LASER MEASURING SYSTEM AND METHOD FOR TURNING MACHINE
Technical Field
This invention relates to laser measuring systems for machine tools.
Background Art There are a number of factors which influence the dimensional accuracy of a workpiece which can be achieved in a turning operation. Illustrative of such factors, are: the accuracy of the mechanisms which control machine tool slide movement; the deformation of the machine tool and the workpiece due to cutting force; the heat generated during cutting; and the extent of tool wear. The prior art has recognized that the aforementioned unpredictable factors are not susceptible to effective operator monitoring and in response has provided laser optical devices adapted to generate beams which impinge on the periphery of a workpiece, such as shown in U.S. Patent Nos. 3,749,500 and 3,812,376. Such prior art systems have a drawback in that they require positioning units which can be relatively complex. In addition, such systems do not offer the many advantages of laser interferometry.
Currently, some numerically controlled machine tools employ laser interferometry to precisely position the slides of the machine to obtain superior resolution. Typically such systems embody a laser source and one or more receivers, interferometer and retroflector sets. However, laser interferometry has not been adapted to directly measure the dimensions of a turned workpiece.
Disclosure of the Invention In accordance with the invention, laser interferometry is employed to directly measure the interior or
exterior dimensions of a turned workpiece. The only positioning apparatus required for a system is that which is typically incorporated in a two axis lathe or chucker. In brief, a lathe or chucker, having a tool carrying turret mounted upon an X-axis slide movable perpendicular to the spindle axis, is provided with a gage head incorporating a reflector adapted to be positioned for measurement by an indexing rotation of the turret to a particular index station. An interferometer is fixedly mounted upon a Z-axis slide (which carries the X-axis slide) movable parallel to the spindle axis. The interferometer is aligned with the reflector in the gage head when the turret is in the measurement index station and is always aligned with a laser source and receiver mounted upon the machine tool frame or adjacent thereto. The chuck is encircled by a master reference collar of known diameter (internal as well as external) whereby a reference point may be established when the gage head engages the inner or outer periphery of the collar.
A measuring system of the invention may be utilized to determine and compensate for excessive tool wear. For example, a correction signal could be transmitted to the slide position control device of the machine tool when the machining error is greater than a specified dimensional tolerance. In addition, a system of the invention could be employed to determine size of a part just prior to or upon the completion of a final finishing operation. It will of course be appreciated that, under all circumstances, the accuracy of a measuring system of the invention does not depend upon the precision with which the machine tool slides are positioned but is independent thereof.
Accordingly, it is a primary object of the invention to provide a system for measuring the dimensions of a turned workpiece which utilizes laser interferometry.
Another object is to provide a laser interferometer based system and method for measuring the dimensions of a workpiece machined upon a two axis turret lathe wherein the turret thereof includes a gage head incorporating a reflector and the axial slide has an interferometer- mounted thereupon. These and other objects and advantages of the invention will become more readily apparent from the following detailed description when taken in conjunction with the accompanying drawings, in which:
Brief Description of Drawings FIGURE 1 is a schematic diagram of a preferred embodiment of a laser measuring system of the invention.
FIGURE 2 is a block diagram depicting the basic elements of the laser transducer and the receiver of FIGURE 1 and their relationship to other components of the system.
FIGURE 3 is a schematic view of the linear interferometer and retroflector arrangement of FIGURE 1 illustrating the beam paths and the principle of operation. FIGURE 4 is a side elevational view, partly in section, of the gage head of FIGURE 1.
FIGURE 5 is a front elevational view of the gage head, partly in section, taken substantially along the line 5-5 of FIGURE 4. FIGURE 6 is a top view of the gage head, taken substantially along the line 6-6 of FIGURE 4.
FIGURE 7 is a rear elevational view of the gage's roller slide assembly, per se, taken substantially along the line 7-7 of FIGURE 4.
FIGURE 8 is a side elevational view, partly in section, of the roller slide assembly, taken substantially along the line 8-8 of FIGURE 7.
FIGURE 9 is a sectional view of the roller slide assembly, taken substantially along the line 9-9 of FIGURE 7.
FIGURE 10 is a perspective view showing the engagement between the right side rail and a V-way of FIGURE 9.
