基于光时域反射计的全分布式光纤漏油传感器

报道了一种基于光时域反射计的全分布式光纤漏油传感器,该传感器能实现分布式实时监测长输油管道,及时发现小型的漏油事件.传感器沿管道铺设,利用光时域反射计实时测量光纤在长度上的损耗变化特点,及时发现并定位管道上的每一处泄漏事件.模拟实验证明了其实际操作的可行性,长期使用的稳定性和各种抗干扰性,能在15min内发现并定位漏油事件,且定位准确度为3m.

光导纤维pH传感器的光化学pH敏感高分子膜及pH响应性能

pH指示剂在高分子载体上的固定化研究是应光导纤维pH传感器的发展要求而发展起来的新的研究领域。pH指示剂在高分子固态载体上的固定直接决定着光导纤维pH传感器的灵敏度、响应时间、寿命等性能。迄今，吸附、包埋和化学键合三利，固定方法已得到广泛应用。吸附法与包埋法简单易行，但因指示剂易于逸出而无法保证试剂相的使用稳定性及寿命；化学键合法目前仅限于对含氨基等高反应活性基团的指示剂固定。另外，这三种固定技术均存在试剂相与分析对象呈现固／液两相分离的问题，它严重制约了传感器响应性能，成为pH指示剂固定技术发展的“瓶颈”。改善、发展与寻找新的指示剂／载体固定配对体系已成为本领域的研究焦点。本论文针对上述问题，开拓与发展了一系列指示剂固定于固态高分子载体上的新体系。（一）首先开拓与发展了酚红／交联聚乙烯醇与邻甲酚红／交联聚乙烯醇固定对的新体系。在酸性条件下，以甲醛做交联剂，通过在玻璃板上倾涂聚乙烯醇甲醛的凝胶溶液制备了高亲水性的交联聚乙烯醇载体膜；然后采用接枝共聚反应将丙烯酞胺单体与通过酸碱反应接枝有酚红或邻甲酚红的丙烯酞胺混合物接枝固定到交联聚乙烯醇薄膜上，首次将不含氨基的酚红、邻甲酚红在高亲水性的聚乙烯醇载体上固定。利用紫外可见光光谱仪测试了其响应性能。结果表明，固定化指示剂的光谱行为与其相应的水溶液的光谱行为不一致，这可能是固定化过程中新的化学键生成以及载体与指示剂之间的相互作用如氢键的作用等引起的。这也导致了其pH响应范围与相应指示剂水溶液的响应范围的差异。固定酚红交联聚乙烯醇pH敏感膜的pH响应范围为pH=6.72～8.49；固定邻甲酚红交联聚乙烯醇pH敏感膜的两个响应范围分别为［H~+］=0.1mol／L～5mol／L和pH7.97～12.26。这种方式制备的这两种pH敏感薄膜均表现出优异的可重复使用性、可逆性、稳定性及易于制备的特点。更突出的优点在于，与以聚丙烯酰胺为基质直接固定酚红的薄膜（PAM-PR）相比，这种固定技术制备的敏感膜，当其与分析剂溶液接触时，其接枝于表面的水溶性高分子溶解，呈现“液态”，在固态基质表面形成一“液膜”层，从而消除了试剂相与分析剂之间的相界面，克服了指示剂固定化技术中的“瓶颈”问题，大幅度地提高了其响应速度与灵敏度，使响应时间从PAM-PR的数十分钟降至30秒以下。（二）开拓了刚果红醋酸纤维素包埋对的pH敏感膜（CCM）及刚果红／环氧氯丙烷交联聚乙烯醇（PECM）和甲醛交联聚乙烯醇（PFCM）的三种pH敏感膜新体系，测试并比较了三种膜的响应性能。结果表明，固定化刚果红的光谱性质和响应范围与刚果红水溶液不一致，而且用不同载体固定的刚果红的光谱特征与响应范围也各不相同。CCM的响应范围为pH＝2.5～4.5，PECM的响应范围在［H~+］=2mol/L～pH＝6.8之间，PFCM响应范围为pH＝2.90～5.48。这也可能是固定化过程中的氢键效应、空间位阻、指示剂与载体间发生的化学反应不同及载体本身结构的差异等引起的。这三种膜也具有良好的重现性、可逆性及响应迅速（平均响应时间低于25秒）的特点。另外发现醋酸纤维素包埋刚果红的敏感膜具有特殊的稳定性。对这种特殊的稳定性原因的分析表明选择合适尺寸分子的指示剂与载体配对将可能克服包埋技术中指示剂逸出的缺点。（三）对制备的pH敏感膜及对应的水溶液的pH线性响应范围给出了相应的线性回归方程（R＞98.2）。结果表明这些敏感膜对响应范围内的pH均具有良好的线性响应关系。这些结果与思想不仅丰富了光导pH传感器的试剂相内容，也为后续工作提供了一些有益的借鉴。

An Ameliorated Phase Generated Carrier Demodulation Algorithm With Low Harmonic Distortion and High Stability

A novel ameliorated phase generated carrier (PGC) demodulation algorithm based on arctangent function and differential-self-multiplying (DSM) is proposed in this paper. The harmonic distortion due to nonlinearity and the stability with light intensity disturbance (LID) are investigated both theoretically and experimentally. The nonlinearity of the PGC demodulation algorithm has been analyzed and an analytical expression of the total-harmonic-distortion (THD) has been derived. Experimental results have confirmed the low harmonic distortion of the ameliorated PGC algorithm as expected by the theoretical analysis. Compared with the traditional PGC-arctan and PGC-DCM algorithm, the ameliorated PGC algorithm has a much lower THD as well as a better signal-to-noise-and-distortion (SINAD). A THD of below 0.1% and a SINAD of 60 dB have been achieved with PGC modulation depth (value) ranges from 1.5 to 3.5 rad. The stability performance with LID has also been studied. The ameliorated PGC algorithm has a much higher stability than the PGC-DCM algorithm. It can keep stable operations with LID depth as large as 26.5 dB and LID frequency as high as 1 kHz. The system employing the ameliorated PGC demodulation algorithm has a minimum detectable phase shift of 5 mu rad/root Hz @ 1 kHz, a large dynamic range of 120 dB @ 100 Hz, and a high linearity of better than 99.99%.

