CN105259602A - Novel aspheric panoramic reflector design method - Google Patents
Novel aspheric panoramic reflector design method Download PDFInfo
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- CN105259602A CN105259602A CN201510843620.6A CN201510843620A CN105259602A CN 105259602 A CN105259602 A CN 105259602A CN 201510843620 A CN201510843620 A CN 201510843620A CN 105259602 A CN105259602 A CN 105259602A
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/08—Mirrors
- G02B5/10—Mirrors with curved faces
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/0012—Optical design, e.g. procedures, algorithms, optimisation routines
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Lenses (AREA)
- Optical Elements Other Than Lenses (AREA)
- Closed-Circuit Television Systems (AREA)
Abstract
The invention discloses a novel aspheric reflector design method for an omnidirectional vision system. The method is characterized by comprising steps: the diameter, the thickness and the maximum incidence angle of the reflector are determined, a proper sampling point number is selected according to the maximum incidence angle and required processing precision, the diameter and the thickness are subdivided according to the sampling point number, as for a cluster of coaxial hyperbolic curves with the same focus and with real axis lengths increased linearly, curve segments are intercepted horizontally for finite element splicing to obtain a surface-type curve meeting certain requirements, an iterative formula is substituted, coordinates of the sampling points are obtained, the sampling points generated by an iterative equation are used for fitting an aspheric contour curve equation, and the equation is converted into ZMAX recognition optical equation.
Description
Technical field
The invention belongs to omni-directional visual process field, particularly relate to a kind of new aspheric panorama mirror design method.
Background technology
Constantly perfect along with overall view visual system, panoramic vision technology has had preliminary application in vision and optical field.In indoor and outdoor surroundings, panoramic vision is just progressively applied to the field such as monitoring and long-range reality.Due to its angular field of view of 360 degree, overall view visual system in outdoor environment the most directly application be monitoring field application.Video camera based on omnibearing vision sensor has very outstanding advantage, its looking away (360 degree), Information Compression in a hemisphere visual field can be become piece image, the quantity of information of piece image is larger, any point in panoramic picture all corresponds to a certain point determined monitored in space, therefore space position calibration algorithm is simple, without run-home during monitoring, making the algorithm of the moving object in the acquisition of visual information, detection and tracking monitoring range more simple, is a kind of quick, reliable panoramic vision information acquisition means.But current panorama system, carrying out the very large pattern distortion of panoramic picture expansion existence, propose a lot of method for reducing and eliminating this distortion, improving curved surface of reflector profile is one relatively directly effective method, greatly can improve the linearity that mirror image launches.
Summary of the invention
The nonlinear distortion that method object in the present invention exists in being to provide a kind of direct effective method abatement panoramic picture to launch, realizes the accurate reproduction of image information.
The technical solution adopted in the present invention is: the new method that a kind of non-spherical reflector for fully-directional visual system designs, and determines the diameter of catoptron, thickness and maximum incident angle three parameters.According to the machining precision of maximum incident angle and requirement, choose suitable sampling number, diameter and thickness determine the size of the useful area of minute surface, according to sampling number, diameter and thickness are segmented, substitute into iterative formula, ask for the coordinate of sampled point, carry out curve fitting according to the coordinate of all sampled points afterwards, and be converted into the Optical equations of ZMAX identification.The coaxial hyperbolic curve that real axis length linear increases progressively to cluster focal length is identical, level intercepts segment of curve and carries out finite element splicing, expands the method for the good imaging area of the linearity under the condition meeting single view constraint.
The invention has the beneficial effects as follows: improve image quality, the distortion of horizontal direction and vertical direction in removal of images unfolding calculation by the curvature of curve improving mirror surface band portions corresponding.
Accompanying drawing explanation
In order to be illustrated more clearly in the embodiment of the present invention or technical scheme of the prior art, be briefly described to the accompanying drawing used required in embodiment or description of the prior art below, apparently, accompanying drawing in the following describes is only some embodiments of the present invention, for those of ordinary skill in the art, under the prerequisite not paying creative work, other accompanying drawing can also be obtained according to these accompanying drawings.
