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CN105318891A - Star sensor reference cube-prism installation error calibration apparatus - Google Patents

Star sensor reference cube-prism installation error calibration apparatus Download PDF

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Publication number
CN105318891A
CN105318891A CN201410360805.7A CN201410360805A CN105318891A CN 105318891 A CN105318891 A CN 105318891A CN 201410360805 A CN201410360805 A CN 201410360805A CN 105318891 A CN105318891 A CN 105318891A
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star sensor
star
simulator
axis
dimensional adjustment
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CN105318891B (en
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姜云翔
崔桂利
郭雨蓉
魏小林
赵天承
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China Academy of Launch Vehicle Technology CALT
Beijing Aerospace Institute for Metrology and Measurement Technology
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China Academy of Launch Vehicle Technology CALT
Beijing Aerospace Institute for Metrology and Measurement Technology
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Abstract

本发明属于光电设备标定技术领域,具体涉及一种星敏感器基准立方镜安装误差的标定装置。在基准平面上的两个正交的轴上分别放置光电自准直仪和单星模拟器,在两轴的交点处放置被测星敏感器,使被测星敏感器基准棱体的两正交反光面的法线与两正交的轴分别平行,经纬仪分别将光电自准直仪和单星模拟器的光轴调节至与基准平面平行;星敏感器安装在其三维调整基座上,通过星敏感器三维调整基座将星敏感器的输入光轴和单星模拟器的输出光轴调至平行;被测基准立方镜安装在被测星敏感器壳体上表面;运用光电自准直测量基准立方镜绕X轴和Y轴的安装角度误差,将星敏感器三维调整基座旋转90°,测量基准立方镜绕Z轴的安装角度误差。

The invention belongs to the technical field of photoelectric equipment calibration, and in particular relates to a calibration device for installation errors of star sensor reference cube mirrors. Place a photoelectric autocollimator and a single star simulator on two orthogonal axes on the reference plane, and place the star sensor to be measured at the intersection of the two axes so that the two positive sides of the reference prism of the star sensor to be measured The normal line of the cross-reflective surface is parallel to the two orthogonal axes respectively, and the theodolite adjusts the optical axes of the photoelectric autocollimator and the single-star simulator to be parallel to the reference plane; the star sensor is installed on its three-dimensional adjustment base, The input optical axis of the star sensor and the output optical axis of the single star simulator are adjusted to be parallel through the three-dimensional adjustment base of the star sensor; the measured reference cube mirror is installed on the upper surface of the measured star sensor housing; photoelectric self-alignment is used Directly measure the installation angle error of the reference cube mirror around the X-axis and Y-axis, rotate the three-dimensional adjustment base of the star sensor by 90°, and measure the installation angle error of the reference cube mirror around the Z-axis.

Description

A kind of caliberating device of star sensor benchmark prism square alignment error
Technical field
The invention belongs to optoelectronic device calibration technique field, be specifically related to a kind of caliberating device of star sensor benchmark prism square alignment error.
Background technology
Star sensor, as the high-precision spatial attitude optical sensor of one, obtains extensive and deep application at space industry.Surving coordinate system due to star sensor is virtual sightless, must accurately measure position and attitude relation, the i.e. alignment error of benchmark prism square of benchmark prism square coordinate system on star sensor surving coordinate system and its housing when ground-mounted.Namely star sensor is realized in the requirement of spaceborne geometry installation accuracy by the benchmark prism square measured on star sensor.
The domestic method for star sensor reference-calibrating prism square alignment error mainly contains two kinds at present: one adopts heavy caliber autocollimator mensuration, and one is by light pipe and star simulator multiple measurement method.Heavy caliber autocollimator mensuration is enough large with a bore, simultaneously to cover star sensor and benchmark prism square autocollimator, by light pipe and benchmark prism square being collimated, the position coordinates then reading autocollimator inner cross cross hair focus in star sensor resolves star sensor and the alignment error of benchmark prism square in pitching and orientation two-dimensional direction.Light pipe and star simulator multiple measurement method are that autocollimator and star simulator are installed on a logical support, and both keep optical axis parallel.During calibrated error, the benchmark prism square above autocollimator collimation star sensor, then reads the image space coordinate of star simulator, namely calculates star sensor and the alignment error of benchmark prism square in pitching and azimuth direction in star sensor.
