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Polymers 2013, 5(1), 45-55; doi:10.3390/polym5010045
Abstract: Pd doped WO3 fibers were synthesized by electro-spinning. The sol gel method was employed to prepare peroxopolytungstic acid (P-PTA). Palladium chloride and Polyvinyl pyrrolidone (PVP) was dissolved in the sol Pd:WO3 = 10% molar ratio. The prepared sol was loaded into a syringe connected to a high voltage of 18.3 kV and electrospun fibers were collected on the alumina substrates. Scanning electron microscope (SEM), X-ray powder diffraction (XRD) and X-ray photoelectron spectroscopy (XPS) techniques were used to analyze the crystal structure and chemical composition of the fibers after heat treatment at 500 °C. Resistance-sensing measurements exhibited a sensitivity of about 30 at 500 ppm hydrogen in air, and the response and recovery times were about 20 and 30 s, respectively, at 300 °C. Hydrogen gas sensing mechanism of the sensor was also studied.
Hydrogen burns cleanly without releasing pollutants or greenhouse gases and therefore, in recent years, more attention has been paid to hydrogen as an excellent candidate for fossil fuel replacement in household and transportation applications. However, hydrogen is a highly flammable fuel with a wide combustion range of 4%–75%. Besides, it has a large diffusion coefficient of 0.61 cm2/s in air. Therefore, detection and leakage control of this gas is a challenging subject. Today, development of a hydrogen sensor with negligible power consumption and high stability, sensitivity and fast response is desired.
Reports of various technologies for hydrogen sensing include FETs [1,2], optical fibers [3,4], thermoelectric [5,6], Schottky diodes [7,8,9], surface acoustic wave devices [10,11] and metal oxides [12,13,14,15,16,17]. Metal oxide sensors are under intensive development and have been studied for decades [18,19]. In metal oxide sensors, the electrical resistance of the film changes when exposed to a target gas. Also, among metal oxides, WO3 is widely used to detect many gases like H2, H2S, NO2 and VOC [20,21,22,23]. Moreover, it has been shown that the addition of an appropriate amount of noble metal additives promotes chemical reactions by reducing activation energy between the surface of metal oxide and target gas. Also, this increases the response and selectivity as well as decreasing the maximum working temperature of the sensors. For hydrogen sensors, modification of metal oxides, especially WO3, by metal additives such as Pt, Pd, or Au, using different techniques is under intensive investigation [24,25,26,27,28,29,30,31].
It is known that gas absorption depends on the surface area, which is affected by the preparation method. Increasing the surface to volume ratio to enhance gas sensing properties is currently under development by introducing different nanostructures such as nanowires, nanorods, nanobelts and nanofibers. Nanofibers have high density of surface sites that make them excellent candidates for gas sensing applications .
Among different fabrication methods, electrospinning is a simple and cost effective method for preparing one dimensional materials. Recently, several researches have reported fabrication of metal oxide nanofibers [33,34,35,36,37,38,39] in which metal oxide nanoparticles can be added to a polymer matrix to make nanocomposite fibers. Heat treatment removes polymer and leaves metal oxide material with fiber shape.
Metal oxide fibers could be synthesized by combining sol-gel and electrospinning methods. Adding catalysts to the solution (sol) produces nanofibers with improved catalytic properties for selective gas detection at lower temperatures. Polymer matrix can be decomposed through heat treatment and leaves metal oxide fiber with lengths from several hundred nanometers to few micrometers.
Preparing one dimensional WO3 fibers by sol-gel method was first reported by Lu et al. . Others used pure WO3 fiber for detecting ammonia, NO2 and CO gasses [41,42]. In our previous work , the sensitivity of both pure and Pd-modified WO3 thin films was measured towards hydrogen as a function of operating temperatures in the range of 30 °C to 350 °C. A systematic increase in sensitivity was observed for the modified films in the whole temperature range. The sensitivity increased due to a reduction of the activation energy between the WO3 surface and the hydrogen gas in the presence of Pd (PdO). It was seen that the sensitivity of Pd:W = 10% films have considerable amounts at room temperature and the working temperature (the temperature which has maximum sensitivity) decreased by increasing the Pd concentrations.
