[go: up one dir, main page]

CN107861192A - Cone is drawn to combine the method that chemical attack prepares optical fiber F P sensors based on optical fiber - Google Patents

Cone is drawn to combine the method that chemical attack prepares optical fiber F P sensors based on optical fiber Download PDF

Info

Publication number
CN107861192A
CN107861192A CN201711216215.7A CN201711216215A CN107861192A CN 107861192 A CN107861192 A CN 107861192A CN 201711216215 A CN201711216215 A CN 201711216215A CN 107861192 A CN107861192 A CN 107861192A
Authority
CN
China
Prior art keywords
optical fiber
fiber
sensor
pstrain
single mode
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201711216215.7A
Other languages
Chinese (zh)
Inventor
祝连庆
周康鹏
何巍
张雯
娄小平
董明利
陈少华
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Beijing Information Science and Technology University
Original Assignee
Beijing Information Science and Technology University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Beijing Information Science and Technology University filed Critical Beijing Information Science and Technology University
Priority to CN201711216215.7A priority Critical patent/CN107861192A/en
Publication of CN107861192A publication Critical patent/CN107861192A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/25Preparing the ends of light guides for coupling, e.g. cutting
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/255Splicing of light guides, e.g. by fusion or bonding
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/255Splicing of light guides, e.g. by fusion or bonding
    • G02B6/2553Splicing machines, e.g. optical fibre fusion splicer

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Optical Transform (AREA)

Abstract

本发明提供了一种基于光纤拉锥结合化学腐蚀制备光纤F‑P应变传感器的方法,通过拉锥结合化学腐蚀方法制备光纤上的F‑P微结构,来实现物理量的测量,拉锥后的光纤的纤芯和包层变细,测量应变时测量腔长变化会更明显,进而灵敏度更高,适合高精度测量;在锥形结构上又构造出F‑P结构会使传感灵敏度进一步提高。本发明制备的光纤F‑P应变传感器器件的结构简单,稳定性可靠,并可以根据要求制备不同腔长的器件,制备方法简便,其中拉锥和化学腐蚀技术成本较低,重复性高,易于实现器件的批量加工。

The invention provides a method for preparing an optical fiber F-P strain sensor based on optical fiber tapering combined with chemical corrosion. The F-P microstructure on the optical fiber is prepared by the tapering combined with chemical corrosion method to realize the measurement of physical quantities. The core and cladding of the optical fiber become thinner, the change of the measurement cavity length will be more obvious when measuring the strain, and the sensitivity is higher, which is suitable for high-precision measurement; the F-P structure is constructed on the tapered structure to further improve the sensing sensitivity . The optical fiber F-P strain sensor device prepared by the present invention has simple structure, reliable stability, and devices with different cavity lengths can be prepared according to requirements. Realize batch processing of devices.

Description

基于光纤拉锥结合化学腐蚀制备光纤F-P传感器的方法Method for preparing optical fiber F-P sensor based on optical fiber tapering combined with chemical etching

技术领域technical field

本发明涉及光纤器件领域,特别涉及一种光纤拉锥制成的光纤F-P传感器的方法。The invention relates to the field of optical fiber devices, in particular to a method for an optical fiber F-P sensor made of optical fiber tapering.

背景技术Background technique

光纤传感器具有诸多优良特性,可实现复杂环境下的测量工作具有非常广泛的应用价值。它具有抗电磁干扰、抗辐射、灵敏度高、重量轻、绝缘防爆、耐腐蚀等特点,且光纤尺寸微小,具有良好的光传输性能。在各种类型的光纤传感器中,目前精度最高的是干涉型光纤传感器。其中,光纤F-P传感器因只用一根光纤且结构简单体积小、动态范围大,在生物医学、磁场、微机电系统中受到广泛关注。Optical fiber sensors have many excellent characteristics, which can realize measurement work in complex environments and have a very wide range of application values. It has the characteristics of anti-electromagnetic interference, anti-radiation, high sensitivity, light weight, insulation explosion-proof, corrosion resistance, etc., and the fiber size is small, with good optical transmission performance. Among various types of fiber optic sensors, the most accurate one is the interferometric fiber optic sensor. Among them, the optical fiber F-P sensor has received extensive attention in biomedicine, magnetic field, and micro-electromechanical systems because it only uses one optical fiber and has a simple structure, small size, and large dynamic range.

