|Publication number||US1358413 A|
|Publication date||Nov 9, 1920|
|Filing date||May 12, 1919|
|Priority date||May 12, 1919|
|Publication number||US 1358413 A, US 1358413A, US-A-1358413, US1358413 A, US1358413A|
|Original Assignee||Brodsky Gregory|
|Export Citation||BiBTeX, EndNote, RefMan|
|Referenced by (8), Classifications (5)|
|External Links: USPTO, USPTO Assignment, Espacenet|
etiree-a GREGORY BRODSKY, OF LONDON, ENGLAND.
Specification of Letters Patent.
Patented Nov. 9, 1920.
Application filed May 12, 1919. Serial No. 296,685.
To alt whom it may concern.
Be it known that I, GREGORY BRODSKY, a subject of the King of Great Britain, and residing at 3 Glazbury road, London, W. 14., England, have invented certain new and useful Improvements in Polarizing-Prisms, of which the following is a specification.
This invention relates to polarizing prisms. It is the object of the invention to provide an improved form of polarizer which can be manufactuped in any required quantities and sizes and at no great expense, so that it can be used as a substitute for crystals of Iceland spar. There are in fact a great many uses for polarizers which have not been developed in practice because of the difiiculty of making suitable polarizing devices on a substantial scale.
According to the present invention, the desired resultis attained by combining with a pile of plates, a pair of prisms, one in front and one behind the pile, of a suitable angle such that when the faces of the prisms are applied to opposite sides of the pile of plates, the proper conditions for polarizing the light passing through the combination, are secured with the plates at a larger and much more convenient angle to the light. The increased angle reduces the depth of the combination and therefore the weight and bulk. At the same time, difliculty due to reflected light. displacement of the beam, and chromatic aberration is largely diminished. The device can be reduced in depth and weight still further by arranging it in sections with plane surfaces between them, the edges of the piles of glass plates between the prisms terminating at these surfaces. Any difficulty due to lateral displa ement of the beam of light, or to chromatic aberration, is avoided when necessary by dividing the system into two sections, in one of which the plates are inclined in the opposite direction to the other, the light passing through both sections successively. These and other features of the invention are hereinafter set forth with reference to the accompanying drawings, wherein I Figure 1 shows in longitudinal section, and
Fig. 2 shows in front elevation with parts broken away, one form of the polarizer according to the invention.
Figs. 3 and 4 are diagrams explanatory of the optical principles involved in the invention.
Fig. 5 shows in longitudinal section, and Fig. 6 shows in front elevation a form of title piolarizer constructed on the lines of Fig. 7 shows in longitudinal section, and
Fig. 8 shows in front elevation, another form of the polarizer, built up in sections.
In Fig. 1. c is the pile of lass plates, say ten plates or more, each preferably of about one millimeter or less in thickness, while d and e are the two prisms placed at the front and back respectively of the combination. The prisms d and e are of a form which would be obtained by cleava e on a diagonal line of a cylinder of glass. %he plates 0 are placed close together, or separated by a very thin film such as is produced by laying rings of very thin metal foil between each plate and the next adjacent to their circumference. The prisms and plates are fitted together in a cylindrical mount 7 with a flanged ring 9 closing the rear thereof and-leaving a suitable aperture. The prisms are secured together with the plates around their edges by a suitable optical cement such as Canada balsam, so as to build up a complete composite cylinder with plane front and rear faces, and with a large number of internal cleavage faces in the pile of plates 0.
The angle at which the plates 0 stand may be determined as indicated in Fig. 3. If a prism cl of glass with an apex angle a is chosen, a beam of light entering the prism axially strikes the inclined face at an angle a to the normal, and is refracted to an angle 6 to the normal where it leaves this face.
The angle 1) represents the angle at which the whole of the light strikes the face of the first plate in the pile c. The angle to the normal at which the light must strike the pile of plates when formed of any given lass, in order to secure the maximum oiu'izing effect is about 65, although t 1s angle is best determined by experiment. Applicant finds 67 to be satisfactory though Wood (Physical Optics) has referred to angles of about -65. Without the prisms d and e therefore, it would be necessary for the pile of plates 0 to be inclined at an angle of 67 to the vertical plane through the axis. and with such a large angle the depth of the combination would be large and awkward to deal with. When the prisms d and e are used, the effect is to reduce the angle of the pile of plates to the vertical from b to a in Fig. 3, and
thus substantially to reduce the depth or thickness of the combination. If m is the refractive index of the glass used for the prisms, then sin b sin a If I) has to be 67 for the maximum polarizing effect with the pile of plates used, and if the refractive index for the prisms d and e is m=1.604, then from the above equation the angle a is found to be approximately 35. This is the angle, therefore, of the pile of plates to the vertical plane in the examples of construction illustrated. The larger the refractive index of course, the smaller the angle a, will become, but it will be found to be in the neighborhood of 35 for most suitable types of glass.
