飞机尾翼转角测量系统设计

针对飞机尾翼转角测量及远距离监控问题,设计了一种基于数字式MEMS加速度传感器测量飞机尾翼转角的测量系统。分析了电容式加速传感器测角原理;利用数字式MEMS加速度传感器ADXL345,结合无线ZigBee技术采用CC2430模块,以嵌入式STM32单片机作为控制器构建了一种测量飞机尾翼转角大小的测量系统。采用三维转台对飞机尾翼转动进行了模拟,完成了±90°范围内转角的测量。实验结果表明,在±90°转角范围内,测量误差的最大值为0.277°,满足小于0.3°的误差要求。该测量系统可以有效地完成飞机尾翼转角测量工作。     

太阳紫外光谱辐射地面测量装置中的入射光学系统的研制

以聚四氟乙烯(PTFE)材料制成的积分球为基础,研制了7种组合型入射光学系统,并对它们的余弦特性进行了测试。其中PTFE积分球、磨砂石英半球型漫射器和修正环的组合型入射光学系统的设计具有创新性。在±30°入射角范围内,余弦误差小于0.23%;在±60°入射角范围内,余弦误差小于1.14%;在±75°入射角范围内,余弦误差小于2.5%;在±80°入射角范围内,余弦误差小于5.5%,积分余弦误差〈f2〉=0.94%,指标达到国际先进水平。组合型入射光学系统能够很好地满足太阳紫外光谱辐射地面测量的需求。     

三线摆实验仪角度控制装置的设计与制作

用三线摆测刚体转动惯量的实验条件是转动圆盘角度要小于 5°,在实验中因仪器没有配置角度的控制装置 ,因此无法准确控制角度 ,不能满足实验条件 ,造成实验结果误差增大。装上角度控制装置后 ,转动角度可精确控制小于 5°,保证了实验条件和实验结果的误差减小。     

光学棱镜的角误差检验

光学棱镜的角度误差,如90°误差、等腰棱镜底边的两角差、塔差等,通常是用平行光束通过被检验棱镜的光学方法进行检验的。此时,具有反射棱面的棱镜,其入射角小于全内反射角(БП-90°,БУ-45°,ВР-45°等)时,应在对诸反射棱面做金属镀膜之后进行检验。这是因为内反射造成的光能损失很大,最初的检验较为困难。     

用自准直法测量玻璃靠体内90°角

<正> 对于基准而和与其垂直的四个工作面(光胶零件面)的90°角误差要求为±5″的玻璃靠体,以前我们是用度盘格值为2″、自准直望远镜的分划板格值为15″的测角仪来测量的。先测量90°标准角块的角度,求得标准角度的综     

GNSS测姿系统天线设置及精度分析

GNSS测姿系统的天线设置是影响测姿精度的重要因素之一;针对GNSS天线设置对测姿精度的影响问题,在分析GNSS测姿算法的基础上,对天线设置的3个决定因素,即天线数量、基线夹角和基线长度与姿态角误差的关系进行了理论推导,仿真分析了三者对测姿误差的影响程度;理论推导结果表明,对航向角、俯仰角和横滚角的测量至少需要三个固定天线,天线构成的固定基线相互垂直时姿态角的误差较小,姿态角的误差与基线长度的平方成反比;仿真结果验证了上述结论并进一步表明,两基线长度分别为1 m、2 m、3 m时,航向角和俯仰角的误差分别在2°、1°、0.5°以内,横滚角的误差分别在3°、2°、1°以内。     

切线位移法测量微小角度偏转

叙述了将光电传感器的光轴相对固联于地理坐标系的转轴作切线运动并利用其切线位移模拟小角度偏转的方法。根据两轴初始零位对准值及切线位移量,由光电传感器的输出和所对应的角度偏移关系,获取光电传感器光轴的微小角度偏转量。该方法是一种简单有效的小角度偏移光电检测方法,可实现对微小角度偏移量的精密测量和实时读取,角度测量范围:±15°;测角精度:1″。     