传统的制作方法工序复杂、重复性差,对于法珀腔还需要进行腔长的标定,这使得光法布里-珀罗的批量生产较为困难,从而在一定程度上限制了光纤法布里-珀罗传感器的进一步广泛应用。光纤F-P传感器与传统的传感器相比,光纤法布里-珀罗传感器具有诸多优良特性,如不受电磁干扰、适用范围广、稳定性好、可靠性好、分辨率高、精度高、体积小、重量轻等显著优点。The traditional manufacturing method has complex procedures and poor repeatability. For the Fabry-Perot cavity, the cavity length needs to be calibrated, which makes the mass production of optical Fabry-Perot difficult, thus limiting the optical fiber Fabry-Perot to a certain extent. The further wide application of Luo sensor. Compared with traditional sensors, fiber optic F-P sensors have many excellent characteristics, such as no electromagnetic interference, wide application range, good stability, good reliability, high resolution, high precision, small size , light weight and other significant advantages.

光纤Fabry-Perot(F-P)传感器主要包括非本征型和本征型两大类。非本征型结构的光纤F-P传感器是利用光纤和一个具有反射面结构的非光纤原件组成;本征型光纤F-P结构的加工方法一般为将光纤两端面镀膜,通过封装或对接制成,但由于光纤的直径在微米量级,镀膜材料难以选择,镀膜难度大,且在封装或对接时需要精确地控制镀膜光纤和精确连接光纤以减小耦合损失,操作难度大。Optical fiber Fabry-Perot (F-P) sensors mainly include two types: extrinsic type and intrinsic type. The fiber optic F-P sensor with extrinsic structure is composed of an optical fiber and a non-fiber optic element with a reflective surface structure; the processing method of the intrinsic fiber F-P structure is generally made by coating the two ends of the fiber and packaging or docking, but due to The diameter of the optical fiber is on the order of microns. It is difficult to choose the coating material, and the coating is difficult. In addition, it is necessary to accurately control the coated optical fiber and connect the optical fiber to reduce the coupling loss during packaging or docking, and the operation is difficult.

目前,常见的F-P腔制备方法为:化学腐蚀法、电弧放电法、飞秒激光制备法等。针对利用飞秒刻写形成的光纤F-P传感器,当飞秒激光聚焦到光纤纤芯上时,会使材料性质发生改变,使其折射率发生改变,而光纤的表面不会受到任何影响。而通过化学腐蚀法制备光纤传感器时,可以通过控制腐蚀时间、调配HF酸溶液浓度、设置腐蚀时间等手段设定传感器腔长,成本较低、制作简单,在一定成都上可实现大批量的生产。At present, the common F-P cavity preparation methods are: chemical corrosion method, arc discharge method, femtosecond laser preparation method, etc. For the optical fiber F-P sensor formed by femtosecond writing, when the femtosecond laser is focused on the fiber core, the material properties will be changed and the refractive index will be changed, while the surface of the fiber will not be affected in any way. When the optical fiber sensor is prepared by chemical etching, the length of the sensor cavity can be set by controlling the etching time, adjusting the concentration of HF acid solution, setting the etching time, etc., the cost is low, the production is simple, and mass production can be realized in a certain area. .

因此,需要一种基于光纤拉锥结合化学腐蚀来制备非本征型结构的光纤F-P应变传感器的方法。Therefore, there is a need for a method for fabricating an optical fiber F-P strain sensor with an extrinsic structure based on optical fiber tapering combined with chemical etching.

发明内容Contents of the invention

为了解决上述技术问题,本发明提供一种基于光纤拉锥结合化学腐蚀制备光纤F-P应变传感器的方法,包括以下步骤:In order to solve the above-mentioned technical problems, the present invention provides a method for preparing an optical fiber F-P strain sensor based on optical fiber tapering combined with chemical corrosion, comprising the following steps:

步骤一:采用普通单模光纤,将其放置在高精度单芯熔接机中拉锥;Step 1: Use ordinary single-mode fiber and place it in a high-precision single-core fusion splicer to taper;

步骤二:用切割刀将拉锥后的普通单模光纤从中间切断,并将其中一端置于40%的氢氟酸中腐蚀10分钟,直至被腐蚀的光纤端面形成凹槽;Step 2: Use a cleaver to cut off the tapered ordinary single-mode optical fiber from the middle, and place one end in 40% hydrofluoric acid to corrode for 10 minutes until the corroded optical fiber end face forms a groove;

步骤三:将上述被腐蚀的光纤端面洗净残留氢氟酸,并与普通单模光纤另一端在熔接机中熔接,形成F-P腔结构,得到光纤F-P应变传感器的结构。Step 3: Clean the end face of the corroded optical fiber with residual hydrofluoric acid, and weld it with the other end of the ordinary single-mode optical fiber in a fusion splicer to form an F-P cavity structure, and obtain the structure of the optical fiber F-P strain sensor.

