Note: Descriptions are shown in the official language in which they were submitted.
BACKGROUND_OF TIIE INVENTION
Field of the Invention
This invention relates to a system for optically detecting flaws in
bottles, CllpS, bowls, cans, and various other containers or like articles. A
more specific aspect of the invention concerns such a system for automatically
detecting flaws in used and cleaned bottles for beverages or liquors, prior to
the refilling of such bottles. By the term l'flaws" are meant cracks, breaches,
fissures, scratches, adhering foreign matter, and any other imperfections de-
tectable by the system of this invention.
D ription of the Prior Art
Bottles for some beverages or liquors are recycled; that is, they arerecovered from the consumers, cleaned, and put to reuse. Bottle cleaning ma-
chines in current use are such, however, that they may not necessarily make
the bottles free of all foreign matter firmly sticking thereto. Further, some
bottles may have cracks and similar defects formed therein. All such faulty
bottles must be discriminated from flawless ones before they are refilled, and
should not be reused from the standpoint of hygiene or of the forestallment of
actual or potential danger.
According to a typical conventional apparatus for the detection of bot-
tle flaws, a light source ~mderlying a bottle to be tested irradiates the com-
plete surface of its bottom. Disposed at the mouth of the bottle, a photode-
tector senses the presence of a flaw, if any, in the bottle from the intensity
of the incident light that has passed through its bottom.
An objection to this prior art apparatus as its comparatively poor ab-
ility of detecting localized flaws and those lying adjacent to the bottom per-
imeter or on the side wall of the bottle. This drawback arises principally
from the application of light only to the bottom of the bottle and from the
insufficient intensity of the light. Additionally, since the light falls on
the bottle at one time, the photodetector is required to sense i-ts possible
flaw from a small change in the incident radiation.
Another objection to the prior art apparatus is its inability, or at
least very poor ability, to detect such transparent foreign matter as cello-
phane adhering
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to a bottle. This is an inevltable result of i.ts operating principle of sens-
ing flaws in a bo-ttle from the intensity of the light that has penetrated its
bot-tom.
S~mary of the Invention
It is an object of this invention to provide an improved system for
accurately detecting all sorts of possible flaws in bottles and other articles.
Another object of the invention is to provide such a system capable
of detecting flaws lying not only at the bottom but also on the side wall of a
bottle or the like.
A further object of the invention is to provide such a system which
correctly responds even to transparent foreign matter sticking to a bottle or
the like in any position thereon.
A still further object of the invention is to provide such a flaw
detecting system which works even under bright ambi.ent light without loss or
diminution of the above noted advantages.
In accordance with the present invention, there is provided in a
system for detecting flaws in bottles or like articles having a neck or con-
stricted area near the top thereof, said system including a light beam generat-
ing means, a device for causing scanning motion of said light beam through an
article to be tested, and a photoelectric detecting means adaptea for detect-
ing variation of said scanned light beam thereby to detect a flaw in the
article; the improvement wherein said system comprises: a laser beam generat-
ing means for generating a narrow beam of light; mirror means comprising two
mirrors having respective reflective surfaces arranged so as to reflec-t said
laser beam one after the other and supported so as to be os-ci]lated about
respective axes at right angle to each.otherj means for imparting correlated
oscillations to said -two mirrors whereby -the beam is angularly scanned in a
spiral path; a positi~e lens for receiving said scanned beam and for redirect-
ing it through a cross-over point or small region positioned within said bot-
tle or article at said neck or constricted area; and a pho-toelectric detector
-i~eans adapted for receiving said spirally scanned laser beam after it has
passed through or been reflected by said article thereby to detect a flaw in
the article to be tes-ted.
