CN201852990U - Long-wave infrared continuous zoom lens - Google Patents
Long-wave infrared continuous zoom lens Download PDFInfo
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- CN201852990U CN201852990U CN2010205423917U CN201020542391U CN201852990U CN 201852990 U CN201852990 U CN 201852990U CN 2010205423917 U CN2010205423917 U CN 2010205423917U CN 201020542391 U CN201020542391 U CN 201020542391U CN 201852990 U CN201852990 U CN 201852990U
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- wave infrared
- infrared continuous
- continuous zoom
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Abstract
The utility model discloses a long-wave infrared continuous zoom lens; four lenses are arranged in sequence along an optical axis from object space to image space, wherein the first lens and the third lens are fixed on the optical axis and can not move; the second lens and the fourth lens can move along the optical axis; the second lens is a variable-time lens and the fourth lens is a compensation lens; and a fixed system diaphragm is arranged between the second lens and the third lens. In the utility model, zoom with high multiple proportions is realized by adopting the four lenses, so that the system is more compact in structure, lighter in weight, lower in processing cost and simpler for assembly. Furthermore, in the utility model, in a lens group, the fixed system diaphragm is adopted at a specific position so that the long-wave infrared continuous zoom lens keeps a fixed relative aperture in the zoom process all the time, therefore, the problem that the system sensitivity of the traditional design changes in the zoom process is solved; and proved by practices, the technical scheme has better application effect.
Description
Technical field
The utility model relates to a kind of zoom lens, relates in particular to a kind of non-refrigeration type detector compact long-wave infrared continuous zoom lens that is used for.
Background technology
At present, the development of continuous magnification lens and application more and more are extensive.Especially be applied in the long-wave infrared continuous zoom lens on the non-refrigeration type detector, obtained increasing use especially.
This be because, at first, the non-refrigeration detector technology of LONG WAVE INFRARED more and more be the maturation; The second, the non-refrigeration type detector has characteristics such as compact conformation, power consumption is little, cost is low; These characteristics have determined non-refrigeration detector to be widely used in dual-use each field.
Wherein, the infrared continuous magnification lens of its configuration can change system's focal length within the specific limits by mobile lens set, makes the big or small continuous variable of image planes scenery to reach big visual field ferret out, and the purpose of small field of view object observing has a good application prospect.
In the existing public technology, non-refrigeration long-wave infrared continuous zoom lens eyeglass quantity is mostly more than 5 and 5, and camera lens relative aperture in the continuous vari-focus process is unfixing, has problems such as the continuous vari-focus system length is long, Installation and Debugging are difficult, cost height.
The utility model content
Zoom system, pancreatic system length at traditionally zoom lens is long, the unfixed deficiency of relative aperture in the continuous vari-focus process, the utility model provides a kind of long-wave infrared continuous zoom lens, this zoom lens has compact conformation, technological merit that transmitance is high, and, described zoom lens can be realized the change multiple proportions of 4 times even 5 times by 4 eyeglasses, solve existing continuous magnification lens unfixed problem of relative aperture in the zoom process, had technological merit preferably.
The technical scheme that the utility model solves the problems of the technologies described above is as following description:
A kind of long-wave infrared continuous zoom lens, be disposed with four lens along optical axis from object space to picture side, wherein, described first lens and the 3rd lens are to be fixed on the optical axis and can not to move, described second lens and the 4th lens can move along optical axis, wherein, second lens are that Zoom lens, the 4th lens are offset lens.
Further, the diameter of described first lens and system's length overall satisfy following expression formula:
1.1＜(D1/FNO)/ft＜1.2 and
TT/ft＜1.5；
Wherein, D1 is the diameter of first lens;
FNO is the F number of LONG WAVE INFRARED continuous magnification lens;
Focal length when ft is the burnt state of the length of long-wave infrared continuous zoom lens;
TT is the distance that image planes are arrived on object space centre of surface summit in first lens.
Further, described first lens, second lens, the 4th lens satisfy following expression formula:
-1.0＜f2/f1＜-0.1 and
f4/ft＞0.5；
Wherein, f1 is the focal length of first lens;
F2 is the focal length of second lens;
F4 is the focal length of the 4th lens;
Ft is the focal length of long-wave infrared continuous zoom lens when the burnt state of length.
Further, between described second lens and the 3rd lens fixing system stop is arranged.