Since high response and recovery times were observed at low working temperatures. Given the results of our previous experiments on Pd modified WO3 films, we decided to study structure effect on modification of sensing behavior. Therefore, a combination of electrospinning and the sol gel method was studied to compare the result of the sensing behavior of Pd:WO3 thin film with the electrospun Pd doped WO3 nanofiber samples with the same ratio (Pd:W = 10%). In this work, we prepared WO3 nanoparticles by the sol-gel method and then Pd and PVP were added to the sol. To remove polymer and make WO3 nanoparticles with fiber shape, samples were annealed in air at 500 °C for 1 h. The Pd doped WO3 nanofibers showed fast response time and high sensitivity toward hydrogen gas at low temperature.
2. Experimental Section
In our sol-gel route, Peroxopolytungstic acid (P-PTA) sol was prepared according to the Kudo route . Five grams of tungsten wire and 20 mL of H2O2 (30%) was stirred at room temperature for 48 h until the whole tungsten wire was dissolved. Unreacted H2O2 was removed by using platinum net. Then 20 mL ethanol was added and the solution was heated at 80 °C which resulted in a sol color change from clear to orange.
For the activation process we used Pd catalyst. Since in our previous report, we obtained best sensitivity for Pd:W = 10% molar ratio , we chose this ratio for adding PdCl2 salt (Merk) directly to the P-PTA sol.
To fabricate fibers, 1.0 g polyvinyl pyrrolidone (PVP) (Aldrich) was added into the P-PTA sol and was stirred for one day. The resulting solution was loaded into a plastic syringe and its needle was connected to a high-voltage DC supply up to 30 kV. A voltage of 18.3 kV was applied between the needle and grounded target. Al2O3 substrates were placed on a piece of flat aluminum with 20 cm distance from the tip of the needle to collect fibers. The prepared samples were annealed in air at 500 °C for 1 h.
X-ray powder diffraction (XRD) analysis was recorded by a Philips X'pert instrument operating with CuKα radiation (λ = 1.54178 Ǻ) at 40 kV/40 mA. A Philips XL30 model Scanning electron microscope (SEM) was used to obtain the SEM images. For the X-ray photoelectron spectroscopy (XPS) experiment, an Al anode X-ray source was employed with a concentric hemispherical analyzer (Specs model EA10 plus) to analyze the energy of the emitted photoelectrons. Gas sensing properties of the as-fabricated sensor were measured using a static test system. A data logger was used to collect the data and the whole system was automatically controlled by computer.
For measuring the electrical resistance, Au/Ti comb-like interdigitated electrodes with 150 nm thickness were evaporated on the sample surface through a mask. The samples were placed in a small stainless steel chamber with several electrical feed-through, gas inlet and gas outlet. For measuring sensitivity, a constant dc voltage of 5 V was applied to the circuit; including the sensor in series with a constant resistor. Voltage variation across the resistor was measured. During the measurements, the fibers were warmed by a heater located on the back of the substrates. We used dry air as the reference gas and hydrogen as the target gas. Sensitivity was defined as S = (Vrg – Vra)/Vra, where Vrg and Vra are the sensor voltage in the presence and absence of hydrogen, respectively. The measurement setup consists of mass flow controllers and a data acquisition system for recording resistance changes. We define the response time as the time taken for the sensor’s resistance to undergo a 90% variation with respect to its equilibrium value and recovery time as the time taken to achieve 60% variation to reach its initial value in air after the removal of H2. The gas sensing performance was tested at hydrogen concentration of 500 ppm in the range of 30 °C to 300 °C.
3. Results and Discussion
3.1. Structure Analysis
SEM images of as-spun PVP composite fibers and the sintered fibers at 500 °C for 1 h are displayed in Figure 1a,b, respectively. Figure 1a shows the used Aluminum foil surface and some PVP composite fibers with an average diameter of about 500 nm. The heating process compresses the fibers and reduces their average thickness to about 150 nm while keeping their morphology as is shown in Figure 1b. Heat treatment at 500 °C removes the polymer and leaves metal oxide material with fiber shapes. SEM images show continuous fibers with lengths of several tens micrometers. By electrospinning, a huge number of fibers electrospun over the substrate and form as a film. To observe better by SEM, we made a sample with low density fibers (Figure 1a,b). Figure 1c shows another sample with high density of fibers (sample for gas sensing experiments). Both high fibrous surface area as well as high porosity increase effective sensitive surface area.
