The present invention relates to a sensor element.
Gas sensors are used for identifying gas components and/or for determining the gas concentration in measuring gas mixtures, and they generate a measuring signal while taking into account the oxygen content in a measuring chamber that is in gas-conducting contact with the measuring gas.
So-called lambda probes are one type of such sensors, In their case, limiting current probes are involved, based on a ceramic solid electrolyte which connects two electrodes in an ion-conducting manner. The measuring chamber is preferably equipped with a diffusion barrier which steadies and also limits the access of the measuring gas to the measuring chamber.
In order to set the oxygen content in the measuring chamber, the two electrodes are able to have applied to them an electrical pump voltage, using an appropriate circuit. The measure for the oxygen ion current, in this instance, between the pump electrode situated in the measuring chamber and the pump counterelectrode situated outside the measuring chamber, is the electric current flowing between the two electrodes. Depending on a lack of oxygen or an excess of oxygen in the measuring chamber, which means a rich or a lean mixture in exhaust gases, a corresponding voltage is applied to the two electrodes by the circuit. This voltage causes an electrical field between the two electrodes, whose field forces cause an oxygen ion current through the solid electrolyte.
A change, caused by the measuring gas flowing into the measuring chamber via the diffusion barrier, in the oxygen concentration, that is set to be constant in the measuring chamber, may be determined using a so-called measuring cell. It is preferably also made up of a solid electrolyte and a measuring electrode situated in the measuring chamber and a reference electrode exposed to a reference gas, preferably air. The voltage present between the measuring electrode and the reference electrode is a measure for the difference in the oxygen concentrations between the gas mixture in the measuring chamber and the reference gas. When the oxygen content in the reference gas is known, that is, approximately 21% in the case of air, the absolute oxygen concentration in the measuring chamber is also known upon rectification of the concentration.
Such gas sensors, frequently also called probes, are used for the regulation of combustion processes. They are used for putting a value on the exhaust gases thus created, whereby, using appropriate further measures, already a massive reduction in pollutants is able to be achieved, for instance, in the case of internal combustion engines. Based on the increasing importance of pollutant emissions, however, it would be desirable to get a better grip on mobile as well as immobile combustion processes.
Example embodiments of the present invention provide for improving a sensor of the type mentioned at the outset.
Accordingly, example embodiments of the present invention provide a sensor element for determining gas components in measuring gas mixtures, particularly gas components in exhaust gases of combustion devices, having a measuring chamber that is in gas-conducting connection with the measuring gas mixture, and having a solid electrolyte which connects a pump electrode situated in the measuring chamber and a pump counterelectrode while conducting oxygen ions, in order to set the oxygen content in the measuring chamber. This sensor element stands out by having the pump counterelectrode situated in a reference gas chamber.
This positioning of the pump counterelectrode in a reference gas chamber is based on the realization that one may achieve a very great signal steadiness of the probe, especially at the lambda=1 transition. The lambda=1 ripple of the pump current, used as the measuring signal, which has been known up to now from the related art, may be greatly reduced using a sensor element thus designed. The reason is particularly that the gas change between rich and lean in the measuring gas has no influence on the pump counterelectrode situated in the reference gas chamber for the oxygen ion takeup, for the oxygen supply of the measuring chamber. For, the strongly changing oxidation and reduction processes, especially in the lambda=1 transition, are not able to have any effect on the quantitative change that influences the measuring signal, in the free oxygen ions available for the pump process at the surface of the pump counterelectrode, because of the gas-tight separation between the measuring gas and the pump counterelectrode.
Because of a gas-conducting connection of the reference gas chamber to the ambient air, it may not only be assured that this measuring signal stabilization is ensured over the entire service life of the sensor element. But a clearly broadened field of use of the sensor element may furthermore be made available, in the direction to very rich, that is, oxygen-poor measuring gas mixtures.
On the condition that the reference gas chamber that is connected to the ambient air is dimensioned in such a way that the limiting current at the pump counterelectrode is sufficiently large to produce the transport of O2− to the pump electrode in the measuring gas chamber, it may be assured in addition that, even in extremely rich exhaust gases, there cannot be any damage to the sensor element by decomposition of the solid electrolyte, and no brown coloration going along with that, because of a reaction ZrO2+4e−−>Zr+2O2−). In response to suitable dimensioning of the reference gas chamber, the pump counterelectrode that is in connection with the ambient air may also make available sufficient O2−, even in measurements in very rich exhaust gas mixtures, in order to oxidize completely the rich exhaust gas present at the pump electrode in the measuring chamber. That being the case, the device according to example embodiments of the present invention will be able to determine the λ value reliably even in very rich gas mixtures and over longer time periods.
In order to reduce the production effort and also the production costs of such a sensor element, in appropriately modified example embodiments, for example, the pump electrode may be developed in common with a first measuring electrode and/or the pump counterelectrode may be developed in common with a second measuring electrode. In the respectively common development of the pump electrode with the first measuring electrode in the measuring chamber, and the pump counterelectrode with the second measuring electrode in a reference gas chamber, also called a reference electrode, the number of electrodes may even be reduced to two, if the material are selected suitably. The wiring configuration of the sensor element, in this instance, has to be adapted corresponding to the number of electrodes, and in dependence upon the example embodiment.