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In accord.ance wi-th the present invention, there is further provided
in a system f`or detec-ting flaws in bottles or like ar-ticles, said system com-
prising a light beam generating means, a device for causing scanning motion of
said light beam through an article to be tested, and a photoelectric de-tecting
means adapted for detecting variation of said scanned light beam thereby -to
detect a fla~ in the article; an improvement, wherein (a) said light beam
generating means is a ]aser beam generating means adapted for generating a
narro~ linearly polarized laser beam; (b) said device for causing scanning
motion comprises optical means disposed in the path of said polarized laser
beam and adapted to move in a prescribed manner for imparting angular deflec-
tions to said beam to cause it -to undergo an annular or spiral scanning motion,
and comprises a positive lens for receiving said scanned laser beam and for
redirecting it through a cross-over point or a small region positioned within
said bo-ttle or article and above -the surface to be inspected to thereby enable
said beam to scan through said article; and (c) said photoelectric detecting
means comprises means for receiving (said polarized laser beam that has scann-
ed the article and for separating therefrom depolarized rays, if any, that
have been scattered by a flaw in the article) light of said laser beam which
is reflected from the article, the reflected light including depolarized rays
produced as a result of scattering of the polarized laser beam by a flaw of
the article, means for separating the depolarized rays from the reflected light,
and means for sensing the presence of the flaw in the article by receiving only
the separated depolarized rays.
Stated in brief, this- invention provides a flaw detecting system
comprising means for generating a light beam, means disposed in the path of
light beam for imparting an annular or spiral scanning motion thereto, such
that the light beam is enabled to scan all surfaces of an article.being held
in a preassigned position to be tes-ted as to the presence or absence of a
flaw, and means for receiving the light beam that has scanned the. article and
for sensing a flaw, if any, in the article from the intensity of the
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incident light.
The flaw detecting system usually employs a laser, such as a gas
laser, as the light source. Various means can be employed to cause the annu-
lar or spiral scanning motion of the laser beam. According to an example of
such various possible means disclosed herein, two mirrors capable of succes-
sively reflecting the laser beam are arranged for correlated oscillation
about respective axes at right angles to each other.
If the article being tested is a beer bottle, for example, with
its constricted mouth, then a converging lens may be disposed between the
oscillatory mirror system and the bottle lying in the preassigned position.
Focused at the mouth of the bottle, the converging lens serves to direct the
laser beam into the bottle so as to enable the beam to scan the bottom as
well as the side wall of the bottle point by point.
A variety of means can also be employed for receiving the laser
beam that has scanned the bottle and for sensing therefrom a possible flaw
in the bottle. One example includes an integrating sphere arranged to re-
ceive the laser beam that has passed through the bottle, and a photodetector
mounted in the window of the integrating sphere so as to be irradiated by
the light reflected from its inside surface. Any flaw in the bottle mani-
fests itself as a change in the electrical output of the photodetector.Thus, with its point-by-point scanning principle, the invention enables the
detection of a flaw in a bottle or the like with great accuracy.
The above and other objects, features and advantages of this inven-
tion and the manner of attaining them will become more readily apparent, and
the invention itself will best be understood, from the following description
and appended claims, with reference to the accompanying drawings showing sev-
eral preferred embodiments of the invention.
