Reversing system for a sighting telescope
20170255000 · 2017-09-07
Assignee
Inventors
Cpc classification
G02B23/00
PHYSICS
G02B7/10
PHYSICS
F41G1/38
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
G02B23/16
PHYSICS
International classification
G02B23/16
PHYSICS
Abstract
The invention concerns a reversing system for a sighting telescope, where the reversing system has at least two mutually displaceable lenses in a tube of the reversing system parallel to an optical axis of the reversing system, where displacement of the at least two displaceable lenses modifies the reproduction scale at which an image projected onto a first image plane of the reversing system is shown on a second image plane of the reversing system, where the at least two displaceable lenses are arranged in all positions between the first and the second image plane, where a surface of the inside of a tube facing the optical axis having at least one absorption area with absorption zones for absorbing incident light and with sliding surfaces located between neighbouring absorption zones for bearings of the at least two displaceable lenses, where the total area of the sliding surfaces is smaller than the total area of the absorption zones, where the at least one sliding surface is arranged at a different distance from the optical axis than the at least one absorption zone.
Claims
1. A reversing system for a sighting telescope, where the reversing system has at least two lenses arranged in a tube of the reversing system and being mutually displaceable parallel to an optical axis of the reversing system, where displacement of the at least two displaceable lenses modifies the reproduction scale at which an image projected onto a first image plane of the reversing system is shown on a second image plane of the reversing system, where the at least two displaceable lenses are arranged in all positions between the first and the second image plane, characterised by a surface of the inside of a tube facing the optical axis having at least one absorption area with absorption zones for absorbing incident light and with sliding surfaces located between neighbouring absorption zones for bearings of the at least two displaceable lenses, where the total area of the sliding surfaces is smaller than the total area of the absorption zones, where the sliding surfaces are arranged at a different distance from the optical axis than the absorption zones.
2. The reversing system according to claim 1, wherein a ratio of the area content of the at least one absorption zone and the area content of the at least one sliding surface being greater than or equal to 2:1.
3. The reversing system according to claim 1, wherein the at least one absorption zone having a distance from the optical axis that is at least 30 μm larger or smaller than that of the at least one sliding surface.
4. The reversing system according to claim 1, wherein a longitudinal section parallel to the optical axis of the inside of the tube having sliding surfaces and absorption zones placed alternately one after the other.
5. The reversing system according to claim 1, wherein the at least one absorption zone having at least one groove running diagonally to or across the optical axis, where the at least one groove in the surface of the tube facing the optical axis is formed by removing material forming one wall of the tube, where the sliding surfaces are formed of at least one stop ridge formed of material of the wall of the tube that has not been removed.
6. The reversing system according to claim 5, wherein the at least one stop ridge having a width with a value from a range between 0.05 mm and 0.5 mm.
7. The reversing system according to claim 5, wherein the at least one groove having a depth with a value from a range between 0.05 mm and 1 mm.
8. The reversing system according to claim 5, wherein the at least one groove having a width at its widest point with a value from a range between 0.2 mm and 2 mm.
9. The reversing system according to claim 5, wherein the at least one groove being formed by a screw-shaped depression in a wall of the tube on the inner surface of the tube that faces the optical axis and running around the optical axis.
10. The reversing system as per claim 9, wherein at least one screw-shaped circular groove having a gradient with a value from a range between 0.2 mm and 2 mm.
11. The reversing system according to claim 5, wherein an angle bisector of an opening angle of the at least one groove being slanted towards the first image plane of the reversing system.
12. The reversing system according to claim 5, wherein the at least one groove having a leading edge in the direction of the first image plane and that merges into the least one stop ridge and a back edge running diagonally to the leading edge, where the leading edge and the back edge form an acute angle to each other and the leading edge makes an angle with the optical axis with a value taken from a range between 20° and 24°.
13. The reversing system according to claim 12, wherein a transitional area between the back edge and the leading edge having a radius of curvature smaller than 0.05 mm.
14. The reversing system according to claim 5, wherein the at least one absorption zone have multiple grooves placed one after another in the direction of the optical axis.
15. The reversing system according to claim 1, the tube having a length whose value comes from a range between 80 mm and 150 mm.