优选地,在步骤一中,拉锥后的光纤的长度为15000μm-20000μm,相应的腰椎直径为50μm-100μm。Preferably, in step 1, the length of the tapered optical fiber is 15000 μm-20000 μm, and the corresponding lumbar diameter is 50 μm-100 μm.

优选地,在步骤一中,所述普通单模光纤的型号为SMF-28,所述光纤的包层直径为125μm,纤芯直径为9μm。Preferably, in step 1, the model of the common single-mode optical fiber is SMF-28, the cladding diameter of the optical fiber is 125 μm, and the core diameter is 9 μm.

优选地,在步骤一中,所述高精度单芯熔接机采用日本Fujikura公司的80S高精度单芯熔接机。Preferably, in step 1, the high-precision single-core welding machine adopts the 80S high-precision single-core welding machine of Japan Fujikura Company.

其中,在步骤二中,光纤的纤芯与光纤的包层相比,其掺锗元素较高,与氢氟酸溶液的反应速率较快,经过一段时间后被腐蚀的光纤端面会形成凹槽。Among them, in step 2, compared with the cladding of the optical fiber, the core of the optical fiber has higher germanium-doped elements, and the reaction rate with the hydrofluoric acid solution is faster, and after a period of time, grooves will be formed on the end face of the corroded optical fiber. .

优选地,在步骤三中,所述光纤F-P腔结构为将腐蚀好的普通单模光纤端面与所述普通单模光纤另一端相对熔接后形成的微腔,所述F-P腔结构包括两个反射端面,所述反射端面分别为被腐蚀好的普通单模光纤端面形成的凹槽以及所述普通单模光纤另一端熔接时熔化形成的另一个凹槽,所述两个反射端面可形成圆。Preferably, in step 3, the optical fiber F-P cavity structure is a microcavity formed after the corroded common single-mode fiber end face is relatively fused with the other end of the common single-mode fiber, and the F-P cavity structure includes two reflecting The end face, the reflective end face is a groove formed by the corroded end face of the common single-mode fiber and another groove formed by melting when the other end of the common single-mode fiber is fused, and the two reflective end faces can form a circle.

更优选地,所述F-P腔结构中两个反射端面的距离为50μm-6000μm,该范围干涉效果最佳。More preferably, the distance between the two reflective end faces in the F-P cavity structure is 50 μm-6000 μm, and the interference effect is best in this range.

优选地,本发明的制备方法,可以根据要求制备出不同腔长的光纤F-P应变传感器器件。Preferably, the preparation method of the present invention can prepare optical fiber F-P strain sensor devices with different cavity lengths according to requirements.

本发明具有以下有益效果:The present invention has the following beneficial effects:

1.采用拉锥结合化学腐蚀的方法制备,制备方法简便。1. It is prepared by the method of tapering combined with chemical etching, and the preparation method is simple.

2.制备得到的非本征型光纤F-P应变传感器器件的结构简单,稳定性可靠,并可以根据要求制备不同腔长的器件。2. The prepared extrinsic optical fiber F-P strain sensor device has a simple structure and reliable stability, and devices with different cavity lengths can be prepared according to requirements.

3.拉锥和化学腐蚀技术成本较低,重复性高,易于实现器件的批量加工。3. Tapering and chemical etching technologies have low cost and high repeatability, and are easy to realize batch processing of devices.

应当理解,前述大体的描述和后续详尽的描述均为示例性说明和解释,并不应当用作对本发明所要求保护内容的限制。It should be understood that both the foregoing general description and the following detailed description are exemplary illustrations and explanations, and should not be used as limitations on the claimed content of the present invention.

附图说明Description of drawings

参考随附的附图,本发明更多的目的、功能和优点将通过本发明实施方式的如下描述得以阐明,其中:With reference to the accompanying drawings, more objects, functions and advantages of the present invention will be clarified through the following description of the embodiments of the present invention, wherein:

图1示出了根据本发明制备的光纤F-P应变传感器的结构示意图。Fig. 1 shows a schematic diagram of the structure of an optical fiber F-P strain sensor prepared according to the present invention.

图2示出了测试本发明制备的光纤F-P应变传感器性能的应变系统结构示意图。Fig. 2 shows a schematic structural diagram of a strain system for testing the performance of the optical fiber F-P strain sensor prepared by the present invention.

图3示出了根据本发明制备的光纤F-P应变传感器在不同应变下的干涉谱图。Fig. 3 shows the interference spectra of the optical fiber F-P strain sensor prepared according to the present invention under different strains.