Best Mode of Carrying Out the Invention
Referring to FIGURE 1, there is shown a numerically controlled lathe or chucker, generally shown at 10, incorporating a measuring system of the invention. The particular form of lathe shown embodies a vertically indexing turret 12 capable of movement along two axes. This type of lathe Csometimes termed a universal lathe) is well-known in the art and an example thereof is illustrated in U.S. Patent No. 3,191,470. It will be appreciated that although the invention is specifically illustrated and described with reference to a machine tool having a vertically indexing turret, it is also applicable to other lathes or chuckers.
The lathe 10 embodies a frame 14, the outline of which is shown by phantom lines. Mounted upon the frame for rotation about a horizontal axis is a spindle 16 having a workpiece holding chuck 18 attached thereto. The chuck also has a master reference collar 20 (discussed hereinafter) mounted upon the chuck in encircling relationship thereto. A pair of longitudinally extending ways 22 and 24 are secured to frame 14 for guiding the longitudinal motion (Z-axis) of a Z-axis slide 26. Carried by the Z-axis slide 26 are ways 28 and 30 upon which is slideably mounted an χ-axis slide 32. The χ-axis is, of course, perpendicular to both
the Z-axis and the chuck or workpiece axis . The turret 12 is mounted for rotation upon the X-axis slide 32 to a plurality of discrete index stations about an axis parallel to the chuck axis. The turret may be configured to carry a plurality of turning tools, a plurality of boring tools or both turning tools and boring tools. Slide positioning and turret indexing are controlled by a computer numerical control unit (CNC) 34 which commands all machine tool operations. A gage head, generally indicated at 36, is fixedly mounted upon the turret 12 at an index station by means of a bracket 38. The heart of the gage head is a reflector 40 (which in this case is a retroflector) which is movable with a gage arm 42 having O.D. (Outside diameter) and I.D. (Inside diameter) tips or probes 44 and 46, respectively. In the measuring index station depicted in FIGURE 1, the retroflector 40 is in precise alignment with an interferometer 48 (which in this case is a linear interferometer). The inter ferometer 48 is rigidly secured to the Z-axis slide 26 by means of an L-shaped mounting arm 50. Hence, any movement of the Z-axis slide 26 when the turret is at the measuring index station does not in any manner affect the alignment of the interferometer and the reflector 40. In like manner, movement of the X-axis slide does not alter alignment but only the distance between the interferometer 48 and the reflector 40.
A laser transducer 52 is the source of the laser beam directed at the interferometer 48, the outgoing main beam being shown by a dashed line. A portion of the outgoing main beam (shown by dashed line) is directed by the interferometer to the reflector 40 which sends a return beam (solid line) back to the interferometer in a latterally offset and parallel relationship. The return beam from the reflector interferes with another portion of the main beam in the interferometer
to produce a return main beam (solid line) directed at a receiver 54. The return main beam is offset from and parallel to the outgoing main beam. The receiver 54, which senses the main return beam generates an RF measurement signal which is applied to a pulse converter 56. The receiver also incorporates a means to verify proper alignment. The pulse converter 56 also receives an RF reference signal from the laser transducer 52. The RF measurement and reference signals are transformed by the Pulse converter 56 into displacement information in pulse format (e.g., up pulses and down pulses) which can be utilized, for example, by a reversible counter dot shown) in the CNC unit 34. A power supply 58 functions to provide the laser transducer 52 with a positive voltage D.C. supply and a. negative voltage D.C. supply.
