CN101957227B - Photonic crystal fiber optic liquid level sensor and sensing system formed by same - Google Patents
Photonic crystal fiber optic liquid level sensor and sensing system formed by same Download PDFInfo
- Publication number
- CN101957227B CN101957227B CN2010105181325A CN201010518132A CN101957227B CN 101957227 B CN101957227 B CN 101957227B CN 2010105181325 A CN2010105181325 A CN 2010105181325A CN 201010518132 A CN201010518132 A CN 201010518132A CN 101957227 B CN101957227 B CN 101957227B
- Authority
- CN
- China
- Prior art keywords
- photonic crystal
- fiber
- liquid level
- crystal fiber
- optical fiber
- 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.)
- Expired - Fee Related
Links
- 239000000835 fiber Substances 0.000 title claims abstract description 141
- 239000004038 photonic crystal Substances 0.000 title claims abstract description 101
- 239000007788 liquid Substances 0.000 title claims abstract description 79
- 238000005253 cladding Methods 0.000 claims abstract description 57
- 239000013307 optical fiber Substances 0.000 claims abstract description 57
- 230000004927 fusion Effects 0.000 claims abstract description 27
- 238000001228 spectrum Methods 0.000 claims description 15
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 claims description 8
- 229910052709 silver Inorganic materials 0.000 claims description 8
- 239000004332 silver Substances 0.000 claims description 8
- 239000013078 crystal Substances 0.000 claims 2
- 238000005259 measurement Methods 0.000 abstract description 12
- 230000035945 sensitivity Effects 0.000 abstract description 7
- 238000004519 manufacturing process Methods 0.000 abstract description 6
- 240000008415 Lactuca sativa Species 0.000 description 17
- 235000012045 salad Nutrition 0.000 description 17
- 230000001681 protective effect Effects 0.000 description 12
- 238000000034 method Methods 0.000 description 10
- 230000003287 optical effect Effects 0.000 description 10
- 238000010586 diagram Methods 0.000 description 6
- 238000007526 fusion splicing Methods 0.000 description 5
- 238000005457 optimization Methods 0.000 description 5
- 238000003466 welding Methods 0.000 description 5
- 239000011248 coating agent Substances 0.000 description 4
- 239000011247 coating layer Substances 0.000 description 4
- 238000000576 coating method Methods 0.000 description 4
- 230000008878 coupling Effects 0.000 description 4
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 239000003292 glue Substances 0.000 description 4
- 230000005540 biological transmission Effects 0.000 description 3
- 230000008859 change Effects 0.000 description 3
- 239000010410 layer Substances 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 3
- 240000005702 Galium aparine Species 0.000 description 2
- 235000014820 Galium aparine Nutrition 0.000 description 2
- 230000007547 defect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 238000007499 fusion processing Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000001902 propagating effect Effects 0.000 description 2
- 238000002310 reflectometry Methods 0.000 description 2
- 235000012239 silicon dioxide Nutrition 0.000 description 2
- 238000006124 Pilkington process Methods 0.000 description 1
- 230000002238 attenuated effect Effects 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 230000007812 deficiency Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000010291 electrical method Methods 0.000 description 1
- 239000002360 explosive Substances 0.000 description 1
- 238000009776 industrial production Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 239000011241 protective layer Substances 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Images
Landscapes
- Optical Transform (AREA)
Abstract
本发明属于液位测量,具体涉及光子晶体光纤液位传感器及其组成的系统。一种光子晶体光纤液位传感器,其特征在于包括单模光纤SMF-28与光子晶体光纤SC-4.0,所述的单模光纤SMF-28与光子晶体光纤SC-4.0的始端熔接,光子晶体光纤的始端包层空气孔在熔接点闭合形成始端完全塌陷区域,所述的始端完全塌陷区域长度等于65μm;用熔接机对光子晶体光纤末端放电形成末端塌陷区域,光子晶体光纤末端镀有反射膜。整个传感器完全光纤化,不需要腐蚀光纤,制作方便。传感系统不受杂散光和温度的影响,信号噪声小,系统灵敏度高、可靠性好。
The invention belongs to liquid level measurement, and in particular relates to a photonic crystal optical fiber liquid level sensor and a system composed thereof. A photonic crystal fiber liquid level sensor is characterized in that it comprises a single-mode fiber SMF-28 and a photonic crystal fiber SC-4.0, the beginning of the single-mode fiber SMF-28 and the photonic crystal fiber SC-4.0 are fused, and the photonic crystal fiber The beginning cladding air hole is closed at the fusion point to form a completely collapsed region at the beginning, and the length of the completely collapsed region at the beginning is equal to 65 μm; a fusion splicer is used to discharge the end of the photonic crystal fiber to form a collapsed region at the end, and the end of the photonic crystal fiber is coated with a reflective film. The entire sensor is completely optical fiber, no need to corrode the optical fiber, and it is easy to manufacture. The sensing system is not affected by stray light and temperature, the signal noise is small, the system has high sensitivity and good reliability.
Description
技术领域 technical field
本发明属于液位测量,具体涉及光子晶体光纤液位传感器及其组成的系统。 The invention belongs to liquid level measurement, and in particular relates to a photonic crystal optical fiber liquid level sensor and a system composed thereof.
背景技术 Background technique
在工业生产中经常需要对液位进行测量,传统的检测方法有人工法、浮子法、电学法等,但这些方法在自动化、精密度、安全性等方面存在固有缺陷。光纤传感器本质安全、精密度高的特点,正好克服了传统方法的缺陷。在众多的光纤液位传感器中,以光强度调制型的为主,有泄露模式的[1]、基于全内反射的[2]-[5]、液面反射式等。但这些光纤液位传感器也有明显不足,有的受所测液体的理化性质严重限制、有的量程小、有的精度不高、有的可靠性不够干涉型的光纤传感器具有更高的精度,而光纤法布里-珀罗(F-P)腔干涉仪结构简单,近年来也得到了广泛研究。另外近来还出现了一些基于光纤光栅的液位传感器[6],[7]。 In industrial production, it is often necessary to measure the liquid level. Traditional detection methods include manual methods, float methods, and electrical methods, but these methods have inherent defects in automation, precision, and safety. The characteristics of intrinsic safety and high precision of optical fiber sensor just overcome the defects of traditional methods. Among the many optical fiber liquid level sensors, the light intensity modulation type is the main type, and there are leakage mode [1], total internal reflection based [2]-[5], liquid surface reflection type, etc. However, these optical fiber liquid level sensors also have obvious deficiencies. Some are severely limited by the physical and chemical properties of the liquid to be measured, some have a small range, some have low precision, and some have insufficient reliability. Interferometric fiber optic sensors have higher accuracy, while Fiber-optic Fabry-Perot (F-P) cavity interferometer has a simple structure and has been extensively studied in recent years. In addition, some liquid level sensors based on fiber gratings have appeared recently [6], [7].