Distributed Temperature Sensing System Based on Rayleigh Scattering BOTDA

A distributed temperature sensor based on Rayleigh scattering Brillouin optical time domain analysis (Rayleigh-BOTDA) is proposed in this paper. The sensor uses Rayleigh backscattering effect of microwave modulated pulse base sidebands as probe wave and a high sensitive photon counting detector for Brillouin signal intensity detection. Compared with a conventional BOTDA system, the Rayleigh-BOTDA effectively suppresses polarization-induced signal fluctuation resulting in improved signal intensity. The experimental scheme presented is simplified by using a single laser with one-end access. The temperature accuracy of the new sensing system was demonstrated as 1 degrees C on spatial resolution of 3 m.

A novel fiber Bragg grating high-temperature sensor

A novel fiber Bragg grating (FBG) sensor for the measurement of high temperature is proposed and experimentally demonstrated. The interrogation system of the sensor system is simple, low cost but effective. The sensor head is comprised of one FBG and two metal rods. The lengths of the rods are different from each other. The coefficients of thermal expansion of the rods are also different from each other. The FBG will be strained by the sensor head when the temperature to be measured changes. The temperature is measured basis of the wavelength shifts of the FBG induced by strain. A dynamic range of 0-800 degrees C and a resolution of 1 degrees C have been obtained by the sensor system. The experiment results agree with theoretical analyses. (c) 2007 Elsevier GmbH. All rights reserved.

Fiber Bragg grating pressure sensor with enhanced sensitivity

A novel fiber Bragg grating (FBG) pressure sensor with the enhanced sensitivity has been demonstrated. A piston-like diaphragm with a hard core in the center is used to enhance the sensitivity. Both the theoretical analysis and the experimental result show that the radius of the hard core has significant effect on the pressure sensitivity. When the radius of the hard core is 1.5 mm, a pressure sensitivity of 7.23 nm/MPa has been achieved.

MEMBRANE-BASED FIBER BRAGG GRATING PRESSURE SENSOR WITH HIGH SENSITIVITY

A fiber Bragg grating (FBG) pressure sensor packaged by using a hard core in the membrane is presented. By utilizing the unique membrane-based FBG packagine method, its pressure sensitivity has been effectively enhanced. The pressure sensitivity of the FBG reaches 5.75 X 10(-3)/MPa within the pressure range of 0.0.16 Mpa. (C) 2009 Wiley Periodicals, Inc. Microwave Opt Technol Lett 51 1279-1281, 2009; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.24335

Fiber Bragg grating pressure sensor with ultrahigh sensitivity and reduced temperature sensitivity

A fiber Bragg grating (FBG) pressure sensing scheme based on a flat diaphragm and an L-shaped lever is presented. An L-shaped lever transfers the pressure-induced defection of the flat diaphragm to the axial elongation of the FBG. The curve where the L-shaped lever contacts the diaphragm is a segment of an Archimedes spiral, which is used to enhance the responsivity. Because the thermal expansion coefficient of the quartz-glass L-shaped lever and the steel sensor shell is different, the temperature effect is compensated for by optimizing the dimension parameters. Theoretical analysis is presented, and the experimental results show that an ultrahigh pressure responsivity of 244 pm/kPa and a low temperature responsivity of 2.8 pm/degrees C are achieved. (c) 2009 Society of Photo-Optical Instrumentation Engineers. [DOI 10.1117/1.3081058]

High-performance multiplexed vibration sensor system based on fiber lasers - art. no. 683019

This paper describes a high-performance multiplexed vibration sensor system using fiber lasers. A serial vibration sensor array consists of four short cavity fiber lasers. The system employs a single, polarization-insensitive, unbalanced Michelson interferometer to translate individual laser wavelength shifts induced by vibration signals into interferometer phase shifts. A dense wavelength division demultiplexor (DWDM) with high channel isolation is inserted to demultiplex each laser signal as a wavelength filter. Finally, a digital phase demodulator based on the phase generated carrier technique is used to achieve high-resolution interrogation. Experimental results show that no observable crosstalk is measured on the output channels, and the minimal detectable acceleration of this system is similar to 200ng/root Hz at 250Hz, which is fundamentally limited by the frequency noise of the lasers.

Characterization of a dissolved oxygen sensor made of plastic optical fiber coated with ruthenium-incorporated solgel

A dissolved oxygen sensor made of plastic optical fiber as the substrate and dichlorotris (1, 10-phenanthroline) ruthenium as a fluorescence indicator is studied. Oxygen quenching characteristics of both intensity and phase were measured; the obtained characteristics showed deviation from the linear relation described by the Stern-Volmer equation. A two-layer model is proposed to explain the deviation, and main parameters can be deduced with the model. (C) 2009 Optical Society of America