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针对惯性导航系统现有加速度计电流信号转换电路的不足,提出了一种基于电荷平衡和自动跟踪原理的加速度计电流数字转换方法(CDC),从工作原理上大幅提升转换电路性能。CDC对输入电流和反馈跟踪电流积分输出误差电压,依据该误差电压实时调整其数字输出d以及与d成比例的反馈跟踪电流,实时反馈控制使误差电压稳定在0附近,实现输入电流和反馈跟踪电流二者电荷平衡。设计了单路CDC电路用于原理验证和性能测试。实验表明,±40 mA电流范围内CDC电路标度因数不对称性优于5 ppm,非线性优于10 ppm,电流分辨率优于0.5 nA,动态范围大于164 dB;采用查找表技术补偿后-40℃~+60℃温度区间零偏变化小于30 nA、标度因数变化小于20 ppm,且各性能指标均有较大改善空间。电荷平衡和自动跟踪型加速度计电流数字转换技术具有动态范围大、精度高、分辨率高、易补偿等优点,具有非常好的应用前景。 相似文献
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为了提高激光陀螺旋转惯导系统的环境适应性,需要对惯性测量单元(IMU)进行磁屏蔽设计。对IMU的磁屏蔽效率进行了理论计算和有限元仿真,对磁屏蔽材料的厚度、接缝宽度及接缝处贴片的大小等参数进行了仿真分析。利用赫姆霍兹线圈对IMU进行了磁敏感性测试,实验结果表明:设计的IMU磁屏蔽结构的屏蔽效率在23~30 dB范围内,磁场引起的三个激光陀螺漂移小于0.002°/h/mT,满足高精度单轴旋转惯导系统的实用要求。该方法对旋转惯导系统的结构设计及磁屏蔽设计具有一定的参考意义。 相似文献
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单轴旋转对惯导系统误差特性的影响 总被引:9,自引:0,他引:9
分析了单轴旋转惯导系统自动补偿的基本原理,对陀螺和加速度计常值漂移、安装误差、标度因数误差等因素在单轴旋转下的调制情况进行了研究。通过仿真分析了转动速度对各种误差的影响规律,指出了实际系统旋转速度和方式的选择要综合考虑陀螺的常值漂移和标度因数误差的影响。利用激光捷联惯导系统在实验室中进行了单轴旋转IMU实验,其定位精度优于1nm/24h。研究结果可以为单轴旋转惯导系统的进一步优化和工程设计提供理论参考。 相似文献
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Bias of ring-laser-gyroscope (RLG) changes with temperature in a nonlinear way. This is an important restraining factor for improving the accuracy of RLG. Considering the limitations of least-squares regression and neural network, we propose a new method of temperature compensation of RLG bias building function regression model using least-squares support vector machine (LS-SVM). Static and dynamic temperature experiments of RLG bias are carried out to validate the effectiveness of the proposed method. Moreover, the traditional least-squares regression method is compared with the LS-SVM-based method. The results show the maximum error of RLG bias drops by almost two orders of magnitude after static temperature compensation, while bias stability of RLG improves by one order of magnitude after dynamic temperature compensation. Thus, the proposed method reduces the influence of temperature variation on the bias of the RLG effectively and improves the accuracy of the gyro scope considerably. 相似文献
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轴向陀螺漂移是影响单轴旋转惯导系统导航精度的主要因素。对于轴向陀螺漂移的预测,提出了一种基于支持向量机的算法。利用初始对准12 h内系统纬度误差和温度变化量作为训练数据,构造了以多项式、径向基、小波函数为核函数的支持向量机、最小二乘支持向量机、遗忘因子最小二乘支持向量机,对比了它们用于轴向陀螺漂移预测的泛化性能。试验结果表明:遗忘因子最小二乘支持向量机可有效地用于轴向陀螺漂移预测,具有很高的预测精度,极大地提高了单轴旋转激光陀螺惯导系统的导航精度。 相似文献
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本文主要介绍采用冷心放肩微量提拉法技术生长高质量大尺寸蓝宝石晶体的新型设备,由于晶体生长是在高温、高真空、籽晶升降与旋转平稳、晶体测重精准、功率稳定的状态下进行生长.所以我们配备了具有高冷却性能的腔体部件;大抽速,低反油率的高真空系统;无抖动、无爬行籽晶轴(俗称:籽晶热交换器)升降及旋转系统;高精度、高分辨率测重系统;稳定可靠的电控系统及电源加热系统.实验结果表明:设备简化的设计模式,不仅提高了工人的操作速度,操作更加简单,节约了劳动时间,提高了设备的利用率.优良的测重系统在早期晶种生长的好坏,有这很大的关系;解决晶体是否粘埚也起着很大的作用.电控系统对加热电源的稳定控制是能否生长高质量大尺寸晶体关键之一. 相似文献
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The composite films consisting of hydroxyapatite (HAP) submicron particles embedded in the gel composed of the titania nanoparticles were prepared on commercial Ti6A14V plates with titania buffer layer obtained by a spin-coating technique. The films were calcined in air at various temperatures, and the bioactivities of the films were investigated by immersing them in acellular simulated body fliud (SBF). X-ray diffraction(XRD), Fourier transform infrared spectroscopy (FTIR), Field emission-scanning electron microscopy(FESEM) and Energy dispersive X-ray (EDS) analysis were employed to investigate the phase formation and structure of the films before and after immersion, and the variations of Ca and P contents in SBF were measured by Inductively Coupled Plasma Spectroscopy(ICP). The results show that the as-prepared films were dense, homogeneous, all well-crystallized, and there was a close interracial bond between the film and the substrate. The characterisatics of the grown layer on the surfaces of the HAP/TiO2 films after immersion in SBF for different periods of time are specially discussed. 相似文献
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Measurement of intensity difference squeezing via non-degenerate four-wave mixing process in an atomic vapor 下载免费PDF全文
We report the measurement of the intensity difference squeezing via the non-degenerate four-wave mixing process in a rubidium atomic vapor medium. Two pairs of balanced detection systems are employed to measure the probe and the conjugate beams, respectively. It is convenient to get the quantum shot noise limit, the squeezed and the amplified noise power spectra. We also investigate the influence of the input extra quadrature amplitude noise of the probe beam. The influence of the extra noise can be minimized and the squeezing can be optimized under the proper parameter condition. We measure the -3.7-dB intensity difference squeezing when the probe beam has a 3-dB extra quadrature amplitude noise. This result is slightly smaller than -4.1 dB when the ideal coherent light (no extra noise) for the probe beam is used. 相似文献