In Fig. 3 the pile of plates 0 is omitted, so that the light leaving the prism is shown passing though air, but if the plates were inserted the light striking the first plate in the pile situated after an air gap would be refracted back again toward the horizontal, would leave the farther face of the first plate again at an angle of approximately 5 to the axis, would be refracted toward the horizontal again in the next plate, and so on. The result would be a little lateral displacement of the ray of light in passing through the set of plates, represented by the arrow in big. 4, in which d is the first prism as before, and c is a pile of plates. In order to determine this lateral displacement (assuming the refractive index m to be the same for both prisms and plates) we may use the formula: displacement x= cos b where 3 is the air gap between the plates and n is the number of plates used, while the refractive index is assumed to be the same for the prisms and the plates of the pile. With an air gap 1 of about one-tenth of a millimeter, and with the angles as above stated, the axial displacement x will be about two millimeters for a pile of twelve plates. The displacement can not be exactly computed of course, owing to the difiiculty of measuring the almost infinitesimal air gaps accurately, but it is found in practice to be of the order stated above. This axial displacement is different of course for rays of light of different colors, and thus some chromatic aberration is set up. This is not detected in a simple beam of light except around the edges, and if the flange of the ring 9 cuts off the borders of the beam of light for about two millimeters, the beam which emerges will appear practically as white light. The construction of Fig. 1 therefore is sufficient for many purposes,
and the polarizing effect may be rendered more complete without much loss of light I light passes, the walls of the tubes being blackened internally to absorb any divergent rays. A certain amount of light may pass through the optical combination without complete polarization, and such rays at an angle to the axis are largely cut off by the tubular structure or grid it. Such a structure may be built up readily from thin metal plates stamped out with projecting ridges, which, when suitably placed together, form a honeycomb structure as is well known. A certain amount of light is lost of course apart from the cutting off of rays at an angle, by the thickness of the walls of the tubular structure, and the device h is only used, therefore, where the strength of the beam of light can be sacrificed to considerations of complete polarizin with the exclusion of all divergent rays. ifiiculties due to displacement of the beam and chromatic aberration can be disposed of in various ways, for example by using plates for the pile c of a difierent refraotive index from that of the prisms d and 6, so as to bring back the beam of light toward the axis, but this is only an approximate method. A more accurate method is that shown in Fig. 4, wherein the pile of plates is split up into two sets 0 and c placed at opposite angles to the axis, with a double prism is between them and a prism Z behind similar to 03. A single prism k is used at the center in place of two prisms equivalent to e, and e reversed, as there would be no point in making two separate prisms to be united in that way. Evidently however, the middle prism k is optically equivalent to two prisms e placed back to back. The ray of light parallel to the axis, but displaced therefrom as indicated while passing through the middle prism 70, is brought back again to the axis in passing through the second pile of plates 0 and out again through the rear prism Z. At the same time chromatic aberration is corrected as the combination comprises two parts, one the replica of the other in a reverse position. If twelve plates are required for polarizing, half of this number can be placed in the pile 0 and the other half in the pile 0 as the polarizing effect is continued through the two piles. One or two additional plates may be used in each pile however, to render the polarizing action as complete as possible.
Figs. 5 and 6 illustrate the complete combination of Fig. 4, in a cylindrical mount f closed by a flanged ring g, and such com-- bination can be used for optical purposes where eifective polarization without lateral displacement or chromatic aberration is oi great importance.
For polarizers of larger sizes, even with the pile of plates at an angle of 35 to the vertical plane the depth or thickness of the combination would become considerable if a single continuous pile of plates were used. In such cases the pile may be split up into any required number of sections, according to the size of the polarizer. For example, Figs. 7 and 8 illustrate a polarizer with the pile split up into two sections, reducing the width or depth of the combination to a substantial extent. \Vhere only two sections are used as in Figs. 7 and 8, the piles of plates may be oppositely inclined to the axis as shown, to prevent risk of appreciable separation of the two parts of the beam of light at the transverse diameter where the two sections abut one against another. In a combination of more than two sections however, they would all preferably be placed with the piles of plates inclined in the same direction, and it is found that the planes of separation between the units of the combination cannot be detected at any great distance from the polarizer, although close to the polarizer there are narrow dark bands, of approximately two millimeters depth between the light emitted from one section and the next, as is evident from the considerations stated in connection with Fig. 4. The sections of the combination in Figs. 7 and 8 are made up and united by optical cement such as Canada balsam, and in order that the faces may be as closely as possible in the same plane, glass disks 0 and p are preferably placed in the mount in front and behind all the sections, cemented to these latter, and making up with them a complete optical structure with plane front and rear faces. This is shown as being arranged in a cylindrical mount f with a flanged ring 9 at the rear as before. The front prisms of the sections are marked d and d and the rear prisms e and e in Fig. 7, their form corresponding with that which would be obtained by diagonal cleavage 01 a semi-cylindrical block of glass. At the diametral plane of cleavage, the sections of the combination are preferably cemented together with an opaque varnish which will absorb reflected light, and the same opaque varnish may be used around the circumference of the whole combination for the same purpose. Such a varnish can be made from Canada balsam mixed with lamp-black or a black dye.
