1. Background
With conventional chemiresistive gas sensors, the conductivity of the sensitive materials depends on the actual concentration of the component to be measured (i.e., the analyte). If it is intended to measure the smallest concentrations of a gaseous analyte, the classical resistance measurement using metal oxide gas sensors reaches its limits. Although the response time may be short and the sensitivity high, the recovery time is mostly very long. The determination of hourly mean values requires a timely integration of the sensor signal over one hour, and for classical metal oxides, inaccuracies and long sensor recovery times might lead to large errors.
2. Measuring Principle
Resistive gas dosimeters could provide a remedy. A typical design consists of an alumina substrate with screen-printed interdigital electrodes (IDEs) covered with layers of the dosimeter material. Such sensors follow an integrating (accumulative) measurement principle. The sensitive material stores the gas component (it accumulates it) and changes its conductivity or electrical impedance (preferred linearly) with the amount of the stored component. Two basic application modes appear possible. Since the integration takes place directly in the material, the sensor signal is proportional to the exposed analyte amount (the dose), and its changes correlate directly to timely averages, e.g., to hourly mean values (if the integration time is one hour). Advantageously, due to the timely accumulation of the analyte, gas concentrations even in the sub-ppm or ppb range can be detected. In addition, the timely derivation of the sensor signal provides information about peak concentrations and the temporal evolution of the analyte exposure. When the material starts to saturate, a deviation from linearity occurs and the sensor material has to be regenerated (mostly thermally). Due to the linearity, the exact zero point hardly matters. Thus, zero drifts can be eliminated.
A scheme of one operation cycle with long sorption times (measuring mode) and short regeneration times is shown in
Figure 1. The sensor signal, typically the resistance, is accumulative. The actual concentration can be obtained by timely derivation.
3. Example for a Measurement Curve
A typical example for an earlier version of the NO
2 dosimeter uses a potassium-based carbonate (
Figure 2). It is operated at 380 °C and can be regenerated at 600 °C. The relative resistance change |Δ
R|/
R0 increases in the presence of NO
2 and is proportional to the timely integral of the NO
2 concentration (green). The derivative |d
R/d
t| (right) correlates with the actual NO
2 concentration. As will be shown at the conference, this method is also suitable for detecting pulses of 50 ppb accurately. Due to the operation above 300 °C, water (r.h.) variations do not affect the sensor signal. CO, CO2, or VOC also do not affect the sensor signal. A short heating pulse of a few tens of seconds (after an over one-hour measuring phase) is sufficient to regenerate the sample and to start a new measuring cycle.
Author Contributions
All authors, R.M., A.G. and D.S.-K., contributed equally to this manuscript. All authors have read and agreed to the published version of the manuscript.
Funding
This research received funding from several sources.
Data Availability Statement
All relevant data presented in the article are stored according to institutional requirements and as such are not available online. However, all data used in this paper can be made available upon request to the authors.
Conflicts of Interest
The authors declare no conflicts of interest.
References
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