Analysis of the applicability of singlemode optical fibers for measurement of deformation with distributed systems BOTDR

OPTICS AND OPTOELECTRONICS VOLUME: 14 |NUMBER: 4 |2016 |SPECIAL ISSUE Analysis of the Applicability of Singlemode Optical Fibers for Measurement of Deformation with Distributed Systems BOTDR Marcel FAJKUS, Jan NEDOMA, Lukas BEDNAREK, Jaroslav FRNDA, Vladimir VASINEK Department of Telecommunications, Faculty of Electrical Engineering and Computer Science, VSB–Technical University of Ostrava, 17. listopadu 15, 708 33 Ostrava, Czech Republic marcel.fa[email protected], [email protected], lukas.b[email protected], jarosla[email protected], vladimir.v[email protected] DOI: 10.15598/aeee.v14i4.1785 Abstract. Distributed optical fiber sensors allow monitoring physical effects across the whole cable. The paper presents results obtained from the performed tests and shows that single mode fibers can provide analyses of the deformation changes, when distributed optical systems BOTDR used. We used standard optical fiber G.652.D with primary and secondary protected layers and specialized cable SMC-V4 designed for this purpose. The aim was to compare the deformation sensitivity and determine which fiber types are the best to use. We deformed the fiber in the longitudinal and transverse directions and mechanically stressed in orthogonal directions to find how to localize optical fibers. They could be deployed in real use. For achieving optimal results of mechanical changes and acting forces, sensor fibers have to be located carefully. Keywords Deformation, distributed system, sensor, special cable, standard telecommunication fiber. 1. Introduction Distributed fiber optic sensors is a group of fiber-optic sensors. Distributed sensors enable the measurement of quantity along the entire length of optical fiber. The general principle of these systems is the phenomenon called light scattering. Based on the light scattering analysis, we distinguish several types of such systems. Rayleigh scattering is used for the measurement of attenuation profile of the optical fiber [1]. Raman scattering is possible to use for monitoring the temperature along the optical fiber [2] and Brillouin scattering can be used for measuring the temperature and deformation [3] and [4]. This article is focused on the measurement of deformation utilizing Brillouin Time Domain Reflectometry (BOTDR). The principle is based on the measurement of the stimulated Brillouin scattering. The frequency shift of Brillouin scattering is linearly dependent on the temperature and deformation. Distributed sensors are used in many areas of measurement, for example, for monitoring of the condition of building structures, the temperature distribution along the electrical cables, etc. Special optical cable SMCV4 is designed for measurement of deformation with BOTDR system. However, this cable is more expensive, and implementation of the cable is considerably expensive for the measurement of long distance. The alternative possibility is the use of standard telecommunications optical fiber, which is not recommended for these purposes. The disadvantage of standard optical fiber is a non-tight bond between the optical fiber itself and the secondary protection in the case of measurement of the deformation. For this reason, it is considered that the applied deformation is weakly transmitted to the optical fiber itself. Standard telecommunications optical fibers G.652.D can be used for the measurement of deformation, where there is not a big emphasis on accuracy of measurement, for example, in security systems. This combination offers less accuracy, but the main requirement is knowledge about a disruption of perimeter system. This solution represents a possible low-cost alternative solution of perimeter systems using BOTDR systems. The aim of this article is the comparison of sensitivity to deformation of these types of optical fiber and determining the suitability of these standard optical fibers for the measurement of deformation with distributed systems. c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 453 OPTICS AND OPTOELECTRONICS VOLUME: 14 |NUMBER: 4 |2016 |SPECIAL ISSUE 2. Distributed System BOTDR In practical applications, optical fiber is sticked on the surface of an analyzed structure. The optical fiber is mounted directly inside of the building structure for the analysis of construction. In this paper, we use of a special cable SMC-V4, because the emphasis is placed on the accuracy of measurement. Special cables, with higher tensile strength and better protection, are also more suitable for measurement of the terrain and soil layers [5]. The authors [6] and [7] show that it is possible to use different types of cables for measurement of deformation. BOTDR (Brillouin Optical Time Domain Reflectometry) operates on the principle of measurement of stimulated Brillouin scattering. Brillouin scattering arises