共查询到18条相似文献,搜索用时 45 毫秒
1.
2.
3.
4.
5.
利用3×3耦合器和法拉第旋转镜等光学元件,构造了一个基于迈克尔逊干涉系统的光纤振动传感器.使用外调制的方法对传输光进行相位生成载波调制,并将该光纤振动传感器应用于长距离的安全监测中.通过对该传感器的干涉输出信号进行贝塞尔展开分析,发现干涉输出信号中含有与外调制所使用的载波频率相同的信号成分.因此,使用一个中心频率为载波频率且通带很窄的带通滤波器,可以同步地提取载波信号.同步提取的载波信号用于干涉输出信号的相位生成载波被动零差解调,可以得到作用于光纤振动传感器上的外界振动信号.本文提出了从输出信号中同步提取载波的方法,通过理论推导得出了该方法的可行性,并且通过软件仿真和实验验证了该理论的正确性.文中还对提取的载波受低频信号干扰,造成其幅度不稳定的现象进行分析并提出了解决方法.研究表明,同步载波提取法适用于相位调制器与干涉信号输出端距离较远,相位生成载波解调需要的同源载波获取较困难的情况. 相似文献
6.
干涉型光纤水听器相位波调制及解调方案研究 总被引:3,自引:1,他引:3
概述了直接调制光源产生相位载波的马赫-曾德尔(Mach-Zehner)干涉型光纤水听器调制解调技术。重点在于通过严密的数学推导,定量分析了直接调制光源伴生的调幅现象对于解调过程和结果的影响,并有针对性地提出了解决方法。同时就采用直接调制光源的相位载波零差检测方案时,设计中如何合理选择各相关参数,以达到最佳匹配进行了原理性探讨。给出了有关实验结果,这些理论分析和实验结果对于全光纤化水听器的研究及检测 相似文献
7.
相位生成载波(PGC)调制解调是干涉型光纤水听器常用的解调方法。首先,分析并建立了PGC解调系统的噪声传递模型,研究了光源强度噪声对PGC解调输出噪声的影响机理,分析了调制深度和工作点两个参数对PGC解调噪声稳定性的影响。然后,提出了一种基于3×3耦合器的多相PGC解调方案,即在传统PGC解调架构中引入3×3耦合器进行多相检测,利用3×3耦合器的相移特性对三路干涉信号进行融合处理。在不同的调制深度条件下,该方案可以降低水听器工作点变化所引起的光源强度噪声传递系数波动范围。实验结果显示,在常用的调制深度范围(1.7~3.4)内,工作点变化导致的噪声传递系数波动峰谷值小于0.5 dB,噪声稳定性相比传统PGC解调系统显著提升。 相似文献
8.
9.
提出了一种改进型边缘滤波波长解调技术,解决干涉型或谐振型光纤传感器输出的干涉谱波长的快速解调问题。该波长解调技术基于啁啾光栅和长周期光栅的光谱特点,以啁啾光栅作为矩形滤波器,提取传感器输出干涉谱的一个干涉峰;以长周期作为边缘滤波器,将干涉峰的波长信息转化为光强信息进行检测。该波长解调技术波长解调范围为传感器输出干涉谱的一个自由光谱范围(FSR),解调速度快,克服了当前波长解调技术中存在的测量范围与测量速度难以同时提高的问题,同时还具有系统成本低 ,体积小,能够灵活多路扩展的特点。详细介绍了解调系统的工作原理以及系统结构,并将其实际应用于一种干涉型光纤电流传感器输出干涉谱的波长解调中。通过实验证明电流传感器工作在工频及脉冲电流(脉冲宽度25 μs)情况下,该解调系统对传感器输出干涉谱具有准确、快速的解调效果。该研究对推进干涉或谐振型光纤传感器的实际工程化水平的提高具有重要意义。 相似文献
10.
干涉型光纤传感器的消偏振衰落技术研究 总被引:1,自引:0,他引:1
本文对消除干涉型光纤传感器信号偏振衰落的偏振分集接收PDR(Polarization Diversity Receiver)技术进行了理论分析.通过三态PDR方式,对输出的最大有效幅度信号进行选取,能够避免传输光偏振态变化导致干涉信号完全衰落的现象,使干涉信号有效幅度在一定范围内变化.采用基于反正切计算的相位生成载波PGC(Phase Generated Carrier)解调技术的相位测量结果不受由于偏振衰落导致干涉信号有效幅度变化的影响.提出结合三态PDR方式和基于反正切计算的PGC解调技术消除偏振衰落问题的影响,实现干涉型光纤传感器中相位信号的理想解调. 相似文献
11.
光纤光栅传感信号解调技术研究进展 总被引:1,自引:0,他引:1
光纤光栅传感器是一种新型传感器,有着非常广泛的应用前景。限制光纤光栅传感器大量实际应用的主要障碍是传感信号解调,因而,光纤光栅传感信号解调是光纤光栅传感器应用的关键技术之一。本文对现有已报道的光纤光栅传感信号的解调方法进行综述,并归类为:边缘滤波法、匹配滤波法、可调谐滤波法、光源波长可调谐扫描法、射频探测法、光栅啁啾法、CCD分光仪法、干涉法。对各种方法的原理及相关改进方法进行了阐述,并对其优缺点做了比较分析,最后,对光纤光栅传感信号的解调技术发展进行了展望。 相似文献
12.