Heavy caliber light pipe mensuration due to light pipe objective lens diameter large, its machining precision is difficult to ensure, processing cost is high.In addition owing to adopting off-axis light to measure, optical path is by the aberration after optical system, and spherical aberration iseikonia missionary society causes the loss of certain measuring accuracy, cannot meet the requirement of high-acruracy survey.Secondly, this measuring method can only measure star sensor and the alignment error of benchmark prism square in pitching and azimuth direction, cannot measure the alignment error in rolling direction.
Though light pipe and star simulator multiple measurement method larger caliber light pipe mensuration improve measuring accuracy, but still cannot measure the alignment error in rolling direction.
Summary of the invention
The object of the present invention is to provide a kind of caliberating device of star sensor benchmark prism square alignment error, to overcome the deficiency that prior art can only measure two-dimentional alignment error.
For achieving the above object, the technical solution used in the present invention is:
A caliberating device for star sensor benchmark prism square alignment error, what define star sensor input optical axis is reversed Y-axis, and on benchmark prism square, the outgoing normal direction of plane is X-axis, and Z axis is by right-hand rule Nature creating; Two on reference plane orthogonal axles place photoelectric auto-collimator and single star simulator respectively, tested star sensor is placed in the point of intersection of diaxon, make the normal of the pairwise orthogonal reflective surface of tested star sensor benchmark rib body parallel respectively with the axle of pairwise orthogonal, photoelectric auto-collimator and single star simulator are arranged on photoelectric auto-collimator two-dimension adjustment pedestal and single star simulator two-dimension adjustment pedestal respectively, and photoelectric auto-collimator is adjusted to parallel with reference plane with the optical axis of single star simulator by transit respectively; Star sensor is arranged on star sensor three-dimensional adjustment pedestal, when star sensor and single star simulator are all started shooting, is adjusted to parallel by star sensor three-dimensional adjustment pedestal by the input optical axis of star sensor with the output optical axis of single star simulator; Tested benchmark prism square is arranged on tested star sensor housing upper surface; Use photoelectric auto-collimator measuring basis prism square around the setting angle error of X-axis and Y-axis, by star sensor three-dimensional adjustment pedestal half-twist, measuring basis prism square is around the setting angle error of Z axis.
The central axes of benchmark prism square on the rotation of described star sensor three-dimensional adjustment pedestal and tested star sensor.
This device course of work is as follows: be placed on reference plane by standard rib body, with reflective surface before transit collimation standard rib body, then resets transit pitching reading θ V; Keep transit state constant, remove standard rib body; Transit and photoelectric auto-collimator are collimated, adjustment photoelectric auto-collimator two-dimension adjustment pedestal, the output making photoelectric auto-collimator is 0 °, illustrates that the optical axis of photoelectric auto-collimator is parallel with reference plane, fixing photoelectric auto-collimator; Transit and single star simulator are collimated, adjustment single star simulator two-dimension adjustment pedestal, make the output of light single star simulator be 0 °, the output optical axis of instruction book star simulator is parallel with reference plane, fixing single star simulator; Remove described standard rib body, place tested star sensor and star sensor three-dimensional adjustment pedestal in the point of intersection of diaxon; Tested benchmark prism square is arranged on tested star sensor housing upper surface; Star sensor is alignd with single star simulator outline, then adjusts star sensor three-dimensional adjustment pedestal, make the output of star sensor for (0 °, 0 °), the optical axis coincidence of star sensor and single star simulator is described; Now reading (the θ of photoelectric auto-collimator x, θ y) be the alignment error that benchmark prism square 10 and star sensor surving coordinate tie up to X and Y-direction; Rotate star sensor three-dimensional adjustment pedestal, make it rotate 90 °, now reading (the θ of photoelectric auto-collimator x, θ z) be the alignment error that benchmark prism square and star sensor surving coordinate tie up to X and Z-direction; Complete the alignment error (θ of benchmark prism square and star sensor surving coordinate system thus x, θ y, θ z).