图4示出了对本发明制备的光纤F-P应变传感器进行标定后得到的波长-应变关系曲线示意图。Fig. 4 shows a schematic diagram of the wavelength-strain relationship curve obtained after calibration of the optical fiber F-P strain sensor prepared by the present invention.

具体实施方式Detailed ways

通过参考示范性实施例,本发明的目的和功能以及用于实现这些目的和功能的方法将得以阐明。然而,本发明并不受限于以下所公开的示范性实施例;可以通过不同形式来对其加以实现。说明书的实质仅仅是帮助相关领域技术人员综合理解本发明的具体细节。The objects and functions of the present invention and methods for achieving the objects and functions will be clarified by referring to the exemplary embodiments. However, the present invention is not limited to the exemplary embodiments disclosed below; it can be implemented in various forms. The essence of the description is only to help those skilled in the relevant art comprehensively understand the specific details of the present invention.

在下文中,将参考附图描述本发明的实施例。在附图中,相同的附图标记代表相同或类似的部件,或者相同或类似的步骤。Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings. In the drawings, the same reference numerals represent the same or similar components, or the same or similar steps.

参见图1,本发明提供一种基于光纤拉锥结合化学腐蚀制备光纤F-P应变传感器的方法,包括以下步骤:Referring to Fig. 1, the present invention provides a kind of method for preparing optical fiber F-P strain sensor based on optical fiber tapering in combination with chemical corrosion, comprising the following steps:

步骤一:采用普通单模光纤,将其放置在高精度单芯熔接机中拉锥;Step 1: Use ordinary single-mode fiber and place it in a high-precision single-core fusion splicer to taper;

进一步地,所述普通单模光纤的型号为SMF-28,所述光纤的包层直径为125μm,纤芯直径为9μm。Further, the model of the common single-mode optical fiber is SMF-28, the cladding diameter of the optical fiber is 125 μm, and the core diameter is 9 μm.

进一步地,拉锥后的光纤的长度为15000μm-20000μm,相应的腰椎直径为50μm-100μm,如图1中(a)所示。Further, the length of the tapered optical fiber is 15000 μm-20000 μm, and the corresponding lumbar diameter is 50 μm-100 μm, as shown in (a) of FIG. 1 .

步骤二:用切割刀将拉锥后的光纤从中间切断,并将其中一端置于40%的氢氟酸中腐蚀10分钟,直至被腐蚀的光纤端面形成凹槽,如图1中(b)所示。Step 2: Use a cleaver to cut off the tapered optical fiber from the middle, and place one end in 40% hydrofluoric acid for 10 minutes to corrode until the corroded optical fiber end face forms a groove, as shown in Figure 1 (b) shown.

其中,光纤的纤芯与包层相比,其掺锗元素较高,与氢氟酸溶液的反应速率较快,经过一段时间后被腐蚀的光纤端面会形成凹槽。Among them, compared with the cladding, the core of the optical fiber has a higher germanium-doped element, and the reaction rate with the hydrofluoric acid solution is faster. After a period of time, grooves will be formed on the end face of the corroded optical fiber.

步骤三:将上述光纤洗净残留氢氟酸,并与普通单模光纤的另一端在熔接机中熔接,形成F-P腔结构,得到光纤F-P应变传感器的结构。其中,所述高精度单芯熔接机采用日本Fujikura公司的80S高精度单芯熔接机。Step 3: Clean the remaining hydrofluoric acid from the above-mentioned optical fiber, and weld it with the other end of the common single-mode optical fiber in a fusion splicer to form an F-P cavity structure and obtain the structure of an optical fiber F-P strain sensor. Wherein, the high-precision single-core welding machine adopts the 80S high-precision single-core welding machine of Japan Fujikura Company.

如图1(c)所示,在步骤三中,所述光纤F-P腔结构为将腐蚀好的普通单模光纤端面与所述普通单模光纤另一端相对熔接后形成的微腔,所述F-P腔结构包括两个反射端面,所述反射端面分别为被腐蚀好的普通单模光纤端面形成的凹槽以及所述普通单模光纤另一端熔接时熔化形成的另一个凹槽,所述两个反射端面可形成圆,所述F-P腔结构中两个反射端面的距离为50μm-6000μm,该范围干涉效果最佳。As shown in Figure 1 (c), in step three, the cavity structure of the optical fiber F-P is a microcavity formed after the corroded common single-mode fiber end face is relatively fused with the other end of the common single-mode fiber, and the F-P The cavity structure includes two reflective end faces, the reflective end faces are respectively the groove formed by the corroded common single-mode fiber end face and another groove formed by melting when the other end of the common single-mode fiber is fused. The reflective end faces can form a circle, and the distance between the two reflective end faces in the F-P cavity structure is 50 μm-6000 μm, which is the best interference effect.