Fig. 1 is curved design conditional curve schematic diagram.
Embodiment
Below in conjunction with embodiment, the present invention is further described.
Embodiment 1
The new method that a kind of non-spherical reflector for fully-directional visual system designs, determine the diameter of catoptron, thickness and maximum incident angle three parameters, according to the machining precision of maximum incident angle and requirement, choose suitable sampling number, according to sampling number, diameter and thickness are segmented, the coaxial hyperbolic curve that real axis length linear increases progressively to cluster focal length is identical, level intercepting segment of curve carries out finite element splicing and is met necessarily required type curve, substitute into iterative formula, ask for the coordinate of sampled point, the sampled point generated by iterative equation simulates aspheric contour curve equation, and be converted into the Optical equations of ZMAX identification.
Adjacent two incident ray space angles of regulation curved surface are △ θ=(β-α)/m, i.e. unlimited segmentation of catoptron actual observation angle, and m is sampling number; Separately establish △ x=r/m, for sampled point is in the step-length of minute surface horizontal direction displacement, with minute surface bottom centre for system coordinates initial point, n=1 ~ m, iteration asks for sampled point successively, and formula (3) (4) calculate the coordinate of current sampling point, and formula (7) calculates θ
nafter, n adds up automatically, n=n+1, gets back to the coordinate that formula (3) calculates next sampled point, and so forth,
x
0=y
0=0(1)
θ
0=0.5×(90°-α)(2)
x
n=n×△x(3)
y
n=y
n-1+tanθ
n-1×△x(4)
θ
sn=(90°-α)+n×△θ+λ
n(6)
θ
n=0.5×θ
sn-λ
n(7)
λ
nfor the angle of reflection ray and main shaft, θ
snbe the angle of n-th incident ray and corresponding reflection ray, the shape obtained through curve is as the equation of formula (8) form
x
2=a
1z+a
2z
2+…+a
kz
k+…(8)
A
1=2r
0, r
0for the radius-of-curvature on summit, the secondary surface of revolution is had:
x
2=2r
0z-(1+e)z
2(9)
Formula (9) is made into as shown in the formula
z=c
1x
2+c
2z
2(10)
Wherein: c
1=1/2r
0, c
2=(1+e)/2r
0, make x
1=x
2, x
2=z
2, turn to set { x
1i, x
2i, z
imultilinear fitting, obtain following formula
z=c
1x
1+c
2x
2(11)
Derived (14) by formula (12) (13)
r
0=1/c
1(12)
e=2r
0c
2-1(13)
Formula (14) is aspheric contour curve equation.
The foregoing is only preferred embodiment of the present invention, not in order to limit the present invention, within the spirit and principles in the present invention all, any amendment done, equivalent replacement, improvement etc., all should be included in protection of the present invention.
Claims (2)
1. the new method that designs of the non-spherical reflector for fully-directional visual system, it is characterized in that, determine the diameter of catoptron, thickness and maximum incident angle three parameters, according to the machining precision of maximum incident angle and requirement, choose suitable sampling number, according to sampling number, diameter and thickness are segmented, the coaxial hyperbolic curve that real axis length linear increases progressively to cluster focal length is identical, level intercepting segment of curve carries out finite element splicing and is met necessarily required type curve, substitute into iterative formula, ask for the coordinate of sampled point, the sampled point generated by iterative equation simulates aspheric contour curve equation, and be converted into the Optical equations of ZMAX identification.