申请(专利)号CN200420102303.6“光纤法布里-泊罗腔液位传感器”中利用被测液位变化对腔长的影响进行传感。但是制作工艺复杂,不适合批量生产。 Application (Patent) No. CN200420102303.6 "Optical Fiber Fabry-Perot Cavity Level Sensor" uses the influence of the measured liquid level change on the cavity length for sensing. However, the manufacturing process is complicated and not suitable for mass production.
近年来,光纤干涉传感被研究用来监测温度、压力、气体密度或折射率。在单模光纤中实现干涉的一种办法是利用长周期光栅[8],另一种办法是将光从单孔光纤耦合到多孔光纤[9],还有一种办法利用了光纤拉锥[10,11]。2008年,Rajan Jha提出用于绝对折射率测量的光子晶体光纤迈克尔逊干涉仪,他将大模场光子晶体光纤(LMA-8 Crystal Fiber)(图1a)和单模光纤(SMF-28)熔接,并将光子晶体光纤末端用光纤切割刀切割作为反射镜面,干涉条纹会随外部折射率的增加发生红移,熔接后形成的塌陷区长度约300μm,引入损耗5-9dB,损耗大小与塌陷区长度以及熔接参数有关,塌陷区长度越短损耗越小[12]。 In recent years, fiber optic interferometric sensing has been studied to monitor temperature, pressure, gas density or refractive index. One way to achieve interference in a single-mode fiber is to use a long-period grating [8], another way is to couple light from a single-hole fiber to a holey fiber [9], and another way is to use a fiber taper [10 , 11]. In 2008, Rajan Jha proposed a photonic crystal fiber Michelson interferometer for absolute refractive index measurement. He fused a large mode field photonic crystal fiber (LMA-8 Crystal Fiber) (Figure 1a) and a single-mode fiber (SMF-28) , and cut the end of the photonic crystal fiber with a fiber cleaver as a reflective mirror, the interference fringes will red shift with the increase of the external refractive index, the length of the collapsed region formed after welding is about 300 μm, and the loss is 5-9dB. The loss is related to the collapsed region The length of the collapse zone is related to the welding parameters, and the shorter the length of the collapse zone, the smaller the loss [12].
现有的光纤液位测量技术中,对于各种环境下液位感测是采用腐蚀后的光纤光栅或者拉锥光纤或者光纤错位熔接,不仅降低了光纤本身的机械强度,而且还存在温度交叉敏感效应,限制了它们的使用。利用光子晶体光纤迈克尔逊干涉仪来测量液位,可以解决以上问题。需要参与干涉的纤芯模和包层模的模场强度比在液位为零时大于等于1,这样随着液位的增加,干涉条纹对比度才会单调减小,同时为了得到尽可能大的测量范围,熔接时引入的损耗应约为3dB。本专利使用SC-4.0(图1b)和单模光纤(SMF-28)熔接, SC-4.0有小孔的包层部分较小,熔接后的塌陷区较短,等于65μm,熔接过程引入的损耗为3dB。为了增强干涉信号,又为了防止镀膜时银进入包层小孔,预先用光纤熔接机对末端放电,使空气孔闭合后,在光子晶体光纤末端镀上50nm的银膜用来增强反射率。 In the existing optical fiber liquid level measurement technology, for liquid level sensing in various environments, corroded fiber gratings or tapered optical fibers or optical fiber dislocation fusion splicing are used, which not only reduces the mechanical strength of the optical fiber itself, but also has temperature cross sensitivity. effects, limiting their use. Using photonic crystal fiber Michelson interferometer to measure liquid level can solve the above problems. The mode field strength ratio of the core mode and the cladding mode that needs to participate in the interference is greater than or equal to 1 when the liquid level is zero, so that as the liquid level increases, the contrast of the interference fringe will decrease monotonously, and at the same time, in order to get as large as possible The measurement range, the loss introduced during welding should be about 3dB. This patent uses SC-4.0 (Figure 1b) and single-mode fiber (SMF-28) for fusion splicing. The cladding part of SC-4.0 with small holes is smaller, and the collapse zone after fusion is shorter, equal to 65 μm. The loss introduced by the fusion process is 3dB. In order to enhance the interference signal, and to prevent silver from entering the cladding holes during coating, the end of the optical fiber fusion splicer is used to discharge in advance to close the air hole, and then a 50nm silver film is plated on the end of the photonic crystal fiber to enhance the reflectivity.
1、 Giovanni Betta,Antonio Pietrosanto, and Antonio Scaglione, "A Digital Liquid Level Transducer Based on Optical Fiber, "IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, 45(2), 551-555(1996). 1. Giovanni Betta, Antonio Pietrosanto, and Antonio Scaglione, " A Digital Liquid Level Transducer Based on Optical Fiber, "IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, 45(2), 551-555(1996).
2、 Pabitra Nath, Pranayee Datta, and Kanak Ch Sarma, "All fiber-optic sensor for liquid level measurement," MICROWAVE AND OPTICAL TECHNOLOGY LETTERS, 50(7), 1982-1984(2008). 2. Pabitra Nath, Pranayee Datta, and Kanak Ch Sarma, "All fiber-optic sensor for liquid level measurement," MICROWAVE AND OPTICAL TECHNOLOGY LETTERS, 50(7), 1982-1984(2008).
3、 Pekka Raatikainen, Ivan Kassamakov, Roumen Kakanakov an Mauri Luukkala, "Fiber-optic liquid-level sensor," sensors and actuators A, 58 93-97(1997). 3. Pekka Raatikainen, Ivan Kassamakov, Roumen Kakanakov an Mauri Luukkala, "Fiber-optic liquid-level sensor," sensors and actuators A, 58 93-97(1997).
4、 F. P??erez-Oc??on , M. Rubino, J.M. Abril, P. Casanova, J.A. Mart????nez, " Fiber-optic liquid-level continuous gauge," sensors and actuators A,125,124-132(2006). 4. F. P??erez-Oc??on , M. Rubino, J.M. Abril, P. Casanova, J.A. Mart????nez, " Fiber-optic liquid-level continuous gauge," sensors and actuators A,125,124 -132(2006).
5、 Chengning Yang, Shiping Chen, Guoguang Yang, "Fiber optical liquid level sensor under cryogenic environment," sensors and actuators A, 94, 69-75(2001). 5. Chengning Yang, Shiping Chen, Guoguang Yang, "Fiber optical liquid level sensor under cryogenic environment," sensors and actuators A, 94, 69-75(2001).
6、 Binfeng Yun, Na Chen, and Yiping Cui, "Highly Sensitive Liquid-Level Sensor Based on Etched Fiber Bragg Grating," IEEE PHOTONICS TECHNOLOGY LETTERS, 19(21), 1747-1749(2007). 6. Binfeng Yun, Na Chen, and Yiping Cui, "Highly Sensitive Liquid-Level Sensor Based on Etched Fiber Bragg Grating," IEEE PHOTONICS TECHNOLOGY LETTERS, 19(21), 1747-1749(2007).