Beneficial effect acquired by the present invention is:
The present invention directly can calibrate the three-dimensional alignment error of benchmark prism square by one-step installation, avoids repeatedly repeating to install the stochastic error brought; Calibration system is simple to operate, and require low to operating personnel's technical merit, operating personnel only need the reading value of reference star sensor and autocollimator, regulate the attitude of corresponding instrument; The process alignment error calibration of quick, high-precision benchmark prism square can be realized.
Accompanying drawing explanation
Fig. 1 is coordinate system definition schematic diagram;
Fig. 2 calibration system photoelectric auto-collimator adjustment schematic diagram;
Fig. 3 benchmark prism square around X, around Y-direction setting angle error calibration schematic diagram;
Fig. 4 benchmark prism square is around Z-direction setting angle error calibration schematic diagram;
In figure: 1, transit; 2, standard rib body; 3, photoelectric auto-collimator two-dimension adjustment pedestal; 4, photoelectric auto-collimator; 5, single star simulator; 6, single star simulator two-dimension adjustment pedestal; 7, reference plane; 8, star sensor three-dimensional adjustment pedestal; 9, star sensor; 10, benchmark prism square.
Embodiment
Below in conjunction with the drawings and specific embodiments, the present invention is described in detail.
As shown in Figure 1, what definition star sensor 9 inputted optical axis is reversed Y-axis, and on benchmark prism square 10, the outgoing normal direction of plane is X-axis, and Z axis is by right-hand rule Nature creating.
As shown in Figure 2, two on reference plane 7 orthogonal axles place photoelectric auto-collimator 4 and single star simulator 5 respectively, tested star sensor 9 is placed in the point of intersection of described diaxon, photoelectric auto-collimator 4 and single star simulator 5 are arranged on photoelectric auto-collimator two-dimension adjustment pedestal 3 and single star simulator two-dimension adjustment pedestal 6 respectively, and described photoelectric auto-collimator 4 and the optical axis of single star simulator 5 are adjusted to parallel with reference plane 7 by transit 1 respectively; Star sensor 9 is arranged on star sensor three-dimensional adjustment pedestal 8, when star sensor 9 and single star simulator 5 are all started shooting, by star sensor three-dimensional adjustment pedestal 8, the input optical axis of star sensor 9 is adjusted to parallel with the output optical axis of single star simulator 5, now use described photoelectric auto-collimator 4 measuring basis prism square 10 around the setting angle error of X-axis and Y-axis, by star sensor three-dimensional adjustment pedestal 8 half-twist, measuring basis prism square 10 is around the setting angle error of Z axis.The central axes of benchmark prism square 10 on the rotation of described star sensor three-dimensional adjustment pedestal 8 and tested star sensor 9.
Standard rib body 2 is placed on reference plane 7, collimates reflective surface before standard rib body 2 with transit 1, then reset transit 1 pitching reading θ v; Keep transit 1 state constant, remove standard rib body 2; Transit 1 and photoelectric auto-collimator 4 are collimated, adjustment photoelectric auto-collimator two-dimension adjustment pedestal 3, the output making photoelectric auto-collimator 4 is 0 °, illustrates that the optical axis of photoelectric auto-collimator 4 is parallel with reference plane 7, fixing photoelectric auto-collimator 4; Transit 1 and single star simulator 5 are collimated, adjustment single star simulator two-dimension adjustment pedestal 6, make the output of light single star simulator 5 be 0 °, the output optical axis of instruction book star simulator 5 is parallel with reference plane 7, fixing single star simulator 5;
As shown in Figure 3, remove described standard rib body 2, place tested star sensor 9 and star sensor three-dimensional adjustment pedestal 8 in the point of intersection of diaxon; Tested benchmark prism square 10 is arranged on tested star sensor 9 housing upper surface; Star sensor 9 is alignd with single star simulator 5 outline, then adjusts star sensor three-dimensional adjustment pedestal 8, make the output of star sensor 9 for (0 °, 0 °), the optical axis coincidence of star sensor 9 and single star simulator 5 is described; Now reading (the θ of photoelectric auto-collimator 4 x, θ y) be the alignment error that benchmark prism square 10 and star sensor 9 surving coordinate tie up to X and Y-direction.
