et al. | Oct 2012 | A1 |
20130222198 | Kojima | Aug 2013 | A1 |
20160054151 | Nozawa | Feb 2016 | A1 |
20170227380 | Musha | Aug 2017 | A1 |
20170303405 | Fukuchi | Oct 2017 | A1 |
20220206087 | Endo | Jun 2022 | A1 |
Number | Date | Country |
---|---|---|
2004-294225 | Oct 2004 | JP |
3128628 | Jan 2007 | JP |
3136959 | Nov 2007 | JP |
2012-225912 | Nov 2012 | JP |
2016-044967 | Apr 2016 | JP |
6172898 | Aug 2017 | JP |
Number | Date | Country | |
---|---|---|---|
20220268601 A1 | Aug 2022 | US |