90°反射式相位延迟器的设计

铜蒸气激光反射镜在非正入射的时候 ,两个不同的偏振态之间会产生不同的相移。通过优化设计 ,在4 90～ 5 30nm之间p、s波获得了 90°的相移 ,同时也使反射率在 99 998%以上。Ag层的厚度对于相移不敏感 ,并且当其厚度大于一定值的时候 ,对反射率没有影响。根据误差分析 ,制备薄膜时其沉积速率精度控制在± 1%以下 ,在光谱范围内能达到± 15 2 8°的相移误差 ,相移均在 5 0 4nm处附近存在有一个收敛值。折射率的变化控制在± 1%以下 ,在光谱范围内能达到± 12 77°的相移误差。最外一层厚度变化± 1% ,其相移变化达到± 5 5°,2～ 5层和 9～ 16层对相移的影响也在 0 .5°之上 ,其余各层对相移影响非常的小。使用时的入射角控制在± 1°时 ,在光谱范围内能达到± 2 .86°的相移误差。在 5 30nm附近的波段对入射角不敏感。     

用于同步辐射光源的成像板粉末衍射系统

报道了我们研制的一套成像板粉末衍射装置,对其误差来源进行了详细的分析讨论,并与衍射仪进行了比较.该装置的半径为143.3mm,最大测量角度范围不160°，最大角度(2q )偏差小于0.03°,这些性能指标已被实验所证实,完全可应用于粉末衍射全谱的测量.     

基于MEMS传感器的姿态测量系统设计

为解决单目三维扫描装置摄像机标定完成后姿态不能改变的问题,针对单目三维扫描装置使用过程中的运动方式与特点,设计了一款基于 MEMS 传感器的姿态测量系统。采用四元数对姿态进行解算,通过三轴姿态确定(TRAID)算法构建量测模型,以无迹卡尔曼滤波(UKF)算法进行数据融合,能有效抑制姿态解算过程中陀螺仪的漂移问题。实验结果表明,利用该系统进行姿态测量时静态误差低于±0.2°,动态误差低于±1°,系统实时性好、适用于动态三维扫描系统。     

Modeling and analysis for the image mapping spectrometer

The snapshot image mapping spectrometer(IMS) has advantages such as high temporal resolution,high throughput,compact structure and simple reconstructed algorithm.In recent years,it has been utilized in biomedicine,remote sensing,etc.However,the system errors and various factors can cause cross talk,image degradation and spectral distortion in the system.In this research,a theoretical model is presented along with the point response function(PRF) for the IMS,and the influence of the mirror tilt angle error of the image mapper and the prism apex angle error are analyzed based on the model.The results indicate that the tilt angle error causes loss of light throughput and the prism apex angle error causes spectral mixing between adjacent sub-images.The light intensity on the image plane is reduced to 95%when the mirror tilt angle error is increased to ±100 "(≈ 0.028°).The prism apex error should be controlled within the range of 0-36"(0.01°)to ensure the designed number of spectral bands,and avoid spectral mixing between adjacent images.     

基于耦合波理论设计偏振分束光栅

亚波长周期结构光栅具有传统光栅所不具有的特殊性质。针对通信中常用的1.55μm光波,采用严格耦合波理论分析了亚波长光栅的偏振分光特性,设计了对应的偏振分束光栅。所设计的光栅在入射角为56°时,透射消光比和反射消光比都大于9000,且在1.27μm~1.67μm全光波段内,入射角在51°~57°之间时,透射消光比和反射消光比都大于100,达到了宽带宽、宽角度以及透射消光比和反射消光比都较高的要求。     

基于时间控厚离子束溅射技术的宽带减反膜制备

 为了制备满足设计要求的宽角度、宽波段减反膜,利用离子束溅射沉积技术,在时间-功率控厚的模式下,对膜层沉积速率进行了精确修正。在实验中,利用时间-功率控厚的离子束溅射沉积技术,选择HfO₂和SiO₂作为高低折射率组合,在超抛ZF6玻璃基底上制备了宽角度、宽带减反膜,通过对实验后的透过率光谱曲线的数值反演计算,获得膜层厚度修正系数,初步得到了沉积速率随沉积时间变化的规律。利用修正后的沉积参数制备设计的膜系,在0°~30°入射角度下,600~1 200 nm波段的平均透过率达到99%以上。     

Phase retardation measurement by analyzing flipping points of polarization states in laser with an anisotropy feedback cavity

Phase retardation of wave plate is measured by analyzing flipping points of polarization states. Measured result and system error are analyzed. Nonlinearity of piezoelectric ceramic is an important error source. The nonlinearity is measured with an interferometer based on microchip Nd:YAG laser feedback phenomenon. The measured system of phase retardation, in this paper, is calibrated to the frequency splitting system. The accuracy of the system is improved. The measurement repeatability is better than 0.12° and the accuracy is better than 0.22°. This paper has a very important significance for wave plate high precision manufacture.     

