US586708A - Erecting-prism - Google Patents
Erecting-prism Download PDFInfo
- Publication number
- US586708A US586708A US586708DA US586708A US 586708 A US586708 A US 586708A US 586708D A US586708D A US 586708DA US 586708 A US586708 A US 586708A
- Authority
- US
- United States
- Prior art keywords
- prism
- prisms
- erecting
- new
- reflecting
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
Images
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/04—Prisms
Definitions
- This invention relates to a new and improved optical appliance to which the name erecting prism has been applied, and which is designed to change any optical image, real or imaginary, one hundred and eighty degrees in its own plane without material distortion or lateral displacement.
- Figure 1 is a side elevation
- Fig. 2 an end view, of an old form of erectingprism
- Fig. 3 is a side elevation
- Fig. 4 an end view, of 'a modified and improved con struction of the prism
- Fig. l is a side elevation
- Fig. 5 is a side elevation
- Fig. 6 an end view
- Fig. 7 a plan view, of the new inverting or erecting prism.
- the first-named type is known as the Galilian telescope and is universally familiar in its use in opera-glasses.
- the second type is known as the terrestrial telescope or spyglass.
- the objection to type a is the smallness of the field of view, both absolute and apparent, which they possess. This fault is so serious that only very low magnifying powers are generally practicable, say up to tive or six diameters.
- the objections to type b are two-rst, a very material reduction in optical definition, and, second, an inordinate increase in length unless relatively high powers be employed.
- the prism 2 is a right-angle prism-that is to say, its reflecting-surfaces h t' are at an angle of ninety degrees, while the angles of prisms 1 and 3 admit of a wide range of variation, but for most purposes the thirty degrees, sixty degrees, and ninety degrees shown will be found preferable.
- the prisms 1 and 3 are erected one behind the other and extend equally on opposite sides of the line of intersection of the two planes forming the reflecting-surfaces h 1'- of prism 2, so that the rays of light entering prism 1 will emerge from prism 3 in inverted position, but without lateral displacement beyond such as is due to the inversion of the image. This is indicated by the dotted lines in Figs. 5 and 7, representing the course of a single ray of light tra-versing the prism.
- the dimensions of prism are determined by considerations which would at once be obvious to any skilled optician.
- the prism 2 would be of the dimensions indicated by dotted lines in Fig. 6, in which case the prisms 1 and 3 might be cemented directly to the upper surface of prism 2, but as this would involve an unnecessary and useless amount and width of materia-l comprising the right-angle prism 2 the excess at the sides, included in dotted lines, maybe removed or omitted.
- the new erecting-prism is made up of four pieces of glass cemented together, it is perfectly evident that, whether made inone, two, or more parts, so long as the four rlrentingsurfaces tions indicated its performance will be substantially the same.
- the three prisms 1, 2, and 3 may be employed alone or in combination with the parallel-sided plate 4.
- Prism 2 and plate -t may be combined as one piece of glass, or one or both of the prisms 1 and 3 maybe formed integral with plate 4.
- Prism 1 or 3, a portion of plate 4, and the whole of prism 2 might be made from one piece of glass and the other prism 1 or 3 and the remainder of plate i of another.
- the wholemight be formed of asin gle piece of glass, although there would in such case be great technical difficulties in construction experienced.
- the two reflecting-prisms 1 and 3 are arranged and disposed longitudinally of prism 2, with their reflecting-surfaces g and j extending across both reflecting-surfaces h z' of said prism 2, so that the ray of light reflected by surface g or j on one side of the median line will be directed against surface h and be reflected laterally' against surface t', while the rays reflected on the opposite side of themedian line will be directed against surfacet' and be reflected laterally onto surface h, the rays crossing within prism 2 after reflection from g or and finally emerging with a lateral displacement just proper to inversion of image only and which therefore vanishes for an axial ray.
