EP1036269B1 - Procede de controle de l'injection d'un moteur a combustion interne - Google Patents

Procede de controle de l'injection d'un moteur a combustion interne Download PDF

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Publication number
EP1036269B1
EP1036269B1 EP98958328A EP98958328A EP1036269B1 EP 1036269 B1 EP1036269 B1 EP 1036269B1 EP 98958328 A EP98958328 A EP 98958328A EP 98958328 A EP98958328 A EP 98958328A EP 1036269 B1 EP1036269 B1 EP 1036269B1
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EP
European Patent Office
Prior art keywords
probe
measurement signal
integral
value
state
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Expired - Lifetime
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EP98958328A
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German (de)
English (en)
French (fr)
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EP1036269A1 (fr
Inventor
Vasco Afonso
Edouard Simon
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Renault SAS
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Renault SAS
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02DCONTROLLING COMBUSTION ENGINES
    • F02D41/00Electrical control of supply of combustible mixture or its constituents
    • F02D41/02Circuit arrangements for generating control signals
    • F02D41/14Introducing closed-loop corrections
    • F02D41/1438Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor
    • F02D41/1439Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor characterised by the position of the sensor
    • F02D41/1441Plural sensors
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F02COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
    • F02DCONTROLLING COMBUSTION ENGINES
    • F02D41/00Electrical control of supply of combustible mixture or its constituents
    • F02D41/02Circuit arrangements for generating control signals
    • F02D41/14Introducing closed-loop corrections
    • F02D41/1438Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor
    • F02D41/1477Introducing closed-loop corrections using means for determining characteristics of the combustion gases; Sensors therefor characterised by the regulation circuit or part of it,(e.g. comparator, PI regulator, output)
    • F02D41/148Using a plurality of comparators

