WO2019019666A1 - 一种光纤光栅传感解调*** - Google Patents

一种光纤光栅传感解调*** Download PDF

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WO2019019666A1
WO2019019666A1 PCT/CN2018/079799 CN2018079799W WO2019019666A1 WO 2019019666 A1 WO2019019666 A1 WO 2019019666A1 CN 2018079799 W CN2018079799 W CN 2018079799W WO 2019019666 A1 WO2019019666 A1 WO 2019019666A1
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light source
demodulation system
detector
grating sensing
optical
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PCT/CN2018/079799
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French (fr)
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刘柯
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天津求实飞博科技有限公司
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Priority to US16/482,231 priority Critical patent/US20200141769A1/en
Publication of WO2019019666A1 publication Critical patent/WO2019019666A1/zh

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    • G—PHYSICS
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    • G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
    • G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
    • G01D5/35306—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement
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    • G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
    • G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
    • G01D5/35338—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using other arrangements than interferometer arrangements
    • G01D5/35354—Sensor working in reflection
    • G01D5/35358—Sensor working in reflection using backscattering to detect the measured quantity
    • G01D5/35361—Sensor working in reflection using backscattering to detect the measured quantity using elastic backscattering to detect the measured quantity, e.g. using Rayleigh backscattering
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
    • G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
    • G01D5/35306—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement
    • G01D5/35325—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement using interferometer with two arms in reflection, e.g. Mickelson interferometer
    • G—PHYSICS
    • G06—COMPUTING; CALCULATING OR COUNTING
    • G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
    • G06T5/00—Image enhancement or restoration
    • G06T5/20—Image enhancement or restoration using local operators
    • G—PHYSICS
    • G06—COMPUTING; CALCULATING OR COUNTING
    • G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
    • G06T5/00—Image enhancement or restoration
    • G06T5/70—Denoising; Smoothing

