This application is a U.S. National Phase under 35 U.S.C. §371, of International Application No. PCT/EP2007/005015, filed Jun. 6, 2007.
The present invention relates to a method and devices therefor for identifying the various phases of the ionization current released during combustion in a cylinder of an internal combustion engine. The identification of the various phases of the ionization current generated in the combustion chamber of internal combustion engines is of relevant importance for the better functioning of engines for motor vehicles.
It is known that this identification is utilised to maximise the efficiency of the catalytic converters of said engines to maintain the concentration of exhaust gases of said engines in proximity to a set value, to monitor the air/combustible ratio, to evaluate detonation and to monitor combustion quality in said engines.
The devices and methods currently utilised for said identification are based on the use of sensors, i.e. special circuits able to identify a specific phase of the said ionization current, be it chemical or thermal.
Said currently utilised devices and methods are not, however, able to identify the various phases of said current.
The aim of the present invention is to identify a method for identifying each of the various phases of the ionization current released during combustion in each cylinder of an internal combustion engine, overcoming the limitations of the currently known methods or devices which are able to identify solely one specific phase of said ionization current.
The present invention is based on the use of the ionization current released by a device located above each cylinder of said engine. Said ionization current is measured by a Control Unit commonly utilised for the management of said combustion engines.
The aims and advantages will better emerge in the description that follows and the plates enclosed, which illustrate, purely in the form of a non-limiting example, an internal combustion engine with a plurality of cylinders:
With reference to
With reference to
With reference to
The method continues with a subsequent phase (302) relating to the selection of samples of said ionization current IC signal at predetermined intervals of time within windows which vary in length from 5 μs to 50 μs Said interval of time has been identified by experimental tests being able to have precise representation of the ion current, avoiding to make an excessive number of samples. This sampling is called, in the present invention, S.
The subsequent phase of the method (303) relates to the registration of the signal samples selected during the previous phase (302).
In the subsequent phase of the method (304) the value is calculated of the derivative of each sample S selected in the previous phase (302).
This value is called, in the present invention, S1.
The method continues with the phase (305) in which each sample signal S is associated with the corresponding value S1, which was calculated during the previous phase (304).
The method continues with the phase (306) in which the values S1 are ordered in a progressive temporal fashion, starting from the end of the spark occurring in the spark plug (6) and concluding at the end of the ionization phenomenon. The values S1 ordered in a progressive temporal fashion are called, in the present invention, S1O.
The subsequent phase of the method (307) envisages the comparison of each value S1O with the previous value S1O and the subsequent value S1O.
The method continues with the phase (308) comprising the registration of the sample signal S corresponding to the value S1O which proves to be essentially equal to zero and which is preceded by a value S1O with a positive value and followed by a value S1O with a negative value. Each signal registered in the present phase (308) is called, in the present invention, P.
The subsequent phase of the method (309) relates to the measurement of each length of time during which each value P is registered, starting from the end of the spark occurring in the spark plug (6). Each length of time measured is called, in the present invention, TP.
The method concludes with phase 310. In said phase the lengths of time TP are registered.
In a first phase (401), the measurement is effected, in each cylinder (2) of said engine (1), of the ionization current signal. This measurement is effected in the interval of time running from 150 μs to 2 ms from the end of the spark occurring in the spark plug (6) Said interval of time has been identified by experimental tests being able to identify the entire chemical phase of the ion current. This ionization current measured is called, in the present invention, λIC.
The method continues with a subsequent phase (402) comprising the selection of samples of said ionization current λIC signal at predetermined intervals of time within windows which vary in length from 5 μs to 50 μs Said interval of time has been identified by experimental tests being able to have precise representation of the ion current, avoiding to make an excessive number of samples. This sampling is called, in the present invention, λS.
The subsequent phase of the method (403) relates to the registration of the signal samples selected during the previous phase (402).
In the subsequent phase of the method (404) the value is calculated of the derivative of each sample λS selected in the previous phase (402). This value is called, in the present invention, λS1.
The method continues with the phase (405) in which each sample signal λS is associated with the corresponding value λS1, which was calculated during the previous phase (404).
The method continues with the phase (406) in which the values λS1 are ordered in a progressive temporal fashion, within the interval of time running from 150 μs to 2 ms from the end of the spark occurring in the spark plug (6) being said interval of time has been identified by experimental tests being able to identify the entire chemical phase of the ion current. The values λS1 ordered in a progressive temporal fashion are called, in the present invention, λS1O.
The subsequent phase of the method (407) envisages the comparison of each value λS1O with the previous value λS1O and the subsequent value λS1O.
The method continues with the phase (408) comprising the registration of the sample signal λS corresponding to the value λS1O which proves to be essentially equal to zero and which is preceded by a value λS1O with a positive value and followed by a value λS1O with a negative value. Each signal registered in the present phase (408) is called, in the present invention, λP.
The subsequent phase of the method (409) relates to the measurement of the length of time during which each value λP is registered, starting from the end of the spark occurring in the spark plug (6). Each length of time measured is called, in the present invention, λTP.
The method concludes with phase 410. In said phase the length of time λTP is registered.
The method continues with a subsequent phase (502) comprising the selection of samples of said ionization current δIC signal at predetermined intervals of time within windows which vary in length from 5 μs to 50 μs Said interval of time has been identified by experimental tests being able to have precise representation of the ion current, avoiding to make an excessive number of samples. This sampling is called, in the present invention, δS.
The subsequent phase of the method (503) relates to the registration of the signal samples selected during the previous phase (502).
In the subsequent phase of the method (504) the value is calculated of the derivative of each sample δS selected in the previous phase (502).
This value is called, in the present invention, δS1.
The method continues with the phase (505) in which each sample signal δS is associated with the corresponding value δS1, which was calculated during the previous phase (504).
The method continues with the phase (506) in which the values δS1 are ordered in a progressive temporal fashion, within the interval of time running from 2 ms to 5 ms from the end of the spark occurring in the spark plug (6) Said interval of time has been identified by experimental tests being able to identify the entire thermal phase of the ion current. The values δS1 ordered in a progressive temporal fashion are called, in the present invention, λS1O.
The subsequent phase of the method (507) envisages the comparison of each value δS1O with the previous value δS1O and the subsequent value δS1O.
The method continues with the phase (508) comprising the registration of the sample signal δS corresponding to the value δS1O which proves to be essentially equal to zero and which is preceded by a value δS1O with a positive value and followed by a value δS1O with a negative value. Each signal registered in the present phase (508) is called, in the present invention, δP.
The subsequent phase of the method (509) comprises the measurement of the length of time during which each value δP is registered, starting from the end of the spark occurring in the spark plug (6). Each length of time measured is called, in the present invention, δTP.
The method concludes with phase 510. In said phase the length of time δTP is registered.
The description above and the tables enclosed illustrate an embodiment of the present invention and constitute a non-limiting example thereof within the scope of protection of the claims that follow.
Number | Date | Country | Kind |
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MI2006A1151 | Jun 2006 | IT | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2007/005015 | 6/6/2007 | WO | 00 | 4/14/2009 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2007/144099 | 12/21/2007 | WO | A |
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4417556 | Latsch | Nov 1983 | A |
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7290442 | Zhu et al. | Nov 2007 | B2 |
20040084026 | Zhu et al. | May 2004 | A1 |
Number | Date | Country |
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0 895 076 | Feb 1999 | EP |
2 060 062 | Apr 1981 | GB |
WO 9851922 | Nov 1998 | WO |
WO 2007042091 | Apr 2007 | WO |
Number | Date | Country | |
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20100064772 A1 | Mar 2010 | US |