Further, when described camera lens from the wide-angle state when looking in the distance state variation, the distance between described second lens and first lens is increasing always, the distance between the 4th lens and the 3rd lens diminishes earlier and afterwards becomes big.
Further, described first lens be have positive refractive power, convex surface is towards the positive meniscus lens of thing side; Second lens are the double-concave negative lens with negative refractive power, and the 3rd lens, the 4th lens are the lens with positive refractive power.
The utility model compared with prior art has following advantage and beneficial effect:
At first, the utility model realizes that by adopting four eyeglasses high powers than zoom, make the structure of system become more compact, cuts down finished cost and makes the assembling of system become more simple; In addition, because among the lens combination of the present utility model, adopt fixing system stop at ad-hoc location, make described long-wave infrared continuous zoom lens in the process of zoom, remain fixing relative aperture, thereby solved the traditional design problem that system sensitivity changes in the zoom process, facts have proved that this kind technical scheme has effect preferably.
Description of drawings
By the description of its exemplary embodiment being carried out below in conjunction with accompanying drawing, the above-mentioned feature and advantage of the utility model will become apparent and understand easily.
Fig. 1 is the structural representation of the specific embodiment of long-wave infrared continuous zoom lens described in the utility model;
Fig. 2 is the zoom process synoptic diagram of Fig. 1 specific embodiment, and wherein, Fig. 2 a is that wide-angle view, Fig. 2 b are that middle burnt view, Fig. 2 c are the view of looking in the distance;
Fig. 3 A-3C is the Aberration Analysis figure of specific embodiment when the wide-angle state of the described long-wave infrared continuous zoom lens of Fig. 1, and wherein, Fig. 3 A is that longitudinal aberration diagram, Fig. 3 B are that astigmatism figure, Fig. 3 C are distortion figure;
Fig. 4 A-4C is the Aberration Analysis figure of specific embodiment when middle burnt state of the described long-wave infrared continuous zoom lens of Fig. 1, and wherein, Fig. 4 A is that longitudinal aberration diagram, Fig. 4 B are that astigmatism figure, Fig. 4 C are distortion figure;
Fig. 5 A-5C is the Aberration Analysis figure of specific embodiment when looking in the distance state of the described long-wave infrared continuous zoom lens of Fig. 1, and wherein, Fig. 5 A is that longitudinal aberration diagram, Fig. 5 B are that astigmatism figure, Fig. 5 C are distortion figure.
Embodiment
Fig. 1 is the structural representation of long-wave infrared continuous zoom lens described in the utility model.
In general, because long-wave infrared continuous zoom lens is applied in the non-refrigerated thermal imager, therefore, need this kind structure compact and simple in structure as much as possible, in order to overcome the shortcoming of traditional lens more than 5, the utility model has been taked four lens, and, by means of certain focal power parameter designing, can reach the technique effect of the change multiple proportions of 4 times even 5 times.
As shown in the figure, this long-wave infrared continuous zoom lens, it is disposed with from the object side to image side along optical axis: have positive refractive power first lens 100, have second lens 200 of negative refractive power, the 4th lens 400 and the imaging surface 600 that has the 3rd lens 300 of positive refractive power and have positive refractive power, wherein, the picture that enters from first lens 100 passes after the lens, enters at last among the imaging surface 600.
Wherein, described first lens 100 and the 3rd lens 300 are to be fixed on the optical axis and can not to move, and described second lens 200 and the 4th lens 400 can move along optical axis, wherein, second lens 200 are offset lens for Zoom lens, the 4th lens 400
Wherein, these first lens 100 are the positive meniscus lens of convex surface towards the thing side; These second lens 200 are double-concave negative lens, and first lens 100 and the 3rd lens 300 are universal focus lens, and second lens 200 and the 4th lens 400 are zoom lens.
Because the camera lens of design traditionally F number in the continuous vari-focus process is unfixing, has problems such as the continuous vari-focus system length is long, Installation and Debugging are difficult, cost height.
In order to solve this technical problem, we are provided with a fixing system stop 500 at design between second lens 200 and the 3rd lens 300, and, this fixed system diaphragm 500 is chosen as aperture diaphragm, described aperture diaphragm position and size in camera lens zoom process do not change, and the entrance pupil size keeps changing in proportion with focal length, thereby guarantees that relative aperture is constant.
