Explanation of the Non-Linear Electrical Behavior of a Resistive NO_x Dosimeter By Operando DRIFT Spectroscopy

Abstract

Introduction To detect low NOx concentrations is still a focus for air-quality monitoring. The direct detection of the total dose of NOx is beneficial since the air pollution limits are given as hourly and annual mean values. A gas dosimeter for direct detection of the dose of NOx was presented in [1,2,3]. In the sorption phase, NOx molecules are adsorbed on the functional film and the electrical resistance changes. During this phase, the correlation between NOx dose and resistance change is linear until a certain loading state is reached. As soon as the characteristic curve gets non-linear, described often as saturation of the NOx adsorption [1], sensor regeneration is necessary. During thermal regeneration, the sorbed NOx species is desorbed from the surface, and a new sorption cycle can begin. To further understand the sensing mechanism and the effects of non-linearity, NOx dosimeters are investigated by operando DRIFT spectroscopy [4]. The electrical sensor signal and the formation of adsorbed species are investigated operando on the dosimeter. The non-linear behavior of the electrical properties occurring at a certain sensor signal are investigated at various film thicknesses [5] and are combined with the sorption properties. Materials and Methods Potassium-permanganate impregnated on lanthanum-stabilized alumina powder (K/Mn-La-Al2O3) [1] serves as the functional material. It is applied by screen-printing on an alumina substrate equipped with interdigitated Au electrodes and fired at 650 °C. Different layer thicknesses of the functional films are achieved by several screen-printing steps. The sensors are mounted in a gas purgeable operando DRIFTS cell (Fig. 1) [4] and heated by an integrated platinum heating structure to 350 °C. They are exposed to synthetic air (20 % O2 and 2 % humidity in N2 balance). NOx concentrations (ppb-range) are added and validated by a chemiluminescence detector (CLD). The sensor resistance is derived by impedance spectroscopy (f = 200 Hz, U eff = 200 mV) from an R||C equivalent circuit. The sensor signal is defined as the relative resistance change (R-R 0/R 0), with R 0 being the resistance in base gas and R the resistance during NOx exposure. Simultaneous DRIFT spectra are obtained and the absorbance -log(I/I 0), with the intensity I 0 in base gas and the intensity I during NOx adsorption, is calculated. The sensors are regenerated by heating up to 650 °C. Results and Discussion An operando DRIFTS result during exposure to three peaks of 50 ppb NOx with NOx pauses in-between is shown in Fig. 2. The NOx dose in ppm∙s is derived from the integration of the CLD NOx signal. The dose increases linearly during NOx exposure and remains constant during dosing pauses. The sensor signal shows the same behavior: ΔR/R 0 increases linearly when 50 ppb NOx are present and stays constant during NOx absence. The calculated absorbance shows a clear peak at a wave number of 1370 cm-1 occurring during NOx exposure. It can be attributed to the nitrate formation on potassium sites of K/Mn-La-Al2O3 and is characteristic for the sorption phase [4]. The calculated peak area A E of this nitrate peak is shown in Fig. 2, too. A E and therefore the amount of formed nitrates increases linearly during NOx addition and remains constant during NOx pauses. The electrical properties of the dosimeter can be related directly to the NOx dose and to the formed nitrates. One important point is that all curves increase linearly during NOx exposure and no saturation effects can be observed for the sensor signal and the nitrate formation. In Fig. 3, the sensor is exposed to three peaks of 390 ppb NOx. ΔR/R 0 gets non-linear after reaching 40 %. The sensor seems to saturate. The slope during NOx exposure is non-linear and the signal in NOx pauses decreases. In contrast, A E behaves almost linear. It is assumed that the electrically observed non-linearity cannot be explained by a saturation of the adsorption capability of K/Mn-La-Al2O3. It seems that the NOx adsorption capability is not exhausted, but the resistance shows a saturation effect. Conclusions The results show that the sensor behaves like a dosimeter with linear characteristics between NOx dose, sensor signal and formed nitrate species until a certain sensor signal of around 40 % is reached. At higher relative resistance changes, the electrical signal becomes non-linear, whereas the adsorption capability itself, i.e. the nitrate formation, remains linear and the NOx adsorption on K/Mn-La-Al2O3 is not saturated. This behavior will be investigated by operando DRIFTS in dependence on the film thickness. References [1] A. Groß et al., Dosimeter-type NOx sensing properties of KMnO4 and its electrical conductivity during temperature programmed desorption, Sensors, 13, 4428–4449 (2013), doi: 10.3390/s130404428 [2] I. Marr et al., Resistive NOx dosimeter to detect very low NOx concentrations - Proof-of-principle and comparison with classical sensing devices, Sensors and Actuators B: Chemical, 248, 848–855 (2017), doi: 10.1016/j.snb.2016.12.112 [3] A. Groß et al., Dual Mode NOx Sensor: Measuring Both the Accumulated Amount and Instantaneous Level at Low Concentrations, Sensors, 12, 2831-2850 (2012), doi: 10.3390/s120302831 [4] D. Schönauer-Kamin et al., Characterization of the sensitive material for a resistive NOx gas dosimeter by DRIFT spectroscopy, Sensors and Actuators B: Chemical, 320, 128568 (2020), doi: 10.1016/j.snb.2020.128568 [5] A. Groß et al., The Effect of the Thickness of the Sensitive Layer on the Performance of the Accumulating NOx Sensor, Sensors, 12, 12329–12346 (2012), doi: 10.3390/s120912329 Figure 1