Elsevier

Thin Solid Films

Volume 444, Issues 1–2, 1 November 2003, Pages 104-110
Thin Solid Films

Characterization and butanol/ethanol sensing properties of mixed tungsten oxide and copper tungstate films obtained by spray–sol–gel

https://doi.org/10.1016/S0040-6090(03)01048-4Get rights and content

Abstract

Mixed WO3–CuWO4 films have been prepared from an aqueous solution of copper sulfate and polytungsten gel with a molar ratio of Cu/W from 0 to 100%. These solutions were sprayed on to alumina substrates at 220 °C. The obtained films were amorphous and crystallized after annealing at 300 °C in air for 3 h. The annealed films were composed of a mixture of CuWO4 and WO3 phases. The film obtained from a solution with an equimolar ratio of Cu/W was pure CuWO4. The pure WO3 films obtained have high surface ‘irregularities’, such as porosity. These surface ‘irregularities’ in the films were maintained or even increased as Cu/W molar ratio augments in the starting solution up to 10%. The gas sensitivity to butanol and ethanol vapors is also enhanced when the CuWO4 phase increases in the film by up to 7–10%; with further increments to this proportion the detection sensitivity decreases, so compromises are approximately 7–10%. The gas sensitivity of pure CuWO4 was lower than that of pure WO3.

Introduction

Mixed oxides have been investigated intensively to improve or modify their electrochromic, gas sensing and photocatalitic properties. For example, coloration efficiency decreases slightly, but the lifetime of WO3–TiO2 thin films can be five times longer than those made of pure WO3 [1], [2], mixed oxides have recently emerged as a promising candidate for gas detection [3], and the degradation rate of 1,4-dichlorobenzene is enhanced by the addition of WO3 to TiO2 [4]. It has been found that most metal oxide mixtures exhibit increased surface activity.

It is well-known that the conductance of simple metal oxides such as SnO2, WO3, ZnO and TiO2 changes when the composition of the surrounding atmosphere is altered [5]. Different metals and oxides are used as dopants or catalyst in order to improve gas-sensing properties [6]. It has been concluded that the nature of the surface sites and the electron donor/acceptor properties of the gas, the adsorption, the surface reactions and desorption of gases are key features for the performance of semiconductor gas sensors [5]. Surface properties are expected to be influenced by grain boundaries between the grains of different chemical compositions. These phenomena will contribute to the gas-sensing properties. Mixed oxides that form distinct chemical compounds as in the systems Zn–Sn–O [7], Cd–In–O [8] and Sn–W–O [9], [10], [11], [12] have been used successfully in gas detection.

Tamaki et al. [13] have studied different metal tungstates in order to detect nitrogen oxides. However, CuWO4 was missing in that study. A mixture of tungsten oxide and copper oxide heated in vacuum produces CuWO4 with a distorted wolframite type structure [14] and CuWO3 with a cubic structure [15]. The sol–gel technique is well suited for making mixed oxides, and work with W–Ti oxide [1], W–V oxide [16], V–Ti oxide [17] and Fe–Ti oxide [18] has been reported. WxOPy films, obtained by spraying a polytungsten gel mixed with H3PO4 on to a glass substrate at 430 °C, have shown improved electrochromism [19]. Combining the spray pyrolysis and the sol–gel techniques has produced very rough films [19]. This technique is suitable for producing semiconductor metal oxides for gas-sensing applications; due to the fact that it yields a large interface between a solid and a gaseous medium.

We report in this work the characterization and gas sensing properties of mixed WO3–CuWO4 films obtained by spraying aqueous solutions of copper sulfate and polytungsten sol on to alumina substrates at 220 °C. The incorporation of the CuWO4 phase into WO3 improved the gas response to ethanol and butanol with respect to pure WO3.

Section snippets

Experimental

Combined spray pyrolysis and sol–gel techniques were used to obtain mixed tungsten oxide and copper tungstate films on alumina substrates. The process basically consists of producing an aerosol from a gel, which is sprayed on a hot substrate where the film is going to grow. The outline of the spray system used in this work is described elsewhere [20]. A sol was prepared via acidification of 0.1 M sodium tungstate aqueous solution (pH ∼7.8) through a proton exchange resin. Different quantities

Structural properties

The crystal structures of mixed WO3–CuWO4 films obtained were characterized by X-ray diffraction (XRD), and Fourier transform infrared spectroscopy (FTIR). XRD was performed using a Phillips X Pert diffractometer operating with CuKα radiation, and the infrared spectra were measured in the 450–4000 cm−1 wave number range using a Shimadzu 8300 spectrophotometer. For FTIR measurements a scratched film from the alumina substrate was mixed with KBr to make a very thin disc.

X-Ray diffraction patterns

Gas sensing properties

Pt-wire contacts were attached with a low-temperature gold paste to the two gold electrodes on the alumina substrate for electrical conductance measurements. The samples to be tested were placed in a stainless steel chamber (4.4 L) and exposed to different butanol and ethanol vapor concentrations. The films were connected in series with both a known resistor and a 5 V source. The conductance of the films was obtained by measuring the voltage drops across the resistor. Gas-sensing properties of

Discussion and conclusions

The annealed films obtained from a solution with a molar ratio of Cu/W lower than 3% were mainly monoclinic WO3, whereas those obtained from solutions with higher Cu/W molar ratios were composed of a mixture of CuWO4 and WO3 phases. The amount of the CuWO4 phase in the film was increased as the Cu/W molar ratio increased in the starting solution. The film obtained from a solution with a molar ratio of Cu/W of 100% was pure CuWO4. The WO3 films obtained using the combined sol–gel and spray

Acknowledgements

This work has been financially supported by the International Program for Physical Science of Uppsala University (IPPS), the Instituto de Investigación of Universidad Nacional de Ingenieria, and CONCYTEC (Peruvian Research Council).

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