The basic optical elements of the measuring system of the invention, i.e., the retrofleetors, linear interferometer, Laser tranducer, receiver and pulse converter units are all commercially available items manufactured, for example, by the Hewlett Packard Co. The detailed construction of the aforementioned elements, of course, forms no part of the present invention; and it will be understood that other suitable elements could be employed in a measuring system of the invention. However, the laser transducer, receiver linear interferometer and retroflector will be cursorily described to facilitate a better understanding of the present invention. Turning to FIGURE 2, the Laser transducer 52 and the receiver 54 are depicted in block diagram form. The laser transducer 52 comprises a low power Helium- Neon laser 60 which emits a coherent light beam composed of two slightly different optical frequencies, f1 and f2 of opposite circular polarizations. After conversion to orthogonal linear polarizations, the beam is expande
and collimated at 62 and then directed to the reference beam splitter 64 where a small fraction of both frequencies is split off. The downwardly directed portion 66 of the beam is used both to generate a reference frequency and to provide an error signal to the laser cavity tuning system. Beam portion 66 impinges upon a polarizing beam splitter 88 which splits beam 66 into a portion directed to a photodetector 70 and a portion directed at a mirror 72, which, in turn, reflects the portion to another photodetector 74. The output signal of photodetector 70 is directed to an input terminal of D.C. amplifier 76. The output signal of photodetector 74 is directed both to another input terminal of D.C. amplifier 76 and an AC amplifier 78, the latter of which generates the reference signal f1-f2 which is one of the inputs to the pulse converter 56. The output of the D.C. amplifier 76 (the difference in the amplitudes of f1 and f2) is applied to a tuning regulator 80 which is connected to the laser 60. The receiver 54, which senses the main return beam via a photodetector 82, includes an amplifier 84, connected thereto, which produces the measurement signal
Relative motion between the linear interferometer 48 and the retroflector 40 causes a doppler shift
in the difference frequency
(f1-f2) measured by the receiver 54. This Doppler modulated difference frequency
is, of course, amplified by amplifier 84 to become the measurement signal . The pulse converter 56 receives the reference and measurement signals and compares them cycle-by-cycle. The pulse converter 56 produces an appropriate up ordown output pulse whenever one of the signals is one-half cycle ahead of or behind the other. Each pulse corresponds to a retroflector movement of one-quarter wavelength of light. These pulses are directed to
the computer numerical control for counting therein.
With reference to FIGURE 3, the linear interferometer 48 and its relationship to the retroflector 40 are displayed schematically. The outgoing main beam exiting from the laser transducer 52 is split at the surface of a polarizing beam splitter 48a with, one frequency (f1) reflected to a reference cube corner 48b (i.e., a retroflector) mounted on the interferometer housing 48c. The other frequency (f2) is transmitted to the retroflector 40 and returned
parallel to, but displaced from, the outgoing beam. Both return beams interfere with each other at point 48d from where both frequencies are directed back along a common axis to the receiver as the main return beam. The retroflectors are comprised by high quality cube-corners which have the property that incident laser beams are reflected parallel to the incoming direction within seconds of arc and retain their coherence. Such retroflectors are notably advantageous in that their alignment during installation is not subjected to critical tolerances.
The detailed construction of the gage head 36 is shown in FIGURES 4-10. The gage head includes a housing 86 which has mounting bracket 38 secured thereto whereby it may be attached to an index station of the turret 12. The retroflector 40 is cradled within a support90 so as to be upwardly facing to receive and emit light beams through an aperture 86a in the top of the housing 86. The support 90 is attached by means of screws 92 to a slide 94 which is axially movable vertically relative to the housing 86. To the surface of the slide 94 is attached a depending shaft 96 which is secured to the gage arm 42 (which carries probes 44 and 46) at its lower extremity. Shaft 96 extendsdownwardly through an opening 86b in the lower portion
of the housing 86 and is encircled by a seal 98 attached to the base of the housing for preventing the entry of contaminating fluids, such as cutting coolant. Hence, it will be noted that the gage arm 42, shaft 96, slide 94, support 90 and retroflector 40 form an integral structure and are movable in unison relative to housing 86 when the probes 44 and 46 are contacted.
In order to prevent contaminants from entering aperture 86a when the gage is not in use, a cover 100 is pivotally mounted upon a pin 102 supported by a bracket 104 attached to the front of the housing. The bracket 104 and the cover 100 incorporate latterally projecting pins 106 and 108 for mounting springs which hold the cover 100 closed or open. A handle 110 is provided for opening the cover; and a stop 112 , which is secured to the housing, limits the extent of its opening. When closed, the cover rests upon a gasket 114 which acts to seal out contaminants.
The slide 94 is mounted for axial sliding movement upon a base 116 which is securely fastened to the housing 86 by means of screws 118. The slide and base assembly is shown in detail in FIGURES 7,8,9, and 10. The slide 94 comprises a table 120 having longitudinal sides 122 and 124 and end plates 126 and 128 which together define an open box-like structure. As best shown in FIGURES 7 and 8 , the end plates include pins 130 and 132 inserted therein which function as mounting guides for springs 134 and 136. The springs are mounted in cavities 138 and 140 in the base 116 for biasing the slide 94 to the neutral or intermediate position depicted when displaced therefrom. The end plates also include stop bolts 142 and 144 for limiting slide travel in both upward and downward directions.