Fig. 2 is the zoom process synoptic diagram of Fig. 1 specific embodiment, and wherein, Fig. 2 a is that wide-angle view, Fig. 2 b are that middle burnt view, Fig. 2 c are the view of looking in the distance.
As shown in the figure, we can be clear that, when described camera lens from the wide-angle state when looking in the distance state variation, the relative object in the position of described first lens 100 is not moved, second lens 200 are to doing one-way movement as side and progressively near image planes 600; Simultaneously, described the 4th lens 400 move to the direction that deviates from image planes 600 earlier, arriving behind a certain position again, the direction to image planes 600 moves, thereby, we can know, distance between described second lens 200 and first lens 100 is increasing always, and the distance between the 4th lens 400 and the 3rd lens 300 diminishes earlier and afterwards becomes big.
Wherein, the purpose of first lens 100 and the 3rd lens 300 mainly is to converge light path; Second lens 200 are mainly used in the focal length that changes whole zoom lens, increase the change times multiplying power of system.
And the 4th lens 400 mainly are the effects of having played the compensation zoom, and specifically, its effect mainly contains following two: the firstth, and the image planes offset in the bucking-out system zoom process, the secondth, compensation image planes offset under the particular focal length different object distances.
From said process, we can see that at ad-hoc location fixed aperture being set can be implemented in that relative aperture does not change in the camera lens zoom process, thereby solved the traditional zoom camera lens problem that system sensitivity changes in the zoom process, promptly this kind scheme has the better application effect.
In order to realize the effect of whole long-wave infrared continuous zoom lens system compact, we need further to regulate some lens parameters of zoom lens, and as a rule, the adjusting of this kind parameter is to rely on the parameter of regulating first lens 100 to realize.
We preferably select, and the diameter of described first lens and system's length overall satisfy following expression formula:
1.1＜(D1/FNO)/ft＜1.2 and
TT/ft＜1.5；
Wherein, D1 is the diameter of first lens;
FNO is the F number of LONG WAVE INFRARED continuous magnification lens;
Focal length when ft is the burnt state of the length of long-wave infrared continuous zoom lens;
TT is the distance that image planes are arrived on object space centre of surface summit in first lens.
In addition, we for the hypermutation of realizing system doubly and aberration correction, the focal length of first lens combination 100, second lens combination 200 and the 4th lens 400 need meet the following conditions:
-1.0＜f2/f1＜-0.1 and
f4/ft＞0.5；
Wherein, f1 is the focal length of first lens combination;
F2 is the focal length of second lens combination;
F4 is the focal length of the 4th lens combination;
Focal length when ft is the burnt state of system head.
In the present embodiment, the lens materials that we choose above-mentioned four lens is germanium, because germanium has the refractive index height, therefore advantage such as chromatic dispersion is little, and processing cost is low, has better technical effect.
In addition, our preferred first lens 100, second lens 200, the 3rd lens 300 and the 4th lens 400 all are to take non-spherical lens to form.
The characteristics of non-spherical lens are: is continually varying from the lens center to peripheral curvature.Different with the spherical lens that certain curvature is arranged from the lens center to the periphery, non-spherical lens has better radius-of-curvature characteristic, has to improve the advantage of distorting aberration and improving astigmatic image error, can make the visual field become bigger and true.After adopting non-spherical lens, can eliminate the aberration that in imaging, occurs as much as possible, thereby improve image quality.
In general, the shape of non-spherical lens can limit with the certain expression formula.That is:
Above-mentioned non-spherical lens satisfies following expression formula:
In the formula, Z is an aspheric surface along optical axis direction highly for the position of Y the time, apart from the aspheric surface summit apart from rise Sag, R represents the paraxial radius-of-curvature of minute surface, k is circular cone coefficient conic, A, B, C, D, E are the high order aspheric surface coefficient.
Below with reference to following form the utility model is made a more detailed description.
In the present embodiment, the focal length of camera lens is 15-60mm, becomes multiple proportions and is 4, and the F number is 1.2, and the pass of each focal length and systematic parameter is: f2/f1=-0.26, f4/ft=0.515.
Wherein, f1 is the focal length of first lens, and f2 is the focal length of second lens, and f4 is the focal length of the 4th lens, the focal length when ft is the burnt state of system head.
Wherein, table one is the optical component parameter table of present embodiment.
