Rapid and accurate detection of hydrogen in anaerobic condition is more and more important for the safe production and operation of hydrogen energy. A novel fiber hydrogen sensor based on Pd/Ta composite film coating on π-shifted fiber Bragg grating is proposed and its sensing performance is evaluated experimentally. Due to the narrow reflective peak of π-shifted fiber Bragg grating, the proposed sensor has, shown higher accuracy on wavelength shift tracing. A Pd/Ta composite film was deposited on the side of π-shifted fiber Bragg grating by magnetron sputtering process. Compared with the grating hydrogen sensors of other Pd-based composite films, the hydrogen sensitivity and response time of the Pd/Ta composite film coated sensors with different thickness of sensing layer have been improved greatly. When the hydrogen concentration is 1%, The wavelength shifts of π-shifted fiber Bragg grating of Pd/Ta membrane with thicknesses of 100 nm, 200 nm, 300 nm and 800 nm are 16, 31, 50 and 115 pm, respectively, and the response time are 63, 71, 109 and 150 s, respectively. A longtime testing of the sensor proves that the sensor has good long-term stability and repeatability. The proposed hydrogen sensor with Pd/Ta composite film has great potential in the quasi-distributed monitoring of hydrogen leakage in hydrogen generation, refueling stations, and so on.
The correlation between reflected light intensity and hydrogen concentration is the basis of the end-face type hydrogen sensor with WO3 coating. However, the changes of optical propertiesofWO3 under different hydrogen concentrations have not been fully investigated, and its hydrogen sensitivity mechanism is still unclear, which restricts the improvement and optimization of hydrogen sensing performance. Therefore, the relationship between hydrogen concentration and Refractive Index (RI) of WO3 is established in this paper to explore the hydrogen sensitive mechanism. The experimental results show that the RI of WO3 changes when hydrogen is introduced, and the RI varies under different hydrogen concentration. Since there is a certain mathematical relationship between the RI value and the reflectivity of the films, the RI changes measured by ellipsometer is further verified by the intensity-tracing experiments results. Hence, we can clarify that the hydrogen sensitivity mechanism of WO3 is related to its RI changes under different hydrogen concentration, which will provide a basis for the further research and applications.
As one of the cleanest energy sources in the 21st century, the development of hydrogen energy has attracted the attention of all countries in the world, so the monitoring of hydrogen leakage has become a current research focus. This study demonstrates a novel hydrogen sensor that combines a planar polymer grating with a Pd/Ni hydrogen-sensitive material that takes advantage of the hydrogen-absorbing expansion properties of Pd to cause the central wavelength drift of Planar Polymer Bragg Grating (PPBG) by strain transformation. The experimental results show when the hydrogen concentration is 0.3%, 0.6% and 1%, the wavelength shift of the sensor is 50 pm, 85 pm and 110 pm respectively, and the response time is approximately 30 seconds. This hydrogen sensor has the advantages of high sensitivity, low cost and compact structure, leading to great potential in industrial applications.
A hydrogen and humidity simultaneous measurement system based on an integrated FBG sensor is proposed. Experimentally results indicate the sensor shows a high degree of hydrogen discrimination ranging from 100ppm-8000ppm and a high degree of humidity discrimination ranging from 20% - 80%, along with the high performance of anti-mutual interference of hydrogen and humidity.
A fiber-optic carbon monoxide (CO)-sensing system with high sensitivity was proposed by combining Fabry–Perot interferometer (FPI) sensor with sensing material Au/ZnO. The sensitivity is 814 pm / % within the CO concentration range of 0% to 4%. The FPI sensor was fabricated by inserting single-mode fiber into a partially polymer-filled glass capillary to form an air cavity; the length of the air cavity is 76.83 μm. The temperature sensitivity of the FPI is −2.7 nm / ° C, which provides better conditions for measurement of CO. The catalyst Au/ZnO was prepared by coprecipitation, which could catalyze the oxidation of CO at ambient temperature and humidity. X-ray diffraction and scanning electron microscope analysis were employed to reveal the crystalline structure and morphology of the catalyst. To eliminate the influence of ambient temperature change on the accuracy of the concentration test, a fiber Bragg grating with central wavelength of 1550.24 nm was introduced in the experimental setup for the temperature compensation.