An integrated-optic amplitude and phase modulator is used in a network of interferometric sensors to create both a phase carrier and the pulses for multiplexing using time division. A time sampling technique is successfully used to account for the optical crosstalk in TDM processing and a very high frequency phase carrier is demonstrated. 相似文献
13.
为了消除非线性因素对相位生成载波解调结果的干扰,降低相位生成载波解调过程中低通滤波器的频响特性对相位生成载波解调结果的影响,该文提出了一种基于扩展卡尔曼滤波椭圆参数估计的相位生成载波微分交叉相乘解调方法。该方法在综合考虑各种非线性因素对相位生成载波微分交叉相乘解调结果的影响的基础上,对传统的相位生成载波微分交叉相乘解调过程进行了改进。经过计算机仿真和实验验证,该文所提出的扩展卡尔曼滤波微分交叉相乘方法能够有效地抑制非线性因素对相位生成载波解调结果的干扰,相比传统的相位生成载波微分交叉相乘方法,其信噪比提高了35.0 d B,总谐波失真降低了30.7 dB,信噪谐波比提高了31.0 dB,且扩展卡尔曼滤波微分交叉相乘方法受解调过程中低通滤波器频响特性的影响较小。 相似文献
14.
We present a novel reference compensation method for eliminating environmental noise in interferometric wavelength shift demodulation for dynamic fiber Bragg grating (FBG) sensors. By employing a shielded wavelength-division-multiplexed reference FBG in the system, the environmental noise is measured from the reference channel, and then subtracted from the demodulation result of each sensor channel. An approximate 40 dB reduction of the environmental noise has been experimentally achieved over a frequency range from 20 Hz to 2 kHz. This method is also suitable for the elimination of broadband environmental noise. The corresponding FBG sensor array system proposed in this paper has shown a wavelength resolution of . 相似文献
15.
The analysis of a demodulation system for Fiber Bragg Grating sensors based on two fixed spectral filters has been carried out both theoretically and experimentally. Different system configurations were analyzed by modifying the spectral position of the filters as well as the optical power-level of the signal reaching the two photo-detectors. Measurements with integration times that varied from 0.01 to 1 s have been compared with the low-frequency limit predicted for long-term operation. Comparisons between simulated and experimental results show good agreement, and extrapolations indicate that it should be possible to achieve an operating spectrum range of the order of 7 nm, with uncertainties equivalent to less than 2 pm in measurements of the sensor peak position. 相似文献
16.
The maximum signal handling capability (MSHC) is an important parameter for the fiber optic interferometric sensor (FOIS) system. It is restricted by the heterodyne frequency (HF) and the digital quadrature demodulation algorithm (DQDA) in the digital heterodyne demodulation scheme. In this paper we systematically investigate the MSHC of the FOIS based on the digital heterodyne demodulation scheme through comparison of the HF-determined MSHC and DQDA-determined MSHC. When discussing the DQDA-determined MSHC, two widely used methods are included, which are arctangent and differential-cross multiply (DCM). The comparison results reveal that the arctangent-determined MSHC is 12 dB larger than the DCM-determined MSHC. The HF-determined MSHC is between the two types of DQDA-determined MSHC. If the DQDA is arctangent, the MSHC of the system is the HF-determined MSHC. If the DQDA is DCM, the MSHC of the system is the DCM-determined MSHC. Experiments are carried out and the results are consistent with the theoretical analysis. The conclusion in this paper can help us to estimate the MSHC of the FOIS system based on the digital heterodyne demodulation scheme more accurately and provide a useful guideline for the design of the FOIS system with large demodulation dynamic scale. 相似文献
17.
For an accelerometer, it is necessary to distinguish the plus/minus axis rightly before use. Demodulated by phase generated carrier (PGC) technology, a definition of the polarity characteristic for a double-arms optical fiber accelerometer is proposed. It was found that, when the selected modulation depth C > 0, the demodulated result by PGC technology is equal to the optical phase shift in the long arm subtracting the one in the short arm, while opposite result would be obtained when C < 0. Then, a simple model is presented to discuss relations between the output of the accelerometer and relative positions of the two arms and the sound source. We demonstrate that, when C > 0, the response of the accelerometer is coincident with the signal when the long arm is placed pointing to the source, while opposite once the relative positions of the two arms were exchanged. On this condition, the long arm is defined as the plus axis and the short arm to be the minus axis. However, when C < 0, the polarity definition should be opposite. Based on this polarity definition, a combination method is offered to fabricate a three-dimensional optical fiber vector hydrophone (OFVH). Finally, these conclusions are proved by experiments. 相似文献
18.
通过对该系统采集到的法布里-珀罗(F-P)标准具透射谱和光纤布拉格光栅(FBG)传感器反射谱进行寻峰算法以及拟合算法的研究,采用C语言编程和LabVIEW编程相结合的方式,实现了FBG波长信号的解调。其中,由于系统采集到的F-P透射谱和FBG反射谱线时域信号数据都由离散点构成, 且在3 dB带宽内均符合高斯曲线分布,采用高斯拟合对采集到的信号数据进行寻峰处理,提高系统精度;又由于分布式反馈(DFB)激光器的波长扫描存在着一定的非线性,采用二项式拟合对DFB激光器的波长扫描曲线进行拟合,以降低其非线性导致的误差。另外,设置一路标准FBG传感通道用于波长校准。实验研究表明该系统稳定性良好,波长测量范围为1 550.012~1 554.812 nm,分辨力为1 pm,精度为10 pm,验证了该系统可用于FBG波长信号检测的可行性。 相似文献