Definitions

  • the invention relates to internal combustion engines of the injection connected to at least one catalytic converter and, more particularly a method of controlling the injection of such an engine.
  • double wealth loop which are based on information provided by two "lambda” probes, respectively located upstream and downstream of the catalytic converters.
  • the upstream probe, and its associated correction, called the loop upstream allow rapid reaction to wealth excursions, on the single loop model.
  • the downstream probe provides more information filtered but more precise and more representative of the catalytic efficiency.
  • the voltage it delivers is therefore used to construct a correction slow, superimposing on the correction induced by the upstream probe, and thus allowing to bias the average richness of regulation of the loop upstream.
  • double wealth loop mentioned above is able to support this richness correction, and to reduce the quantity of oxygen stored in the desired level.
  • the invention aims to remedy these drawbacks.
  • An object of the invention is to provide a richness correction important, especially during injection cut-off returns or enrichment at full load.
  • the invention also aims to arrive as soon as possible after entry into wealth regulation to a stabilized situation "with regard to catalytic converter "and the various corrective terms for the quantity injected. This can thus make it possible to implement different strategies of diagnostic of the catalytic converter or oxygen sensors.
  • the invention therefore provides a method of controlling injection an internal combustion engine connected to at least one exhaust catalytic, in which we place a first nonlinear probe in upstream of the catalytic converter capable of delivering a representative measurement signal the proportion of one of the engine exhaust components at the inlet of the catalytic converter, and a second nonlinear probe downstream of the catalytic converter capable of delivering a second representative measurement signal the proportion of one of the engine exhaust components at the outlet of the catalytic converter. A corrective value is then determined at from the two measurement signals so as to correct the amount of fuel injected.
  • the first measurement signal to a first predetermined reference signal corresponding to a richness of the mixture present in the combustion substantially equal to 1, so as to define for this first probe "rich” or “poor” states. So the first probe will be in its “rich” state if the value of the first measurement signal is greater than first reference signal and in its “poor” state otherwise.
  • the second measurement signal is also compared to a high threshold. predetermined and at a predetermined low threshold, these two thresholds defining for said mixture a wealth range close to 1.
  • the second three-state probe namely a so-called “rich” state (second measurement signal higher than the high threshold), a state called “poor” (second measurement signal below the low threshold) and a state called “stoichiometric” (measurement signal between the low and high thresholds).
  • an essential feature of the invention is to give greater importance to the information delivered by the downstream probe.
  • the pot catalytic in return for an injection cut, for example, the pot catalytic will be saturated with oxygen.
  • the voltage delivered by the downstream probe will be low corresponding to a fuel-poor mixture.
  • the upstream probe also provides a signal indicative of a poor mixture, the wealth loop will enrich naturally, using a correction, for example of the proportional-integral type, to from the signal delivered by the upstream probe.
  • the upstream probe is representative of a rich mixture, we will still continue to enrich, using a correction, for example of the proportional type integral, from the signal delivered by the downstream probe until sufficient oxygen has been "destocked" from the catalyst and the voltage of the downstream probe is raised to the threshold marking the lower limit of the stoichiometric domain. Only then a double loop of wealth will be set in motion thus avoiding the excesses and instabilities of a double wealth loop described in the prior art.
  • the correction from the downstream probe alone results in a deliberate distance from the stoichiometric operating conditions of the engine.
  • a transition from the poor state to the stoichiometric state corresponds for example a return after a long injection cut-off.
  • the correction phase using the first measurement signal we determines said corrective value with first means of correction of the proportional-integral type having a first gain proportional and a first integral gain.
  • the said measurement is determined corrective value with second means of the proportional-integral type having a second proportional gain and a second gain integral.
  • said corrective value with the first means of correction and third means of correction of the proportional-integral type having a third proportional gain and a third gain integral and receiving as input the difference between the second signal of measurement and a setpoint signal depending on the operating point of the engine.
  • This third correction includes for example the addition at the first proportional term of the first correction means, from corrective term (offset) issued by the third correction means.
  • the full term of the third correction means is advantageously reset to zero each time one leaves a phase of correction using the first measurement signal, which allows resetting to zero the value of the offset.
  • first and second winnings proportional equal are generally gains that have already been proven in terms of driving and comfort for the vehicle user. Choosing second wins equal to the first avoids a additional calibration.
  • a second zero integral gain can be chosen. This allows in particular to limit the excursion on the corrective value of the quantity of fuel injected, in particular when the downstream probe (second probe) is in its poor state and the upstream probe (first probe) is in its rich state.
  • an integral amplitude is calculated at each current instant current equal to the product of the second integral gain by the current duration separating said current instant and the start instant of this phase of correction.
  • the current integral amplitude reaches the minimum value or the value maximum, we freeze the value of this integral amplitude to the value thus reached, i.e. at the minimum or maximum value.
  • the value of the integral amplitude is then subtracted from the corrective value of the quantity of fuel injected, previously determined.
  • the reference CLC generally designates an electronic computer on board the vehicle and commander the quantity QY of fuel to be injected into the engine MOT.
  • Gas of this engine are filtered by a type exhaust CAT catalytic, from which they escape towards the open air.
  • a first SD1 probe (upstream probe) is located at the inlet of the catalytic converter and measures the content of one of the main components of gases exhaust, this component usually being oxygen.
  • This probe is of the non-linear type and is often called by those skilled in the art a "lambda" probe or EGO probe.
  • a second SD2 probe (downstream probe) similar to the first probe, is placed at the outlet of the catalytic converter and also measures the content of one of the main components of the exhaust gas, usually oxygen.
  • the CLC computer has loop control means open MCBO, of realization known per se, determining the quantity of fuel to inject depending on the engine operating point (Rg regime and Ch load). At this quantity supplied by the means in open loop MCBO, multiplies a corrective value KCL delivered by a richness loop using the two measurement signals V1 and V2 delivered by the two probes SD1 and SD2. As we will see in more detail below, this wealth loop is in fact made up here of three loops B1, B2 and B3 feedback.
  • the means of control in open loop, as well as the whole means of the CLC computer illustrated in FIG. 1, are for example performed in software using this computer.
  • the upstream sensor SD1 delivers a first measurement signal electric V1 (voltage across its terminals) which is applied to a circuit comparator CMP1 in which the signal V1 is compared to a voltage Vb which depends on the characteristics of the probe and corresponds to the voltage of tilting of the probe when the stoichiometric conditions are met.
  • This tilting voltage Vb is typically of the order of 450 mV.
  • the downstream probe SD2 delivers a second signal from measure V2 which is compared in a second comparator circuit CMP2 at a high threshold VS2 and at a low threshold VS1, these two thresholds being located on either side of the tilting voltage of this downstream probe, typically equal to 600 mV.
  • the downstream probe When the voltage V2 is above the threshold high VS2, the downstream probe is said to be in a rich state while when the voltage V2 is below the low threshold VS1, the downstream probe is said in a poor state.
  • the probe is then in a third state called stoichiometric (figure 3).
  • the value of the high threshold VS2 is for example taken at 750 mV while the value of the low threshold VS1 is equal for example to 350 mV or to 150 mV depending on the direction of flow of the downstream probe between its lean state and its stoichiometric state.
  • a rich state means that the gas mixture at the probe is rich (respectively lean) in fuel.
  • the first feedback loop B1 (upstream loop) conventionally comprises first correction means COR1 of the proportional-integral type, of realization known per se. These means COR1 have a proportional gain Kp1 and an integral gain Ki1.
  • comparator CMP1 delivers to the input of the means COR1 a first binary signal SGN1 having the values 1 or -1 in function of the position of the voltage V1 with respect to the switching voltage Vb.
  • the output of the first COR1 correction means deliver a first correction signal KCL1.
  • this third loop B3 When this third loop B3 is activated, it forms with the upstream loop B1 a double wealth loop.
  • a second wealth loop B2, or downstream loop, is formed of the CMP2 comparator circuit and of second correction means COR2 of the proportional-integral type having a proportional gain Kp2 and an integral gain Ki2.
  • These second COR2 correction means receive as input the signal SGN2 output from the CMP2 comparator.
  • This signal SGN2 takes for example respectively the values + 1.0 and - 1 depending on whether the downstream probe SD2 is in its state rich, stoichiometric, or poor.
  • the CLC computer also includes control means MCC receiving as input the comparators CMP1 and CMP2 and outputting two command signals SC1 and SC2 commanding respectively two switches I1 and I2 so as to activate selectively the different loops which have just been mentioned.
  • the SD2 downstream probe when the SD2 downstream probe is in its stoichiometric state, we activate then the double loop B1 and B3.
  • the corrective value KCL of injected fuel is then corrected from the two signals V1 and V2 delivered by the two probes, and using a corrector proportional-integral with integral gain Ki1 and equal proportional term the sum of the proportional gain + Kp1 or - Kp1 and the OFS offset.
  • loop B2 is activated and switches to Kp2 and Ki2 gains. It is assumed in this example that the two proportional gains Kp1 and Kp2 are equal. This is the reason for no jump to the KCL signal during switching.
  • the corrective value KCL keeps a constant value until the downstream probe goes into the stoichiometric state. At this time, the corrective value KCL undergoes an amplitude jump - Ks equal to - 2Kp 1 - BM.
  • the double loop B1 and B3 is then activated which has for consequence at first, taking into account that the probe upstream is still in its rich state, leading to a linear evolution of the corrected value KCL with a slope equal to - Ki1, then when the upstream probe goes into lean state, at a jump equal to 2 (Kp1 + OFS) followed of a linear evolution of slope + Ki1.
  • An advantageous variant of the invention makes it possible to ensure that the engine works well at stochiometry before triggering a correction using the B2 loop which causes a voluntary removal compared to this stoichiometry.
  • the correction phase using only the second measurement signal V2 is only authorized if at least one transition of the first measurement signal V1, namely a transition from the state rich in a poor state or vice versa, took place beforehand, that is to say between the moment of entering wealth and the present moment. If this this is not the case, the correction of loop B1 is applied by default using only the first measurement signal V1.
  • having recorded at least one transition of the upstream probe ensures that the engine works well at stoichiometry, and that the voluntary removal caused by the correction of the downstream probe does not start from too rich or too poor a state of the mixture in the combustion chamber.