It will be apparent that all of the prisms hereinbefore described are reversible, as the one side is always a reversed replica of the other. Polarizing prisms made as above described can be used both for projecting beams of polarized light, and also as analyzers for detecting polarized light. The term polarizer therefore is intended to include analyzer wherever used therein. They can be used for a variety of practical and scientitic purposes involving polarization and the detection of polarization, or of the turning of polarized beams of light. Polarizers such as that of Figs. 5 and 6 are more particularly useful in connection with optical systems where the light passes through lenses and so forth, after passing through the polarizer. Chromatic aberration might be emphasized by transmission of the light through such lenses, whereas the polarizer of Figs. 5 and 6 avoids such aberration.
Various-modifications of the constructions described are possible and may be used without departing from the scope of the invention. For example, in the system of Figs. 4, 5 and 6 the whole of the pile of plates may be placed in the one position corresponding to c for example, while in place of an oppositely inclined pile at 0 an air gap may be left of a width just sufficient to allow the beam of light emerging from the prism k to return to its former axis before it strikes the face of the last prism Z. This simultaneously allows of course of the re-combining of the dispersed chromatic light. In the combinations of Figs. 4, 5 and 6 the apex of the prism and the ends of the piles of plates 0 and 0 adjacent thereto, may project a little beyond the bases of the prisms d and Z in order as far as possible to retain in the system the whole of the beam of light entering through the face of prism 61, and to utilize the whole of the prism Z for transmitting this light. This makes a rather inconvenient construction, however, to mount, and it is more convenient as a rule to make the aperture of the flanged ring 9 such as to cut off any irregularities in the light at the edges of the combination.
I claim 1. A polarizing device comprising a plurality of prisms, a plurality of glass plates between said prisms arranged at an angle to the axis of the polarizing device, said prisms being so arranged that one prism deflects the light in one direction so that it strikes the plates at the polarizing angle,
while the next deflects it in the opposite direction, and a mount for holding said prisms and plates.
2. A polarizing device comprising a plurality of prisms, a plurality of glass plates between said prisms arranged at an angle of approximately 35 degrees to the axis of the polarizing device, said prisms being so arranged that one prism deflects the light in one direction so that it strikes the plates at the polarizing angle, while the next deflects it in the opposite direction, and a mount for holding said prisms and plates.
3. A polarizing device comprising a plurality of prisms, a plurality of glass plates between said prisms arranged at an angle to the axis of the polarizing device, said prisms being so arranged that one prism deflects the light in one direction so that it strikes the plates at the polarizing angle, while the next deflects it in the opposite direction, a mount for holding said prisms and plates, and means disposed in front of the prism through which the light issues, for cutting oil any rays of light diverging from a line parallel to the axis of the system.
4:. A polarizing device comprising a plurality of prisms, a plurality of glass plates between said prisms arranged at an angle to the axis of the polarizing device, said prisms being so arranged that one prism deflects the light in one direction so that it strikes the plates at the polarizing angle, while the next deflects it in the opposite direction, a mount for holding said prisms and plates, and a tubular structure mounted at the rear end of the device, having a number of passages of relatively small diameter arranged therein parallel to the axis of the polarizing device, the walls of said tubes being blackened internally.
5. A polarizing device comprising a plurality of plates divided into a plurality of sets disposed at opposite inclinations to the axis of the polarizing device, a double prism'between the sets of plates, a sin 1e prism on each of the remaining sides of t e sets of plates, and a mount for holding the combination, all arranged so that the light is caused to strike the plates at the polariz ing angle.
6. A polarizing device comprising a plurality of plates divided into a plurality of sets disposed at opposite inclinations of approximately 35 degrees to the axis of the polarizing device, a double prism between the sets of plates, a single prism on each of the remaining sides of the sets of plates, and a mount for holding the combination, all arranged so that the light is caused to strike the plates at the polarizing angle.
|Citing Patent||Filing date||Publication date||Applicant||Title|
|US2476014 *||Mar 23, 1945||Jul 12, 1949||Wright Edwin Herbert||Light polariser for producing light beams polarised in planes mutually at right angles from a single light beam|
|US2492809 *||Jun 15, 1946||Dec 27, 1949||Alvin M Marks||Unitary multiply polarizer|
|US3405992 *||Nov 10, 1964||Oct 15, 1968||Bell Telephone Labor Inc||Low reflection lenses and prisms|
|US3740117 *||Jul 22, 1971||Jun 19, 1973||Hewlett Packard Co||Acousto-optic filter having an increased optical beam aperture|
|US5357370 *||May 27, 1992||Oct 18, 1994||Matsushita Electric Industrial Co., Ltd.||Polarizer and light valve image projector having the polarizer|
|US5724184 *||Mar 14, 1994||Mar 3, 1998||Hesline; Raymond||Polarizer with birefringent plate|
|US7016112 *||May 30, 2002||Mar 21, 2006||Lg.Philips Lcd Co., Ltd.||Large scale polarizer and polarizer system employing it|
|US20020145799 *||May 30, 2002||Oct 10, 2002||Choi Jae Beom||Large scale polarizer and polarizer system employing it|
|U.S. Classification||359/485.4, 359/485.6|