As presented in Figure 2, heat treatment at 500 °C resulted in the formation of crystals of both monoclinic WO3 and oxidized Pd. The evidence of PdO after annealing can be observed by XPS analysis. Data in Figure 3a indicates that the surface of the annealed Pd doped WO3 nanofiber is composed of tungsten, oxygen, carbon contamination, and small amounts of palladium. Figure 3b, shows the peaks related to palladium oxide formation after the annealing process.
3.2. Hydrogen Sensing Measurements
Hydrogen sensing properties of the Pd-modified WO3 samples were investigated while they were exposed to 500 ppm H2 at different operating temperatures. Figure 4 shows the changes in the voltage of a series resistor vs. time (transient response). The used electrical circuit is shown in the inset of Figure 4. It presents fast response and recovery times of about 20 and 30 s, respectively.
We measured the sensitivity of the samples as a function of operating temperature in the range of 75 °C to 300 °C. As shown in Figure 5, the sensitivity is noticeable at a temperature of about 75 °C and it is enhanced by increasing the operating temperature to 300 °C. This high sensitivity may be attributed to the reduction of the activation energy between the WO3 surface and hydrogen gas in the presence of Pd (PdO).
Response and recovery times of the Pd-modified WO3 fiber for 500 ppm hydrogen are presented in Figure 6. It presents a decaying behavior with considerable fast response and recovery times at high temperatures (300 °C). At low working temperature the response time is higher due to slow desorption of the formed water molecules on the surface especially at temperatures below 100 °C.
Our results demonstrated faster response and recovery times in the order of 160–190 s for low temperature sensing which is so considerable compare to 60 min recovery time for Pd:WO3 = 10% in the form of thin film . It can be attributed to the facilitate occupancy and desorption of H2 molecules at grain boundaries on the large surface area of nanofibers in a porous network. However, the obtained results of the response magnitudes and the working temperature are not as good as our previous work on thin film sensors.
3.3. Hydrogen Sensing Mechanism
The WO3 fibers have been made of small grains and grain boundary barriers are existed between neighboring grains located in a fiber structure. This structure has an increased surface area as well as providing electronic transmission channels for electron transferring between WO3 particulates. Since WO3 nanofibers in this study are continuous with WO3 grains, we expect sensing mechanism of the single WO3 fiber is principally similar to that of metal oxide films. So, grain size has important effect on sensing performances [44,45,46]. However, despite fibers being continuous media, there are a great number of fiber to fiber connections, where electron current passing through these connection potential barriers has an important role in total current passing through the fibers’ film.
In addition, regarding our previous work , presence of Pd makes a systematic increase in the sensitivity in the whole temperature ranges. This can be attributed to the effect of Pd catalyst in performing electronic sensitization mechanism and reducing the activation energy between the WO3 surface and the hydrogen gas . As shown here in Figure 7a and b, the O2 molecules chemisorb and dissociate on the surface of the WO3 grains. Then they trap and extract electrons from the conduction band of n-type semiconductor (WO3) due to their high electron affinity. A depletion or space-charge region develops on the surface of the grain. This increases the potential barrier height between neighboring grains and also widens it, which is called energy band bending as shown in Figure 7a. This makes electron transferring between grains difficult which decreases the conductance of the fiber. By exposing fibers to hydrogen gas, reaction with the adsorbed oxygen molecule takes place. This re-injects captured electrons to the depletion region and the reverse effect will take place (Figure 7b).
Pd doped WO3 fibers were synthesized by combining electrospinning and sol-gel methods and were characterized by SEM, XRD and XPS methods. The sensor fabricated from these fibers exhibited high sensitivity and rapid response/recovery to hydrogen at 300 °C. The highest sensitivity was about 30 when the sensor was exposed to 500 ppm, and the response and recovery times were about 20 and 30 s, respectively. The WO3 fiber sensors showed fast response times toward hydrogen even at low operating temperatures. These results demonstrate that Pd doped WO3 fibers can be used as the sensing material for fabricating high performance hydrogen sensors. Besides, hydrogen gas sensing mechanism of the sensor was studied and a model proposed.