Wherein D1 is the spacing of first lens 100 and second lens 200; D2 is the spacing of second lens 200 and the 3rd lens 300; D3 is the spacing of the 3rd lens 300 and the 4th lens 400; D4 is the spacing of the 4th lens 400 and image planes 600; We are parallel from object space one side along optical axis, and with each lens number consecutively, the face of first lens 100 is A1, A2, and the face of second lens 200 is A3, A8, and the minute surface of the 3rd lens 300 is A4, A5, and the minute surface of the 4th lens 400 is A6, A7.A1, A2, A3, A4, A5, A6, A7 are aspheric surfaces.A8 can be for sphere, also can be aspheric surface.
Table two is above-mentioned aspheric aspherical surface data table, and wherein, what A, B, C, D, E represented is the high order aspheric surface coefficient of each lens; Table three is the relation of zoom group position and lens combination spacing.
Table one, optical component parameter table
Table two: aspherical surface data
Table three is tabulations of the spacing between zoom lens and the lens combination in the above-mentioned long-wave infrared continuous zoom lens, and wherein, D1 is the spacing of first lens and second lens; D2 is the spacing of second lens and the 3rd lens; D3 is the spacing of the 3rd lens and the 4th lens; D4 is the spacing of the 4th lens and image planes.
The relation of table three, zoom group position and lens combination spacing
Wherein, during the wide-angle state focal length of lens combination minimum, the state of looking in the distance is maximum focal length.
Can find from table three, in this preferred embodiment, above-mentioned long-wave infrared continuous zoom lens camera lens relative aperture when wide-angle side is changed to telescope end remains unchanged, this is the difference of this programme and scheme before, can eliminate a series of problems that camera lens causes owing to the relative aperture difference in the zoom process, also shorten the length of camera lens simultaneously.
Below with reference to Aberration Analysis figure effect of the present utility model is done further detailed description.
Fig. 3 A-3C is the Aberration Analysis figure of specific embodiment when the wide-angle state of the described long-wave infrared continuous zoom lens of Fig. 1, and wherein, Fig. 3 A is that longitudinal aberration diagram, Fig. 3 B are that astigmatism figure, Fig. 3 C are distortion figure;
Fig. 4 A-4C is the Aberration Analysis figure of specific embodiment when middle burnt state of the described long-wave infrared continuous zoom lens of Fig. 1, and wherein, Fig. 4 A is that longitudinal aberration diagram, Fig. 4 B are that astigmatism figure, Fig. 4 C are distortion figure;
Fig. 5 A-5C is the Aberration Analysis figure of specific embodiment when looking in the distance state of the described long-wave infrared continuous zoom lens of Fig. 1, and wherein, Fig. 5 A is that longitudinal aberration diagram, Fig. 5 B are that astigmatism figure, Fig. 5 C are distortion figure.
Wherein f is the effective focal length of zoom lens, and ω is the visual field of zoom lens.In astigmatism figure, S is the radial astigmatism curve, and T is tangential astigmatism curve.
We can find from figure, and various differing well proofreaied and correct, and can obtain the image of higher quality, and the utility model long-wave infrared continuous zoom lens has optical effect preferably.
It should be noted that the concrete parameter in the above table only is exemplary, the parameter of each lens is not limited to the shown value by above-mentioned each numerical value embodiment, can adopt other value, can reach the similar techniques effect.
Though described principle of the present utility model and embodiment above; but; under above-mentioned instruction of the present utility model; those skilled in the art can carry out various improvement and distortion on the basis of the foregoing description, and these improvement or distortion drop in the protection domain of the present utility model.It will be understood by those skilled in the art that top specific descriptions just in order to explain the purpose of this utility model, are not to be used to limit the utility model.Protection domain of the present utility model is limited by claim and equivalent thereof.
Claims (5)
1. long-wave infrared continuous zoom lens, it is characterized in that, be disposed with four lens along optical axis from object space to picture side, wherein, described first lens and the 3rd lens are to be fixed on the optical axis and can not to move, described second lens and the 4th lens can move along optical axis, and wherein, second lens are that Zoom lens, the 4th lens are offset lens.
