a shows an exemplary embodiment of a particle sensor having measuring electrodes situated on a substrate element, in top view.
b shows another exemplary embodiment of a particle sensor having measuring electrodes situated on a substrate element, in top view, and
a shows another exemplary embodiment of a particle sensor having measuring electrodes situated on a substrate element, in top view.
b shows another exemplary embodiment of a particle sensor having measuring electrodes situated on a substrate element, in top view.
c shows another exemplary embodiment of a particle sensor having measuring electrodes situated on a substrate element, in top view.
In a first exemplary embodiment according to
As explained previously, the soot concentration in a gas may ultimately be determined from the measured values. The two measuring electrodes 10, 15 are configured according to the exemplary embodiment and/or exemplary method of the present invention in such a way that by applying a voltage between measuring electrodes 10, 15 an asymmetric electric field is formed on measuring area 12. A symmetric electric field is characterized in that the field has a constant direction and intensity all over the field. Such a field is formed, for example, by the interdigital comb electrodes known from the related art. The individual finger electrodes are typically implemented by unstructured, linear track conductors, which are all parallel to one another. This results in a constant electric field between the finger electrodes.
However, as
A conductive path is first produced in the area of sides 30, 35 situated close to one another. Since the distance between measuring electrodes 10, 15 is very narrow at this point, a relatively slight particle deposition is sufficient for forming a conductive path and triggering a measuring signal. The sensitivity of sensor 1 is thus increased. As further particles deposit, conductive paths are also formed between sides 30, 35 of measuring electrodes 10, 15, which are farther apart. Due to the percolation characteristics of the deposited soot, whenever an additional conductive path is completed, a stronger increase in conductivity of the entire measuring area 12 takes place, which may be determined via measuring electrodes 10, 15. A stronger signal increase is thus achieved over a longer time period than would be possible in the case of measuring electrodes arranged in parallel. After short-circuiting measuring electrodes 10, 15 along all sides 30, 35, further deposits additionally keep increasing the conductivity continuously, i.e., measurement is also possible during this phase. Since the special configuration and arrangement of measuring electrodes 10, 15 allows a larger measuring area 12 to be formed for particle deposition, higher currents may also be achieved before they reach the saturation range compared to previously known interdigital measuring electrodes. The sensor signal is thus strengthened.
A varying distance between the finger electrodes may also be achieved in a conventional interdigital comb structure by modifying its shape. As
All exemplary embodiments described so far have constantly smooth, unstructured sides of measuring electrodes 10, 15 or of individual finger electrodes 40. Alternatively (
Summarizing, measuring electrodes 10, 15 are configured in all embodiments in such a way that by applying a voltage between measuring electrodes 10, 15 an asymmetric electric field is formed on measuring area 12. The asymmetric electric field is an electric field that is non-homogeneous in space. The special design of the field distribution makes targeted particle deposition control in space possible. In particular, the formation of conductive paths in preferred areas may be controlled. Path growth over time may also be steered in a desired direction. If necessary, more than two measuring electrodes 10, 15 may be provided for this purpose, for example, at least one central electrode (not shown in the figures) may be additionally provided between first and second measuring electrodes 10, 15. The geometric shape of and the potential applied to all electrodes is to be adapted to the desired field distribution.
Number | Date | Country | Kind |
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10 2004059650.6 | Dec 2004 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP05/55307 | 10/17/2005 | WO | 00 | 4/11/2007 |