- Yamaguchi, T.; Kiwa, T.; Tsukada, K.; Yokosawa, K. Oxygen interference mechanism of platinum–FET hydrogen gas sensor. Sens. Actuators A Phys. 2007, 136, 244–248. [Google Scholar] [CrossRef]
- Higuchi, T.; Nakagomi, S.; Kokubun, Y. Field effect hydrogen sensor device with simple structure based on GaN. Sens. Actuators B Chem. 2009, 140, 79–85. [Google Scholar]
- Villatoro, J.; Moreno, D.L.; Monzón-Hernández, D. Optical fiber hydrogen sensor for concentrations below the lower explosive limit. Sens. Actuators B Chem. 2005, 110, 23–27. [Google Scholar]
- Slaman, M.; Dam, B.; Schreuders, H.; Griessen, R. Optimization of Mg-based fiber optic hydrogen detectors by alloying the catalyst. Int. J. Hydrog. Energy 2008, 33, 1084–1089. [Google Scholar]
- Nishibori, M.; Shin, W.; Izu, N.; Itoh, T.; Matsubara, I.; Yasuda, S.; Ohtani, S. Robust hydrogen detection system with a thermoelectric hydrogen sensor for hydrogen station application. Int. J. Hydrog. Energy 2009, 34, 2834–2841. [Google Scholar]
- Huang, H.; Luan, W.; Zhang, J.S.; Qi, Y.S.; Tu, S.T. Thermoelectric hydrogen sensor working at room temperature prepared by bismuth–telluride P–N couples and Pt/g-Al2O3. Sens. Actuators B Chem. 2008, 128, 581–585. [Google Scholar] [CrossRef]
- Ito, K.; Kojima, K. Hydrogen detection by Schottky diodes. Int. J. Hydrog. Energy 1982, 7, 495–497. [Google Scholar] [CrossRef]
- Tang, W.M.; Lai, P.T.; Xu, J.P.; Chan, C.L. Enhanced hydrogen sensing characteristics of MI SiC Schottky-diode hydrogen sensor by trichloroethylene oxidation. Sens. Actuators A Phys. 2005, 119, 63–67. [Google Scholar] [CrossRef]
- Tsai, T.H.; Chen, H.I.; Lin, K.W.; Hung, C.W.; Hsu, C.H.; Chen, L.Y.; Chu, K.-Y.; Liu, W.-C. Comprehensive study on hydrogen sensing properties of a Pd–AlGaN-based Schottky diode. Int. J. Hydrog. Energy 2008, 33, 2986–2992. [Google Scholar]
- Ippolito, S.J.; Kandasamy, S.; Kalantar-Zadeh, K.; Wlodarski, W. Layered SAW hydrogen sensor with modified tungsten trioxide selective layer. Sens. Actuators B Chem. 2005, 108, 553–557. [Google Scholar]
- Jakubik, W.P. Investigations of thin film structures of WO3 and WO3 with Pd for hydrogen detection in a surface acoustic wave sensor system. Thin Solid Films 2007, 515, 8345–8350. [Google Scholar] [CrossRef]
- Comini, E. Metal oxide nano-crystals for gas sensing. Anal. Chim. Acta 2006, 568, 28–40. [Google Scholar] [CrossRef]
- Aroutiounian, V. Metal oxide hydrogen, oxygen, and carbon monoxide sensors for hydrogen setups and cells. Int. J. Hydrog. Energy 2007, 32, 1145–1158. [Google Scholar] [CrossRef]
- Adamyana, A.Z.; Adamyana, Z.N.; Aroutiouniana, V.M.; Arakelyana, A.H.; Touryanb, K.J.; Turner, J.A. Sol-gel derived thin film semiconductor hydrogen gas sensor. Int. J. Hydrog. Energy 2007, 32, 4101–4108. [Google Scholar] [CrossRef]
- Korotcenkov, G. Metal oxides for solid-state gas sensors: What determines our choice? Mater. Sci. Eng. B 2007, 139, 1–23. [Google Scholar] [CrossRef]
- Adamyan, A.Z.; Adamyan, Z.N.; Aroutiounian, V.M. Study of sensitivity and response kinetics changes for SnO2 thin-film hydrogen sensors. Int. J. Hydrog. Energy 2009, 34, 8438–8443. [Google Scholar] [CrossRef]
