• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention concerns a high-resolving objective particularly for use in aerial photography based on the double-gauss objective type, covering a wide spectral range, and which at a relative aperture of 1:4 images an image field of 2 sigma >40 DEG without aberrations.
    公开号:SU917157A1
    申请号:SU787770073
    申请日:1978-01-16
    公开日:1982-03-30
    发明作者:Еберхард Дитш；Герхард Еберитц
    申请人:Феб Карл Цейсс-Йена (Инопредприятие)；
    IPC主号:
    专利说明:

    The invention relates to a Gauss extended paired photographic lens with high resolution, designed for a large spectral zone, having a “1: orthoscopic field with a relative orifice of aperture, and is used primarily for aerial photography, especially for multispectral photography .. 10
    Photographic lenses are known with the indicated relative aperture and image field angle.
    However, they do not reach the theoretical value of the resolving power, 16 or reach it only for small image fields and narrow spectral zones.
    There are lenses with apochromatic correction, also designed for us large spectral zones.
    However, to achieve the necessary good aberration elimination from them is possible only for the point lying on the main optical axis, and not for the pain 2S
    Due to this, the resolution power is not high. In addition, these lenses increase the image floor angle. create vignetting and have in the diaphragm box of a paired Gauss objective a combined link consisting of so many separate lenses that there is no space for the shutter to be inserted with the diaphragm.
    The purpose of the invention is to create a high-aperture lens suitable for high-quality photography from a great height and fully utilizing the finest-grained photographic film materials.
    The invention is based on the task of creating a lens that would circumvent the above-mentioned disadvantages and which, with a focal distance of about 125 mm and a relative aperture I: would provide an orthoscopic image of a high-resolution field, with the spectral region extending from A / A 480 to 850 nm. In this case, a high resolving power implies a resolving power due to diffraction and practically independent of aberration.
    The high resolving power in the image field simultaneously requires that the objective be free of vignetting and provide light distribution corresponding to at least the cos law.
    To achieve a uniform transmission through a large spectral zone, as few optical glasses as possible and heavy flints with refractive indices greater than 1.68 should be used as optical media. In addition, such a lens as a result of a change in the air gap alone must ensure, without disturbing the other correction, a change in the focal distance of the order of 1. The implementation of this requirement is important to compensate for the focal distance tolerances associated with the production if in different spectral zones Several lenses are used and it is necessary to achieve exact equality of the values of individual images for subsequent evaluation. 8 to increase the accuracy of the plane of the position of the film or to copy the marks, in some cases, a pressure plate must be applied to the plane of the film.
    This goal is achieved by the fact that the paired Gaussian lens, in which two meniscus cover the diaphragm box with its cavity and both have both from the object side and the image side along one collecting lens, is complemented in such a way that to reduce the secondary spectrum in the box a diaphragm in the direction of light behind the diaphragm is introduced a combined unit consisting of three parts, in which a double-folded lens from a fleece with a short interval of output with a strongly reduced short-wave range In the azone, the dispersion of particles is enclosed between two converging lenses, and to improve the alignment of the image and oblique spherical aberration, a scattering meniscus is located directly in front of the image surface, each having its convex side to the image
    From the Gauss’s paired objective meniscus surrounding the diaphragm, it has, for achromatization on one surface, gluing, and when imaging to infinity from both collective lenses, the lens located on the side of the subject is made in the form of a meniscus, and the lens on the side of the image is in the form Dso kovkrutoy lenses.
    With the proposed lens design, achromatic correction with high resolution for a large field is achieved by using only Flint with an extremely short generation interval, and otherwise using normal glasses. The arithmetic mean of all refractive indices remains less than 1.6. This is important, the necessary uniform transmission through a large spectral range is best achieved by using glasses with low refractive indices, while glasses with high refractive indices, especially heavy flints, more strongly absorb light in the shortwave range.
    Since flints with an extremely short generation interval are generally influenced by atmospheric conditions, it is necessary that the lenses made from them have adequate protection. Most simply, this is achieved by positioning behind the diaphragm of a combined link consisting of three parts.
    In order to avoid the influence of the sensitivity of the centering of strongly bent gluing surfaces that are present in this combined link, the refractive jumps on these gluing surfaces should not be too large and exceed 0.03. Similarly, the Ve weights on these surfaces should not exceed 13, in order to avoid color distortions due to centering.