具体地,当相干光束沿大模场光纤入射到上述微腔时,光在微腔的两个反射端面反射后沿原路返回,并相遇而产生干涉。Specifically, when the coherent light beam is incident on the microcavity along the large mode field fiber, the light is reflected by the two reflective end faces of the microcavity, returns along the original path, and meets to generate interference.

具体地,根据多光束干涉原理,光学F-P腔的反射输出IRSpecifically, according to the principle of multi-beam interference, the reflection output I R of the optical FP cavity is

式中,为光学位相,其中In the formula, is the optical phase, where

其中,n0是腔内材料的折射率,R是两端面的反射率,为入射光与反射端面的夹角,λ和I0分别为入射光波长与光强,L是微腔的腔长,附加的相位π是光由光疏介质入射到光密介质时产生的半波损耗引起的相位差。Among them, n 0 is the refractive index of the material in the cavity, R is the reflectivity of both ends, and is the angle between the incident light and the reflection end surface, λ and I 0 are the wavelength and light intensity of the incident light, respectively, and L is the cavity length of the microcavity , the additional phase π is the phase difference caused by the half-wave loss when light is incident on an optically rarer medium to an optically denser medium.

当F-P腔两端面的反射率R很低时,可用双光束干涉代替多光束干涉,则When the reflectivity R of both ends of the F-P cavity is very low, double-beam interference can be used instead of multi-beam interference, then

由式(1)、(2)和(3)和可知,当外界参量作用于微腔时,可以通过反射光强变化推出相应外界参量的变化,实现传感测量的目的。From formulas (1), (2) and (3), it can be seen that when the external parameters act on the microcavity, the change of the corresponding external parameters can be deduced through the change of the reflected light intensity, and the purpose of sensing and measurement can be realized.

参见图2,为用于测试光纤F-P应变传感器性能的应变系统,该系测试统包括宽带光源1、光纤环行器2、等强度梁3、本发明制备得到的光纤F-P应变传感器4以及光纤传感分析仪5,所述光纤F-P应变传感器4粘贴在等强度梁3上,并通过光纤环行器2与光纤传感分析仪5相连。Referring to Fig. 2, it is a strain system for testing the performance of an optical fiber F-P strain sensor. The system test system includes a broadband light source 1, an optical fiber circulator 2, an equal-intensity beam 3, an optical fiber F-P strain sensor 4 prepared by the present invention, and an optical fiber sensor Analyzer 5, the optical fiber F-P strain sensor 4 is pasted on the equal strength beam 3, and connected to the optical fiber sensor analyzer 5 through the optical fiber circulator 2.

其中,光谱仪采用Yokogawa公司生产的光纤传感分析仪。Among them, the spectrometer adopts the optical fiber sensor analyzer produced by Yokogawa Company.

其中,宽带光源1用于为所述光纤F-P传感器提供测试信号。Wherein, the broadband light source 1 is used to provide test signals for the optical fiber F-P sensor.

本实验通过光纤传感分析仪5采集反射光谱,具体地,通过光纤环行器2将光纤F-P腔产生的反射干涉光谱传输至光纤传感分析仪5。其中,所述光纤F-P应变传感器4粘贴在等强度梁3上,可利用等强度梁3改变应变力大小。具体地,所述等强度梁3还包括基底和螺旋测微头,所述螺旋测微头转动时,所述基底会发生形变,引起贴于基底的F-P腔发生应力变化。其中,对螺旋测微头转动的距离与基底的弯曲程度的关系已标定好。In this experiment, the reflection spectrum is collected by the optical fiber sensing analyzer 5 , specifically, the reflection interference spectrum generated by the optical fiber F-P cavity is transmitted to the optical fiber sensing analyzer 5 through the optical fiber circulator 2 . Wherein, the optical fiber F-P strain sensor 4 is pasted on the equal-intensity beam 3, and the equal-intensity beam 3 can be used to change the magnitude of the strain force. Specifically, the equal-strength beam 3 also includes a base and a spiral micrometer head. When the spiral micrometer head rotates, the base will deform, causing stress changes in the F-P cavity attached to the base. Among them, the relationship between the rotation distance of the spiral micrometer head and the bending degree of the substrate has been calibrated.

参见图3,为本实验得到的反射光谱图,由图可知:当外界温度或压力发生变化,反射光谱谱线会发生平移,3条谱线分别为应变为50με、100με、150με时,所述光纤F-P传感器在1520nm~1610nm范围内的干涉谱图。因此,本发明制备的传感器的应变性良好,结构可行。See Figure 3, which is the reflectance spectrum obtained in this experiment. It can be seen from the figure that when the external temperature or pressure changes, the reflectance spectral lines will shift, and the three spectral lines are respectively when the strain is 50με, 100με, and 150με. The interference spectrum of the fiber optic F-P sensor in the range of 1520nm to 1610nm. Therefore, the strain resistance of the sensor prepared by the invention is good, and the structure is feasible.