2. the new method of the non-spherical reflector design of fully-directional visual system according to claim 1, is characterized in that: the concrete steps of described aspheric contour curve equation are:
Adjacent two incident ray space angles of regulation curved surface are △ θ=(β-α)/m, i.e. unlimited segmentation of catoptron actual observation angle, and m is sampling number; Separately establish △ x=r/m, for sampled point is in the step-length of minute surface horizontal direction displacement, with minute surface bottom centre for system coordinates initial point, n=1 ~ m, iteration asks for sampled point successively, and formula (3) (4) calculate the coordinate of current sampling point, and formula (7) calculates θ
nafter, n adds up automatically, n=n+1, gets back to the coordinate that formula (3) calculates next sampled point, and so forth,
x
0=y
0=0(1)
θ
0=0.5×(90°-α)(2)
x
n=n×△x(3)
y
n=y
n-1+tanθ
n-1×△x(4)
θ
sn=(90°-α)+n×△θ+λ
n(6)
θ
n=0.5×θ
sn-λ
n(7)
λ
nfor the angle of reflection ray and main shaft, θ
snbe the angle of n-th incident ray and corresponding reflection ray, the shape obtained through curve is as the equation of formula (8) form
x
2=a
1z+a
2z
2+…+a
kz
k+…(8)
A
1=2r
0, r
0for the radius-of-curvature on summit, the secondary surface of revolution is had:
x
2=2r
0z-(1+e)z
2(9)
Formula (9) is made into as shown in the formula
z=c
1x
2+c
2z
2(10)
Wherein: c
1=1/2r
0, c
2=(1+e)/2r
0, make x
1=x
2, x
2=z
2, turn to set { x
1i, x
2i, z
imultilinear fitting, obtain following formula
z=c
1x
1+c
2x
2(11)
Derived (14) by formula (12) (13)
r
0=1/c
1(12)
e=2r
0c
2-1(13)
Formula (14) is aspheric contour curve equation.
Priority Applications (1)
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CN201510843620.6A CN105259602B (en) | 2015-11-26 | 2015-11-26 | A kind of aspherical panorama mirror design method |
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CN201510843620.6A CN105259602B (en) | 2015-11-26 | 2015-11-26 | A kind of aspherical panorama mirror design method |
Publications (2)
Publication Number | Publication Date |
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CN105259602A true CN105259602A (en) | 2016-01-20 |
CN105259602B CN105259602B (en) | 2018-06-22 |
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ID=55099362
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CN201510843620.6A Expired - Fee Related CN105259602B (en) | 2015-11-26 | 2015-11-26 | A kind of aspherical panorama mirror design method |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2017214774A1 (en) * | 2016-06-12 | 2017-12-21 | 合肥工业大学 | Deflection film design method and liquid crystal display device |
CN113552717A (en) * | 2021-07-19 | 2021-10-26 | 森思泰克河北科技有限公司 | Lens design method, lens and laser radar |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS56126803A (en) * | 1980-03-11 | 1981-10-05 | Kunihiko Hosaka | Reflector having multifaceted reflection element |
US20070002444A1 (en) * | 2004-04-05 | 2007-01-04 | Patricia Piers | Ophthalmic lenses capable of reducing chromatic aberration |
CN102620683A (en) * | 2012-03-31 | 2012-08-01 | 中国科学院长春光学精密机械与物理研究所 | Aspheric surface adjustment error compensation method for sub-aperture stitching detection |
-
2015
- 2015-11-26 CN CN201510843620.6A patent/CN105259602B/en not_active Expired - Fee Related
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS56126803A (en) * | 1980-03-11 | 1981-10-05 | Kunihiko Hosaka | Reflector having multifaceted reflection element |
US20070002444A1 (en) * | 2004-04-05 | 2007-01-04 | Patricia Piers | Ophthalmic lenses capable of reducing chromatic aberration |
CN102620683A (en) * | 2012-03-31 | 2012-08-01 | 中国科学院长春光学精密机械与物理研究所 | Aspheric surface adjustment error compensation method for sub-aperture stitching detection |
Non-Patent Citations (3)
Title |
---|
沙定国,全书学,朱秋东,苏大图: "一种光学非球面检测技术中的数据处理问题", 《光子学报》 * |
沙定国,全书学,朱秋东,苏大图: "光学非球面面形拟合方法研究", 《光子学报》 * |
沙定国,郭剑锋: "光学非球面检测系统的精度仿真分析", 《宇航计测技术》 * |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2017214774A1 (en) * | 2016-06-12 | 2017-12-21 | 合肥工业大学 | Deflection film design method and liquid crystal display device |
CN113552717A (en) * | 2021-07-19 | 2021-10-26 | 森思泰克河北科技有限公司 | Lens design method, lens and laser radar |
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CN105259602B (en) | 2018-06-22 |
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