7、 Tuan Guo, Qida Zhao, Qingying Dou, Hao Zhang, Lifang Xue, Guiling Huang, and Xiaoyi Dong, "Temperature-insensitive fiber Bragg grating liquid-level sensor based on bending cantilever beam," IEEE PHOTONICS TECHNOLOGY LETTERS, 17(11), 2400-2402(2005). 7. Tuan Guo, Qida Zhao, Qingying Dou, Hao Zhang, Lifang Xue, Guiling Huang, and Xiaoyi Dong, "Temperature-insensitive fiber Bragg grating liquid-level sensor based on bending cantilever beam," IEEE TE LE 1 PHOTONICS ), 2400-2402(2005).
8、 H. J. Patrick, A. D. Kersey, and F. Bucholtz, "Analysis of the response of long period fiber gratings to external index of refraction, " J. Lightw. Technol., 16(9), 1606–1612(1998). 8. H. J. Patrick, A. D. Kersey, and F. Bucholtz, "Analysis of the response of long period fiber gratings to external index of refraction," J. Lightw. Technol., 16(9), 1606–1612(1998).
9、 L. Yuan, J. Yang, Z. Liu, and J. Sun, "In-fiber integrated Michelson interferometer, " Opt. Lett., 31(18), 2692–2694(2006). 9. L. Yuan, J. Yang, Z. Liu, and J. Sun, "In-fiber integrated Michelson interferometer," Opt. Lett. , 31(18), 2692–2694(2006).
10、Z. Tian, S. S.-H. Yam, J. Barnes, W. Bock, P. Greig, J. M. Fraser,H. P. Loock, and R. D. Oleschuk, "Refractive index sensingwith Mach–Zehnder interferometer based on concatenating twosingle-mode fiber tapers, " IEEE Photon. Technol. Lett., 20(8), 626–628(2008). 10. Z. Tian, S. S.-H. Yam, J. Barnes, W. Bock, P. Greig, J. M. Fraser, H. P. Loock, and R. D. Oleschuk, "Refractive index sensing with Mach–Zehnder interferometer based on concatenating twosingle-mode fiber tapers , " IEEE Photon. Technol. Lett. , 20(8), 626–628(2008).
11、Z. Tian, S. S.-H. Yam, and H. P. Loock, "Refractive index sensor basedon an abrupt taper Michelson interferometer in a single mode fiber, "Opt. Lett., vol. 33, 1105–1107( 2008). 11. Z. Tian, S. S.-H. Yam, and H. P. Loock, "Refractive index sensor based on an abrupt taper Michelson interferometer in a single mode fiber, " Opt. Lett. , vol. 33, 1105–1107( 2008).
12、Rajan Jha, Joel Villatoro,"Ultrastable in reflection photonic crystal fiber modal interferometerfor accurate refractive index sensing, " APPLIED PHYSICS LETTERS, vol.93, 191106(2008)。 12. Rajan Jha, Joel Villatoro, "Ultrastable in reflection photonic crystal fiber modal interferometer for accurate refractive index sensing," APPLIED PHYSICS LETTERS, vol.93, 191106 (2008).
发明内容 Contents of the invention
一种光子晶体光纤液位传感器,其特征在于包括单模光纤SMF-28与光子晶体光纤SC-4.0, A photonic crystal fiber liquid level sensor is characterized in that it includes a single-mode fiber SMF-28 and a photonic crystal fiber SC-4.0,
所述的单模光纤SMF-28与光子晶体光纤SC-4.0的始端熔接,光子晶体光纤的始端包层空气孔在熔接点闭合形成始端完全塌陷区域;所述的始端完全塌陷区域长度等于65μm;光子晶体光纤的末端熔接形成末端塌陷区域;光子晶体光纤末端镀有反射膜。 The starting end of the single-mode fiber SMF-28 and the photonic crystal fiber SC-4.0 are fused, and the starting cladding air hole of the photonic crystal fiber is closed at the fusion point to form a completely collapsed region at the beginning; the length of the completely collapsed region at the beginning is equal to 65 μm; The end of the photonic crystal fiber is welded to form a collapsed area at the end; the end of the photonic crystal fiber is coated with a reflective film.
可以采用用熔接机对光子晶体光纤末端放电形成末端塌陷区域。 A fusion splicer can be used to discharge the end of the photonic crystal fiber to form an end collapsed region.
作为一种优化方式光子晶体光纤长度为10-50mm。 As an optimization method, the length of the photonic crystal fiber is 10-50mm.
作为进一步优化方式光子晶体光纤长度为20mm。 As a further optimization method, the length of the photonic crystal fiber is 20mm.
作为进一步优化方式所述的反射膜为金属银膜,其厚度为50nm。 The reflective film described as a further optimization method is a metallic silver film with a thickness of 50 nm.
作为进一步优化方式在光子晶体光纤液位传感器外还设有保护套,距光子晶体光纤部分的保护套设有若干小孔。 As a further optimization method, a protective cover is provided outside the photonic crystal optical fiber liquid level sensor, and several small holes are provided on the protective cover away from the photonic crystal optical fiber part.
作为进一步优化方式所述的单模光纤与保护套之间还设有过渡缓冲套。 A transitional buffer sleeve is also provided between the single-mode optical fiber and the protective sleeve described as a further optimization method.
一种光子晶体光纤液位传感器形成的传感系统,其特征在于:包括1510-1590nmASE宽光源、单模光纤、环行器、光子晶体光纤传感器、光谱分析仪和计算机;ASE宽光源接环行器F端口,环行器的G端口与上述的光子晶体光纤液位传感器连接,环行器的H端口与光谱分析仪连接,光谱分析仪的数据读入计算机;所述的光子晶体光纤液体传感器被垂直置于液体中。 A sensing system formed by a photonic crystal fiber liquid level sensor is characterized in that: it includes a 1510-1590nm ASE wide light source, a single-mode fiber, a circulator, a photonic crystal fiber sensor, a spectrum analyzer and a computer; the ASE wide light source is connected to the circulator F Port, the G port of the circulator is connected with the above-mentioned photonic crystal fiber liquid level sensor, the H port of the circulator is connected with the spectrum analyzer, and the data of the spectrum analyzer is read into the computer; the photonic crystal fiber liquid sensor is placed vertically in liquid.