参见图4,通过将所述光纤F-P应变传感器进行标定,在应变为50~400με范围内,每间隔50με施加应变,记录相应应变时的波长,得到波长—应变关系曲线,由图可知:传感器的线性度为99.8%,灵敏度为5.82pm/με,表明该传感器线性度良好,灵敏度高,适用于高精度测量。Referring to Figure 4, by calibrating the optical fiber F-P strain sensor, within the strain range of 50-400με, applying strain at intervals of 50με, recording the wavelength of the corresponding strain, and obtaining the wavelength-strain relationship curve, it can be seen from the figure that: The linearity is 99.8%, and the sensitivity is 5.82pm/με, indicating that the sensor has good linearity and high sensitivity, and is suitable for high-precision measurement.

本发明是通过拉锥结合化学腐蚀方法制备光纤上的F-P微结构,来实现物理量的测量,拉锥后的光纤的纤芯和包层变细,测量应变时测量腔长变化会更明显,进而灵敏度更高,适合高精度测量;在锥形结构上又构造出F-P结构会使传感灵敏度进一步提高。本发明制备的光纤F-P应变传感器器件的结构简单,稳定性可靠,并可以根据要求制备不同腔长的器件,制备方法简便,其中拉锥和化学腐蚀技术成本较低,重复性高,易于实现器件的批量加工。The present invention prepares the F-P microstructure on the optical fiber by tapering and chemical corrosion method to realize the measurement of physical quantity, the fiber core and cladding of the optical fiber after tapering become thinner, and the change of the measurement cavity length will be more obvious when measuring the strain, and then Higher sensitivity, suitable for high-precision measurement; constructing F-P structure on the tapered structure will further improve the sensing sensitivity. The optical fiber F-P strain sensor device prepared by the present invention has simple structure, reliable stability, and devices with different cavity lengths can be prepared according to requirements. The preparation method is simple, and the cost of tapering and chemical etching technology is low, the repeatability is high, and the device is easy to realize. batch processing.

结合这里披露的本发明的说明和实践,本发明的其他实施例对于本领域技术人员都是易于想到和理解的。说明和实施例仅被认为是示例性的,本发明的真正范围和主旨均由权利要求所限定。Other embodiments of the invention will be apparent to and understood by those skilled in the art from consideration of the specification and practice of the invention disclosed herein. The description and examples are considered exemplary only, with the true scope and spirit of the invention defined by the claims.

Claims (7)

1. a kind of draw cone to combine the method that chemical attack prepares optic fiber F-Pstrain sensor based on optical fiber, comprise the following steps:
S1:Using general single mode fiber, place it in and cone is drawn in high-precision single heat sealing machine;
S2:With cutter the general single mode fiber after boring will be drawn to be cut off from centre, and wherein one end is placed in 40% hydrofluoric acid Middle corrosion 10 minutes, until the fiber end face being corroded forms groove;
S3:The above-mentioned fiber end face being corroded is cleaned into residual hydrofluoric acid, and with the general single mode fiber other end in heat sealing machine Welding, F-P cavity structure is formed, obtains optic fiber F-Pstrain sensor device.
2. the method according to claim 1 for preparing optic fiber F-Pstrain sensor, it is characterised in that in S1, after drawing cone Optical fiber length be 15000 μm -20000 μm, corresponding a diameter of 50 μm -100 μm of lumbar vertebrae.
3. the method according to claim 1 for preparing optic fiber F-Pstrain sensor, it is characterised in that in S1, the light Fine cladding diameter is 125 μm, and core diameter is 9 μm.
4. the method according to claim 1 for preparing optic fiber F-Pstrain sensor, it is characterised in that the general single mode The model SMF-28 of optical fiber, the high-precision single heat sealing machine are melted using the 80S high accuracy singles of Japanese Fujikura companies Pick.
5. the method according to claim 1 for preparing optic fiber F-Pstrain sensor, it is characterised in that in S3, the light Fine F-P cavity structure is that will be formed after the welding relative with the general single mode fiber other end of the general single mode fiber end face corroded Microcavity, the F-P cavity structure includes two reflection end faces, and the reflection end face is respectively the general single mode fiber that has been corroded Another to be formed groove is melted when the groove of end face formation and the general single mode fiber other end welding, it is described two anti- Circle can be formed by penetrating end face.
6. the method according to claim 5 for preparing optic fiber F-Pstrain sensor, it is characterised in that the F-P cavity structure In two reflection end faces distances be 50 μm -6000 μm.
7. the method according to claim 1 for preparing optic fiber F-Pstrain sensor, it is characterised in that the light being prepared Fine F-P strain transducers device can prepare different cavity length as requested.
CN201711216215.7A 2017-11-28 2017-11-28 Cone is drawn to combine the method that chemical attack prepares optical fiber F P sensors based on optical fiber Pending CN107861192A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201711216215.7A CN107861192A (en) 2017-11-28 2017-11-28 Cone is drawn to combine the method that chemical attack prepares optical fiber F P sensors based on optical fiber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201711216215.7A CN107861192A (en) 2017-11-28 2017-11-28 Cone is drawn to combine the method that chemical attack prepares optical fiber F P sensors based on optical fiber

