The present application claims priority under 35 U.S.C. § 119 of Japanese Application No. 2017-217998, filed on Nov. 13, 2017, the disclosure of which is expressly incorporated by reference herein in its entirety.
The present invention relates to a simple roundness measuring device that can be used with convenience, such as a compact measuring device.
A roundness measuring device is an example of a measuring device that measures the roundness of a circular column, a cylindrical tube, and the like (Japanese Patent Laid-open Publication Nos. 2016-166766 and 2016-151292). The roundness measuring device is provided with a rotary table and a coordinate measurer. The rotary table is provided with a placement stage on which a measured object (measurable object) is placed, and a rotary driver that rotates the placement stage. The coordinate measurer is provided with a probe that detects a surface of the measured object and a displacement mechanism that displaces the probe two- or three-dimensionally. In addition, the displacement mechanism is provided with a plurality of encoders that detect an amount or angle of displacement.
Of course, a roundness measuring device is necessary for making fine measurements of the roundness of a measured object, but such devices inevitably become large in scale and locations where the devices can be installed are limited. Accordingly, in order to use a roundness measuring device, the measured object must be taken to a place where a roundness measuring device is located. In addition, using a roundness measuring device requires quite cumbersome advance preparations. For example, using a rotary table requires adjusting air bearings or adjusting an inclination and/or position of a placement stage (centering). Moreover, the rotary table rotates during measurement, and therefore there is no alternative but to wait for the rotary table to complete at least one rotation. There may also be a desire to occasionally check roundness in a simple way while processing a work piece W, but using a roundness measuring device for each desired check incurs a significant loss of time and effort.
The present invention provides a simple roundness measuring device that can be used with convenience, such as a compact measuring device.
A roundness measuring device according to the present invention includes an annular ring portion, and a plurality of displacement sensors provided to the ring portion at predetermined intervals. The displacement sensors are arranged such that lines along which measurement axes of the displacement sensors extend intersect at a single point.
In the present invention, preferably, there are at least eight of the displacement sensors.
In the present invention, preferably, the displacement sensor includes a spindle having a stylus head at a distal end, the spindle being provided so as to be capable of advancing and retreating in an axis direction. The displacement sensor is preferably configured so as to detect displacement of the spindle and output the displacement as measurement data. The displacement sensor is preferably arranged such that a projection direction of the spindle is oriented toward an interior of the ring portion.
A cylindricity measuring device according to the present invention is configured by arranging a plurality of the roundness measuring devices to be stacked on top of each other in a vertical direction.
A roundness measuring method according to the present invention is a roundness measuring method using the roundness measuring device above, and includes: calibration, in which the displacement sensors are set to zero with a master that is a perfect circle and serves as a reference; measurement, in which a measured object is measured by the displacement sensors; eccentricity calculation, in which offset between a position of the master during calibration and a position of the measured object during measurement is calculated as eccentricity; and roundness calculation, in which the eccentricity obtained in the eccentricity calculation is subtracted from measured values of the displacement sensors obtained in the measurement, and offset of the measured object from a perfect circle is calculated.
In the present invention, preferably, in the eccentricity calculation, when the eccentricity is split into an X axis component and a Y axis component and expressed by (ΔCx, ΔCy), the eccentricity (ΔCx, ΔCy) is found by
ΔCx=2×(Σi=1i=n{di·cos θi})/n
ΔCy=2×(Σi=1i=n{di·sin θi})/n
Here, di is a measured value for each of the displacement sensors. Also, the X axis is treated as a reference line, and an angle formed by the X axis and the measurement axis of each displacement sensor is represented by θi.
The present invention is further described in the detailed description which follows, in reference to the noted plurality of drawings by way of non-limiting examples of exemplary embodiments of the present invention, in which like reference numerals represent similar parts throughout the several views of the drawings, and wherein:
The particulars shown herein are by way of example and for purposes of illustrative discussion of the embodiments of the present invention only and are presented in the cause of providing what is believed to be the most useful and readily understood description of the principles and conceptual aspects of the present invention. In this regard, no attempt is made to show structural details of the present invention in more detail than is necessary for the fundamental understanding of the present invention, the description taken with the drawings making apparent to those skilled in the art how the forms of the present invention may be embodied in practice.
An embodiment of the present invention is illustrated in the drawings and is described with reference to the reference signs assigned to each component in the drawings.
The measurer 200 includes an annular ring portion 210 and electric micrometers (displacement sensors) 231 to 238, which are provided on the ring portion 210 at predetermined angular intervals.
The ring portion (ring) 210 is a ring having a diameter that is a size larger than the measured object. The ring portion 210 can be substantially circular and does not need to be a minutely perfect circle. In addition, the ring portion 210 may have an angular shape rather than being circular, and could for example be octagonal. Also, a slit may be formed in a portion of the ring portion 210, and the ring portion 210 may be capable of opening and closing or of separating.