BRIEF DESCRIPTION OF TIE DRAWINGS
Figure 1 is a schematic representation of a preferred form of the
flaw detecting system in accordance with this invention;
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Figure 2 is a schematic representation explanatory of means of os-
cillating each mirror of an oscillatory mirror system employed in the flaw
detecting system of Figure 1 to impart an annular or spiral scalming motion
to the laser beam;
Figure 3 is a sectional view of photoelectric sensing means in the
system of Figure 1, the view showing in particular the integrating sphere of
the photoelectric sensing means in its correct positional relationship to the
bottle being tested;
Figure ~ is a fragmentary, enlarged vertical sectional view of the
bottle being tested, the view being explanatory of the refraction of the
scanning laser beam as the same passes through the perimeter of the bottom
of the bottle;
Figure 5A is a plan view of a sheet of ground glass covering the
inlet opening of the integrating sphere in the system of Figure 1, the view
further showing the path as traced on the ground glass by the laser beam dur-
ing its single scanning cycle, the letter A in this view denoting the pres-
ence of a flaw in the bottle being tested;
Figure 5B graphically represents the intensity of the light fall-
ing~ during the single scan of the laser beam as depicted in Figure 5A, on
the photodetector forming a part of the photoelectric sensing means in the
system of Figure 1, the letter B in this graph indicating a drop in the in-
tensity of the incident light corresponding to the bottle flaw A in Figure
5A;
Figure 6 is a perspective view explanatory of how the annular or
spiral scanning motion is imparted to the laser beam by the oscillatory mir-
ror system used in the flaw detecting system of Figure l;
Figures 7A and 7B are graphic representations of the operating
principle of the oscillatory mirror system of Figure 6;
Figure 8 is a schematic representation of another preferred form
of the flaw detecting system in accordance with the invention;
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Figure 9 is a schematic representation of still another preferred
form of the flaw detecting system in accordance with the invention;
Figure 10 is also a schematic representation explanatory of the
operating principle of the flaw detecting system of Figure 9;
Figure 11 is a schematic side view of a modification of the oscil-
latory mirror system used in the flaw detecting systems of Figures 1, 8 and
9, tlle view showing only one of the required two mirrors together with means
directly associated therewith;
Figure 12 is a schematic perspective view of second modified means
for imparting an annular or spiral scanning motion to the laser beam in the
flaw detecting system of either Figure 1, 8 or 9;
Figure 13 is a perspective view of third modified means for im-
parting an annular or spiral scanning motion to the laser beam in the system
of either Figure 1, 8 or 9;
Figure 14 is a perspective view of fourth modified means for im-
parting an annular or spiral scanning motion to the laser beam in the system
of either Figure 1, 8 or 9; and
Figure 15 is a sectional view of the means of Figure 14, taken
along the plane indicated at XV-XV in that figure.
DESCRIPTIO~ OF THE PREFERRED EMBODIMENTS
The present invention is shown embodied, first of all, in the bot-
tle flaw detecting system of Figure 1, which includes a laser unit or a laser
lO such as that of the helium-neon or carbon dioxide variety. A converging
lens 12 is positioned adjacent to the laser 10, across the path of the laser
beam 11 emitted thereby, for collimating the same. The collimated laser
beam falls upon an oscillatory mirror system 13 which functions to i.mpart an
annular or spiral scanning motion to the beam.
The oscillatory mirror system 13 comprises first 14 and second 15
reflecting mirrors. The first mirror 14 is arranged to directly receive the
collimated laser beam 11 and is angled with respect to the beam axis. The
second mirror 15 is arranged to reflect the laser beam 11 that has been re-
flected from the first mirror 14, and is likewise angled with respect to the
incident beam axis.
As better shown in Figure 2, each of the mirrors 14 and 15 of the
oscillatory mirror system 13 is pivoted by a pair of trunnions 28 affixed
collinearly to its metal base, for oscillation thereon. The trunnions 28 of
each oscillatory mirror 14, 15 are electrically connected to an alternating
current ~AC) source 16 to form a closed electric circuit 17. This closed
circuit includes a coil winding 18 connected directly to one of the mirror
trunnions 28 and disposed in a magnetic field generated by a permanent magnet
19 .
Thus, by sending out alternating currents 90 degrees out of phase
with each other into the respective closed circuits 17 of the mirrors 14 and
15, these mirrors can be oscillated about the trunnions 28 by the coil wind-
ing 18 lying in the prepared magnetic fields, as dictated by Fleming's rule.
The noted phase relationship of the alternating currents correlates the os-
cillations of the mirrors 14 and 15 so that they may coact to impart an annu-
lar scanning motion to the collimated laser beam 11 as the latter is reflect-
ed by the successive mirrors. A continuous change in the angles or ampli-
tudes of oscillation of the mirrors 14 and 15 results in a continuous changein the diameter of the scanning loop of the laser beam as measured in any
fixed plane. More will be said presently concerning this function of the os-
cillatory mirror system 13.