一种光子晶体光纤液位传感器的制做方法: A method of manufacturing a photonic crystal fiber optic liquid level sensor:
光子晶体光纤液位传感器是将光子晶体光纤SC-4.0(图1b)与普通单模光纤SMF-28用光纤熔接机熔接,在熔接点光子晶体光纤的包层空气孔完全塌陷形成塌陷区域,此塌陷区域长度等于65μm,引入纤芯损耗3dB,只有一半能量在光子晶体光纤纤芯中传播,另一半未进入纤芯的能量在包层中继续传播。因此塌陷区域在这里的作用相当于耦合效率为3dB的耦合器,将在单模光纤纤芯中传输的光分成能量相等的两束分别在光子晶体光纤纤芯和包层中传输;在距离熔接点约10-50mm的光纤末端用光纤切割刀切断,预先用光纤熔接机对末端放电使空气孔闭合后在该端面上镀上反射膜作为反射镜。由单模光纤、熔接点、光子晶体光纤包层、光子晶体光纤纤芯、反射膜形成一个光纤迈克耳逊干涉仪。在该迈克耳逊干涉仪上,光子晶体光纤只有光纤纤芯和光纤包层,光子晶体光纤长度为10-50mm,这就构成了光子晶体光纤液位传感器,利用光纤包层中传输的光能量损耗和光纤包层与光纤芯的光干涉条纹特征来测量被测液体液位。上述被测液体的折射率大于光子晶体光纤包层的折射率。 The photonic crystal fiber liquid level sensor is to weld the photonic crystal fiber SC-4.0 (Figure 1b) and the ordinary single-mode fiber SMF-28 with a fiber fusion splicer, and the cladding air hole of the photonic crystal fiber is completely collapsed at the fusion point to form a collapsed area. The length of the collapsed region is equal to 65 μm, and the core loss is 3dB. Only half of the energy propagates in the core of the photonic crystal fiber, and the other half of the energy that does not enter the core continues to propagate in the cladding. Therefore, the role of the collapsed area here is equivalent to a coupler with a coupling efficiency of 3dB, which divides the light transmitted in the core of the single-mode fiber into two beams with equal energy and transmits them in the core and cladding of the photonic crystal fiber respectively; The end of the optical fiber with a point of about 10-50mm is cut off with a fiber cleaver, and the end is pre-discharged with an optical fiber fusion splicer to close the air hole, and then the end surface is coated with a reflective film as a reflector. An optical fiber Michelson interferometer is formed by a single-mode optical fiber, a fusion point, a photonic crystal fiber cladding, a photonic crystal fiber core, and a reflection film. In this Michelson interferometer, the photonic crystal fiber only has the fiber core and the fiber cladding, and the length of the photonic crystal fiber is 10-50mm, which constitutes the photonic crystal fiber liquid level sensor, which uses the light energy transmitted in the fiber cladding The loss and optical interference fringe characteristics of the fiber cladding and the fiber core are used to measure the liquid level of the measured liquid. The refractive index of the liquid to be measured is greater than the refractive index of the cladding of the photonic crystal fiber.
本传感器的传感原理是利用光纤迈克耳逊干涉仪中的光纤包层光在光子晶体光纤和外部环境界面处的能量损耗和光干涉特性来测量液位的: The sensing principle of this sensor is to use the energy loss and light interference characteristics of the optical fiber cladding light in the optical fiber Michelson interferometer at the interface between the photonic crystal fiber and the external environment to measure the liquid level:
(1)单模光纤纤芯中传输的光到达熔接点塌陷区域时被分为两部分,一部分光继续在光子晶体光纤纤芯中向前传输形成芯模,另一部分被耦合到光子晶体光纤包层中传输形成包层模。 (1) The light transmitted in the core of the single-mode fiber is divided into two parts when it reaches the collapsed region of the fusion splicing point. One part of the light continues to travel forward in the core of the photonic crystal fiber to form a core mode, and the other part is coupled to the photonic crystal fiber package Transport in the layer forms cladding modes.
(2)当光子晶体光纤被置于空气中或水中或其他折射率小于光子晶体光纤包层折射率的液体中时,包层光在包层与外部环境的界面处发生全反射,由于光子晶体光纤长度只有10-50mm,包层光能量可近似认为不损耗。 (2) When the photonic crystal fiber is placed in air or water or other liquids whose refractive index is lower than the refractive index of the photonic crystal fiber cladding, the cladding light is totally reflected at the interface between the cladding and the external environment, due to the photonic crystal The length of the optical fiber is only 10-50mm, and the light energy of the cladding can be considered as no loss.
(3)当光子晶体光纤一部分或全部被置于折射率大于光子晶体光纤包层折射率的液体(如食用色拉油)中时,包层光在包层与外部液体的界面处发生反射和折射,从而导致包层中光能量的衰减。 (3) When part or all of the photonic crystal fiber is placed in a liquid (such as edible salad oil) whose refractive index is greater than the refractive index of the photonic crystal fiber cladding, the cladding light is reflected and refracted at the interface between the cladding and the external liquid , resulting in attenuation of light energy in the cladding.
(4)被衰减后的包层光和能量不变的纤芯光到达反射膜时分别反射回光子晶体光纤包层和纤芯并反向继续传输。光纤包层光继续产生反射和折射。被测液体液位越高被折射出去的能量越多。综合(3)(4),本发明测量对象为折射率大于光子晶体光纤包层折射率的液体液位。 (4) When the attenuated cladding light and the core light with constant energy reach the reflective film, they are respectively reflected back to the cladding and core of the photonic crystal fiber and continue to transmit in reverse. Optical fiber cladding continues to reflect and refract light. The higher the liquid level to be measured, the more energy will be refracted. Combining (3) and (4), the measurement object of the present invention is the liquid level whose refractive index is greater than the refractive index of the photonic crystal fiber cladding.
(5)反射回来的光纤包层和光纤纤芯的光再次到达熔接点时,光子晶体光纤纤芯的光和光子晶体光纤包层光发生干涉,该干涉光在单模光纤中传输。 (5) When the reflected fiber cladding and fiber core light reaches the fusion point again, the photonic crystal fiber core light and photonic crystal fiber cladding light interfere, and the interference light is transmitted in the single-mode fiber.
(6)在产生干涉的两束光中,光子晶体光纤纤芯中的光不受外界液位的影响;但光子晶体光纤包层中的光因发生折射而使能量衰减,但其相位不发生变化。这样就影响了干涉信号的条纹对比度。液位越高,包层中光能量衰减越多,条纹对比度就越小,它们之间的变化关系是确定的。 (6) Among the two beams of light that interfere, the light in the core of the photonic crystal fiber is not affected by the external liquid level; but the light in the cladding of the photonic crystal fiber attenuates energy due to refraction, but its phase does not occur Variety. This affects the fringe contrast of the interference signal. The higher the liquid level, the more attenuation of light energy in the cladding, the smaller the fringe contrast, and the relationship between them is definite.
(7)干涉信号通过环行器由光谱分析仪读出。光谱分析仪的数据读入计算机,计算出干涉条纹对比度,就可测量被测液体液位。 (7) The interference signal is read out by the spectrum analyzer through the circulator. The data of the spectrum analyzer is read into the computer, and the contrast of the interference fringes is calculated to measure the liquid level of the measured liquid.
熔接点塌陷区域分光耦合原理(如图7): The principle of optical coupling in the collapsed area of the welding point ( as shown in Figure 7):
Z为光波传输距离,在Z=0处光波从单模光纤进入光子晶体光纤的塌陷区,单模光纤的基模发生衍射,模场变宽,模场直径MFD可由高斯光束近似估算。 Z is the light wave transmission distance. At Z=0, the light wave enters the collapse region of the photonic crystal fiber from the single-mode fiber, the fundamental mode of the single-mode fiber is diffracted, and the mode field becomes wider. The mode field diameter MFD can be approximated by a Gaussian beam.