due to the interaction of acoustic waves and pump of the light beam, under the condition of supercritical power of light passing through the optical fiber. The transmitted light is diffused according to the changes in the refractive index. The scattered light is shifted due to Doppler effect on frequency by an amount υB. This value is given by: υB=2nVa λ0 ,(1) where λ0is the wavelength of transmitted light, nrepresents the refractive index of the core of the optical fiber and Vadenotes the propagation velocity of acoustic waves within the optical fiber. The resultant value is given by: Va=rK σ,(2) where σis the density of the material and Kexpress module of volume compressibility. The value σis determined by the magnitude of deformation and temperature on the optical fiber itself. The strain response is defined as follows: υB(ε, n) = Cε1ε+Cε0,(3) where coefficient Cε1is 0.5 GHz/% and coefficient Cε0 is 10.87 GHz [8] for standard ITU-G.652 optical fiber at wavelength 1550 nm. Figure 1 shows a Brillouin frequency shift, which is linearly dependent on the applied deformation and temperature. The value of the magnitude of applied deformation and temperature is obtained by scan Brillouin frequency shift using the probing of light. The light is directed into the optical fiber from the opposite end. Experimental measurements were performed using a distributed system for the measurement of deformation and temperature DiTEST STA-R from Omnisens, Stokes components Brillouin Brillouin Rayleigh λ 0 Wavelength T, εT, ε Anti-Stokes components Fig. 1: Rayleigh and Brillouin scattering. which exploits the sensitivity of the Brillouin frequency shift for sensing of temperature and strain. This technique uses standard low-loss single mode optical fiber. The optical fiber offers the longest distance range with unrivaled performances and a compatibility with standard telecommunication components. The functionality principle consists of the frequency measurement of the Brillouin scattered light. The spatial resolution of 1 m is a distance of 20 km in the optical fiber, resolution 2 m is a distance 30 km, and value of resolution 3 m is a maximum length of optical fiber 50 km. The system contains two independent channels with a reach of 50 km. A step of measurement of 10 cm can be set for short segments of optical fibers in hundreds of meters. A maximum of measuring steps is limited to a value of 100 000 measurement points across the length of optical fiber. In Fig. 2, we can see how to measure the Brillouin frequency shift with a BOTDR. Pulsed light is introduced into the optical fiber (from one end of the optical fiber), and the power of spontaneous Brillouin backscattered light is then measured in the time domain using heterodyne detection. The frequency of the incident light slightly changes. Therefore, the same measurements 10.843 10.894 10.945 15 20 25 30 35 0 1 0.2 0.4 0.6 0.8 Brillouinafrequencya[GHz] Distancea[m] Normalizedapowera[-] Fig. 2: Principle of BOTDR strain measurement. c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 454 OPTICS AND OPTOELECTRONICS VOLUME: 14 |NUMBER: 4 |2016 |SPECIAL ISSUE are carried out to obtain the Brillouin spectrum repeatedly at many frequencies. The specific frequency, which indicates the peak power, is calculated by fitting the spectrum to a Lorentzian curve. It must be calculated at each point of the optical fiber. The strain is obtained from this frequency. The distance Ddefines a place, where the pulsed light is released into the position, where the scattered light is generated. D=cT 2n,(4) where nis the refractive index, cis the light velocity in a vacuum and Tis the time interval between receiving the scattered light and launching the pulsed light. 3. Experimental Setup The constructed preparation was used to deform of the optical fiber for experimental measurement (Fig. 3). The preparation consists of galvanized sheet with dimensions 100×100 cm. Sheet with glued optical fiber is affixed to the wooden frame. Subsequently, this sheet is bending from the unloaded state ’0’ (0◦) to the maximum bend ’10’ (180◦). Fig. 3: Equipment for deformation measurement. Bragg grating was used for the deformation assessment of glued optical fiber at preparation in Fig. 3 for various size of radius bending in the individual positions ’1’–’10’. Deformation was zero in position ’0’. Figure 4 shows the size of deformation at each position. Two types of standard telecommunications fibers G.652.D (in primary protection and in a tight secondary protection) were used for experimental measurements, and special optical cable SMC-V4 was also used. This cable is designed for the deformation Position 1 2 3 4 5 6 7 8 9 10 Deformation [ strain] 600 800 1000 1200 1400 1600 µ Fig. 4: Deformation of optical fiber with the Fiber Bragg grating glued on preparation for various size of radius bending in the individual positions ’1’–’10’. measurement. It provides the