2. long-wave infrared continuous zoom lens according to claim 1 is characterized in that,
The diameter of described first lens and system's length overall satisfy following expression formula:
1.1＜(D1/FNO)/ft＜1.2 and
TT/ft＜1.5；
Wherein, D1 is the diameter of first lens;
FNO is the F number of LONG WAVE INFRARED continuous magnification lens;
Focal length when ft is the burnt state of the length of long-wave infrared continuous zoom lens;
TT is the distance that image planes are arrived on object space centre of surface summit in first lens.
3. long-wave infrared continuous zoom lens according to claim 1 is characterized in that,
Described first lens, second lens, the 4th lens satisfy following expression formula:
-1.0＜f2/f1＜-0.1 and
f4/ft＞0.5；
Wherein, f1 is the focal length of first lens;
F2 is the focal length of second lens;
F4 is the focal length of the 4th lens;
Ft is the focal length of described long-wave infrared continuous zoom lens when the burnt state of length.
4. long-wave infrared continuous zoom lens according to claim 1 is characterized in that, between described second lens and the 3rd lens fixing system stop is arranged.
5. long-wave infrared continuous zoom lens according to claim 1 is characterized in that, described first lens be have positive refractive power, convex surface is towards the positive meniscus lens of thing side; Second lens are the double-concave negative lens with negative refractive power, and the 3rd lens, the 4th lens are the lens with positive refractive power.
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| Application Number | Priority Date | Filing Date | Title |
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| CN2010205423917U CN201852990U (en) | 2010-09-21 | 2010-09-21 | Long-wave infrared continuous zoom lens |
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| Application Number | Priority Date | Filing Date | Title |
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| CN2010205423917U CN201852990U (en) | 2010-09-21 | 2010-09-21 | Long-wave infrared continuous zoom lens |
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Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101950067A (en) * | 2010-09-21 | 2011-01-19 | 宁波舜宇红外技术有限公司 | Long-wavelength infrared continuous zoom lens |
| CN102590991A (en) * | 2012-04-01 | 2012-07-18 | 昆明物理研究所 | U-shaped folded medium wave infrared 30-times continuous zooming optical system |
| CN107121765A (en) * | 2017-04-10 | 2017-09-01 | 凯迈（洛阳）测控有限公司 | A kind of optical lens of non-brake method dual field-of-view infrared optical system and the application system |
| CN108267849A (en) * | 2018-01-10 | 2018-07-10 | 佛山华国光学器材有限公司 | A kind of remote zoom system, pancreatic system of big zoom ratio and laser illumination system |
| CN111025529A (en) * | 2019-12-04 | 2020-04-17 | 湖北久之洋红外系统股份有限公司 | Ultra-small F number medium-long wave infrared fixed-focus lens |
-
2010
- 2010-09-21 CN CN2010205423917U patent/CN201852990U/en not_active Expired - Fee Related
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101950067A (en) * | 2010-09-21 | 2011-01-19 | 宁波舜宇红外技术有限公司 | Long-wavelength infrared continuous zoom lens |
| CN101950067B (en) * | 2010-09-21 | 2012-11-07 | 宁波舜宇红外技术有限公司 | Long-wavelength infrared continuous zoom lens |
| CN102590991A (en) * | 2012-04-01 | 2012-07-18 | 昆明物理研究所 | U-shaped folded medium wave infrared 30-times continuous zooming optical system |
| CN102590991B (en) * | 2012-04-01 | 2013-10-30 | 昆明物理研究所 | U-shaped folded medium wave infrared 30-times continuous zooming optical system |
| CN107121765A (en) * | 2017-04-10 | 2017-09-01 | 凯迈（洛阳）测控有限公司 | A kind of optical lens of non-brake method dual field-of-view infrared optical system and the application system |
| CN108267849A (en) * | 2018-01-10 | 2018-07-10 | 佛山华国光学器材有限公司 | A kind of remote zoom system, pancreatic system of big zoom ratio and laser illumination system |
| CN108267849B (en) * | 2018-01-10 | 2020-07-28 | 佛山华国光学器材有限公司 | Large-zoom-ratio remote zooming system and laser lighting system |
| CN111025529A (en) * | 2019-12-04 | 2020-04-17 | 湖北久之洋红外系统股份有限公司 | Ultra-small F number medium-long wave infrared fixed-focus lens |
| CN111025529B (en) * | 2019-12-04 | 2021-12-17 | 湖北久之洋红外系统股份有限公司 | Ultra-small F number medium-long wave infrared fixed-focus lens |
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Granted publication date: 20110601 Termination date: 20140921 |
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