首页|基于光纤光栅法珀干涉结构的热线式风速计

基于光纤光栅法珀干涉结构的热线式风速计

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为提高热线式光纤光栅风速计的性能,提出一种基于光纤光栅法珀干涉结构的热线式风速计。该风速计通过在两个光纤布拉格光栅的中间熔接一段长度为500 μm的掺钴光纤以形成法珀干涉结构(FPI),该掺钴光纤吸收1 480 nm激光后产生热量从而形成热线,根据热膨胀效应和热光效应,温度变化会引起掺钴光纤中光程的变化,使得FPI的干涉谱红移。当气流流过FPI风速计时,掺钴光纤的热量散失速率加快,温度降低进而导致FPI干涉谱蓝移,蓝移量与风速成固定的关系。因此,通过测量FPI干涉谱的波长改变量,可以计算出风速值。实验中,在0~9 m/s的范围进行了风速测量,获得热线式风速计的典型响应,灵敏度随风速增大逐渐降低。在风速为0。1 m/s时,风速计的灵敏度达到-1 053。86 pm·m-1·s,而风速为0。5 m/s和5。0 m/s时,灵敏度分别为-746。47 pm·m-1·s和-15。15 pm·m-1·s。与已报道的热线式光纤光栅风速计相比,所提出的光纤光栅FPI风速计具有灵敏度高、结构简单紧凑、易于制造、成本低等优点。
Hot-wire Anemometer Based on Fiber Grating Fabry-Perot Interferometer
Airflow velocity measurement is important in many fields such as meteorological monitoring and wind power generation.Currently,it is common to utilize ultrasonic,differential pressure,eddy current,or heat transfer methods for measuring.However,in some extreme environments,these measurements may be encounter interference,resulting in less accurate or non-functional results.Fiber optic anemometers have attracted much attention because of their advantages of electrically passive operation,resistance to electromagnetic interference,high sensitivity,integrated structure,and the ability to measure over long distances.In order to enhance the performance of fiber optic anemometers,this paper proposes a hot-wire anemometer based on fiber grating Fabry-Perot Interferometer(FPI)structure.Fiber grating FPI anemometers are prepared by sandwiching a section of cobalt-doped fiber with a length of 500 μm in the middle of two Fiber Gratings(FBGs).The cobalt-doped fiber in the interference cavity is heated with a 1 480 nm laser to form a hot wire.Due to the effect of thermal expansion and thermo-optic,the optical range difference of the FPI cavity length changes with the temperature of the cobalt-doped fiber,which brings about the wavelength redshift of the interference spectrum.As air flows through the FPI anemometer,the heat dissipation from the FPI is accelerated.The temperature of the FPI decreases,causing a blue shift in the interference spectrum,and the airflow velocity value can be calculated by measuring the change in the interference spectrum.We first performed temperature calibration experiments on the FPI anemometer probe by placing the anemometer probe in a temperature-controlled box.The output power of the broadband light source was set to 5 mW,and the output of the 1 480 nm laser was turned off to avoid the heat generated by the cobalt-doped fiber absorbing the laser.The temperature of the temperature control box was adjusted to gradually increase from-20 ℃ to 110℃ in 10 ℃ steps,and the interference spectral drift of the anemometer in this temperature range was measured.Thus,the wavelength response of the FPI anemometer to temperature is obtained.The temperature sensitivity obtained by the linear fitting is 11.8 pm/℃,and the linear R2 is 0.997.To explore the impact of laser power on the initial temperature of the anemometer,we recorded the interference spectra of the FPI when the laser power was increased from 0 mW to 500 mW at a step of 10 mW.The experimental results show that the peak wavelength of the FPI interference spectrum shifts by 1.71 nm when the laser power is increased to 500 mW,which corresponds to an increase of 144.92 ℃ in the initial temperature of the anemometer.Finally,we carried out airflow velocity measurement experiment at different laser powers of 150,330 and 500 mW.The airflow velocity was changed from 0 to 9 m/s.The experimental results indicate that the sensitivity of the FPI anemometer increases with laser power but decreases with airflow velocity.It reached-1 053.86 pm·m-1·s at a airflow velocity of 0.1 m/s when laser power was 500 mW.It was decreased to-746.47 and-15.15 pm·m-1·s for airflow velocity of 0.5 and 5 m/s,respectively.The sensitivity of an anemometer exhibits an exponential decay trend due to Newton's law of cooling,which states that the rate of temperature decrease of a hot wire is proportional to the temperature difference between the wire and the surrounding environment.In low airflow velocity conditions,the temperature difference between the cobalt-doped optical fiber and the airflow is significant,resulting in a high rate of temperature decrease.However,as the airflow velocity increases,the temperature difference between the cobalt-doped optical fiber and the airflow sharply decreases,leading to a reduction in the sensitivity of the anemometer.The fiber grating FPI anemometer proposed in this paper has the advantages of high sensitivity,simple and compact structure,easy fabrication and low cost when compared with the previously reported optical fiber hot-wire anemometers.It is expected to be widely used for airflow velocity measurement in the related fields.

Fiber optic sensorsHot-wire anemometerFiber Bragg gratingFabry-Perot interferometerCobalt-doped optical fiberAirflow velocity measurement

林颖、唐玉涵、杜浪哲、徐鹏柏、董新永

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广东工业大学 信息工程学院 先进光子技术研究院,广州 510006

广东工业大学 通感融合光子技术教育部重点实验室,广州 510006

广东工业大学 广东省信息光子技术重点实验室,广州 510006

光纤传感器 热线式风速计 光纤布拉格光栅 法布里珀罗干涉仪 掺钴光纤 风速测量

2024

光子学报
中国光学学会 中国科学院西安光学精密机械研究所

光子学报

CSTPCD北大核心
影响因子:0.948
ISSN:1004-4213
年,卷(期):2024.53(12)