16. The reversing system according to claim 1, wherein the tube having an external diameter smaller than 35 mm.
17. The reversing system according to claim 1, wherein value of the reproduction scale between the first and second image plane of the reversing system being at least 7 in the position of the at least two displaceable lenses that corresponds to the largest magnification of the reversing system.
18. The reversing system according to claim 1, wherein the value of the reproduction scale between the first and second image plane of the reversing system being at least 0.9 in the position of the at least two displaceable lenses that corresponds to the smallest magnification of the reversing system.
19. The reversing system according to claim 18, wherein the value of the reproduction scale between the first and second image plane of the reversing system being a maximum of 1.2, in the position of the at least two displaceable lenses that corresponds to the smallest magnification of the reversing system.
20. The reversing system according to claim 1, wherein the position of the at least two displaceable lenses that corresponds to the largest reproduction scale at which the image projected on the first image plane of the reversing system is shown upright and magnified on the second image plane of the reversing system, the at least one absorption area being located behind the at least two displaceable lenses when viewed from the direction of the at least two displaceable lenses.
21. The reversing system according to claim 1, wherein each of the bearings of the at least two displaceable lenses being executed as a tubular sleeve, where at least three glide stops are arranged on the external surface of each bearing to support the particular bearing on the surface of the inside of the tube that faces the optical axis.
22. The reversing system according to claim 21, wherein the tube whose surface facing the optical axis has the at least one absorption zone, having at least one longitudinal channel running parallel to the optical axis and placed in a guide rod that can be twisted around the optical axis, where the guide rod has at least two curved guide channels and each of the bearings has at least one tappet that engages both in the longitudinal channel and in one of the at least two guide channels, where the tappets of different bearings engage in different guide channels, where at least one reinforcing ring is placed touching the sheath surface of the guide rod such that it grasps the sheath surface in a ring.
23. The reversing system according to claim 1, wherein the position of the first image plane and the position of the second image plane of the reversing system being constant, independently of the current position of the at least two displaceable lenses, viewed in the direction of the optical axis.
24-29. (canceled)
Description
[0038] To facilitate better understanding of the invention, it will be explained in detail using the figures below.
[0039] Extremely simplified, schematic depictions show the following:
[0040]
[0041]
[0042]
[0043]
[0044]
[0045]
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[0048] In introduction, let it be noted that in the variously described embodiments, identical parts are provided with identical reference signs or identical component names, and that the disclosures contained in the description as a whole can be carried over analogously to identical parts with identical reference signs or identical component names. Likewise, positional information selected in the description, e.g. above, below, on the side, etc. refer to the directly described and depicted figure and if the position is changed, this positional information carries over analogously to the new position.
[0049] All information regarding ranges of values in this description should be understood to mean that these include any and all partial ranges, e.g. the statement 1 to 10 should be understood to mean that all partial ranges starting from the lower threshold 1 and the upper threshold 10 are included, i.e. all partial ranges begin with a lower threshold of 1 or larger and with an upper threshold of 10 or less, e.g. 1 to 1.7 or 3.2 to 8.1 or 5.5 to 10.
[0050]
[0051]
[0052]
[0053] As these optical elements, the optical system of the reversing system 5 comprise a field lens 13 placed in an end area of the reversing system 5 on the objective side. In the direction towards an ocular-side end area, a first zoom lens 15, a second zoom lens 16, and a diverging lens 17 follow along an optical axis 14. The two zoom lenses 15, 16 are each held in a bearing 18, 19 and are mutually displaceable along the optical axis 14. To achieve this, the two bearings 18, 19 are situated touching the inside 20 of the reversing system tube 12 and are displaceable in the direction of the optical axis 14.
[0054] Each of the bearings 18, 19 has a tappet 21, 22 protruding in the axial direction (in reference to the optical axis 14). These tappets 21, 22 extend through a longitudinal channel 23 formed in the reversing system tube 12 and into one of the two guide channels 10, 11 of the guide rod 9. In this way a cam mechanism is formed between the reversing system tube 12, the guide rod 9, and the two bearings 18, 19 with the zoom lenses 15, 16 by which the zoom lenses 15, 16 can be displaced in the axial direction. For this purpose, the curved shapes of the guide channels 10, 11 in the guide rod 9 are designed so that when the zoom lenses 15, 16 are displaced the position of the two intermediate image planes 61, 62 is not changed (at least for the limiting case of an image of an object at infinity).