In an example embodiment, the pump counterelectrode may be positioned close to the heating element, so that the pump counterelectrode is able to be brought rapidly to the operating temperature, and is thus ready to be used without interference. In this connection, it is especially advantageous if a heat transfer, that is as free as possible of interference, between the heating element and the measuring cell can be provided. For this purpose, in an example embodiment, a part of the reference gas chamber developed between the heating element and the pump counterelectrode is developed to be as small as possible, taking into account a sufficient oxygen supply even for rich mixtures. To do this, one might want to consider a tapering at the end of a large-volume reference gas chamber in that region in which the pump counterelectrode is situated.
A further positive influencing of the measuring signal may be accomplished by a diffusion barrier preconnected to the measuring chamber in the direction towards the measuring gas mixture, which, regarded over its effective cross section, forms a substantially equally large diffusion resistance before the surface of the pump electrode facing it. One may thereby achieve a uniform ageing of the pump electrode over its entire effective cross section. This is based on the fact that, as seen over the effective cross section of the pump electrode, all parts have approximately the same participation in the formation or reduction of oxygen ions for keeping constant the oxygen proportion in the gas in the measuring chamber.
Example embodiments of the present invention are explained in more detail on the basis of the drawings and the description referring to it below.
In detail,
For this, pump electrode 4 is situated in a measuring chamber 7, and is connected via solid electrolyte 3 which conducts oxygen ions to a pump counterelectrode 5 situated in a reference gas chamber 8, according to example embodiments of the present invention, so as to provide a constant oxygen concentration in measuring chamber 7. The positioning of pump counterelectrode 5 in a reference gas, in the current example the ambient air, has the effect of good signal steadiness of the probe, especially at a lambda λ=1 transition of the measuring gas mixture.
Negative effects on the measuring signal, as are observed in the devices known up to now as non-monoticity of the oxygen signal during the transition of the exhaust gas composition through λ=1, which is attributed to the positioning of the pump counterelectrode in the measuring gas, may be switched off using this sensor element construction.
An additional advantage of the present sensor element is a clearly broader field of application of the sensor element, in response to a suitable dimensioning of reference gas chamber 8. For instance, in the case of positioning such a sensor element in an exhaust gas tract, the pump counterelectrode, even in the case of very rich exhaust gas, is able to supply sufficient O2− from O2 according to O2+2e−−>2O2− to the pump electrode, so as to ensure a reliable signal. To do this, however, the correct dimensioning of the reference air channel is important. That is, the limiting current at the pump counterelectrode has to be sufficiently large to ensure the transport of the O2− & to the pump electrode. The richer the gas mixture that is to be measured, the larger the limiting current for the reference air channel has to be selected, because more O2 has to be additionally supplied.
However, if the pump counterelectrode were situated in the exhaust gas, then, in rich exhaust gas, O2− could only be obtained from CO2 (CO2+2e−−>CO+O2−) or H2O(H2O+2e−−>H2+O2−. For these reactions, a clearly higher pump voltage would be required. If after such reactions sufficient O2− could no longer be formed (above all, there would be the danger in the case of very rich mixtures, because in that case a great deal of O2− is required), there would be decomposition of the ZrO2 ceramic (ZrO2+4e−−>Zr+2O2−), and there would be damage to the sensor element (brown discoloration). Such damage to the sensor element may, however, be prevented by the design according to example embodiments of the present invention.
Sensor element 1 according to
In an example embodiment, pump electrode 4 and measuring electrode 12 are developed in common. In the present case, pump counterelectrode 5 and reference electrode 11 are developed separately, but in modified example embodiments they might also be developed in common, for instance, for reasons of savings. Alternatively, the reference electrode may be operated in an additional reference gas chamber, in deviation from
In order to be able to reduce the effects of the great flow fluctuations, that appear especially in exhaust gas systems of internal combustion engines, on the measuring signals of the sensor element, sensor element 1, as in
Additional design features of this sensor element is shown in
In order to be able to ensure a sufficient supply of oxygen to the pump counterelectrode of the measuring cell of sensor element 1, the following relationship is proposed, for instance:
b>r>s and t≧s, and s≦b/4.
The following estimation may be used to estimate the required limiting current of the reference air channel on the air:
The reference air channel has to be dimensioned so that IRK(air)≧|Ip(richexhaustgas)| applies.
IRK(air): Limiting current for cathodically operated pump counterelectrode on air |Ip(richexhaustgas)|: Amount of pump current at the pump electrode for rich exhaust gas. The smaller λ, the greater |Ip(richexhaustgas)|.
I
rel
=|I
p(richexhaustgas)|/Ip(air)
Ip(air): Limiting current for cathodically driven pump electrode in air
This makes IRK(air)≧Irel*IP(air) valid
In the following table, Irel is determined up to λ=0,4 (Assumption: The C:H-ratio in the fuel is 1:2; this is about an ideal rich exhaust gas, i.e. the rich exhaust gas is composed only of CO, H2, CO2, H2O und N2).
Irel is calculated for two different rich exhaust gases: KP (equilibrium constant for water equilibrium)=3.5 corresponds to a typical engine exhaust gas and KP=2 corresponds to a rich exhaust gas that is rich in H2.
Number | Date | Country | Kind |
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10 2005 052 430.3 | Nov 2005 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP06/67597 | 10/20/2006 | WO | 00 | 10/7/2008 |