(1) (1)
为单模光纤模场半径,约4.5μm ,n1是纯石英折射率1.46。通过65μm的塌陷区后,在波长为1550nm时MFD约扩大到Z=0处的1.5倍,约为13.5μm,而光子晶体光纤基阶芯模模场半径仅为3.5 μm。所以通过约65μm的塌陷区后会激发出基阶芯模和高阶包层模。两个受激模分别在光子晶体光纤纤芯和包层中传播,被反射模反射后又都回到熔接点,在这里两者发生干涉。干涉强度I由下式给出 The mode field radius of the single-mode fiber is about 4.5μm, and n1 is pure silica with a refractive index of 1.46. After passing through the collapse region of 65 μm, the MFD expands to about 1.5 times that at Z=0 at a wavelength of 1550 nm, which is about 13.5 μm, while the fundamental mode field radius of the photonic crystal fiber is only 3.5 μm. Therefore, after passing through the collapsed region of about 65 μm, the fundamental core mode and the higher-order cladding mode will be excited. The two excited modes propagate in the core and cladding of the photonic crystal fiber respectively, and after being reflected by the reflection mode, they both return to the splicing point, where the two interfere. The interference intensity I is given by
(2) (2)
其中,为光程差, I1 是纤芯中传播的光强,不受液位变化影响,I2 是包 in , is the optical path difference, I 1 is the light intensity propagating in the fiber core, which is not affected by the liquid level change, I 2 is the package
层中传播的光强,随被测液位的变化而变化。最大和最小光强由下面两式给出 The light intensity propagating in the layer varies with the measured liquid level. The maximum and minimum light intensities are given by the following two equations
(3) (3)
(4) (4)
(5) (5)
其中 ΔP 是最大最小光强对数差。 当液位在一定范围内变化时,ΔP 将随液位近似线性减小。从上式中还可以看出这种液位传感系统可以消除由于光源波动和光路干扰产生的误差。 where ΔP is the logarithmic difference between the maximum and minimum light intensities. When the liquid level changes within a certain range, ΔP will decrease approximately linearly with the liquid level. It can also be seen from the above formula that this liquid level sensing system can eliminate errors caused by light source fluctuation and optical path interference.
相关材料related materials
1、PCF型号SC-4.0-1040-46,具体参数 1. PCF model SC-4.0-1040-46, specific parameters
材料: 纯石英 Material: Pure Quartz
折射率:1.46 Refractive index: 1.46
芯径: 4.2 ± 0.5 μm Core diameter: 4.2 ± 0.5 μm
包层直径: 125 ± 3 μm Cladding diameter: 125 ± 3 μm
涂敷层直径: 245 ± 5μm Coating layer diameter: 245 ± 5μm
模场直径(MDF)1550nm: 3.4 ± 0.2 μm Mode Field Diameter (MDF) 1550nm: 3.4 ± 0.2 μm
衰减 1550 nm : < 2.2 dB/km Attenuation 1550 nm : < 2.2 dB/km
2、SMF-28具体参数 2. Specific parameters of SMF-28
芯径: 8.2 μm Core diameter: 8.2 μm
包层直径: 125 ± 1 μm Cladding diameter: 125 ± 1 μm
涂敷层直径: 250 ± 1μm Coating layer diameter: 250 ± 1μm
模场直径(MDF)1550nm: 9.2 ± 0.8 μm Mode field diameter (MDF) 1550nm: 9.2 ± 0.8 μm
3、色拉油折射率:1.47 3. Refractive index of salad oil: 1.47
4、光环行器(如图6) 4. Optical circulator ( as shown in Figure 6)
光环行器是一种三端口的非互易磁性器件,在光网络中用于信号的上、下载。端口F输入,端口G输出;端口G输入,端口H输出 An optical circulator is a three-port non-reciprocal magnetic device used for uploading and downloading signals in an optical network. Port F input, port G output; port G input, port H output
有益效果Beneficial effect
1、现有的光纤液位测量技术中,对于各种环境下液位感测是采用腐蚀后的光纤光栅或者拉锥光纤或者光纤错位熔接,不仅降低了光纤本身的机械强度,而且还存在温度交叉敏感效应,限制了它们的使用。利用光子晶体光纤迈克尔逊干涉仪来测量液位,可以解决以上问题。要求参与干涉的纤芯模和包层模的模场强度比在液位为零时大于等于1,这样随着液位的增加,干涉条纹对比度才会单调减小,同时为了得到尽可能大的测量范围,需要熔接时引入的损耗约为3dB。本专利使用SC-4.0(图1b)和单模光纤(SMF-28)熔接, SC-4.0有小孔的包层部分较小,熔接后的塌陷区较短,等于65μm,熔接过程引入的损耗为3dB。为了增强干涉信号,又为了防止镀膜时银进入包层小孔,预先用光纤熔接机对末端放电,使空气孔闭合后,在光子晶体光纤末端镀上50nm的银膜用来增强反射率。 1. In the existing optical fiber liquid level measurement technology, for liquid level sensing in various environments, corroded optical fiber gratings or tapered optical fibers or optical fiber dislocation fusion are used, which not only reduces the mechanical strength of the optical fiber itself, but also has temperature Cross-sensitivity effects limit their use. Using photonic crystal fiber Michelson interferometer to measure liquid level can solve the above problems. It is required that the mode field strength ratio of the core mode and the cladding mode participating in the interference is greater than or equal to 1 when the liquid level is zero, so that as the liquid level increases, the contrast of the interference fringe will decrease monotonously, and at the same time, in order to obtain the largest possible Measurement range, the loss introduced when welding is required is about 3dB. This patent uses SC-4.0 (Figure 1b) and single-mode fiber (SMF-28) for fusion splicing. The cladding part of SC-4.0 with small holes is smaller, and the collapse zone after fusion is shorter, equal to 65 μm. The loss introduced by the fusion process is 3dB. In order to enhance the interference signal, and to prevent silver from entering the cladding holes during coating, the end of the optical fiber fusion splicer is used to discharge in advance to close the air hole, and then a 50nm silver film is plated on the end of the photonic crystal fiber to enhance the reflectivity.