With reference back to Figure 1, the colliminated laser beam 11
that has received the annular scanning motion passes through another converg-
ing lens 20 into a bottle 22, such as a used and cleaned beer bottle, which
is being held in a preassigned position to be tested as to the presence of
flaws. The surface curvature of this converging lens 20, which is shown to
be of the double convex type, and its distance from the bottle 22 are so de-
termined that its focus may lie at the mouth of the bottle or thereabouts.
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1~28~67
Thus the converging lens 20 serves to direct the scanning laserbeam 11 into the bottle 22 through its mouth. By continuously varying the
diameter of the scanning loop of the beam in any fixed plane, as noted prev-
iously, the beam will scan not only the inside surface of the bottom, but
also that of the entire side wall, of the bottle 22.
A sheet of ground glass 24 is disposed across the path 23 of the
scanning laser beam that has passed through the bottle 22, so as to be irradi-
ated thereby. After thus irradiating the ground glass 24, the laser beam is
directed onto photoelectric sensing means generally labelled 25. In this
particular embodiment the photoelectric sensing means 25 comprises an inte-
grating sphere 26 mounted immediately under the ground glass 24, with its in-
let opening 26a held against the glass, and a photoelectric detector 27
mounted in the usual window of the integrating sphere.
Attention is now called to the details of the photoelectric sens-
ing means 25 given in Figure 3. The photosensitive face of the photoelectric
detector 27 is disposed flush with the inside surface of the integrating
sphere 26 and, preferably, is oriented toward the bottom center of the sphere.
Receiving the laser beam from the ground glass 24 through its inlet opening
26a, the integrating sphere 26 functions to reflect the incoming beam onto
the photoelectric detector 27. The diameter Do of the integrating sphere
opening 26a is made suitably greater than the diameter d of the bottle 22 in
Order that the laser beam that has scanned every part of the bottle may
enter the sphere.
Glass bottle making techniques today are such that the bottoms of
bottles, particularly their peripheral regions, are often of uneven thick-
ness. This, possibly combined with the refractive power of the bottom walls,
may cause irregular diffusion or deElection of the scanning laser beam. In
some instances, as depicted in Figure 4, the laser beam scanning the perim-
eter of the bottle bottom may be refracted outwardly through an angle ~ of
as much as 50 degrees from its straight-line path. The inlet opening 26a of
the integrating sphere 26 should therefore be sufficiently large, in rela-
tion to the bottle diameter d and to the distance I, between bottle and
sphere, to recaive all such outwardly refracted light.
Preferably, the diameter D of the integrating sphere opening 26a
is about 80% of the inside diameter Dl of the sphere. This relative opening
diameter is greater than that of ordinary integrating spheres available com-
mercially. The integrating sphere 26 with such a large opening 26a can be
reduced in its overall size without sacrifice of its ability to collect the
laser beam. The use of such a small-sized integrating sphere also contrib-
utes materially to the reduction of the installation space for the completeflaw detecting system and further to the ease of installation, supervision,
and maintenance.
If it is assumed that the bottles to be tested have diameters of
up to about 75 millimeters (mm), che integrating sphere 26 may have an in-
side diameter Dl of 150 mm and an opening diameter Do of 120 mm. As is well
known, the spherical inside surface of the integrating sphere 26 reflects
the incident laser beam onto the photoelectric detector 27.
The photoelectric detector 27 exhibits a change in its output cur-
rent amplitude when the incident radiation has been modulated by some flaw in
Z0 the bottle 22. This change in the output of the photoelectric detector 27
serves as an indication of the presence of a flaw in the bottle being tested.
More detailed explanation of this process of flaw detection follows.