Optical fiber hydrogen sensing system based on weak fiber Bragg grating (WFBG) array deposited with palladium (Pd) film is proposed and experimentally demonstrated. For multi-point measurement, three hydrogen WFBG sensors array are weld in a single optical fiber. A time-division multiplexing (TDM) interrogation system is employed to demodulate the sensing array. Sensing experiments to different hydrogen concentrations ranging from 0 to 3.6% are conducted, and the results show good agreement with standard FBG technology. Due to its strong multiplexing capability of weak FBG, the system is possible to integrate thousands of WFBG hydrogen sensors in a single optical fiber.
A novel optic fiber hydrogen sensor is proposed in this paper. Two Bragg gratings with different reflectivity were written in single mode fiber with phase mask method by 248 nm excimer laser. The end-face of singe mode fiber was deposited with WO3-Pd-Pt multilayer films as sensing element. The peak intensity of low reflectivity FBG is employed for hydrogen characterization, while that of high reflectivity FBG is used as reference. The experimental results show the hydrogen sensor still has good repeatability when the optic intensity in the fiber is only 1/3 of its initial value. The hydrogen sensor has great potential in measurement of hydrogen concentration.
A fiber refractive index sensor based on porous alumina is fabricated by pasting porous alumina film with 42.36μm on single mode fiber tip using the UV-cured adhesive. Experimental results show that the proposed sensor has a very high correlation with glycerine concentration (0.0%~80.0%) with correlation coefficient of 99.771%. Its sensitivity and resolution was measure to be 99.771%, 154 nm/RIU and 1×10-4 respectively when the refractive index changes from 1.333 to 1.443.
A novel hydrogen sensor based on Pd/Ni co-sputtered coating on micro fiber Bragg grating (MFBG) is proposed and experimentally demonstrated. The microfiber is stretched uniformly and the Bragg grating is directly inscribed on the microfiber without hydrogen loading using 193 nm ArF excimer laser and a phase mask. Palladium and nickel coatings are co-sputtered on the micro fiber Bragg grating for hydrogen sensing. The MFBG hydrogen sensors are characterized concerning their response to the hydrogen, ambient temperature and ambient refractive index, respectively. The performance of the proposed MFBG hydrogen sensor is obviously enhanced, especially when compared to standard FBG hydrogen sensors.
A miniaturized fiber tip Fabry-Perot interferometer (FPI) with Pt/WO3 coating was demonstrated as a hydrogen sensor.
The air-cavity of FPI was formed by inserting a single mode fiber (SMF) into a partially polymer-filled glass capillary,
which was highly sensitive to temperature. A layer of Pt/WO3 was coated on the glass capillary of the FPI serving as a reaction heater upon hydrogen exposure. The heat locally raised the FPI temperature, which led to the wavelength shift of interference spectrum. The average wavelength shift of two interference dips was -20.3 nm upon exposure to ~20000 ppm hydrogen concentration. The hydrogen sensitivity of the sensor was estimated to be better than 1 pm/ppm.
A novel method was proposed to improve hydrogen sensitive performance of fiber Bragg grating (FBG) hydrogen sensor. The hydrogen performance of the sensor can be greatly improved by combing Pt/WO3 composite film annealed under 315°C for 1 h and temperature sensitive FBG. At room temperature of 25°C, FBG coated with Pt/WO3 composite film has 536 pm wavelength shift towards 10000 ppm hydrogen, and hydrogen detection threshold of FBG hydrogen sensor can reach to 200 ppm. The hydrogen performance of FBG hydrogen sensor was studied under different humidity, and ambient humidity has little effect on the hydrogen performance of FBG hydrogen sensor.
In this paper, a femtosecond (fs) laser fabricated fiber in-line micro Michelson interferometer (MI) with palladium (Pd)
film deposited on the fiber end face for hydrogen detection is proposed and demonstrated. Beam Propagation Method
(BPM) is used to analyze the influence of refractive index (RI) of Pd film on reflection spectrum. As for the
experimental results, the variation of optical power and shift of interference peak wavelength are -4.904 dBm and -4.2
nm respectively with the increase of hydrogen concentration from 0% to 16%. The developed system has high potential
in hydrogen sensing with high sensitivity.