The electric micrometers 231 to 238 each include a spindle 222 which advances and retreats in an axis direction through an interior of a tubular stem 221. A stylus head 223 is provided to a distal end of the spindle 222. The electric micrometers 231 to 238 detect the displacement of the spindles 222 advancing and retreating in the axis direction through the interior of the stems 221 and output the displacement as measurement data.
An X axis runs from right to left in
θ1=0°
θ2=45°
θ3=90°
θ4=135°
θ5=180°
θ6=225°
θ7=270°
θ8=315°
In the design, the electric micrometers 231 to 238 are arranged at 45° intervals, but an actual product may not necessarily achieve accurate 45° intervals. In a case where the angles θ1 to θ8 of the electric micrometers 231 to 238 of the actual product differ from the design values, preferably the angle is actually measured in order to accurately find θ1 to θ8.
The measured value from each of the electric micrometers 231 to 238 is wired or wirelessly transmitted to the calculator 300, and computation is performed by the calculator 300. The calculator 300 is, for example, a personal computer (specifically, a CPU and memory), and calculates the roundness of the measured object by executing a roundness calculation program. (So long as a device is capable of executing the roundness calculation program, a smart phone or tablet may of course be substituted for the personal computer.) Next, a method of using a roundness measuring device is described, including a specific processing protocol performed by the calculator 300 (roundness calculation program).
Measurement Procedure
At this point, the master MW is preferably at the exact center of the ring portion 210, but there is no issue even if the master MW is offset from the exact center. In other words, the position of the master MW at the time of zero-setting may be any position.
The measured value for each of the electric micrometers 231 to 238 is expressed by Di, where i is an integer from 1 to 8. Specifically, the measured value of the first electric micrometer 231 is expressed by D1, the measured value of the second electric micrometer 232 is expressed by D2, and so on. When set to zero, the values are as follows:
D1=0.00
D2=0.00
D3=0.00
D4=0.00
D5=0.00
D6=0.00
D7=0.00
D8=0.00
This zero-set calibration is preferably performed each time, but there is no need to perform zero-set calibration each time so long as the values are stored in the memory.
Next, the master MW is removed and the measured object (work piece) W is set in the measurer 200 (ST112).
Then, the stylus head 223 of each of the electric micrometers 231 to 238 is confirmed as being in contact with a side surface of the work piece W and a measured value of each of the electric micrometers 231 to 238 is acquired (ST113). The measured values of the first electric micrometer 231 through the eighth electric micrometer 238 are designated as d1 to d8.
D1=d1
D2=d2
D3=d3
D4=d4
D5=d5
D6=d6
D7=d7
D8=d8
The measured values d1 to d8 are imported into the calculator 300.
Next, the “eccentricity” between the master MW and the work piece W at the time of measurement is found (ST114). As illustrated in
ΔCx=2×(Σi=1i=8{di·cos θi})/8
ΔCy=2×(Σi=1i=8{di·sin θi})/8
Then, when the eccentricity is subtracted from the measured value di of each of the electric micrometers 231 to 238, a difference in shape between the work piece W and the master MW is extracted. Specifically, the roundness of the work piece W is found (ST115). Here, the difference in shape between the work piece W and the master MW at the position of the first electric micrometer 231 is expressed as ΔR1. Likewise, the difference in shape between the work piece W and the master MW at the position of the ith electric micrometer 231 to 238 is expressed as ΔRi, where i is 1 to 8.
ΔR1=d1−(ΔCx·cos θ1+ΔCy·sin θ1)
ΔR2=d2−(ΔCx·cos θ2+ΔCy·sin θ2)
ΔR3=d3−(ΔCx·cos θ3+ΔCy·sin θ3)
ΔR4=d4−(ΔCx·cos θ4+ΔCy·sin θ4)
ΔR5=d5−(ΔCx·cos θ5+ΔCy·sin θ5)
ΔR6=d6−(ΔCx·cos θ6+ΔCy·sin θ6)
ΔR7=d7−(ΔCx·cos θ7+ΔCy·sin θ7)
ΔR8=d8−(ΔCx·cos θ8+ΔCy·sin θ8)
From among ΔR1 to ΔR8 which are found in this way, the maximum value is designated Rmax and the minimum value is designated Rmin.
Rmax=MAX{ΔR1,ΔR2,ΔR3,ΔR4,ΔR5,ΔR6,ΔR7,ΔR8}
Rmin=MIN{ΔR1,ΔR2,ΔR3,ΔR4,ΔR5,ΔR6,ΔR7,ΔR8}
Then, the roundness is found as the difference between Rmax and Rmin.
Roundness=Rmax−Rmin
There are also other ways to define the roundness. Even in such cases, the geometric variance of the work piece W relative to a perfect circle is found using ΔR1 to ΔR8, and therefore any appropriate calculation can be performed in accordance with the definition of roundness.