[0055] In the example embodiment shown, the guide channel 10 determines a displacement range in the axial direction with a length 81 of approx. 55 mm for the bearing 18 and/or zoom lens 15. The guide channel 11 allows the zoom lens 16 and/or the second bearing 19 a range of movement with a length 82 of approx. 61 mm, where the reversing system tube 12 has a length 83 of 115.2 mm. In modified embodiments of the reversing system 5, the length 83 of the reversing system tube 12 can take values from a range between 80 mm to 150 mm.
[0056] The lenses of the reversing system 5 have the following focal lengths, in each case based on a wavelength of light of 546 nm. The field lens 13 has a focal length of +54.1 mm; the first zoom lens 15 a focal length of +37.8 mm; the second zoom lens 16 a focal length of +41.6 mm and the diverging lens 17 a (negative) focal length of −29.6 mm. The placement of the lenses relative to each other is chosen so that a distance 63 between the first image plane 61 and the field lens 13 has a value of 11.3 mm and a distance 64 between the diverging lens 17 and the second image plane 62 has a value of 30.8 mm, where an image plane distance 65 of the second image plane 62 to the first image plane 61 has a value of 137 mm.
[0057] In alternative embodiments of the reversing system 5, the values of the focal lengths can fall in the following ranges. The focal length of the field lens 13 between 44.1 mm and 64.1 mm; the focal length of the first zoom lens 15 between 27.8 mm and 47.8 mm; the focal length of the second zoom lens 16 between 31.6 mm and 51.6 mm and the focal length of the diverging lens 17 between −39.6 mm and −19.6 mm. Accordingly, the values of the aforesaid lengths and distances can be varied by +/−20%.
[0058] In the preferred embodiment of the invention, adjusting the zoom lenses 15, 16 along the optical axis 14 can produce a reproduction scale of a range between −1.038 (the smallest total magnification of the telescope 1) to −8.238 (the largest total magnification of the telescope 1), achieving a zoom factor with a value of 8.
[0059] Such high zoom factor values (compared to previously standard values of up to 4 or up to 6) necessitate high accuracy of fit of the guiding of the bearings 18, 19 in the reversing system 12, as well as high precision in the displacement of the bearings 18, 19 in the axial direction caused by the interaction of the tappets 21, 22 with the guide channels 10, 11 and/or the longitudinal channel 23. For this reason, a reinforcement ring 24 is further specified for the reversing system 5 which is arranged touching or affixed to the circumference of the guide rod 9.
[0060] As depicted in
[0061]
[0062] To avoid stray light, it is in general specified that the internal walls of lens mounts and optical housings be blackened (e.g. anodised in black). However, it occurs that, in particular with very smooth surfaces and very shallow or glancing angles of incidence of the light rays, blackening the surface alone is not sufficient. Incidentally, where this description speaks of “stray light,” please refer to the standard measurement as per DIN ISO 11490-6 (Optics and photonics, testing procedure for telescopes, part 6: Specification of stray light proportion).
[0063] To suppress stray light, it can be provided that the area 25 of the inside 20 of the reversing system tube 12 be designed with a tightly placed succession of grooves or channels 26. As depicted in
[0064] In an alternative embodiment, the channels 26 are formed by a screw-shaped or thread-shaped depression. The grooves or channels 26 in the area 25 of the inside 20 can also run diagonal to or across the optical axis 14 of the reversing system 5.
[0065] Each of the channels 26 forms an absorption zone for light rays incident on it. These channels 26 are preferably produced by removing some of the material forming the wall of the reversing system tube 12, for example through milling or lathing. This produces a succession of depressions/grooves forming the channels 26 and sliding surfaces 27 located between neighbouring channels 26. In this example embodiment, the channels 26 are produced with a width 28 with a value of 0.25 mm and a depth 29 with a value of 0.1 mm. The width 30 of the sliding surfaces 27 between two neighbouring channels 26 has a value of 0.1 mm. The ratio of the width 28 of a channel 26 to the width 30 of a sliding surface 27 is preferably larger than 1:1. It is beneficial for the light-absorbing effect if the area ratio of the channel 26 or the absorption zones is proportionally high. The choice of the width 28 of the channels 26 and the width 30 of the sliding surfaces 27 is favourable when the area content of the channel 26 to the area content of the sliding surface 27 has a ratio of larger than or equal to 2:1.