As shown in Figure 4, rotate star sensor three-dimensional adjustment pedestal 8, make it rotate 90 °, now reading (the θ of photoelectric auto-collimator x, θ z) be the alignment error that benchmark prism square 10 and star sensor 9 surving coordinate tie up to X and Z-direction.Complete the alignment error (θ of benchmark prism square 10 and star sensor 9 surving coordinate system thus x, θ y, θ z).

Claims (3)

1.一种星敏感器基准立方镜安装误差的标定装置,其特征在于:定义星敏感器(9)输入光轴的反向为Y轴,基准立方镜(10)上平面的出射法线方向为X轴,Z轴由右手螺旋法则自然生成;在基准平面(7)上的两个正交的轴上分别放置光电自准直仪(4)和单星模拟器(5),在两轴的交点处放置被测星敏感器(9),光电自准直仪(4)和单星模拟器(5)分别安装在光电自准直仪二维调整基座(3)和单星模拟器二维调整基座(6)上,经纬仪(1)分别将光电自准直仪(4)和单星模拟器(5)的光轴调节至与基准平面(7)平行;星敏感器(9)安装在星敏感器三维调整基座(8)上,在星敏感器(9)和单星模拟器(5)均开机的情况下,通过星敏感器三维调整基座(8)将星敏感器(9)的输入光轴和单星模拟器(5)的输出光轴调至平行;被测基准立方镜(10)安装在被测星敏感器(9)壳体上表面;运用光电自准直仪(4)测量基准立方镜(10)绕X轴和Y轴的安装角度误差,将星敏感器三维调整基座8旋转90°,测量基准立方镜(10)绕Z轴的安装角度误差。1. a kind of calibration device of star sensor reference cube mirror installation error, it is characterized in that: the reverse of definition star sensor (9) input optical axis is Y axis, the outgoing normal direction of plane on reference cube mirror (10) is the X-axis, and the Z-axis is naturally generated by the right-handed spiral rule; the photoelectric autocollimator (4) and the single-star simulator (5) are respectively placed on the two orthogonal axes on the reference plane (7), and the two-axis The star sensor (9) to be measured is placed at the intersection point, the photoelectric autocollimator (4) and the single star simulator (5) are respectively installed on the two-dimensional adjustment base of the photoelectric autocollimator (3) and the single star simulator On the two-dimensional adjustment base (6), the theodolite (1) adjusts the optical axis of the photoelectric autocollimator (4) and the single-star simulator (5) to be parallel to the reference plane (7) respectively; the star sensor (9 ) is installed on the three-dimensional adjustment base (8) of the star sensor. When both the star sensor (9) and the single-star simulator (5) are turned on, the star sensor The input optical axis of the device (9) and the output optical axis of the single-star simulator (5) are adjusted to be parallel; the measured reference cube mirror (10) is installed on the upper surface of the measured star sensor (9) housing; The collimator (4) measures the installation angle error of the reference cube mirror (10) around the X axis and the Y axis, rotates the three-dimensional adjustment base 8 of the star sensor by 90°, and measures the installation angle of the reference cube mirror (10) around the Z axis error. 2.根据权利要求1所述的星敏感器基准立方镜安装误差的标定装置,其特征在于:所述星敏感器三维调整基座(8)的旋转轴线与被测星敏感器(9)上基准立方镜(10)的中心轴线重合。2. the calibration device of star sensor reference cube mirror installation error according to claim 1, it is characterized in that: the rotation axis of described star sensor three-dimensional adjustment base (8) is on the same plane as the measured star sensor (9). The central axes of the reference cube mirrors (10) coincide. 3.