双菱体λ/4消色差相位延迟器的设计

根据菲涅尔全内反射相变理论,给出了双菱体λ/4消色差器的结构设计、性能分析和测量方法.由有效通光孔径和光线追迹设计出BK7玻璃在波长532 nm时相位延迟λ/4的双菱体的结构,用作532 nm至1 064 nm波长范围的标准λ/4相位延迟器.理论分析了入射角变化和波长变化对双菱体相位延迟的影响,当入射角变化限制在±4.3°以内时,其影响得到补偿;波长从532 nm到1 064 nm产生的误差为－0.65°.采用椭偏法中的消光技术,分别实测了双菱体在532 nm和1 064 nm波长下的相位延迟为：90.08±0.14°和88.99±0.1°,可知两不同波长产生的相位延迟误差为－1.09°.     

A high precision,polychromatic, automatic ellipsometer

The design and performance of a versatile, high precision, automatic ellipsometer, which follows rapid changes in surface properties, scans through the entire visible spectrum and through angles of incidence between 50° and 89°, is described. The state of polarization of the light beam is phase and amplitude modulated by means of two Faraday modulators working at a single frequency but in quadrature. Out-of-balance error signals are electronically processed and applied to a servodrive system which rotates the polarizing elements to the null positions. The angular positions of the prisms are measured by means of moiré fringe-counting systems which have digital displays reading to 0.001° over a range of 360°. The absolute accuracy of measurement of Δ and ψ, once all effects of intrinsic component imperfections and misalignments have been minimised, is better than ±0.013° in ψ and ±0.014° in Δ. The ellipsometer has been shown to work satisfactorily for a wide range of surface problems and in particular for surfaces with reflectivities as low as 0.001. The mechanical construction of the ellipsometer allows simultaneous movement of the two optical arms in opposite directions hence allowing a change in angle of incidence to be effected without any sample realignment. The ellipsometer has been designed with a sufficiently large sample space to allow the inclusion of bulky environmental chambers such as cryostats or vacuum systems and may be used to examine either vertical or horizontal surfaces.     

Broadband high-efficiency controllable asymmetric propagation by pentamode acoustic metasurface

We utilise the pentamode metasurface to realise broadband high-efficiency and controllable asymmetric transmission. The designed metasurface can manipulate the acoustic waves, as expected from the generalised Snell's law, and exhibits unique characteristics such as extraordinary broadband acoustic control, apparent negative refraction, and conversion from the propagating wave to surface mode. The asymmetric transmission features of positive refraction for the forward incidence (FI) and negative refraction for the reverse incidence (RI) can be realised within the range of 2600 Hz to 5600 Hz by controlling the incident angle from 0° to 35° with the transmission efficiency higher than 85.4% for the FI and RI. In addition, by further adjusting the angle of incidence in the range of 25° to 90°, asymmetric transmission characteristics can be expressed as surface wave transmission for the FI and transmitted wave transmission for the RI within the same frequency ranges.     

光纤Bragg光栅倾角传感器的标定与不确定度分析

实现光纤Bragg光栅倾角传感器的静态的测试和性能分析。设计了一种量程为5°的倾角传感器标定装置,对其进行校准实验。通过对光纤光栅解调仪的中心波长差和标定装置产生的倾角值进行最小二乘法拟合,求出静态标定系数,并对倾角传感器标定装置的不同不确定度分量进行分析以求出合成不确定度。实验结果表明,光纤传感器的灵敏度为0.17343nm/(°),线性度为99.993%,重复性误差为0.0552%,标定装置的合成不确定度为8.606×10-2°。     

光致电化学法提高垂直结构发光二极管出光效率的研究

研究了在垂直结构发光二极管(VLED)器件中, 光致电化学法(PEC)刻蚀N极性n-GaN的速率受不同刻蚀条件(刻蚀浓度、刻蚀时间和光照强度)的影响. 并选择N极性n-GaN表面含有较理想六角金字塔结构(侧壁角为31°)的样品制成器件, 研究PEC刻蚀对VLED的欧姆接触和光电性能的影响. 结果表明, 与未粗化样品相比, PEC刻蚀后的样品接触电阻率明显降低, 形成更好的欧姆接触; 其电学特性有较好的改善, 光输出功率有明显提高, 在20 mA电流下光输出功率增强了86.1%. 对不同金字塔侧壁角度的光提取效率用时域有限差分法(FDTD)模拟, 结果显示光提取效率在侧壁角度为20°– 40°有显著提高, 在23.6° (GaN-空气界面的全反射角)时达到最大.