If the bottom of ~he bottle 22 has some foreign matter sticking
thereto, or has a scratch, crack or other defect formed therein, then the
annularly or spirally scanning laser beam will undergo depolarized reflec-
tion on impinging on such faulty part of the bottle bottom. This of course
results in a decrease in the intensity of the light entering the integrating
sphere 26 through the ground glass 24. If some flaw lies in the side wall
of the bottle 22, on the other hand, then the flaw will either intercept or
depolarizingly reflect the scanning laser beam. The result, again, is a
,~ _ _
decrease in the intensity of the light trave]ling into the integrating
sphere 26. Since the total incident light of the integrating sphere Z6 is
thereby reflected onto the photoelectric detector 27, the latter senses the
presence of a flaw anywhere in the bottle 22 from the reduction of the in-
cident radiation.
A consideration of Figures 5A and 5B will further clarify the
function of the photoelectric detector 27. Figure 5A pictures the path of
the scanning laser beam as traced on the ground glass 24 during its single
annular or circular sweep of the bottle 22. The scanning beam has just en-
countered a flaw at A, which actually may be anywhere in the bottom or side
wall of the bottle. At this faulty spot A the scanning beam has been either
blocked or depolarizingly reflected, resulting in a corresponding change in
the intensity of the light received by the integrating sphere 26 and there-
fore by the photoelectric detector 27.
The graph of Figure 5B shows a curve of the corresponding incident
radiation on the photoelectric detector 27, and therefore of its output cur-
rent, against time. The bottle flaw at A, encountered by the scanning laser
beam as described above, has caused a sudden drop at B in the incident radia-
tion and hence in the output current of the photoelectric detector 27. This
drop in the output current indicates the presence of the flaw in the bottle.
The following is a description of how the oscillatory mirror sys-
tem 13 operates to impart the desired annular or spiral scanning motion to
the converged laser beam 11. In the closed electric circuit of Figure 2,
including the coil winding 18 disposed in the magnetic field of the perman-
ent magnet 19, ~he flow of an alternating current therethrough results in
the exertlon of forces on the coil winding in alternately reversed direc-
tions at right angles to the net directions of current flow through the coil
winding and to the direction of the magnetic lines of force, in accordance
with Fleming's left hand rule. Such forces cause oscillation of each mirror
14, 15 about the trunnions 28.
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As clearly shown in Figure 6, the First 14 and the second 15 mir-
rors of the oscillatory mirror system 13 are disposed with their axes of
oscillation in right angular relationship to each other. Further, the al-
ternating current. driving the two mirrors 14 and lS have a phase difference
of 90 degrees. If the first mirror 14 is oscillated as described above to
cause the swinging motion x of the laser beam along the X-axis, as shown in
Figure 7A, then
x = a sin w t .......... ~1)
where a is a constant proportional to the magnitude of the alternating cur-
rent driving each mirror; _ is the angular velocity ~= 2~f); and t is the
time.
The second mirror 15 oscillates to cause the swinging motion y of
the laser beam along the Y-axis as in Figure 7~. Since the alternating cur-
rent driving this second mirror 15 is 90 degrees out of phase with that
driving the first mirror,
y = a sin ~ w t - ~/2) = a cos w t .. ~2)
The laser beam 11 is reflected successively by these oscillating mirrors 14
and 15. Hence, from equations ~1) and ~2),
2 ~ y2 = a2 .................. ~3)
The two oscillatory mirrors 14 and 15 thus coact to impart the de-
sired annular scanning motion to the laser beam 11. A continuous change in
the magnitude of the alternating currents driving the mirrors 14 and 15
affords a spiral scanning motion, with the diameter of the scanning loop of
the laser beam in any fixed plane changing continuously. As required, more-
over, the mirrors 1~ and 15 may be oscillated with the magnitudes of the
driving currents held at a prescribed ratio, to cause the laser beam to fol-
low an elliptic scanning path.