maximum sensitivity on deformation and the ability to detect very small deformations. Individual types of optical fibers were glued on the test sheet in the longitudinal and the transverse direction (Fig. 5) along its entire length. The directions were chosen based on previous research [9]. Polymer adhesive MAMUT Glue was used for gluing. Then measurements were carried out for each arrangement and each condition and each fiber, thus a total 600 repetitions. deformation a) b) Fig. 5: Arrangement of optical fiber. Distributed system BOTDR is based on measurement of Brillouin scattering, whose frequency is dependent on applied deformation. Figure 6 shows individual waveforms of Brillouin frequency depending on the distance of optical fiber for deformation at positions ’1’ to ’10’. Figure 6(a) shows the waveforms of Brillouin frequency for longitudinally mounted optical fiber G.652.D in the primary protection. Figure 6(b) shows the waveforms of Brillouin frequency for longitudinally mounted optical cable SMC-V4. In this cable, the optical fiber is characterized by the shifted Brillouin frequency towards lower frequencies (see waveform between 3 and 5 m in Fig. 6(b)). c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 455 OPTICS AND OPTOELECTRONICS VOLUME: 14 |NUMBER: 4 |2016 |SPECIAL ISSUE Distance [m] 6 7 8 9 10 Brillouin frequency [GHz] 10.85 10.9 10.95 (a) G.652.D in primary protection. Distance [m] 02468 Brillouin frequency [GHz] 10.5 10.6 10.7 10.8 10.9 (b) SMC-V4. Fig. 6: Dependence of Brillouin frequency on applied deformation. Following Fig. 7 (sef of 6 images) displays dependencies of the Brillouin frequency on deformation in positions ’1’–’10’ for all three types of optical fibers in the longitudinal and transverse configuration. Position 12345678910 Brillouin frequency [GHz] 10.89 10.9 10.91 10.92 10.93 10.94 G.652.D / primary / longtidunally Position 1 2 3 4 5 6 7 8 9 10 Brillouin frequency [GHz] 10.858 10.859 10.86 10.861 10.862 G.652.D / primary / transversally Position 12345678910 Brillouin frequency [GHz] 10.9 10.92 10.94 10.96 10.98 11 G.652.D / secondary / longitudinal Position 1 2 3 4 5 6 7 8 9 10 Brillouin frequency [GHz] 10.85 10.855 10.86 10.865 G.652.D / secondary / transverse Position 12345678910 Brillouin frequency [GHz] 10.55 10.6 10.65 10.7 10.75 10.8 SMC-V4 / longitudinal c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 456 OPTICS AND OPTOELECTRONICS VOLUME: 14 |NUMBER: 4 |2016 |SPECIAL ISSUE Position 1 2 3 4 5 6 7 8 9 10 Brillouin frequency [GHz] 10.4625 10.463 10.4635 10.464 10.4645 SMC-V4 / transverse Fig. 7: The dependence of Brillouin frequency on deformation in positions ’1’ to ’10’ for all types of optical fibers and the arrangement. Figure 8 shows the comparison of different configurations. The individual curves represent the average value of the measured data for each configuration and the type of optical fibers. Deformation [7strain] 800 1000 1200 1400 1600 Brillouin frequency shift [MHz] 10.4 10.6 10.8 11 G.652.D / primary / longitudinal G.652.D / primary / transverse G.652.D / secondary / longitudinal G.652.D / secondary / transverse SMC-V4 / longitudinal SMC-V4 / transverse Fig. 8: Comparison of individual configuration and types of optical fibers. A sensitivity of Brillouin frequency on deformation and the maximum change of deformation were calculated for shown arrangement (Tab. 1). 4. Conclusion The presented results show that the tested optical fibers have a small sensitivity to transverse deformation. This sensitivity reaches lower values than Tab. 1: The sensitivity of Brillouin frequency on the type of arrangement of the optical fiber during measurement of deformation and the maximum change of deformation. Sensitivity Max Brillouin Configuration change frequency (kHz/µstrain) (MHz) G.652.D/ primary/ 53.561 58.09 longitudinal G.652.D/ primary/ 0.981 1.064 transverse G.652.D/ secondary/ 90.688 98.356 longitudinal G.652.D/ secondary/ 0.459 0.497 transverse SMC-V4/ 221.952 240.72 longitudinal SMC-V4/ -0.733 -0.7995 transverse 1 kHz/µstrain. It can be stated that the tested types of optical fibers are not suitable for measurement of transverse deformations. The sensitivity of SMC-V4 is 4.15 times greater than the sensitivity of G.652.D in the primary protection, and 2.45 times greater than the sensitivity of G.652.D in tightly secondary protection in the case of longitudinal deformation. The ratio of sensitivity is 1.69:1 between the optical fiber G.652.D with tight secondary protection and primary protection. An optical cable SMC-V4 is characterized by shifted of typical Brillouin frequency to lower frequencies about 350 MHz. This article confirms further the possibility of using standard single-mode fiber for the measurement of deformation using apparatus DiTEST STA-R, which is based on measurement of the Brillouin frequency. However, there is the significant difference in sensitivity between the longitudinal and transverse