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基于扭曲长周期光纤光栅的高灵敏度压力传感器 总被引:2,自引:4,他引:2
研究了高频CO2激光脉冲写入的长周期光纤光栅在扭曲状态下的横向负载特性.发现扭曲降低了光纤光栅谐振波长横向负载灵敏度的方向相关性,使得这种光栅在各圆周方向上谐振波长对横向负载都不敏感,而谐振峰幅度随横向负载的增加线性减小,且谐振峰幅度的负载灵敏度随扭曲率的增加而提高.在扭曲率为1.8°mm-1时负载灵敏度可达0.47 dB/(g·mm-1),是自由状态长周期光纤光栅横向负载灵敏度的7倍,最后给出了利用这种扭曲长周期光纤光栅通过强度解调实现压力传感的实验研究结果. 相似文献
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利用高频CO2激光脉冲写入的周期达数毫米的超长周期光纤光栅(ULPFG),实验研究了这种新型ULPFG的扭曲特性,发现它的某些高阶谐振波长漂移与扭曲率之间具有良好的线性关系和方向相关性,其灵敏度可达0.2244nm/(rad/m),是高频CO2激光脉冲写入法写入的普通LPFG扭曲灵敏度的4倍.初步的理论分析表明,新型ULPFG横截面折变的非对称性以及导模与高阶包层模之间发生的耦合使得扭曲具有方向相关性和很高的灵敏度.基于这种ULPFG独特的扭曲特性,设计了一种可
关键词:
光纤传感
光纤光栅
2激光')" href="#">CO2激光
扭曲测量
双折射 相似文献
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利用有限元法和局域耦合模理论对空芯光子带隙光纤成栅机理进行了分析。建立了空芯光子带隙光纤包层空气孔塌缩模型,分析计算了纤芯基模(LP01)和一阶包层模(LP11)在塌缩区域内有效折射率分布和耦合系数分布,得到了LP01和LP11耦合的传输谱。在此基础上研究了光纤结构参数(空气孔直径和孔间距)、光栅参数(光栅周期和周期个数)、塌缩程度和塌缩方式对谐振波长的影响。研究结果表明,随着空气孔直径的增大、孔间距的减小、光栅周期的增大和塌缩程度的减小,其谐振波长向短波方向发生漂移;随着周期个数的增大,其谐振波长未发生明显漂移;此外,与圆对称塌缩相比,非对称塌缩谐振波长向短波方向移动。 相似文献
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金属包层长周期光纤光栅的理论和实验研究 总被引:3,自引:0,他引:3
金属包层长周期光纤光栅可用于对谐振波长的调谐。通过实验和理论研究了长周期光纤光栅在沉积金属包层前后谐振波长的变化规律。分析了金属包层光纤的特点,给出了金属包层光纤包层模的本征方程,并给出了这一复本征方程的求解方法。长周期光纤光栅在沉积金属包层后,对低阶包层模,谐振波长会向长波方向偏移,模次增加,偏移会增大;对高阶包层模,谐振波长向短波方向偏移。不同金属包层,谐振波长的偏移量也有一定差别。所给出的理论分析方法,可用于预测谐振波长的偏移方向和大小,对设计和制做这类长周期光纤光栅提供理论参考。 相似文献
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A new high-birefringence (Hi-Bi) fiber torsion sensor demodulated by a Hi-Bi fiber Bragg grating (FBG) is proposed in this study. The twisted Hi-Bi fiber sensor characteristics are analyzed using the Jones matrix. The intensity ratio from two reflected Bragg wavelengths is associated with the twist angle of the measured Hi-Bi fiber. It is found that the twist angle resolution is estimated at around 0.3° under ±0.1 dB readout from an optical spectrum analyzer if the polarization state of the light source is stable. The advantages of this new torsion sensor are: (1) insensitivity to intensity variations from the light source, (2) insensitivity to the torsion gauge length, and (3) absolute measurement in the twist angle. However, the polarization state of light in the proposed method needs to be controlled, and any birefringence change in the twisted Hi-Bi fiber needs to be prevented. 相似文献
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报道了一种用高频CO2 激光脉冲写入的新型长周期光纤光栅 (LPFG) .发现该LPFG具有独特的应变、温度、弯曲、扭曲和横向负载特性 .分析表明这些特性与单侧CO2 激光加热导致光栅横截面折射率分布不均匀有关 .基于这些独特的特性提出了几种新型的LPFG传感器 :1)能彻底解决弯曲与其他参量之间交叉敏感问题的弯曲不敏感的传感器 ;2 )不仅能绝对测量扭曲率而且能判断扭曲方向的扭曲传感器 ;3 )单个LPFG实现温度和横向负载同时测量的传感器 .这些新型的传感器具有方法简单易行、体积小、能埋入智能材料的优点 ,可实现对工程结构的实时监测 ,具有广泛的应用前景 相似文献
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报道了一种用高频CO2激光脉冲写入的新型长周期光纤光栅(LPFG).发现该LPF G具有独特的应变、温度、弯曲、扭曲和横向负载特性.分析表明这些特性与单侧CO2激光 加热导致光 栅横截面折射率分布不均匀有关.基于这些独特的特性提出了几种新型的LPFG传感器:1)能 彻底解决弯曲与其他参量之间交叉敏感问题的弯曲不敏感的传感器;2) 不仅能绝对测量扭 曲率而且能判断扭曲方向的扭曲传感器;3)单个LPFG实现温度和横向负载同时测量的传感器 .这些新型的传感器具有方法简
关键词:
长周期光纤光栅
光纤传感器
应变传感器
温度传感器
弯曲传感器
扭曲传感器 相似文献
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A novel bend-insensitive long-period fiber grating (LPFG) sensor written using focused CO2 laser pulses is demonstrated, for the first time, to our knowledge. It is found that the central wavelength shift of such a LPFG is only −0.018 nm even for a curvature of 1.1 m−1 at the most bend-insensitive position of the LPFG. Experimental results show that the bend sensitivity of the central wavelength of the LPFG has a periodic distribution along its circular directions. Such a bend-insensitive sensor could be used to solve the problem of cross-sensitivity between bend and other measurands, such as temperature, strain or refractive index, which is an unsolved problem for LPFG sensors in practice. In addition, the bend sensitivity of the LPFG can be adjusted by selecting its circular positions. 相似文献
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In this paper we have presented long period fiber grating (LPFG) as temperature sensor. Temperature based sensors have found a number of applications in commercial and industrial fields. In LPFG based temperature sensors, they respond to shift in various peak resonant wavelengths corresponding to various attenuation bands of the transmission spectrum. Temperature effect on the various attenuation bands of a LPFG have been investigated to create a highly sensitive measurement device. The temperature sensitivities of various attenuation bands of a LPFG over the wavelength region of 1.1–1.7 μm, for a grating period of 280 μm period, are obtained by monitoring the wavelength shift of each peak resonant wavelength with temperature increment of 20 °C, ranging from 0 °C to 100 °C. 相似文献