Definitions

  • the invention belongs to the field of fiber Bragg grating sensor demodulation, and in particular relates to a fiber grating sensing demodulation system.
  • the existing common demodulation systems include tunable fiber FP filtering system, unbalanced MZ interference system, matching grating system and edge filtering system, etc., which are related to various optical modules.
  • the structure is complicated and it is difficult to achieve miniaturization.
  • the nonlinearity and repeatability of the tunable fiber F-P filter system affect the demodulation accuracy, and when the scanning frequency of the light source is increased, the side mode suppression ratio of the fiber grating reflection signal will be significantly reduced, further improving the demodulation difficulty.
  • the non-balanced MZ interference system is only suitable for the measurement of dynamic parameters because the optical path difference between the reference arm and the measuring arm needs to be strictly controlled by changes in the external environment, and the system is extremely sensitive to changes in external environmental changes. Demodulation of constant parameters cannot be achieved.
  • the matching grating system requires that the reference grating and the measurement grating have completely consistent performance parameters, which is difficult to implement in practical applications, which results in a small price reduction space for the method. For edge filtering systems, the coupling ratio of the coupler and the stability of the filter will seriously affect the accuracy of the demodulation results, reducing the stability of such systems.
  • the present invention aims to propose a fiber grating sensing demodulation system, which is especially suitable for a small demodulation system, which can reduce the system volume and reduce the cost.
  • a fiber grating sensing demodulation system comprising a light source, an optical circulator, a sensor device, a spectrum analyzer and a computer,
  • the light source is used to implement continuous output of the light source
  • the optical circulator is connected to the light source for transmitting the light emitted by the light source to the sensor device, and transmitting the optical signal reflected by the sensor device to the optical spectrum analyzer, the optical spectrum analyzer comprising the detector and the collector;
  • the detector is coupled to an output of the circulator for converting the optical signal into an electrical signal
  • the collector is coupled to the detector for receiving electrical signals and transmitting the data to a computer.
  • the light source adopts a tunable distributed feedback laser diode, and the output wavelength of the tunable distributed feedback laser diode is changed by adjusting the magnitude of the injection current, so that the light source realizes continuous wavelength output under the condition that the injection current continuously changes.
  • the sensor device uses a fiber Bragg grating, which can be expanded according to the number of layouts and the number of channels.
  • the detector uses a PIN diode.
  • the collector uses the AVR chip ATmega16L-8AI to implement data acquisition.
  • a fiber coupler can be used instead of the optical circulator.
  • a fiber grating sensing demodulation system Compared with the prior art, a fiber grating sensing demodulation system according to the present invention has the following advantages: the present invention overcomes the disadvantages of the conventional demodulation system that it is difficult to achieve miniaturization, light weight, and modularization; Convenient, low processing cost and high production efficiency.
  • FIG. 1 is a schematic structural diagram of a fiber grating sensing demodulation system according to an embodiment of the present invention
  • FIG. 2 is a schematic circuit diagram of a detector according to an embodiment of the present invention.
  • FIG. 3 is a schematic circuit diagram of a collector according to an embodiment of the present invention.
  • connection In the description of the present invention, it should be noted that the terms “installation”, “connected”, and “connected” are to be understood broadly, and may be fixed or detachable, for example, unless otherwise explicitly defined and defined. Connected, or integrally connected; can be mechanical or electrical; can be directly connected, or indirectly connected through an intermediate medium, can be the internal communication of the two components.
  • Connected, or integrally connected can be mechanical or electrical; can be directly connected, or indirectly connected through an intermediate medium, can be the internal communication of the two components.
  • the specific meaning of the above terms in the present invention can be understood by a person of ordinary skill in the art.
  • a fiber grating sensing demodulation system uses a tunable distributed feedback laser diode as a light source to change the output wavelength of the tunable distributed feedback laser diode by adjusting the magnitude of the injection current, thereby continuously changing the injection current.
  • the light source realizes continuous wavelength output;
  • the tunable distributed feedback laser diode replaces the combination of ASE light source and filter in the traditional demodulation system, which is the key to miniaturization of the system;
  • the laser diode is small in size, based on Integration, continuous adjustment of the output wavelength can be achieved by changing the magnitude of the external injection current;
  • the optical circulator is connected to the light source for transmitting the light emitted by the light source to the sensor device, and then transmitting the optical signal reflected by the sensor device to the detector; when the power of the light source is large, the optical fiber coupler can be used instead
  • Fiber Bragg grating is the sensing component connected to the optical circulator in this system. Due to the wavelength selection characteristics of the grating, the center wavelength of the reflection is related to the ambient temperature. When the ambient temperature changes, the reflection wavelength is biased. Shift, the offset of the external temperature can be determined by this offset, so that the temperature parameter measurement can be realized; the number of the number and the number of ways can be expanded according to the layout requirement, and the measurement range can be effectively increased by increasing the number of sensors.
  • the detector mainly realizes the function of converting the optical signal reflected by FBG into an electrical signal, which is connected with the output of the circulator.
  • the optical signal is usually very weak, in order to improve the signal-to-noise ratio and enhance the detection stability, the detector is detected.
  • the amplifier is connected on the basis of the signal to achieve the purpose of signal amplification; the invention adopts a PIN diode as a detector, which has the characteristics of high response frequency, fast response speed, low power supply voltage and stable operation; and improving signal noise of weak electrical signals
  • the system uses AD18606AR amplification chip, connected with the PIN diode to achieve signal amplification; circuit diagram shown in Figure 2.
  • the collector is connected to the detector for receiving the electrical signal, that is, obtaining the spectrum of the FBG real-time reflection, and transmitting the data to the computer, which can be used for wavelength demodulation and measurement parameter conversion;
  • the invention adopts the AVR chip ATmega16L-8AI To realize the data acquisition function, first construct its minimum system, including power line, reset line, crystal line, AD conversion filter line, ISP download interface and JTAG simulation interface; then connect the corresponding interface with the detection module to realize signal acquisition;
  • the circuit diagram is shown in Figure 3.
  • the computer in the system is connected to the detector and collector circuit, and the data obtained by the spectrum analyzer is stored and processed to obtain the final measured value and displayed.
  • the working process of the invention is as follows: the system light source is set as an integrated optical component, and the distributed feedback laser diode can be tuned, and the continuous wavelength output of the light source is realized by adjusting the injection current of the laser diode.
  • the fiber grating is placed in a temperature-changing environment, and the light generated by the light source is transmitted to the fiber Bragg grating (array) for reflection through the optical circulator.
  • the fiber grating reflection spectrum before and after the temperature change is obtained by the detector and the acquisition mold, respectively.
  • the computer completes the reception, storage and processing of the spectral data before and after the temperature change, and obtains the wavelength offset by demodulation, and then converts it into a corresponding measurement value for display.