2、本传感器具有一般光纤传感器的优越性,不易受电磁干扰,传感器结构简单、尺寸小,适用于易燃易爆等恶劣环境。除此之外,本传感器还有很多独特的优点。(1)实现了全光纤迈克耳逊干涉仪,在光纤上实现了分光、传光、耦合光、反射、合束及干涉的功能,传感器结构微型化。(2)传感系统不受杂散光的影响。因为本传感系统测量的是干涉光谱信号,而杂散光与信号光不满足相干条件。因此,杂散光不影响测量结果。(3)传感系统不受温度的影响。因为温度的变化会影响纤芯光和包层光的相位差,使干涉条纹平移,但不会改变条纹对比度。而本传感系统测量的是干涉条纹对比度,因此温度变化不影响测量结果。(3)传感器制作方便,不需要腐蚀光纤,信号噪声小。总之,本传感器及其系统结构简单、微型化、全光纤化。利用光纤包层光反射、折射和光的干涉特性来测量液体液位,利用单模光纤、光子晶体光纤实现一个完整的微结构迈克耳逊干涉仪及液位传感器,系统灵敏度高、可靠性好。本传感器测量的液体折射率大于光子晶体光纤包层折射率。 2. This sensor has the advantages of ordinary optical fiber sensors, it is not susceptible to electromagnetic interference, the sensor structure is simple, the size is small, and it is suitable for harsh environments such as flammable and explosive. In addition, this sensor has many unique advantages. (1) The all-fiber Michelson interferometer is realized, and the functions of light splitting, light transmission, coupling light, reflection, beam combining and interference are realized on the optical fiber, and the sensor structure is miniaturized. (2) The sensing system is not affected by stray light. Because the sensing system measures interference spectrum signals, stray light and signal light do not satisfy the coherence condition. Therefore, stray light does not affect the measurement results. (3) The sensing system is not affected by temperature. Because the temperature change will affect the phase difference between the core light and the cladding light, the interference fringes will be shifted, but the fringe contrast will not be changed. However, this sensor system measures the contrast of interference fringes, so temperature changes do not affect the measurement results. (3) The sensor is easy to manufacture, does not need to corrode the optical fiber, and has low signal noise. In a word, the sensor and its system are simple in structure, miniaturized and fully optical. The liquid level is measured by using the light reflection, refraction and light interference characteristics of the fiber cladding, and a complete microstructure Michelson interferometer and liquid level sensor are realized by using single-mode fiber and photonic crystal fiber. The system has high sensitivity and good reliability. The refractive index of the liquid measured by the sensor is greater than the refractive index of the photonic crystal fiber cladding.
附图说明 Description of drawings
图1a是光子晶体光纤LMA-8 Crystal Fiber端面图; Figure 1a is the end view of photonic crystal fiber LMA-8 Crystal Fiber;
图1b是本传感器使用的光子晶体光纤SC-4.0端面图; Figure 1b is the end view of the photonic crystal fiber SC-4.0 used in this sensor;
图1c是光子晶体光纤SC-4.0小孔完全塌陷后的端面图; Figure 1c is the end view of the photonic crystal fiber SC-4.0 hole completely collapsed;
图2是光子晶体光纤液位传感器的结构图; Fig. 2 is a structural diagram of a photonic crystal fiber optic liquid level sensor;
其中:光纤涂敷层1、单模光纤包层2、单模光纤纤芯3、熔接点4、光子晶体光纤包层5、光子晶体光纤纤芯6、反射膜7、保护套8、端部固化胶9、固化胶10、过渡缓冲套11;
Among them: optical fiber coating 1, single-mode optical fiber cladding 2, single-mode
图3是光子晶体光纤液位传感系统的结构示意图; Fig. 3 is a structural schematic diagram of a photonic crystal fiber optic liquid level sensing system;
图4是光子晶体光纤液位传感系统中计算机获取的干涉信号光谱图; Fig. 4 is the interference signal spectrogram obtained by the computer in the photonic crystal fiber liquid level sensing system;
图5是用光子晶体光纤液位传感器测量色拉油液位与干涉条纹对比度的关系图; Fig. 5 is a relationship diagram between measuring salad oil liquid level and interference fringe contrast with photonic crystal fiber optic liquid level sensor;
图6是光环形器示意图,其中端口F输入,端口G输出;端口G输入,端口H输出; Fig. 6 is a schematic diagram of an optical circulator, wherein port F is input and port G is output; port G is input and port H is output;
图7是熔接点塌陷区域分光耦合原理示意图; Fig. 7 is a schematic diagram of the optical coupling principle in the collapsed area of the fusion point;
具体实施方式 Detailed ways
实施例1 Example 1
下面结合附图,以测量色拉油的液位为例来说明上述传感器及系统的实施。其他折射率大于光子晶体光纤包层的液体液位测量方法与之相同,不同之处在于不同折射率的液体液位传感的灵敏度不同。 The implementation of the above-mentioned sensor and system will be described below by taking the measurement of the liquid level of salad oil as an example in conjunction with the accompanying drawings. The liquid level measurement method of other liquids whose refractive index is larger than that of the photonic crystal fiber cladding is the same, the difference is that the sensitivity of liquid level sensing of different refractive indices is different.
一种光子晶体光纤液位传感器,其特征在于包括单模光纤SMF-28与光子晶体光纤SC-4.0,所述的单模光纤SMF-28与光子晶体光纤SC-4.0的始端熔接,光子晶体光纤的始端包层空气孔在熔接点闭合形成熔接点完全塌陷区域;用熔接机对光子晶体光纤末端放电形成末端塌陷区域,末端镀有反射膜;所述的熔接点塌陷区域长度等于65μm。其中, A photonic crystal fiber liquid level sensor is characterized in that it comprises a single-mode fiber SMF-28 and a photonic crystal fiber SC-4.0, the beginning of the single-mode fiber SMF-28 and the photonic crystal fiber SC-4.0 are fused, and the photonic crystal fiber The cladding air hole at the beginning of the fusion splicing point is closed to form a completely collapsed region of the fusion point; the end of the photonic crystal fiber is discharged by a fusion splicer to form a terminal collapsed region, and the end is coated with a reflective film; the length of the fusion point collapsed region is equal to 65 μm. in,
光子晶体光纤长度为20mm。 The photonic crystal fiber length is 20mm.
所述的反射膜为金属银膜,其厚度为50nm。 The reflective film is a metallic silver film with a thickness of 50nm.
在光子晶体光纤液位传感器外还设有保护套,距光子晶体光纤部分的保护套设有若干小孔。 A protective cover is also provided outside the photonic crystal fiber liquid level sensor, and several small holes are arranged on the protective cover away from the photonic crystal fiber part.
所述的单模光纤与保护套之间还设有过渡缓冲套。 A transitional buffer sleeve is also provided between the single-mode optical fiber and the protective sleeve.
其制作方法是: Its production method is:
(1)将一根单模光纤(SMF-28,石英光纤,其光纤芯径约8.2μm,光纤包层直径125μm)与一根光子晶体光纤(SC-4.0,其光纤芯径约4.2μm,光纤包层直径125μm)用光纤熔接机熔接,光子晶体光纤包层5的空气孔在熔接点4闭合形成完全塌陷区域,塌陷区域长度等于65μm,熔接点起到耦合器作用,将单模光纤的基模分成光子晶体光纤纤芯模和包层模,并且使两者的能量相当。 (1) Connect a single-mode fiber (SMF-28, silica fiber, with a core diameter of about 8.2 μm and a fiber cladding diameter of 125 μm) with a photonic crystal fiber (SC-4.0, with a fiber core diameter of about 4.2 μm, Fiber cladding diameter 125μm) is welded with a fiber optic fusion splicer. The air hole of the photonic crystal fiber cladding 5 is closed at the fusion point 4 to form a completely collapsed area. The length of the collapsed area is equal to 65 μm. The fusion point acts as a coupler, and the The fundamental mode is divided into the core mode and the cladding mode of the photonic crystal fiber, and the energy of the two is equal.