    The surface of the gluing Y 8, concave towards the diaphragm, consisting of three parts of the combined link exerts a growing astigmatic growth with increasing deflection; the effect, which is the stronger the chromatic astigmatism, the greater the Ve jump on this surface. To astigmatic chromatic aberration to the floor. The image remained minimal, the jump Vc on this surface should not be too large, or the radius V of the gluing surface, facing its concavity towards the diaphragm, based on the focal distance of the whole system, should not be too small. Interfering color astigmatism is prevented if the condition V 0.0 f (AVc) is met, and this is the difference in the dispersion coefficients of the glasses on both sides of the mentioned gluing surface v Chromatic astigmatism is further suppressed if the gluing surface in the meniscus: located in the direction of the light beam behind, consisting of three parts of the combined link, is towards the diaphragm. To limit to a minimum the sensitivity of the centering of the entire combined link. Consisting of three parts, its focal length. must be positive, and by the equation with the focal distance of the whole system, at least twice as large as. The positive focal length of this link, smaller than 6f, is beneficial in that it has a positive effect on the total optical power of the lens and reduces individual refractive forces of all other lenses, thereby reducing aberrations. This leads to , that the influence of the original scattering meniscus located in the direction of the light beam behind the combined link (in the classical paired Gaussian object) is weakened and becomes almost afocal, and its focal distance remains ts nym negative or positive, in the amount of pain PWM than 5f. In order for the proposed design to withstand the effect of large temperature fluctuations, it is necessary to pay attention to the fact that “in a three-piece combination unit with strongly curved combined surfaces, match the linear expansion coefficient of the glasses used. Since flints with an extremely short production interval have relatively low thermal expansion coefficients, only a small number of glass combinations can be used for the combined link, for example, Shot KZFS2 glass combinations with SKU and BaLF, as well as KZFSIc SSR2, SK9 or SK6 . Immediately before the image plane, the located scattering meniscus influences the alignment of the image and reduces the effect of the scattering meniscus of the Gauss objective surrounding the aperture, so that the spherical aberration is reduced. However, such a lens also shifts the front main point of the lens, which in turn affects the secondary transverse spectrum. In order to keep the resulting secondary transverse spectrum within the required limits, the influence directly in front of the image plane of the dispersed meniscus should not be too strong, and its focal length should be significantly larger than f. The change in the focal distance of the finished optical system is carried out by changing the air gap before this meniscus, and the correction state is not disturbed if the meniscus is bent in such a way that its convex surface is facing the image. To ensure a flat position of the film or to copy marks when shooting in the image plane, a plane-parallel plate may be located, the astigmatic effect of which must be taken into account during correction. The drawing shows the proposed lens section. In tab. I- presents the limits within which optical systems according to the invention can be constructed. In the air gap Lj there is a diaphragm. The optical link, conventionally designated as d ,, is a plane-parallel plate used as a pressure plate and for copying marks. The link, conditionally designated as d ,, dj, dj, d, dg and dg, correspond to the classical paired Gauss lens. Due to the expansion of this lens corresponding to the invention, the splicing element located on the side of the image and conventionally designated as dy-dgi acquires an almost afocal shape, and the objectives of the lenses 7 9171578 can be realized with (for example, Table C, bi
    t. Relative hole 1:
    Angle floor image 2 and M
    Table 1
     one
    Relative hole i: k Angle floor image 26 ttf 1 Relative hole I: Angle floor image 2 6 k
    di 0.0720
     +05553 jj, - 0.0096
    Tj +1.2827
    ten
    917157 Table
    Table 3
    51.5
    1.53187
    13
    权利要求:
    Claims (1)
    [1]
    1. A photographic lens for the object side represents a large spectral zone, in which the battle is convex relative to the object of the mediscus, each of which has a bottom, and a collective lens, has a single gluing surface and its curved side on the image side. closes the diaphragm box, with a double-convex: lens, they are removed both by the lens from the side of the lens, and from the image side with the reading data:
      1 Relative otversion} L
    Angle floor image 2 k
    d ,,
     +0.5771
    f ,, 0080
     -1.1395
    +0.3863
    , 0910
     +1.0873
    , 0320
    , 1780
     +0,239+
    +1.8213
    , 0720
    dg.0
    - -0.179
    917157
    ) Continuation of the table. "
    -Complete lens, spread5) is false
    5t, iO
    1.51678
    17
    tj 0,
    -0.8211 d, o. 0,
    -0.5616 e 0.0320.
    - / t, it928 dfl 0.0720
    18
    18
    917157 Continuation of the table
    63.87
    1.51859
    63.87 1.51859
     1991715720
    I. Lens under item 1, about tl and h ayush and y- with the following calculated data:
     f 1 Elongation 1: 4
    Angle floor image 2 (s kt
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    同族专利:
    公开号 | 公开日
    DE2753759A1|1978-08-03|
    DD129698B1|1980-07-23|
    US4206972A|1980-06-10|
    DD129698A1|1978-02-01|
    引用文献:
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    US3524699A|1967-05-13|1970-08-18|Nippon Kogaku Kk|Symmetrical relay lens of equi-magnification|
    US3551030A|1969-05-20|1970-12-29|Minnesota Mining & Mfg|Objective lens for microfilm camera|
    JPS4712957U|1971-03-12|1972-10-16|
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    US8289633B2|2007-07-20|2012-10-16|James Brian Caldwell|UV-VIS-IR imaging optical systems|
    WO2010096198A1|2009-02-23|2010-08-26|Pinotage L.L.C.|Lens assembly|
    KR101471612B1|2013-07-01|2014-12-12|남부대학교산학협력단|Solar position Tracking Precision Measurement system based on precision optical lenses.|
    JP6808428B2|2016-09-30|2021-01-06|キヤノン株式会社|Optical system and optical equipment with it|
    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    DD19710577A|DD129698B1|1977-01-27|1977-01-27|HIGH DEFLECTIVE LENS FOR A LARGE SPECTRAL AREA|
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