- Boon-Bretta, L.; Bousek, J.; Morettoa, P. Reliability of commercially available hydrogen sensors for detection of hydrogen at critical concentrations: Part II—Selected sensor test results. Int. J. Hydrog. Energy 2009, 34, 562–571. [Google Scholar] [CrossRef]
- Sakai, G.; Matsunaga, N.; Shimanoe, K. Theory of gas-diffusion controlled sensitivity for thin film semiconductor gas sensor. Sens. Actuators B Chem. 2001, 80, 125–131. [Google Scholar] [CrossRef]
- Eranna, G.; Joshi, B.C.; Runthala, D.P.; Gupta, R.P. Oxide materials for development of integrated gas sensors—A comprehensive review. Crit. Rev. Solid State Mater. Sci. 2004, 29, 111–188. [Google Scholar] [CrossRef]
- Ippolito, S.J.; Kandasamy, S.; Kalantar-Zadeh, K.; Wlodarski, W. Hydrogen sensing characteristics of WO3 thin film conductometric activated by Pt and Au catalysts. Sens. Actuators B Chem. 2005, 108, 154–158. [Google Scholar] [CrossRef]
- Ionescu, R.; Hoel, A.; Granqvist, C.G.; Llobet, E.; Heszler, P. Ethanol and H2S gas detection in air and in reducing and oxidizing ambience: Application of pattern recognition to analyze the output from temperature-modulated nanoparticulate WO3 gas sensors. Sens. Actuators B Chem. 2005, 104, 124–131. [Google Scholar]
- Penza, M.; Martucci, C.; Cassano, G. NOx gas sensing characteristics of WO3 thin films activated by noble metals (Pd, Pt, Au) layers. Sens. Actuators B Chem. 1998, 50, 52–59. [Google Scholar]
- Luo, Sh.; Fu, G.; Chen, H. Gas-sensing properties and complex impedance analysis of Ce-added WO3 nanoparticles to VOC gases. Solid-State Electron. 2007, 51, 913–919. [Google Scholar] [CrossRef]
- Veith, G.M.; Lupini, A.R. Magnetron sputtering of gold nanoparticles onto WO3 and activated carbon. Catal. Today 2007, 122, 248–253. [Google Scholar]
- Cabot, A.; Arbiol, J.; Morante, J.R. Analysis of the noble metal catalytic additives introduced by impregnation of as obtained SnO2 sol-gel nanocrystals for gas sensors. Sens. Actuators B Chem. 2000, 70, 87–100. [Google Scholar]
- Opara, U.; Ovec, K.; Orel, B.; Georg, A.; Wittwer, V. The gasochromic properties of sol-gel WO3 films with sputtered Pt catalyst. Pergamon 2000, 68, 541–551. [Google Scholar]
- Ruiz, A.; Arbiol, J.; Cirera, A.; Cornet, A.; Morante, J.R. Surface activation by Pt-nanoclusters on titania for gas sensing applications. Mater. Sci. Eng. C 2002, 19, 105–109. [Google Scholar]
- Moreno, D.L.; Monzón-Hernández, D. Effect of the Pd–Au thin film thickness uniformity on the performance of an optical fiber hydrogen sensor. Appl. Surf. Sci. 2007, 253, 8615–8619. [Google Scholar] [CrossRef]
- Fardindoost, S.; Iraji zad, A.; Rahimi, F.; Ghasempour, R. Pd doped WO3 films prepared by sol-gel process for hydrogen sensing. Int. J. Hydrog. Energy 2010, 35, 854–860. [Google Scholar]
- Epifani, M.; Abriol, J.; Pellicer, E.; Comini, E.; Siciliano, P.; Faglia, G.; Morante, J.R. Synthesis and gas sensing properties of Pd-Doped SnO2 nanocrystals. A case study of general morphology for doping metal oxides nanocrystals. Cryst. Growth Des. 2008, 8, 1774–1778. [Google Scholar] [CrossRef]
- Malyshev, V.V.; Pislyakov, A.V. Investigation of gas-sensitivity of sensor structures to hydrogen in a wide range of temperature, concentration and humidity of gas medium. Sens. Actuators B Chem. 2008, 134, 913–921. [Google Scholar] [CrossRef]