- An erecting system or apparatus such as described, the same comprising four reflectingsurfaces, of which the intermediate surfaces are two planes intersecting at an angle of substantially ninety degrees, and the first and fourth surfaces are arranged one behind the other,in the direction of movement of light through the system, with the line of intersection of their planes substantially at right angles to the line of intersection of the intermediate surfaces, said first and fourth It may be found advantageous to cover all the reflecting-surfaces with a coating of silver or other reflectl ing material to protect them from soiling, &c. l
- An erecting system or prism such as described, the same comprising four reflectingsurfaces, g, h, 'i and j, of which the interme diate surfaces h and z' are arranged on intersecting planes, and the first and fourth sur-A faces, g and 7, are arranged in line longitudinally of said surfaces h and li, said surfaces g and j constituting converging planes lying transverse to and extending on opposite sides of the line of intersection between said surfaces h and z.
- An erecting system of prisms such as described, combining in its structure a prism 2, and two prisms 1 and 3, the latter arranged CHARLES S. HASTINGS.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Elements Other Than Lenses (AREA)
Description
UNITED STATES PATENT OFFICE.
CHARLES S. HASTINGS, OF NEV HAVEN, CONNECTICUT.
ERECTlNG-PRISM.
SPECIFICATION forming part of Letters Patent No. 586,708, dated July 20, 1897.
Application tiled May 5, 1897. Serial No. 635,228. (No model.)
.To all whom it may concern,.-
Be it known that I, CHARLES S. HASTINGS, a citizen of the United States, residing at New lIaven, in the county of New Haven and State of Connecticut, have invented certain new and useful Improvements in Erectin g-Prisms; and I do hereby declare the following to be a full, clear, and exact description of the same, reference being had to the drawings forming a part of this specification, and to the gures and letters of reference marked thereon.
This invention relates to a new and improved optical appliance to which the name erecting prism has been applied, and which is designed to change any optical image, real or imaginary, one hundred and eighty degrees in its own plane without material distortion or lateral displacement.
The said invention consists in certain new arrangements and combinations of re fleeting surfaces or prisms, as will hereinafter more fully appear, the novel features being pointed out in the claims.
In the accompanying drawings, illustrating the preferred form of embodiment of the said invention, Figure 1 is a side elevation, and Fig. 2 an end view, of an old form of erectingprism. Fig. 3 is a side elevation, and Fig. 4 an end view, of 'a modified and improved con struction of the prism, Fig. l. Fig. 5 is a side elevation, Fig. 6 an end view, and Fig. 7 a plan view, of the new inverting or erecting prism.
Similar figures and letters of reference in the several figures indicate the same parts.
One of the principal and most important applications of the new erecting-prism is in connection with telescopic instruments, as a substitute for the inverting lens or lenses heretofore commonly employed for converting inverting-telescopes, large or small, into erecting (terrestrial) telescopes. As is well known, the most perfect refractng-telescope which has heretofore been constructed presents to the eye of the observer an inverted image. Since this is immaterial in an astronomical use where everything should be sacrificed to perfection of definition, such telescopes, which, moreover, are the simplest in construction, are called astronomical telescopes; but inverted aspects of terrestrial objects are ordinarily not acceptable to any except the very small group of philoso- I' lf phers who have succeeded in emancipatng f" themselves from the purely arbitrary conceptions of up and down. llence it is usual to employ some means for correct-ing this perverted condition of affairs as it appears to the majority.
There are two methods in general use for modifying the telescope to meet the wants of the larger portion lof mankind not included in the class defined above-namely, by using (a.) a negative (i. e., essentially concave) lens at the proper distance for distinct vision inside the focus of the telescopic objective, or (1)) by replacing the simple ocular of the astronomical telescope by a more complex one, which is in fact a compound microscope, and thus yields an inverted view of the inverted image.
The first-named type is known as the Galilian telescope and is universally familiar in its use in opera-glasses. The second type is known as the terrestrial telescope or spyglass. The objection to type ais the smallness of the field of view, both absolute and apparent, which they possess. This fault is so serious that only very low magnifying powers are generally practicable, say up to tive or six diameters. The objections to type b are two-rst, a very material reduction in optical definition, and, second, an inordinate increase in length unless relatively high powers be employed.
There is an entirely distinct method of inverting the image-namely, by oblique reflections from plane surfaces. This has been accomplished by the employment of two polyhedra cemented together, as represented in Figs. 1 and 2, the rays of light entering at a being reflected by the surfaces Z), c, d, and e and emerging at f.