Publications (1)

Publication Number Publication Date
CN107861192A true CN107861192A (en) 2018-03-30

Family

ID=61703651

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201711216215.7A Pending CN107861192A (en) 2017-11-28 2017-11-28 Cone is drawn to combine the method that chemical attack prepares optical fiber F P sensors based on optical fiber

Country Status (1)

Country Link
CN (1) CN107861192A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109632712A (en) * 2019-01-16 2019-04-16 北京信息科技大学 Femtosecond direct writing FBG temperature and refractive index measurement method with fiber taper structure
CN109682513A (en) * 2018-12-27 2019-04-26 北京信息科技大学 A kind of pressure detection method based on side throwing formula full-optical fiber F-P structure
CN109708803A (en) * 2019-02-25 2019-05-03 北京信息科技大学 A sensor preparation method for negative pressure monitoring of all-fiber F-P cavity structure
CN111596403A (en) * 2020-05-08 2020-08-28 武汉锐科光纤激光技术股份有限公司 Optical fiber device and method for manufacturing the same
CN112444502A (en) * 2020-11-19 2021-03-05 哈尔滨理工大学 Lead ion/bacterium monitoring double-parameter optical fiber sensing device and implementation method
CN112444503A (en) * 2020-11-19 2021-03-05 哈尔滨理工大学 Copper ion/bacterium monitoring dual-parameter optical fiber sensing device and implementation method

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001280922A (en) * 2000-03-29 2001-10-10 Tokyo Sokki Kenkyusho Co Ltd Optical fiber type strain sensor, and manufacturing method therefor
US20070041019A1 (en) * 2003-10-03 2007-02-22 Siegmar Schmidt Rugged fabry-perot pressure sensor
CN101034007A (en) * 2007-01-24 2007-09-12 冉曾令 Optical fiber Fabry-Perot sensor and manufacture method therefore
CN101655353A (en) * 2009-06-26 2010-02-24 南京师范大学 Miniature extrinsic Fabry-Perot type optical fiber pressure transducer and manufacturing method thereof
CN102508337A (en) * 2011-11-03 2012-06-20 上海大学 Optical fiber fused taper-based intrinsic Fabry-Perot device and manufacturing method thereof
US20140208858A1 (en) * 2011-08-09 2014-07-31 Junfeng Jiang High stable fiber fabry-perot pressure sensor with glue-free packing and its fabrication method
CN105180980A (en) * 2015-10-14 2015-12-23 南京信息工程大学 Symmetrical all-fiber Fabry-Perot sensor and manufacturing method thereof
CN106052912A (en) * 2016-07-11 2016-10-26 中国计量大学 Optical fiber stress sensing device based on Fabry-Perot microcavity structure

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001280922A (en) * 2000-03-29 2001-10-10 Tokyo Sokki Kenkyusho Co Ltd Optical fiber type strain sensor, and manufacturing method therefor
US20070041019A1 (en) * 2003-10-03 2007-02-22 Siegmar Schmidt Rugged fabry-perot pressure sensor
CN101034007A (en) * 2007-01-24 2007-09-12 冉曾令 Optical fiber Fabry-Perot sensor and manufacture method therefore
CN101655353A (en) * 2009-06-26 2010-02-24 南京师范大学 Miniature extrinsic Fabry-Perot type optical fiber pressure transducer and manufacturing method thereof
US20140208858A1 (en) * 2011-08-09 2014-07-31 Junfeng Jiang High stable fiber fabry-perot pressure sensor with glue-free packing and its fabrication method
CN102508337A (en) * 2011-11-03 2012-06-20 上海大学 Optical fiber fused taper-based intrinsic Fabry-Perot device and manufacturing method thereof
CN105180980A (en) * 2015-10-14 2015-12-23 南京信息工程大学 Symmetrical all-fiber Fabry-Perot sensor and manufacturing method thereof
CN106052912A (en) * 2016-07-11 2016-10-26 中国计量大学 Optical fiber stress sensing device based on Fabry-Perot microcavity structure