effect of deformation, which is a hundred times larger in a longitudinal action than in a transverse action. The article confirms further the use of standard telecommunication fibers in security systems, where there is not a big emphasis on the measurement accuracy of deformation. According to the results, this combination offers less accuracy, but the primary requirement is knowledge about a disruption of perimeter system. This solution represents a possible low-cost alternative solution of perimeter systems using BOTDR systems. Acknowledgment This article was supported by projects Technology Agency of the Czech Republic TA03020439 and TA04021263 and Ministry of Education of the Czech Republic within the project no. SP2016/149. The Minc 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 457 OPTICS AND OPTOELECTRONICS VOLUME: 14 |NUMBER: 4 |2016 |SPECIAL ISSUE istry of Education has partially supported the research, Youth and Sports of the Czech Republic through grant project no. CZ.1.07/2.3.00/20.0217 within the frame of the operation program Education for competitiveness financed by the European Structural Funds and from the state budget of the Czech Republic. This article was supported too by project VI20152020008 (GUARDSENSE II). References [1] HAGEMANN, H. J., J. UNGELENK and D. U. WIECHERT. Optical time-domain reflectometry (OTDR) of diameter modulations in single mode fibers. 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In: 10th International Conference on Electronic Measurement &Instruments (ICEMI). Chengdu: IEEE, 2011, pp. 38–41. ISBN 978-14244-8158-3. DOI: 10.1109/ICEMI.2011.6037942. [9] FAJKUS, M., J. NEDOMA, S. KEPAK, J. JAROS, J. CUBIK, O. ZBORIL, M. NOVAK, and V. VASINEK. Effect of the geometric deformations on the Brillouin scattering in the standard single-mode optical fiber. In: Proceedings of SPIE 9889: Optical Modelling and Design IV. Bellingham: SPIE, 2016, pp. 1–6. ISBN 978-151060134-5. DOI: 10.1117/12.2239550. About Authors Marcel FAJKUS was born in 1987 in Ostrava. In 2009 he received Bachelor’s degree from VSB– Technical University of Ostrava, Faculty of Electrical Engineering and Computer Science, Department of Telecommunications. Two years later he received on the same workplace his Master’s degree in the field of Telecommunications. Currently, he is employee and Ph.D. student of Department of Telecommunications. He works in the field of optical communications and fiber optic sensor systems. Jan NEDOMA was born in 1988 in Prostejov. In 2012 he received Bachelor’s degree from VSB– Technical University of Ostrava, Faculty of Electrical Engineering and Computer Science, Department of Telecommunications. Two years later he received on the same workplace his Master’s degree in the field of Telecommunications. Currently, he is employed and Ph.D. student of Department of Telecommunications. He works in the field of optical communications and fiber optic sensor systems. Lukas BEDNAREK was born in 1988 in FrydekMistek. In 2011 he received Bachelor’s degree from VSB–Technical University of Ostrava, Faculty of Electrical Engineering and Computer Science, Department of Computer Science. Two years later he received Master’s degree in the field of Telecommunications on Department of Telecommunications. He is currently Ph.D. student, and he works in the field of optical communications and aging of the optical components. Jaroslav FRNDA was born in 1989 in Martin, c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 458 OPTICS AND OPTOELECTRONICS VOLUME: 14 |NUMBER: 4 |2016 |SPECIAL ISSUE Slovakia. He received his M.Sc. from the VSB– Technical University of Ostrava, Department of Telecommunications, in 2013, and now he is continuing his Ph.D. study at the same place. His research interests include Quality of Triple play services and IP networks. Vladimir VASINEK was born in Ostrava. In 1980 he graduated in Physics, specialization in Optoelectronics, from the Science Faculty of Palacky University. He was awarded the title of RNDr. at the Science Faculty of Palacky University in the field of Applied Electronics. The scientific degree of Ph.D. was conferred upon him in the branch of Quantum Electronics and Optics in 1989. He became an associate professor in 1994 in the branch of Applied Physics. He has been a professor of Electronics and Communication Science since 2007. He pursues this branch at the Department of Telecommunications at VSB–Technical University of Ostrava. His research work is dedicated to optical communications, optical fibers, optoelectronics, optical measurements, optical networks projecting, fiber optic sensors, MW access networks. He is a member of many societies: OSA, SPIE, EOS, Czech Photonics Society; he is a chairman of the Ph.D. board at the VSB–Technical University of Ostrava. He is also a member of habitation boards and the boards appointing to professorship. c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 459