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Abstract

一种光纤光栅传感解调***，包括光源、光环形器、传感器件、光谱分析仪以及计算机，光源用于实现光源的连续输出；光环形器连接光源，用来将光源发出的光发送到传感器件，再将传感器件反射的光信号传输至光谱分析仪，光谱分析仪包括探测器以及采集器；探测器连接环形器的输出，用于将光信号转化为电信号；采集器连接探测器，用于接收电信号，并将数据传输至计算机。光纤光栅传感解调***克服了传统解调***难以实现小型化、轻型化、模块化的劣势；具有结构简单，维修方便，加工成本低、生产效率高等优点。

Description

一种光纤光栅传感解调*** 技术领域
本发明属于光纤布拉格光栅传感器解调领域，尤其是涉及一种光纤光栅传感解调***。
背景技术
在光纤光栅传感解调领域中，现有的常见解调***包括可调谐光纤F-P滤波***、非平衡的M-Z干涉***、匹配光栅***及边缘滤波***等，这些***给涉及多种光学模块，结构复杂，难以实现小型化。
其中，可调谐光纤F-P滤波***的非线性及重复性差影响解调精度，并且当增加光源的扫描频率时，光纤光栅反射信号的边模抑制比将明显降低，进一步提高解调难度。而非平衡的M-Z干涉***由于参考臂与测量臂的光程差需要严格受控于外界环境的变化，并且***对外界环境变化的响应极为敏感，因此这种方法只适用于对动态参量的测量，无法实现恒定参量的解调。匹配光栅***要求参考光栅与测量光栅有完全一致的性能参数，这在实际应用中是很难实现的，进而导致该方法的降价空间很小。对于边缘滤波***，耦合器的耦合比与滤波器的稳定性将严重影响解调结果的精确性，使这种***的稳定性降低。
由于目前的解调***大多采用离散的光学器件，无法应用到集成光学器件，实现模块化的解调，从而陷入解调***体积大、成本高的困境。
发明内容
有鉴于此，本发明旨在提出一种光纤光栅传感解调***，尤其适合小型的解调***，可减小***体积，降低成本。
为达到上述目的，本发明的技术方案是这样实现的：
一种光纤光栅传感解调***，包括光源、光环形器、传感器件、光谱分析仪以及计算机，
所述光源用于实现光源的连续输出；
所述光环形器连接光源，用来将光源发出的光发送到传感器件，再将传感器件反射 的光信号传输至光谱分析仪，所述光谱分析仪包括探测器以及采集器；
所述探测器连接环形器的输出，用于将光信号转化为电信号；
所述采集器连接探测器，用于接收电信号，并将数据传输至计算机。
进一步的，所述光源采用可调谐分布反馈激光二极管，通过调节注入电流的大小改变可调谐分布反馈激光二极管的输出波长，从而在注入电流连续变化的条件下，使光源实现连续的波长输出。
进一步的，所述传感器件采用光纤布拉格光栅，可根据布设需要进行个数及路数的拓展。
进一步的，所述探测器采用PIN二极管。
进一步的，所述采集器使用AVR芯片ATmega16L-8AI实现数据采集功能。
进一步的，当光源功率较大时，可采用光纤耦合器替代光环形器。
相对于现有技术，本发明所述的一种光纤光栅传感解调***具有以下优势：本发明克服了传统解调***难以实现小型化、轻型化、模块化的劣势；具有结构简单，维修方便，加工成本低、生产效率高等优点。
附图说明
构成本发明的一部分的附图用来提供对本发明的进一步理解，本发明的示意性实施例及其说明用于解释本发明，并不构成对本发明的不当限定。在附图中：
图1为本发明实施例所述的一种光纤光栅传感解调***的结构示意图；
图2为本发明实施例所述的探测器的电路示意图；
图3为本发明实施例所述的采集器的电路示意图。
具体实施方式
需要说明的是，在不冲突的情况下，本发明中的实施例及实施例中的特征可以相互组合。
在本发明的描述中，需要说明的是，除非另有明确的规定和限定，术语“安装”、 “相连”、“连接”应做广义理解，例如，可以是固定连接，也可以是可拆卸连接，或一体地连接；可以是机械连接，也可以是电连接；可以是直接相连，也可以通过中间媒介间接相连，可以是两个元件内部的连通。对于本领域的普通技术人员而言，可以通过具体情况理解上述术语在本发明中的具体含义。
下面将参考附图并结合实施例来详细说明本发明。
如图1所示，一种光纤光栅传感解调***，采用可调谐分布反馈激光二极管作为光源，通过调节注入电流大小改变可调谐分布反馈激光二极管的输出波长，从而在注入电流连续变化的条件下，使光源实现连续的波长输出；采用的可调谐分布反馈激光二极管代替了传统解调***中ASE光源与滤波器的组合，是本***实现小型化的关键；这种激光二极管体积小，基于集成，可通过外界注入电流大小的改变，实现输出波长的连续调节；
光环形器：与光源连接，用来将光源发出的光发送到传感器件，再将传感器件反射的光信号传输至探测器；当光源功率较大时，可采用光纤耦合器替代
传感器件：光纤布拉格光栅是本***中与光环形器相连的传感元件，由于光栅的波长选择特性，其反射的中心波长大小与外界环境温度有关，当环境温度发生变化时，反射波长发生偏移，可通过此偏移量确定外界温度的变化，从而实现温度参数测量；可根据布设需要进行个数及路数的拓展，通过增加传感器数量，可以有效提高测量范围。
探测器：探测器主要实现将FBG反射的光信号转化成电信号的功能，与环形器的输出相连；同时由于光信号通常是十分微弱的，为提高信噪比，增强探测稳定性，在探测器的基础上连接放大器，达到信号放大的目的；本发明采用PIN二极管作为探测器，其具有响应频率高，响应速度快，供电电压低，工作稳定的特点；为提高较微弱电信号的信噪比，需增加放大单元，本***采用AD18606AR放大芯片，与PIN二极管相连，实现信号的放大；电路图如图2所示。
采集器：采集器与探测器相连，用于接收电信号，即获得FBG实时反射的光谱，并将数据传输至计算机，可用于波长解调及测量参量的转换；本发明采用AVR芯片ATmega16L-8AI实现数据采集功能，首先构建其最小***，包括电源线路、复位线路、晶振线路、AD转换滤波线路、ISP下载接口及JTAG仿真接口等；再将对应接口与探测模块相连接，实现信号的采集；电路图如图3所示。
计算机：***中计算机与探测器及采集器电路相连接，并将光谱分析仪获得的数据进行存储与处理，得到最终的测量值，并进行显示。
本发明的工作过程如下：将***光源设置为集成光学元件，即可调谐分布反馈激光二极管，通过调节该激光二极管的注入电流，实现光源的连续波长输出。将光纤光栅放置在变温环境下，光源产生的光经由光环形器传输至光纤布拉格光栅(阵列)发生反射。由探测器及采集模器分别获得温度变化前后的光纤光栅反射光谱。计算机完成对温度变化前后光谱数据的接收、存储并进行处理，通过解调，获得波长偏移量，再转换为对应测量值，进行显示。
以上所述仅为本发明的较佳实施例而已，并不用以限制本发明，凡在本发明的精神和原则之内，所作的任何修改、等同替换、改进等，均应包含在本发明的保护范围之内。