- Huang, Z.M.; Zhang, Y.Z.; Kotaki, M.; Ramakrishna, S. A review on polymer nanofibers by electrospinning and their applications in nanocomposites. Compos. Sci. Technol. 2003, 63, 2223–2253. [Google Scholar] [CrossRef]
- Wang, Z.; Liu, L. Synthesis and ethanol sensing properties of Fe-doped SnO2 nanofibers. Mater. Lett. 2009, 63, 917–919. [Google Scholar] [CrossRef]
- Song, X.; Liu, L. Characterization of electrospun ZnO–SnO2 nanofibers for ethanol sensor. Sens. Actuators A 2009, 154, 175–179. [Google Scholar]
- Song, X.; Zhang, D.; Fan, M. A novel toluene sensor based on ZnO-SnO2 nanofiber. Appl. Surf. Sci. 2009, 255, 7343–7347. [Google Scholar] [CrossRef]
- Park, J.A.; Moon, J.; Lee, S.J.; Lim, S.C.; Zyung, T. Fabrication and characterization of ZnO nanofibers by electrospinning. Curr. Appl. Phys. 2009, 9, S210–S212. [Google Scholar] [CrossRef]
- Liu, L.; Zhang, T.; Li, S.; Wang, L.; Tian, Y. Preparation, characterization, and gas-sensing properties of Pd-doped In2O3 nanofibers. Mater. Lett. 2009, 63, 1975–1977. [Google Scholar]
- Zhang, H.; Li, Z.; Liu, L.; Wang, C.; Wei, Y.; MacDiarmid, G.A. Mg2+/Na+-doped rutile TiO2 nanofiber mats for high-speed and anti-fogged humidity sensors. Talanta. 2009, 79, 953–958. [Google Scholar] [CrossRef]
- Wang, Y.; Ramos, I.; Santiago-Avilés, J.J. Detection of moisture and methanol gas using a single electrospun tin oxide nanofiber. IEEE Sensors J. 2007, 7, 1347–1348. [Google Scholar]
- Lu, X.; Liu, X.; Zhang, W.; Wang, C.; Wei, Y. Large-scale synthesis of tungsten oxide nanofibers by electrospinning. J. Colloid Interface Sci. 2006, 298, 996–999. [Google Scholar]
- Wang, G.; Ji, Y.; Huang, X.; Yang, X.; Gouma, P.I.; Dudley, M. Fabrication and characterization of polycrystalline WO3 nanofibers and their application for ammonia sensing. J. Phys. Chem. B 2006, 110, 23777–23782. [Google Scholar]
- Piperno, S.; Passacantando, M.; Santucci, S.; Lozzi, L.; La Rosa, S. WO3 nanofibers for gas sensing applications. J. Appl. Phys. 2007, 101, 124504–124507. [Google Scholar] [CrossRef]
- Kudo, T.; Okamoto, H.; Matsumoto, K.; Sasaki, Y. Peroxopolytungstic acids synthesized by direct reaction of tungsten or tungsten carbide with hydrogen peroxide. Inorg. Chim. Acta 1986, 111, L27–L28. [Google Scholar] [CrossRef]
- Choi, S.-W.; Park, J.Y.; Kim, S.S. Dependence of gas sensing properties in ZnO nanofibers on size and crystallinity of nanograins. J. Mater. Res. 2011, 26, 1662–1665. [Google Scholar] [CrossRef]
- Choi, S.-W.; Park, J.Y.; Kim, S.S. Growth behavior and sensing properties of nanograins in CuO nanofibers. Chem. Eng. J. 2011, 172, 550–556. [Google Scholar] [CrossRef]
- Park, J.Y.; Asokan, K.M.; Choi, S.-W.; Kim, S.S. Growth kinetics of nanograins in SnO2 fibers and size dependent sensing properties. Sens. Actuators B Chem. 2011, 152, 254–260. [Google Scholar] [CrossRef]
- Arbiol, J. Metal Additives Distribution in TiO2 and SnO2 Semiconductor Gas Sensor Nanostructured Materials. Ph.D. Thesis, Barcelona University, Barcelona, Spain, July 2001..
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