The oscillatory mirror system 13 thus enables the laser beam 11 to
scan, point by point, the bottom and side wall of a bottle or the like of
almost any shape or si~e. Furthermore, since the scanning laser beam has
been collimated by the converging lens 12, any flaw in the bottle being
tested causes a very substantial change in the intensity of the light fall-
ing on the photoelectric detector 27. The invention thus succeeds in pro-
viding a highly reliable flaw detecting system.
Figure 8 illustrates another preferred embodiment of this inven-
tion, which differs from the system of Figure 1 only in its photoelectric
sensing means. The other parts or components of this modified system are
identified in Figure 8 by the same reference numerals as those used to de-
note the corresponding parts of the Figure 1 system, and the`ir description
will be omitted.
The modified photoelectric sensing means, generally designated by
25a in Figure 8, comprises a converging lens 31 disposed next to the sheet
o ground glass 24, and a photoelectric detector 32 disposed at the focal
point of the converging lens 31 away from the ground glass. The converging
lens 31 serves to direct on the photoelectric detector 32 the laser beam
that has scanned the bottle 22 and which has further passed through the
ground glass 24. Continuously receiving the scanning laser beam directed
thereon, the photoelectric detector 32 senses any flaw in the bottle 22 from
the intensity of the incident beam. The other details of construction and
operation will be apparent from the foregoing.
According to still another preferred embodiment of the invention
shown in Figure 9, any flaw in a bottle or other article is detected from
the depolarized rays of the scanning laser beam that have been reflected
from the flaw in the bottle. In this respect, the system of Figure 9 con-
trasts with the two preceding embodiments of the invention which both rely
for flaw detection on the intensity of the laser beam that has passed through
the test article. Some parts or components of this Figure 9 system also
have their counterparts in the systems of Figures 1 and 8. Such correspond-
ing parts are identified by like reference characters and will not be de-
scribed in any detail.
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A helium-neon or carbon dioxide laser lOa incorporated in the sys-
tem shown in Figure 9 includes Brewster windows at opposite ends of its dis-
charge tube (not shown), so that its output beam lla is linearly polarized
(or plane-polarized), with its polarization plane kept constant. The con-
struction of this laser lOa is known and by itself forms no novel feature of
this invention.
The converging lens 12 of the preceding embodiments of the inven-
tion is not used here; instead, a totally reflecting mirror is disposed at
35 at an angle to the axis of the linearly polarized beam lla being generat-
ed by ~he laser lOa. The mirror 35 reflects and redirects the laser beamlla onto the oscillatory mirror system 13 comprising the first 14 and the
second 15 oscillatory mirrors.
The oscillatory mirror system 13 functions as above explained to
impart an annular or spiral scanning motion to the laser beam lla. The
laser beam subsequently reaches the converging lens 20, which directs the
beam at or adjacent the mouth of the bottle 22 being tested. How the laser
beam scans the bottle 22 is clear from the foregoing description of the sys-
tem shown in Figure 1, in particular.
Included in means 41 for deriving from the reflected laser beam
the depolarized rays that have been scattered by some flaw in the bottle 22,
a beam splitter (half mirror) 36 is disposed between converging lens 20 and
bottle 22 and functions to separate the reflected beam from the incident
light. Of course, the beam splitter 36 transmits the incident scanning
laser beam and reflects the light 38 that has been reflected back from the
inside surfaces of the bottle 22. The deriving means 41 further comprises
an interference filter 37 and a polarizing filter 3g.
The interference filter 37 is arranged to directly receive the re-
flected light 38 from the beam splitter 36. The function of this interfer-
ence filter is to permit the passage therethrough of only a preselected
wavelength ~e.g., 5328 angstroms (~) in the case of the He-Ne gas laser
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beam) of the incoming light and -to filter out all other wavelengths by in-
terference phenomenon. The particular wavelength of the reflected laser
beam that has passed the interference filter 37 subsequently falls on the
polarizing filter 39.