Claims (6)

  1. 一种光纤光栅传感解调***，其特征在于：包括光源、光环形器、传感器件、光谱分析仪以及计算机，
    所述光源用于实现光源的连续输出；
    所述光环形器连接光源，用来将光源发出的光发送到传感器件，再将传感器件反射的光信号传输至光谱分析仪，所述光谱分析仪包括探测器以及采集器；
    所述探测器连接环形器的输出，用于将光信号转化为电信号；
    所述采集器连接探测器，用于接收电信号，并将数据传输至计算机。
  2. 根据权利要求1所述的一种光纤光栅传感解调***，其特征在于：所述光源采用可调谐分布反馈激光二极管，通过调节注入电流的大小改变可调谐分布反馈激光二极管的输出波长，从而在注入电流连续变化的条件下，使光源实现连续的波长输出。
  3. 根据权利要求1所述的一种光纤光栅传感解调***，其特征在于：所述传感器件采用光纤布拉格光栅，可根据布设需要进行个数及路数的拓展。
  4. 根据权利要求1所述的一种光纤光栅传感解调***，其特征在于：所述探测器采用PIN二极管。
  5. 根据权利要求1所述的一种光纤光栅传感解调***，其特征在于：所述采集器使用AVR芯片ATmega16L-8AI实现数据采集功能。
  6. 根据权利要求1所述的一种光纤光栅传感解调***，其特征在于：当光源功率较大时，可采用光纤耦合器替代光环形器。
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