Pd/Ag and Pd/Y composite films were deposited on the side-face of side-polished fiber Bragg grating (FBG) as sensing
elements with magnetron sputtering process. Compared to standard FBG coated with same hydrogen sensitive film,
side-polished FBG significantly increase the sensor's sensitivity. When hydrogen concentration is 4% in volume
percentage, the wavelength shifts of side-polished FBG sputtered with Pd/Ag and Pd/Y are 18 and 23 pm respectively.
The experimental results show the hydrogen sensor coated with Pd/Y composite film has higher sensitivity and quicker
response rate, and the sensor's hydrogen response is reversible. The side-polished FBG hydrogen sensor with Pd-based
composite films has great potential in measurement and monitor of hydrogen concentration.
A hydrogen sensor based on side-polished fiber Bragg grating (FBG) coated with Pd thin film by magnetron sputtering is
proposed. Hydrogen concentration is correlated with the shift of FBG central wavelength, since refractive index change
in hydrogen sensitive Pd coating deposited on side-polished FBG affects the effective refractive index of FBG, and
therefore Bragg wavelength is shifted. Experimental results demonstrate that FBG wavelength shifts to lower wavelength
as the hydrogen concentration increases. The proposed optical fiber hydrogen sensor shows 15pm wavelength shift in
0.01% volume percentage of hydrogen concentration, and totally 246pm offset exists in pure hydrogen environment.
A novel optical fiber magnetic sensor based on magnetic fluid is proposed in this paper. Stable nano-particle CoFe2O4magnetic fluid was synthesized firstly; the CoFe2O4 magnetic fluid was injected in capillaries containing side-polished
fiber Bragg grating (SPFBG) as sensing element. The reflected Bragg wavelength was changed by varying the magnetic
field which is perpendicular to the axial of SPFBG. Magnetic field sensing experiment show that 35pm of wavelength
shift at a magnetic field intensity of 16mT.
A novel optical fiber humidity sensor using polyvinylidene fluoride (PVDF) as sensitive material was proposed in this paper. Three-layer coating was deposited on the end-face of optical fiber, which constructs an extrinsic Fabry-Perot (F-P) interference structure. Ag layer deposited by DC magnetron sputtering was used as mirror layer in the F-P interference structure. PVDF layer was realized with Czochralski method as F-P cavity. Simulation was performed using data fitting to analysis the relevant parameters on sensor performance. Experimental result shows the interference fringe shifts to longer wavelength when relative humidity increases. The fringe shifted 2.4nm with a good linearity response when relative humidity increases from 11% to 97%. The linearity of interference fringe shift to relative humidity was 0.98415, the response time was less than 1min.
Two kinds of self-loading Farby-Perot (F-P) fiber sensors were prepared by creating micro-grooves on side-face of
single mode fiber-28 (SMF-28) and photonic crystal fiber (PCF) with 157 nm excimer laser. Self-loading F-P
interference fringe shifts were measured under different temperature, stress and alcohol solution. Temperature sensing
experiments show that the sensitivity of PCF and SMF F-P sensors are 0.0580nm/°C and 0.0535nm/°C when the
temperature ranges from 30 °C to100 °C. The interference fringe shifts of PCF and SMF F-P sensors are 1.6 nm and 2.2
nm when they were loaded with 80 μm elongation along fiber axis, which correspond to stress sensitivity of 1.41pm/με
and 1.50pm/με respectively. The interference fringe shifts of the SMF F-P sensor and the all-solid PCF sensor are
0.4775nm and 0.3490nm when the quality percentage of alcohol changes from 0 to 99.99%.
Access to the requested content is limited to institutions that have purchased or subscribe to SPIE eBooks.
You are receiving this notice because your organization may not have SPIE eBooks access.*
*Shibboleth/Open Athens users─please
sign in
to access your institution's subscriptions.
To obtain this item, you may purchase the complete book in print or electronic format on
SPIE.org.
INSTITUTIONAL Select your institution to access the SPIE Digital Library.
PERSONAL Sign in with your SPIE account to access your personal subscriptions or to use specific features such as save to my library, sign up for alerts, save searches, etc.