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
上官春梅 等: "采用化学腐蚀法制备光纤Fabry-Perot应变传感器", 《激光与红外》 *

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109682513A (en) * 2018-12-27 2019-04-26 北京信息科技大学 A kind of pressure detection method based on side throwing formula full-optical fiber F-P structure
CN109682513B (en) * 2018-12-27 2021-07-13 北京信息科技大学 A pressure detection method based on side-throw all-fiber F-P structure
CN109632712A (en) * 2019-01-16 2019-04-16 北京信息科技大学 Femtosecond direct writing FBG temperature and refractive index measurement method with fiber taper structure
CN109708803A (en) * 2019-02-25 2019-05-03 北京信息科技大学 A sensor preparation method for negative pressure monitoring of all-fiber F-P cavity structure
CN111596403A (en) * 2020-05-08 2020-08-28 武汉锐科光纤激光技术股份有限公司 Optical fiber device and method for manufacturing the same
CN112444502A (en) * 2020-11-19 2021-03-05 哈尔滨理工大学 Lead ion/bacterium monitoring double-parameter optical fiber sensing device and implementation method
CN112444503A (en) * 2020-11-19 2021-03-05 哈尔滨理工大学 Copper ion/bacterium monitoring dual-parameter optical fiber sensing device and implementation method
CN112444502B (en) * 2020-11-19 2021-09-24 哈尔滨理工大学 Lead ion/bacterium monitoring double-parameter optical fiber sensing device and implementation method
CN112444503B (en) * 2020-11-19 2021-09-24 哈尔滨理工大学 Copper ion/bacterium monitoring dual-parameter optical fiber sensing device and implementation method

Similar Documents

Publication Publication Date Title
CN107861192A (en) Cone is drawn to combine the method that chemical attack prepares optical fiber F P sensors based on optical fiber
CN102261924B (en) A Fabry-Perot interference sensor based on solid-core photonic crystal fiber and its manufacturing method
CN101825479B (en) Method for manufacturing composite fiber F-P sensor based on self-focusing effect
EP3163340B1 (en) Method of fabrication of an optical waveguide sensor and such optical waveguide sensor
CN108020248A (en) The method that large mode field fibre-optical F-P sensor is prepared based on chemical corrosion method
CN101614601B (en) Micro-Michelson interference sensor integrated in optical fiber and its manufacturing method
CN101424547B (en) Resonance type optical fiber F-P sensor and method of producing same
CN113959606B (en) Mixed type transverse pressure sensor based on cascade enhancement vernier effect
CN101650235B (en) Optical fiber interferometric temperature sensor integrated in miniature optical fiber and manufacturing method thereof
CN102374874A (en) Quartz capillary tube embedded all-silica fiber Fabry-Perot interferometric sensor and manufacturing method thereof
CN104880267A (en) Fiber micro-nano Fabry-Perot interference type pressure sensor and manufacturing method thereof
WO2022160822A1 (en) High-sensitivity high-temperature sensor based on suspended optical fiber dislocation fusion splicing
WO2008092372A1 (en) An optical fiber febry-perot sensor and the manufacture method thereof
CN108168584A (en) Full single mode optical fiber F-P sensors and preparation method thereof
CN208155479U (en) The fiber optic temperature and pressure sensor of double cavity structure
CN101424696A (en) All-optical fiber temperature self-compensating miniature F-P acceleration sensor and method for making same
CN102778306A (en) Refractive index and temperature sensor of photonic crystal fiber, manufacturing method and measuring system
CN101303300A (en) Miniature optical fiber F-P sensor and manufacturing method, liquid tester based on sensor
CN106052727A (en) Senor device based on fiber miniature Fabry-Perot cavity
CN210221338U (en) Optical fiber high-temperature sensor based on parallel vernier effect
CN111337060A (en) Hybrid sensor based on vernier effect of parallel structure and manufacturing method thereof
CN110987229A (en) An optical fiber end face Fa-Per cavity temperature sensor
CN110927113A (en) Fiber integrated hydrogen sensor and manufacturing method thereof
CN107300437B (en) A fiber optic pressure sensor based on a micro-ellipsoidal air cavity and its manufacturing method
CN113267206B (en) A low-cost and reproducible fiber-optic non-enclosed Fabry-Perot sensor

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication
RJ01 Rejection of invention patent application after publication

Application publication date: 20180330