For a better understanding of the function of the polarizing filter
39, reference is direc~ed to the explanatory representation of this flaw de-
tecting system in Figure 10. If the laser beam lla as generated by the laser
10a is linearly polarized in the y direction, for example, then the polariz-
ing filter 39 is preadjusted to pass the incoming light polarized in the x
direction only and to filter out that which is polarized in the y direction.
Thus, provided that the bottle 22 has no flaw therein, the polarizing filter
39 blocks all the incoming light that has been reflected from the inside sur-
faces of the flawless bottle.
In the event that the bottle 22 has some flaw therein, however, the
laser beam on scanning the flaw will undergo depolarized reflection, thereby
creating components polarized in the x direction. The polarizing filter 39
passes such components of the depolarizingly reflected rays onto a photo-
electric sensing assembly ~0. Thus irradiatecl, a photoelectric detector ~not
shown) built into this assembly ~0 senses the presence of the flaw in the
bottle 22.
One of the features of the system shown in Figure 9 resides in the
interference filter 37. Since this filter blocks all but the reflected laser
beam, the system permits accurate detection of any flaw in the bottle even in
bright ambient light. This system is further capable of detecting any such
transparent material as cellophane that may be attached to the bottle, be-
cause the laser beam is reflected even by such transparent material. An ad-
ditional, but no less important, advantage of this system is that it finds
use not only with glass bottles but also with cans or other open-ended con-
tainers of nontransparent material. It will of course be seen that the beam
splitter or half mirror 36 of Figure 9 can be replaced by a reflecting mirror
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6'7
havlng an aperture fo~med centrally therein or by an optical glass fiber.
A variety of modifications are possible for the oscillatory mirror
system 13 which has been described with particular reference to Figures 2, 6
and 7 and which has been incorporated in all the three preceding embodiments
of the invention illustrated in Figures 1, 8 and 9. Figure 11 schematically
illustrates one of such possible modifications. The modified oscillatory
mirror system 13a also employs two mirrors 14a and 15a arranged just like
the mirrors 14 and 15 of the orlginal system 13. The modification resides
in the means for imparting oscillations to the two mirrors. Since the two
mirrors are oscillated by identical means, only one of the mirrors will be
shown and described in connection with its own oscillating means.
Figure 11 shows the representative mirror 14a, 15a as being pivot-
ally supported along one edge 50 on a support 51. At or adjacent its free
edge the mirror 14a, l5a rests upon a piezoelectric crystal unit 52 recessed
into the support 51 and elect.rically connected to an AC source 53. Of the
type available commercially, the piezoelectric crystal unit 52 includes a
piezoelectric crystal element which vibrates at a desired frequency when
placed in an electric circuit as in the illustrated arrangement.
Thus, upon application of an alternating current to the piezo-
electric crystal unit 52 from the AC source 53, the crystal element gener-
ates mechanical vibrations at the frequency o:E the alternating current. The
amplitude of the alternating current determines the amplitude of the crystal
vibrations. The piezoelectric crystal unit 52 thus oscillates the mirror
14a, 15a at a desired frequency and with a desired amplitude.
The other, unshown mirror of the modified mirror system 13a is
likewise oscillated at a desired frequency and with a desired amplitude.
Witoh their oscillations properly correlated, the two mirrors 14a and 15a of
the modified mirror system coact to impart an anT~ular or spiral scanning mo-
tion to the laser beam by successively reflecting the same. For Q more ex-
tensive discussion of the method of thus imparting the annular or spiral
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scanning motion to the laser beam, reference is directed to the description
of Figures 6, 7A and 7B and, by way of comparison, to that of Figure 2.
Figure 12 illustrates another modification 13_ of the oscillatory
mirror system 13, which modification also employs two mirrors 14_ and 15_
arranged to successively reflect the incident laser beam. The first mirror
14b is coupled flatwise to the piston rod 54 of a fluid actuated cylinder 55
for linear reciprocation. The second mirror 15_ is arranged for oscillation
like the mirrors of the above described oscillatory mirror systems 13 and
and 13a. The means of either Figure 2 or Figure 11 may be employed to oscil-
ate the second mirror 15b.