(2)用光纤涂敷机在熔接点周围包层涂敷上光纤涂敷层1。 (2) Use an optical fiber coating machine to coat the optical fiber coating layer 1 around the fusion point.
(3)在距熔接点20mm处用光纤切割刀切断光子晶体光纤,用光纤熔接机对末端放电使空气孔闭合后(图1c)在切断面上镀一层50nm的金属银膜作为反射膜7。 (3) Cut off the photonic crystal fiber with a fiber cutter at a distance of 20mm from the fusion point, and use a fiber fusion splicer to discharge the end to close the air hole (Figure 1c) and coat a layer of 50nm metallic silver film on the cut surface as a reflective film7 .
(4)去除反射膜和熔接点间的光纤涂敷层1。 (4) Remove the optical fiber coating layer 1 between the reflective film and the fusion point.
(5)将整根光子晶体光纤包括熔接点附近的单模光纤用固化胶10粘帖到一个带有很多小孔的保护套8内壁,固化胶10粘贴的位置靠近保护套的端部。 (5) Paste the entire photonic crystal fiber including the single-mode fiber near the fusion point to the inner wall of a protective sheath 8 with many small holes with curing glue 10, and the position where the curing glue 10 is pasted is close to the end of the protective sheath.
(6)在保护套的光纤引出端安装一个塑料过渡缓冲套11以避免光纤被折断。 (6) Install a plastic transitional buffer sleeve 11 at the optical fiber lead-out end of the protective sleeve to prevent the optical fiber from being broken.
(7)色拉油能够透过小孔与光子晶体光纤包层接触,保护套内的液位与色拉油的液位等液位。 (7) The salad oil can contact the photonic crystal fiber cladding through the small hole, the liquid level in the protective cover and the liquid level of the salad oil.
(8)传感器从色拉油中取出时,保护套内的色拉油从末端的小孔中流出。 (8) When the sensor is taken out from the salad oil, the salad oil in the protective cover will flow out from the small hole at the end.
(9)该保护层也可不用,直接将本传感器放在色拉油溶液中也能实现检测。 (9) The protective layer can also be omitted, and the sensor can also be detected directly by placing the sensor in the salad oil solution.
光子晶体光纤液位传感系统的构成如图3所示。波长1510nm-1590nm的ASE光源A通过光纤F1输入环行器B的F端口,经过环行器B的G端口和一段光纤F2,到达光子晶体光纤液位传感器C。在传感器C中,光能的一半在光子晶体光纤的纤芯中传输不受外界液位变化的影响,另一半光能被耦合到光子晶体光纤包层中去。光子晶体光纤包层和纤芯中的光到达反射膜时,又分别反射回包层和纤芯。包层中的光在光纤包层与色拉油的界面处产生反射和折射,在光纤包层与空气的界面处只有全反射,折射出去的光能受外界液体液位的影响。反射回的光再次到达熔接点时,光子晶体光纤包层光又被耦合入单模光纤的光纤芯,同时光子晶体光纤纤芯光也被耦合入单模光纤的光纤芯,单模光纤纤芯中的两束光产生干涉。返回的干涉信号光通过环行器B的H端口和光纤F3被传输到光谱分析仪D。光谱分析仪获取的干涉信号光谱数据送入计算机E,由计算机处理干涉信号光谱数据得到并显示色拉油液位。计算机获取的干涉信号光谱数据如图4所示为测量不同液位时的干涉光谱。其测量和计算过程实现标定传感器对色拉油液位的敏感系数,然后测试色拉油液位。标定的关系图如图5所示。测试时,本传感器被垂直放在被测色拉油中,传感系统中的计算机获取干涉信号光谱数据,并根据标定的敏感系数计算得到被测色拉油液位,从而实现色拉油液位的传感。在本实例中,测量色拉油液位的灵敏度0.84dB/mm,分辨率可达到0.05mm。 The composition of the photonic crystal fiber liquid level sensing system is shown in Figure 3. The ASE light source A with a wavelength of 1510nm-1590nm enters the F port of the circulator B through the optical fiber F1, passes through the G port of the circulator B and a section of optical fiber F2, and reaches the photonic crystal optical fiber liquid level sensor C. In sensor C, half of the light energy is transmitted in the core of the photonic crystal fiber without being affected by changes in the external liquid level, and the other half of the light energy is coupled into the cladding of the photonic crystal fiber. When the light in the cladding and core of the photonic crystal fiber reaches the reflective film, it is reflected back to the cladding and core respectively. The light in the cladding produces reflection and refraction at the interface between the fiber cladding and salad oil, and only total reflection at the interface between the fiber cladding and air, and the refracted light energy is affected by the external liquid level. When the reflected light reaches the splicing point again, the cladding light of the photonic crystal fiber is coupled into the fiber core of the single-mode fiber, and the core light of the photonic crystal fiber is also coupled into the fiber core of the single-mode fiber, and the core of the single-mode fiber The two beams of light interfere. The returned interference signal light is transmitted to the spectrum analyzer D through the H port of the circulator B and the optical fiber F3. The interference signal spectrum data obtained by the spectrum analyzer is sent to the computer E, and the interference signal spectrum data is processed by the computer to obtain and display the salad oil level. The interference signal spectrum data obtained by the computer is shown in Figure 4 as the interference spectrum when measuring different liquid levels. The measurement and calculation process realizes the calibration of the sensitivity coefficient of the sensor to the salad oil level, and then tests the salad oil level. The calibration diagram is shown in Figure 5. During the test, the sensor is placed vertically in the tested salad oil, and the computer in the sensing system acquires the spectral data of the interference signal, and calculates the measured salad oil level according to the calibrated sensitivity coefficient, so as to realize the transmission of the salad oil level. feel. In this example, the sensitivity of measuring the salad oil level is 0.84dB/mm, and the resolution can reach 0.05mm.
