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The efficiency of gas sensor application for facilitating the safe use of hydrogen depends to a considerable extent on the response time of the sensor to change in hydrogen concentration. The response and recovery times have been measured for five different hydrogen sensors, three commercially available and two promising prototypes which operate at room temperature.
Experiments according to ISO 26142 show that most of the sensors surpass much for a concentration change from clean to hydrogen containing air the demands of the Standard for the response times t(90) and values of 2 to lös were estimated. For an opposite shift to clean air, the recovery times t(10) are from 7 to 70 s. Results of transient behaviour can be fitted with an exponential approach. It can be demonstrated that results on transient behaviour depend not only from investigation method, and the experimental conditions, like gas changing rate and concentration jump, as well as from operating
Parameters of sensors. In comparison to commercial MOS and MIS-FET hydrogen sensors new sensor prototypes operating at room temperature possesses in particular longer recovery times.
A series of Mg₁₋ₓZnₓTiO₃, x = 0–0.5 (MZT0–MZT0.5) ceramics was synthesised and characterised. The dielectric properties of the samples in the frequency range of
1 Hz – 7.7 GHz were explored using three different methods:
a contacting electrode method, a parallel-plate method and a perturbed resonator method. The electrical properties in the space charge and dipolar polarisation frequency ranges are discussed in relation to the phase composition and microstructure data. Differences in the zinc Substitution divided the dielectrics into two groups, namely MZT0-MZT0.2 and MZT0.3–MZT0.5, each with different amount of a main Mg₁₋ₓZnₓTiO₃ solid solution phase and a secondary solid solution phase. Zinc substitution promoted the density of the ceramics, improved the purity of the main phase and increased the permittivity for frequencies up to 10⁸ Hz, but reduced the permittivity in the microwave range. In the MZT0.3–MZT0.5 samples, for frequencies less than 1 MHz the quality (Q x ƒ) factors were lower and log σ ₐ.c, the AC conductivity, was higher than for the MZT0–MZT0.2 samples. Above 10 MHz, the (Q x ƒ) factors and log σ ₐ.c of the two groups were similar.
Die Messung der Gasfeuchte im Spurenbereich in unterschiedlichen technisch und medizinisch relevanten Gasen erfolgte mit Sensoren, die auf dem coulometrischen Messprinzip basieren. Die verwendeten planaren coulometrischen Sensoren wurden im Frostpunkttemperaturbereich von -70 °C bis -30 °C in synthetischer Luft, Wasserstoff, Stickstoff und Distickstoffmonoxid (Lachgas) untersucht. Als Referenz für die Messungen wurde ein Präzisionstaupunktspiegel-Hygrometer verwendet. Die Gasfeuchte kann mit Hilfe der Sensoren in allen untersuchten Gasen, aber mit geänderten Kalibrierfunktionen, mit einer erweiterten Unsicherheit von kleiner als 2,1 K bestimmt werden. Für die Messungen in unterschiedlichen Gasen muss also der Einfluss der Gasmatrix auf das Sensorsignal berücksichtigt werden. So ist zum Beispiel bei Messungen in befeuchtetem Wasserstoff, aufgrund von Rekombinationseffekten, ein signifikant geändertes Sensorsignal zu beobachten.
Five miniaturized sensors based on dew-point,
capacitance or resistance measurement were tested for the
detection of humidity in compressed gases.
The dew-point sensors with optical or dielectric detection of
condensation were used at gas pressures up to 3 MPa in
dew-point range of -20 to 70°C and show no systematic
deviation and an uncertainty of dew-point temperature
mostly less than 1 K. The LiCl sensor has also a low
uncertainty but exhibit a systematic deviation to higher
values of dew-point. Capacitive polymer sensors can
indicate also a dew-point, even down to -70 °C and have an
uncertainty of about 1 to 2 K. The oxide sensor works in the
dew-point range of -10 to 20°C and has a signal what
exponential decreases with increasing gas pressure up to 10
MPa.
All types of sensor can be applied in compressed gases at
least up to 3 MPa, but their different change of sensor signal
due to the gas pressure has to be considered.
A market survey has been performed of commercially available hydrogen safety sensors, resulting in a total sample size of 53 sensors from 21 manufacturers. The technical specifications, as provided by the manufacturer, have been collated and are displayed herein as a function of sensor working principle. These specifications comprise measuring range, response and recovery times, ambient temperature, pressure and relative humidity, power consumption and lifetime. These are then compared against known performance targets for both automotive and stationary applications in order to establish in how far current technology satisfies current requirements of sensor end users. Gaps in the performance of hydrogen sensing technologies are thus identified and areas recommended for future research and development.