On account of the technical difiiculties in making this prism the improved form represented in Figs. 3 and 4 is to be preferred, it being constructed of three rectangular prisms cemented together, two of said prisms being of like dimensions and the third larger, as represented in the drawings. I
There are general objections to all of these forms of inverting-prisms-namely, their fas-...Kam
har'
width and the fact that the image is displaced l are caused to occupy substantially the relalaterally by a distance depending upon the size of the erecting-prism. This last-named property is especially inconvenient when the prisms are to be used in binocular telescopes. The new type of erecting or inverting prisms illustrated in Figs. 5, (i, and obviates the defect-s mentioned.
In the preferred form shown it may be said to comprise three prisms 1 2, and 3, furnishing the four reflecting-surfaces g, 7i, yi, and j. The prism 2 is a right-angle prism-that is to say, its reflecting-surfaces h t' are at an angle of ninety degrees, while the angles of prisms 1 and 3 admit of a wide range of variation, but for most purposes the thirty degrees, sixty degrees, and ninety degrees shown will be found preferable.
The prisms 1 and 3 are erected one behind the other and extend equally on opposite sides of the line of intersection of the two planes forming the reflecting-surfaces h 1'- of prism 2, so that the rays of light entering prism 1 will emerge from prism 3 in inverted position, but without lateral displacement beyond such as is due to the inversion of the image. This is indicated by the dotted lines in Figs. 5 and 7, representing the course of a single ray of light tra-versing the prism.
Having determined upon the angles and dimensions of prisms 1 and 3, the dimensions of prism are determined by considerations which would at once be obvious to any skilled optician. Thus, under the conditions illustrated, the prism 2 would be of the dimensions indicated by dotted lines in Fig. 6, in which case the prisms 1 and 3 might be cemented directly to the upper surface of prism 2, but as this would involve an unnecessary and useless amount and width of materia-l comprising the right-angle prism 2 the excess at the sides, included in dotted lines, maybe removed or omitted. So, too, the end sections ofprism 2, included in dotted lines, are unnecessary and may be omitted, and all that part intermediate the triangular section bounded byfull lines indicating prism 2 proper and the two prisms 1 and 3 may be omitted without departing from the spirit of the present invention; butit is preferred for obvious reasons that this intermediate space should be filled so as to eliminate reflecting-surfaces. Hence it is preferred to make the prism 2 smallerthat is, proportionally, as indicated in the drawings-and fill the iu terval between it and the prisms 1 and 3 with a parallel-sided plate 4.
As to prism 2, it. maybe said that the right angle must be very accurate-say to within one minute of arc-but the other angles admit of errors vastly greater than this without material injury to the performance.
Although in the preferred construction the new erecting-prism is made up of four pieces of glass cemented together, it is perfectly evident that, whether made inone, two, or more parts, so long as the four rllebtingsurfaces tions indicated its performance will be substantially the same. Thus, as hereinbefore explained, the three prisms 1, 2, and 3 may be employed alone or in combination with the parallel-sided plate 4. Prism 2 and plate -t may be combined as one piece of glass, or one or both of the prisms 1 and 3 maybe formed integral with plate 4. Prism 1 or 3, a portion of plate 4, and the whole of prism 2 might be made from one piece of glass and the other prism 1 or 3 and the remainder of plate i of another. Finally, the wholemight be formed of asin gle piece of glass, although there would in such case be great technical difficulties in construction experienced.
illustrate the manner of applying the new erecting-prism to a telescope, as this will readily be understood by any one skilled in the art, nor is it to be understood that the new prism is limit-ed in use to such instruments, as it is obvious that it could be employed to advantage in other instruments and under different conditions-as, for example, in dissecting-microscopes, &c.