Claims (5)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN2010105181325A CN101957227B (en) | 2010-10-22 | 2010-10-22 | Photonic crystal fiber optic liquid level sensor and sensing system formed by same |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN2010105181325A CN101957227B (en) | 2010-10-22 | 2010-10-22 | Photonic crystal fiber optic liquid level sensor and sensing system formed by same |
Publications (2)
Publication Number | Publication Date |
---|---|
CN101957227A CN101957227A (en) | 2011-01-26 |
CN101957227B true CN101957227B (en) | 2012-01-04 |
Family
ID=43484690
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN2010105181325A Expired - Fee Related CN101957227B (en) | 2010-10-22 | 2010-10-22 | Photonic crystal fiber optic liquid level sensor and sensing system formed by same |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN101957227B (en) |
Families Citing this family (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102261924B (en) * | 2011-04-26 | 2013-02-27 | 南京信息工程大学 | A Fabry-Perot interference sensor based on solid-core photonic crystal fiber and its manufacturing method |
CN102778306A (en) * | 2012-07-13 | 2012-11-14 | 南京信息工程大学 | Refractive index and temperature sensor of photonic crystal fiber, manufacturing method and measuring system |
CN102865946B (en) * | 2012-09-11 | 2014-08-27 | 天津大学 | Photonic crystal fiber temperature sensing probe and measuring system thereof |
CN102928045B (en) * | 2012-11-26 | 2015-09-09 | 西北大学 | Optical fiber Michelson interference liquid level sensor |
CN103558663A (en) * | 2013-11-09 | 2014-02-05 | 哈尔滨工业大学 | S-shaped photonic crystal fiber taper sensor and preparing method thereof |
CN104089682B (en) * | 2014-07-18 | 2018-01-12 | 厦门大学 | A kind of liquid level detection device and its detection method |
CN104154968A (en) * | 2014-07-23 | 2014-11-19 | 中国计量学院 | Liquid level sensor on basis of fine-core tilted fiber bragg grating |
CN105157875A (en) * | 2015-06-19 | 2015-12-16 | 中国计量学院 | Temperature sensor based on Michelson interferometer having optical fiber and air ring cavity structure |
CN105806414B (en) * | 2016-04-26 | 2017-10-31 | 浙江大学 | Optical fiber Temperature Humidity Sensor, temperature and humidity sensing system and humiture demodulation method |
CN106989795A (en) * | 2017-03-10 | 2017-07-28 | 上海电机学院 | A kind of Hollow-Core Photonic Crystal Fibers liquid level sensor and its making, application method |
CN108120489A (en) * | 2017-11-24 | 2018-06-05 | 辽宁世达通用航空股份有限公司 | A kind of agricultural sprinkling liquid capacity sensor based on fiber F-P |
CN109738373A (en) * | 2019-01-22 | 2019-05-10 | 北京信息科技大学 | pH sensor based on photonic crystal fiber and its fabrication method |
CN110864762A (en) * | 2019-12-04 | 2020-03-06 | 武汉工程大学 | A submersible fiber optic liquid level meter without installation |
CN111289473A (en) * | 2020-03-11 | 2020-06-16 | 大连理工大学 | Steel corrosion sensor based on photonic crystal fiber probe |
CN112763024B (en) * | 2020-12-14 | 2022-08-12 | 北京遥测技术研究所 | Point type optical fiber liquid level sensor |
CN114279965A (en) * | 2021-12-30 | 2022-04-05 | 中南林业科技大学 | Mach-Zehnder interferometer photonic crystal fiber refractive index sensor and preparation method |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101303300A (en) * | 2008-05-27 | 2008-11-12 | 重庆大学 | Miniature optical fiber F-P sensor and manufacturing method, liquid tester based on sensor |
CN101368979A (en) * | 2008-10-13 | 2009-02-18 | 重庆大学 | Miniature all-fiber F-P acceleration sensor and its manufacturing method |
CN101561535A (en) * | 2009-05-21 | 2009-10-21 | 浙江大学 | Method for fusing hollow-core photonic crystal fiber and single mode fiber |
CN101650235A (en) * | 2009-09-11 | 2010-02-17 | 重庆大学 | Minitype optical fiber internal integrated optical fiber interference type temperature sensor and manufacturing method thereof |
-
2010
- 2010-10-22 CN CN2010105181325A patent/CN101957227B/en not_active Expired - Fee Related
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101303300A (en) * | 2008-05-27 | 2008-11-12 | 重庆大学 | Miniature optical fiber F-P sensor and manufacturing method, liquid tester based on sensor |
CN101368979A (en) * | 2008-10-13 | 2009-02-18 | 重庆大学 | Miniature all-fiber F-P acceleration sensor and its manufacturing method |
CN101561535A (en) * | 2009-05-21 | 2009-10-21 | 浙江大学 | Method for fusing hollow-core photonic crystal fiber and single mode fiber |
CN101650235A (en) * | 2009-09-11 | 2010-02-17 | 重庆大学 | Minitype optical fiber internal integrated optical fiber interference type temperature sensor and manufacturing method thereof |
Also Published As
Publication number | Publication date |
---|---|
CN101957227A (en) | 2011-01-26 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN101957227B (en) | Photonic crystal fiber optic liquid level sensor and sensing system formed by same | |
Wu et al. | Singlemode-multimode-singlemode fiber structures for sensing applications—A review | |
CN100437036C (en) | Fibre optic sensor for measuring temperature and refractive index of liquid contemporarily | |
CN205940607U (en) | Temperature and refracting index sensor based on multimode fiber intermode interference and FBG | |
CN102323239B (en) | Refractive index sensor based on asymmetric double-core optical fiber | |
CN102226725B (en) | Inner-wall waveguide long-time cycle fiber grating sensor | |
CN102269700B (en) | Capillary fiber refractive index sensor | |
CN101545851B (en) | Reflective optical fiber biochemical sensor based on long-period fiber grating and manufacturing method | |
CN111412938B (en) | Three-parameter measurement mixed structure interferometer sensor | |
CN102778306A (en) | Refractive index and temperature sensor of photonic crystal fiber, manufacturing method and measuring system | |
Niu et al. | Optical fiber sensors based on core-offset structure: A review | |
CN103852191B (en) | The fibre optic temperature sensor that a kind of refractive index is insensitive | |
Hu et al. | A narrow groove structure based plasmonic refractive index sensor | |
CN101303300A (en) | Miniature optical fiber F-P sensor and manufacturing method, liquid tester based on sensor | |
Zhang et al. | Fiber optic liquid level sensor based on integration of lever principle and optical interferometry | |
CN110927113A (en) | Fiber integrated hydrogen sensor and manufacturing method thereof | |
Chen et al. | Novel compact and low-cost ultraweak Fabry–Perot interferometer as a highly sensitive refractive index sensor | |
CN110954239A (en) | Temperature sensor based on double-core single-hole optical fiber | |
Deng et al. | Twisted tapered plastic optical fibers for continuous liquid level sensing | |
CN111208087B (en) | A kind of fiber optic humidity sensor based on thick cone and its working principle and preparation method | |
CN202041465U (en) | A Capillary Optical Fiber Refractive Index Sensor | |
CN101710065A (en) | Thin core optical fiber mode interferometer sensor | |
Feng et al. | Intensity-modulated liquid-level and temperature sensor based on cascaded air bubble and fiber Bragg grating interferometer | |
CN1746641A (en) | Optical fiber temperature measuring instrument and its measuring method | |
CN216385762U (en) | Sensor and sensing experimental device based on resonant reflection waveguide and Mach-Zehnder |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
C14 | Grant of patent or utility model | ||
GR01 | Patent grant | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20120104 Termination date: 20141022 |
|
EXPY | Termination of patent right or utility model |