[0066] The area content of the channel 26 or absorption zone is understood as the value of the area of the channel 26 projected vertically onto the inside 20 of the reversing system tube 12. The given ratios should also be understood in this way and refer to the absorption area or the area 25 of the inside 20 of the reversing system tube 12. It is advantageous if the total area of the sliding surfaces 27 in the area 25 is smaller than the total area of the absorption zones 26.
[0067] The absorption zones predominantly have a 30 μm greater distance or radius from the optical axis 14 than the sliding zone 27.
[0068] It proves to be particularly advantageous if a longitudinal section parallel to the optical axis 14 of the inside 20 of the reversing system tube 12 has sliding surfaces 27 and absorption zones 26 placed alternately one after the other. This is because the reflection-suppressing effect of the absorption area on the inside 20 of the reversing system tube 12 is particularly effective for glancing light incident in the longitudinal direction.
[0069]
[0070] It is particularly beneficial for avoiding the formation of stray light if the back edge 32 together with the optical axis 14 (
[0071]
[0072] The following measurements/ranges of values in particular have proven to be beneficial in designing the fluting in the area 25 of the inside 20 of the reversing system tube 12. The width 30 of the sliding surfaces 27/the stop ridges between neighbouring channels 26 is preferably taken from a range between 0.05 mm and 0.5 mm. The depth 29 of the grooves/channels 26 can take values from a range between 0.05 mm and 1 mm. The depth 28 of the channels 26 can take values from a range between 0.2 mm and 0.3 mm. If the channels 26 are designed as a thread-like or screw-like circular depression, the value of the gradient or the value of the pitch can be chosen from a range between 0.2 mm and 2 mm. During manufacturing of the reversing system tube 12, i.e. especially during manufacturing of the inside 20 and the section 25 of the reversing system tube 12 furnished with grooves, it is specified that a final processing step will hone the stop ridges/sliding surfaces 27 in order to ensure the most precise possible fit of the bearings 18, 19 with the two zoom lenses 15, 16.
[0073]
[0074] Otherwise, the reversing system 5 as per the invention can produce sighting telescopes 1 with a subjective visual field with a value greater than 23.0°, preferably with a value from a range of 23.5° to 24.5°. To achieve this, the reversing system 5 may e.g. be combined with an ocular 3 with a focal length value of 47.9 mm. An example value of the objective in this case might be 46.2 mm.
[0075] The example embodiments show possible variations; let it be noted at this juncture that diverse combinations of the individual variations of embodiments are possible and that this possibility of variation falls within the competence of a person active in this technical field based on the teaching regarding technical action provided by this invention.
[0076] The scope of protection is determined by the claims. However, the description and the drawings should be used to interpret the claims. Individual characteristics or combinations of characteristics from the depicted and described various example embodiments can constitute independent inventive solutions. The aim underlying the independent invented solutions can be taken from the description.
[0077] As a matter of form, let it be noted that, to facilitate a better understanding of the design, elements have in places been portrayed not to scale and/or enlarged and/or scaled-down.
TABLE-US-00001 List of reference signs 1 Sighting telescope 31 Leading edge 2 Objective 32 Back edge 3 Ocular 33 Angle 4 Central tube 34 Angle bisector 5 Reversing system 35 Radius 6 Top turret 36 Sheath 7 Ocular housing 37 Glide stop 8 Adjusting ring 38 9 Guide rod 39 10 Guide channel 40 11 Guide channel 61 First image plane 12 Reversing system tube 62 Second image plane 13 Field lens 63 Distance 14 Optical axis 64 Distance 15 Zoom lens 65 Image plane distance 16 Zoom lens 81 Length 17 Stray light 82 Length 18 Bearing 83 Length 19 Bearing 84 20 Inside 21 Tappet 22 Tappet 23 Longitudinal channel 24 Reinforcement ring 25 Area 26 Channel 27 Sliding surface 28 Width 29 Depth 30 Width