Upon comparison with the older forms of erecting-prisms illustrated in Figs. 1 to i, inclusive, it will be noticed that the new prism presents this point of great importance and advantage, it preserves the axial alinement of the lenses employed, and it. does not effect lateral displacement of the object as viewed in the ocular. This is due to the fact that the two reflecting- prisms 1 and 3 are arranged and disposed longitudinally of prism 2, with their reflecting-surfaces g and j extending across both reflecting-surfaces h z' of said prism 2, so that the ray of light reflected by surface g or j on one side of the median line will be directed against surface h and be reflected laterally' against surface t', while the rays reflected on the opposite side of themedian line will be directed against surfacet' and be reflected laterally onto surface h, the rays crossing within prism 2 after reflection from g or and finally emerging with a lateral displacement just proper to inversion of image only and which therefore vanishes for an axial ray.
Having thus fully described my invention, what I claim as new, and desire to secure by Letters Patent, is-
1. An erecting system or apparatus, such as described, the same comprising four reflectingsurfaces, of which the intermediate surfaces are two planes intersecting at an angle of substantially ninety degrees, and the first and fourth surfaces are arranged one behind the other,in the direction of movement of light through the system, with the line of intersection of their planes substantially at right angles to the line of intersection of the intermediate surfaces, said first and fourth It may be found advantageous to cover all the reflecting-surfaces with a coating of silver or other reflectl ing material to protect them from soiling, &c. l
It has not been considered necessary to surfaces extending across and on opposite sides of the line of intersection of the intermediate planes; substantially as described.
2. An erecting system or prism, such as described, the same comprising four reflectingsurfaces, g, h, 'i and j, of which the interme diate surfaces h and z' are arranged on intersecting planes, and the first and fourth sur-A faces, g and 7, are arranged in line longitudinally of said surfaces h and li, said surfaces g and j constituting converging planes lying transverse to and extending on opposite sides of the line of intersection between said surfaces h and z.
3. An erecting system of prisms, such as described, combining in its structure a prism 2, and two prisms 1 and 3, the latter arranged CHARLES S. HASTINGS.
Witnesses:
C. B. RICHARDS, GEO. II. CLARK.
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US586708A true US586708A (en) | 1897-07-20 |
Family
ID=2655378
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US586708D Expired - Lifetime US586708A (en) | Erecting-prism |
Country Status (1)
| Country | Link |
|---|---|
| US (1) | US586708A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2593904A (en) * | 1949-08-01 | 1952-04-22 | Leitz Ernst Gmbh | Image-inverting optical system |
| US3976368A (en) * | 1973-12-03 | 1976-08-24 | Polaroid Corporation | Special optical element for camera to microscope adaptor |
-
0
- US US586708D patent/US586708A/en not_active Expired - Lifetime
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2593904A (en) * | 1949-08-01 | 1952-04-22 | Leitz Ernst Gmbh | Image-inverting optical system |
| US3976368A (en) * | 1973-12-03 | 1976-08-24 | Polaroid Corporation | Special optical element for camera to microscope adaptor |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN104597600B (en) | A kind of Keplerian optical system of compact conformation | |
| Swift | Image rotation devices—a comparative survey | |
| US1468762A (en) | Telescope, microscope, and the like | |
| US2354614A (en) | Optical projection system | |
| US1955591A (en) | Lens | |
| US1931992A (en) | Anamorphosing prism objective | |
| US2375634A (en) | Prism telescope | |
| US2386621A (en) | Artificial horizon for sextants | |
| US20190258060A1 (en) | Virtual reality image system with high definition | |
| US4779965A (en) | Eccentric close-up lens converting a binocular into a stereomicroscope | |
| US1446634A (en) | Photographic lens | |
| US1843519A (en) | Projection objective | |
| US2135531A (en) | Optical instrument | |
| US1794419A (en) | Magnifier | |
| US1197742A (en) | Lens system. | |
| CN108549145A (en) | A kind of new construction of list object binocular | |
| US2550685A (en) | Optical objective balance assembly | |
| US1712112A (en) | Eyepiece for optical instruments | |
| US2410757A (en) | Optical prism system | |
| JPH0458006B2 (en) | ||
| US3402977A (en) | Wide angle binocular telescopic instrument having the axes of the telescopes converging towards the observer | |
| CN207081887U (en) | A low magnification large field of view telescope | |
| US1637563A (en) | Binocular microscope | |
| US1964075A (en) | Means for reflecting light | |
| US2015527A (en) | Eye-piece having optical members that consist of a lens system and a prism system |