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  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Electrical Control Of Air Or Fuel Supplied To Internal-Combustion Engine (AREA)
EP98958328A 1997-12-05 1998-12-04 Procede de controle de l'injection d'un moteur a combustion interne Expired - Lifetime EP1036269B1 (fr)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
FR9715407A FR2772078B1 (fr) 1997-12-05 1997-12-05 Procede de controle de l'injection d'un moteur a combustion interne
FR9715407 1997-12-05
PCT/FR1998/002621 WO1999030022A1 (fr) 1997-12-05 1998-12-04 Procede de controle de l'injection d'un moteur a combustion interne

Publications (2)

Publication Number Publication Date
EP1036269A1 EP1036269A1 (fr) 2000-09-20
EP1036269B1 true EP1036269B1 (fr) 2002-07-31

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EP98958328A Expired - Lifetime EP1036269B1 (fr) 1997-12-05 1998-12-04 Procede de controle de l'injection d'un moteur a combustion interne

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EP (1) EP1036269B1 (es)
JP (1) JP4054529B2 (es)
DE (1) DE69806964T2 (es)
ES (1) ES2177099T3 (es)
FR (1) FR2772078B1 (es)
WO (1) WO1999030022A1 (es)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE10025034A1 (de) * 2000-05-20 2001-11-22 Dmc2 Degussa Metals Catalysts Verfahren zum Betreiben einer Abgasreinigungsvorrichtung an einem Otto-Motor
US8347866B2 (en) * 2009-09-29 2013-01-08 GM Global Technology Operations LLC Fuel control system and method for more accurate response to feedback from an exhaust system with an air/fuel equivalence ratio offset

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5535181A (en) * 1978-09-05 1980-03-12 Nippon Denso Co Ltd Air fuel ratio control device
JPH0417747A (ja) * 1990-05-07 1992-01-22 Japan Electron Control Syst Co Ltd 内燃機関の空燃比制御装置
JPH06213042A (ja) * 1992-12-21 1994-08-02 Ford Motor Co 内燃機関用排気ガスセンサシステムおよび酸素レベル信号供給工程
US5392598A (en) * 1993-10-07 1995-02-28 General Motors Corporation Internal combustion engine air/fuel ratio regulation
JPH0821283A (ja) * 1994-07-08 1996-01-23 Unisia Jecs Corp 内燃機関の空燃比制御装置

Also Published As

Publication number Publication date
WO1999030022A1 (fr) 1999-06-17
ES2177099T3 (es) 2002-12-01
DE69806964D1 (de) 2002-09-05
EP1036269A1 (fr) 2000-09-20
JP4054529B2 (ja) 2008-02-27
FR2772078A1 (fr) 1999-06-11
DE69806964T2 (de) 2002-12-05
JP2001526353A (ja) 2001-12-18
FR2772078B1 (fr) 2000-02-18

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