根据权利要求1所述的星敏感器基准立方镜安装误差的标定装置,其特征在于:该装置工作过程如下:将标准棱体(2)放置在基准平面(7)上,用经纬仪(1)准直标准棱体(2)的前反光面,然后清零经纬仪(1)俯仰读数θV;保持经纬仪(1)状态不变,移除标准棱体(2);使经纬仪(1)与光电自准直仪(4)准直,调整光电自准直仪二维调整基座(3),使得光电自准直仪(4)的输出为0°,说明光电自准直仪(4)的光轴与基准平面(7)平行,固定光电自准直仪(4);使经纬仪(1)与单星模拟器(5)准直,调整单星模拟器二维调整基座(6),使得光单星模拟器(5)的输出为0°,说明单星模拟器(5)的输出光轴与基准平面(7)平行,固定单星模拟器(5);移除所述标准棱体(2),在两轴的交点处放置被测星敏感器(9)及星敏感器三维调整基座(8);被测基准立方镜(10)安装在被测星敏感器(9)壳体上表面;使得星敏感器(9)与单星模拟器(5)概略对齐,然后调整星敏感器三维调整基座(8),使得星敏感器(9)的输出为(0°,0°),说明星敏感器(9)与单星模拟器(5)的光轴重合;此时光电自准直仪(4)的读数(θX,θY)即为基准立方镜(10)与星敏感器(9)测量坐标系在X和Y方向的安装误差;转动星敏感器三维调整基座(8),使其转动90°,此时光电自准直仪的读数(θX,θZ)即为基准立方镜(10)与星敏感器(9)测量坐标系在X和Z方向的安装误差;由此完成基准立方镜(10)与星敏感器(9)测量坐标系的安装误差(θX,θY,θZ)。3. the calibration device of star sensor reference cube mirror installation error according to claim 1, it is characterized in that: the device working process is as follows: standard prism (2) is placed on the datum plane (7), with theodolite ( 1) collimate the front reflective surface of the standard prism (2), then clear the theodolite (1) pitch reading θ V ; keep the theodolite (1) state unchanged, remove the standard prism (2); make the theodolite (1) Collimate with the photoelectric autocollimator (4), adjust the two-dimensional adjustment base (3) of the photoelectric autocollimator, so that the output of the photoelectric autocollimator (4) is 0°, indicating that the photoelectric autocollimator (4) ) is parallel to the reference plane (7), the photoelectric autocollimator (4) is fixed; the theodolite (1) is collimated with the single-star simulator (5), and the two-dimensional adjustment base of the single-star simulator (6) is adjusted ), so that the output of the light single-star simulator (5) is 0°, indicating that the output optical axis of the single-star simulator (5) is parallel to the reference plane (7), and the fixed single-star simulator (5); remove the The standard prism (2), places the measured star sensor (9) and the three-dimensional adjustment base (8) of the star sensor at the intersection of the two axes; the measured reference cube mirror (10) is installed on the measured star sensor ( 9) The upper surface of the shell; make the star sensor (9) roughly aligned with the single star simulator (5), then adjust the three-dimensional adjustment base (8) of the star sensor so that the output of the star sensor (9) is (0 °, 0°), say that the optical axis of the star sensor (9) coincides with the single star simulator (5); at this time, the reading (θ X , θ Y ) of the photoelectric autocollimator (4) is the reference cube (10) and star sensor (9) measure the installation error of coordinate system in X and Y direction; Rotate star sensor three-dimensional adjustment base (8), make it rotate 90 °, the reading of photoelectric autocollimator this moment ( θ X , θ Z ) is the installation error of the measurement coordinate system of the reference cube (10) and the star sensor (9) in the X and Z directions; thereby completing the measurement of the reference cube (10) and the star sensor (9) The installation error of the coordinate system (θ X , θ Y , θ Z ).
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