In operation the movements of the reciprocating first mirror 14band oscillating second mirror 15b are to be synchronized by means that will
readily occur to the specialists. The synchronized reciprocation and oscil-
lation of the mirrors 14b and 15b serve conjointly to impart an annular or
spiral scanning motion to the laser beam being reflected thereby one after
the other. The laser beam may further be made to trace an elliptic scanning
path as required.
Figure 13 illustrates still another modification 13c of the oscil-
latory mirror system 13. This modification employs a single lens 63 revolv-
ing about an eccentric axis to perform the functions of the two mirrors usedin each of the foregoing mirror systems 13, 13a and 13_. Either diverging or
converging, the lens 63 is immovably fitted in a hole formed eccentrically
in a disc-like lens carrier 60 supported by suitable means ~not shown) for
rotation about its own a~is OD. The lens carrier 60 makes peripheral, fric-
tional contact with a drive disc or roll 61 fixedly mounted on tlle output
shaft of an electric drive motor 62. The drive disc serves to transmit the
rotation of the drive motor 62 to the lens carrier 60~ causing the latter to
rotate about its own axis OD.
Whereas the axis OL of the lens 63 is offset a distance R from the
axis OD of the lens carrier 60, the radius of this lens is greater than the
.
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fi~
cen~er-to-center distance R between lens and lens carrier. Thus, as the
incident laser beam falls on the lens 63 at the axis OD oE the lens carrier
60, the lens 63 revolving about this lens carrier axis imparts the desired
annular scanning motion to the laser beam passing therethrough at its fixed
eccentric point. Gradual axial movement of the lens carrier 60 results in
a continuous change in the diameter of the scanning circle of the laser beam
in any fixed plane. Combined rotary and axial movements of the lens carrier
60, therefore, result in the impartation of a spiral scanning motion to the
laser beam.
According to an additional modification 13d shown in Figures 1~ and
15, a lens holder 67 in the form of a hollow, flanged cylinder immovably
holds a lens 68, which is shown as a double concave one. The lens holder 67
together with the lens 68 is rotatably mounted via a bearing 66 in a hole
formed eccentrically in a disc-like lens carrier 60. This lens carrier 60
is also to be rotated by the motor 62 via the drive roll or disc 61. As in
the preceding example, the radius of the lens 68 is greater than the distance
between lens axis OL and lens carrier axis OD.
One of the most pronounced features in the operation of the arrange-
ment 13d of Figures 14 and 15 is that during the rotation of the lens carrier
65 about its own axis OD, the lens 68 together with its holder 67 is locked
against angular displacement about its own axis OL by suitable means (not
shown). Although the lens 68 revolves about the lens carrier axis OD, its
angular position about its own axis OL remains unchanged during the rOtation
of the lens carrier 65. Falling on the revolving lens 68 at the lens carrier
axis OD, therefore, the incident laser beam follows a circular path on the
lens in passing therethrough to receive the desired annular scanning motion
therefrom. Thus the lens 68 makes more effective use oE its surface area
than the lens 63 of Figure 13.
As in the arrangement 13c of Figure 13, the combined rotary and
axial movements of the lens carrier 65 give a spiral scanning motion to the
laser beam. A rack-and-pinion mechanism, fluid actuated cylinder, or any
other suitable means may be employed to effect such axial movement of the
lens carrier 65, or of the lens carrier 60 of Figure 13. Of course, a con-
verging lens could be used in place of the diverging lens 68, and gearing
and other drives could be substituted for the friction drive used in the
arrangements of both Figures 13 and Figures 14 and 15. Furthermore, as de-
sired, light beams other than a laser beam may be adopted in the practice
of this invention.
The above and various other modifications or changes that will
readily occur to those versed in the art are intended in the foregoing dis-
closure. It is therefore appropriate that the present invention be con-
strued broadly.
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