Turning to FIGURE 9, it may be seen that the base includes two roller straps 146 and 148 attached to the body thereof by mounting screws 150 and 152. The slide
also incorporates a pair of V-ways 154 and 156 secured to the table 120 by mounting screws similar to those associated with the roller strips. The sliding interengagement between the V-ways and roller strips is occasioned by respective axial arrays of crossed roller bearings 158. As shown in FIGURE 10 the roller bearings 158 in each strip have alternately opposed axes. Screw 160 allows for preload adjustment. A slide assembly, as shown, permits superior travel accuracies to be attained. The basic elements of such a slide assembly are commercially available from Micro Slides Inc. of Westbury, New York.
In a typical OD operation, the workpiece is machined to final rough OD dimensions. The turret 12 is then indexed, (i.e., rotated) to the measuring station whereby the retroflector 40 is aligned with the linear interferometer 48 and the gage head 36 is also aligned with a diameter of the workpiece. The gage head 36 is then moved over the master references collar 20 by moving the Z-axis slide 26 to the left as viewed in FIGURE 1 until the probe 44 on the gage arm 42 is aligned with the diameter of the collar. Next, the X-axis slide is moved downwardly until the probe 44 firmly engages the outer periphery of the collar 20. The cover 100 on the gage head 36 is now opened to expose the retroflector 40. Also, at the same time, a cover (should one be provided) on the linear interferometer is opened. The opening of covers could be performed manually or by automatic means such as air cylinders or solenoids. Alignment is now verified by a signal (e.g., a DC voltage or warning light) from the receiver 54 which indicates that the main return beam is being properly received. The distance A is subsequently preset into a memory register in the CNC unit 34 whereupon workpiece measurements are ready to be taken.
The Z-axis slide 26 is then moved to the right until the probe 44 overlies that axial station on the workpiece where the diameter is to be measured. Next, the X-axis slide 32 moves downwardly toward the workpiece, as viewed in FIGURE 1. During this downward travel, the distance between the linear interferometer 48 and retroflector 40 is continuously increasing, thereby causing the pulse converter 56 to issue forth a stream of pulses to the CNC unit 34, the pulses func tioning to decrement the number A stored in the CNC unit. When pulse generation by the pulse converter 56 terminates during X-axis slide movement, the probe 44 has engaged the workpiece and the number in the CNC unit is an extremely precise measurement of a workpiece OD dimension. Similar OD measurements may be taken at other axial stations by simple slide movement without the need for placing the probe 44 again upon the collar 20. During such latter mentioned movements, the pulse converter will, of course, generate incrementing or decrementing pulses to the CNC unit register. Various measurements at different axial stations may be transferred to respective memory locations in the CNC unit.
The gage head is then removed from the workpiece (e.g., to a home position). The part program is then adjusted for the difference in the programmed and measured dimensions and final workpiece finishing is then completed. If desired, final workpiece dimensions may be checked as previously described. Any excessive variation between measured diameters and programmed diameters may indicate excessive tool wear or some other difficulty and corrective action is accordingly mandated.
Measurement of internal diameters may be made by using a similar procedure and contacting the inner periphery of the workpiece with probe 46. It will be noted that for such measurements, an interior reference surface could be provided on the collar, or alternatively
the distance between the tips of the probes could be precisely measured.
At the conclusion of a measuring operation, all covers are closed and the laser transducers and receivers turned off. Cutting cycles are resumed using measured values to properly position the X-axis slide. It will, of course, be understood that all measurements are predicated on the continuity of the laser alignment signal. Loss of this signal during measuring will render subsequent readings unreliable.
Obviously, many modifications and variations are possible in light of the above teachings without departing from the scope or spirit of the invention as defined in the appended claims. For example, a system of the invention could be associated with a lathe having a dual or single level turret mounted on the X-axis slide and rotatable about an axis parallel to the X-axis and intersecting the spindle axis in ortho- ginal or canted relationship thereto. Such a lathe is shown in U.S. Patent No. 3,878,742. In addition, the invention could be utilized with a lathe as shown in U.S. Patent No. 3,750,245. Furthermore it is within the ambit of the invention to utilize other forms of gage heads, reflectors or interferometers with appropriate positioning of the receiver and laser transducer.