In the foregoing description, the position of the master MW during zero-setting is arbitrary, as is the position of the work piece W during work piece measurement. This lack of any need whatsoever for an alignment task ties into the convenience of the roundness measuring device 100 according to the present embodiment. The theoretical point that enables such a simple roundness measurement lies in the fact that a deviation of the work piece W from a perfect circle can be extracted by finding the eccentricity ΔC (ΔCx, ΔCy) between the master MW at the time of zero-setting and the work piece W at the time of measurement, and subtracting the eccentricity ΔC (ΔCx, ΔCy) from the measured value di. A supplemental description of this point is given hereafter.
In
In this example, the coefficient k=1 expresses the eccentricity. After each sensor is set to zero with the master MW, when the work piece W is measured, the measured value of each sensor is acquired as d1 to d8. In view of this, using discrete sampling data (d1 to d8) in the Fourier series for D(θ) can be considered a discrete Fourier transform. Applying this yields the eccentricity as follows.
a1=ΔCx=f(D(θ)·cos θ)dθ
And when discretized:
a1=ΔCx=2×(Σi=1i=8{di·cos θi})/8
Similarly,
b1=ΔCy=f(D(θ)·sin θ)d0
And when discretized:
b1=ΔCy=2×(Σi=1i=8{di·sin θi})/8
In this connection, a0=2×(Σi=1i=8{di})/8, which expresses the difference in size between the master and the work piece.
Then, when the eccentricity is subtracted from the measured value di of each of the electric micrometers 231 to 238, the difference in shape between the work piece W and the master MW is extracted. Specifically, the roundness of the work piece W is found (ST115).
A shape measuring device with measuring devices arranged in a ring shape is described in Japanese Patent Laid-open Publication No. S62-191709 and Japanese Examined Utility Model Publication Nos. S57-037406 and S58-189909, and superficially these devices appear structurally similar to the present embodiment. However, none of these documents provide any disclosure whatever of zero-setting, the method of acquiring the eccentricity, calculating the shape of the work piece by subtracting the eccentricity, or the roundness calculation based on these principles according to the present embodiment.
In the embodiment described above, an example is described of the roundness measuring device 100 having eight electric micrometers (displacement sensors) arranged in a circle at 45° intervals. With eight electric micrometers (displacement sensors) at 45° intervals, in theory an elliptical component of the work piece W can be found, which should be sufficient for a simple evaluation of roundness. However, the number of displacement sensors can, of course, be further increased.
In the embodiment described above, an example is given of the roundness measuring device 100 in which the roundness of the external diameter of the work piece W is measured. However, reversing the projection direction of the spindles 222 of the electric micrometers yields a roundness measuring device that measures the roundness of an internal diameter of a cylindrical tube. (An embodiment according to the second modification is referred to as an internal roundness measuring device. An embodiment of the roundness measuring device according to the first embodiment is referred to as an external roundness measuring device.) If the electric micrometers are configured so as to enable measurement in an inward direction of the ring portion as well as an outward direction, the roundness of both the external diameter and the internal diameter could be measured. This could be adopted by providing two spindles for each electric micrometer with one for inward projection and one for outward projection.
Furthermore, as illustrated in
A plurality of internal roundness measuring devices in which the projection direction of the spindles 222 of the electric micrometers has been reversed, as in the second modification, can also be stacked on top of each other. In such a case, the degree to which an interior circle deviates can be readily understood. An embodiment according to this example is referred to as an internal cylindricity measuring device.
Of course, a configuration is also possible in which an internal cylindricity measuring device is arranged inside the ring of an external cylindricity measuring device. This makes possible a simple cylindricity measuring device that measures the cylindricity (degree of coaxiality) of the cylindrical work piece by simultaneously measuring both the interior and exterior of the cylindrical work piece.
As illustrated in
In addition, the roundness measuring device is preferably used in a horizontal state. Therefore, a level (a simple spirit level is sufficient) can be added. For example, X direction and Y direction levels can both be provided to the ring portion.
Moreover, the present invention is not limited to the embodiment described above, and may be modified as needed without departing from the scope of the present invention. In the embodiment described above, an electric micrometer having a linear drive spindle is given as an example of a displacement sensor. However, the electric micrometer can be replaced by a lever-type test indicator, or can also be replaced by a laser range finder (non-contact sensor). The first embodiment and first to fourth modifications described above can, of course, be combined as appropriate.
It is noted that the foregoing examples have been provided merely for the purpose of explanation and are in no way to be construed as limiting of the present invention. While the present invention has been described with reference to exemplary embodiments, it is understood that the words which have been used herein are words of description and illustration, rather than words of limitation. Changes may be made, within the purview of the appended claims, as presently stated and as amended, without departing from the scope and spirit of the present invention in its aspects. Although the present invention has been described herein with reference to particular structures, materials and embodiments, the present invention is not intended to be limited to the particulars disclosed herein; rather, the present invention extends to all functionally equivalent structures, methods and uses, such as are within the scope of the appended claims.
The present invention is not limited to the above described embodiments, and various variations and modifications may be possible without departing from the scope of the present invention.
Number | Date | Country | Kind |
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2017-217998 | Nov 2017 | JP | national |