METHOD FOR DETERMINING A QUANTITY OF FUEL INJECTED INTO AN INTERNAL COMBUSTION ENGINE
20220195958 · 2022-06-23
Inventors
Cpc classification
F02D41/28
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D2200/0608
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D2200/0602
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D2200/0614
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D2041/286
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D2041/1432
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D2250/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D2200/0616
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D41/40
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02D2200/0606
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
Abstract
A method for determining a quantity of fuel injected into a cylinder of an internal combustion engine including an injection rail includes:—measuring the pressure prevailing in the injection rail during fuel injection from the rail into a cylinder;—filtering the pressure measurement;—determining the relative minimum and maximum points of the filtered pressure curve;—insofar as a first (Pdrop1) pressure drop followed by a pressure rise and then a second (Pdrop2) pressure drop is identified, determining a physical quantity that makes it possible to characterize the first pressure drop and the second pressure drop; and—determining the quantity of fuel injected by applying the bulk modulus for the two pressure drops identified as a function of the temperature in the injection rail.
Claims
1. A method for determining a quantity of fuel injected into a cylinder of an internal combustion engine comprising an injection rail, the method comprising: measuring the pressure prevailing in the injection rail during fuel injection from the rail into a cylinder, filtering the pressure measurement, determining the relative minimum and maximum points of the filtered pressure curve, insofar as a first (Pdrop.sub.1) pressure drop followed by a pressure rise and then a second (Pdrop.sub.2) pressure drop is identified, determining a physical quantity that makes it possible to characterize the first pressure drop and the second pressure drop, determining the quantity of fuel injected by applying the bulk modulus for the two pressure drops identified as a function of the temperature in the injection rail, by determining, using the bulk modulus, an equivalent quantity of fuel injected that corresponds both to the first pressure drop (Pdrop.sub.1) and to the second pressure drop (Pdrop.sub.2), and adding them together.
2. The determination method as claimed in claim 1, further comprising the following step for the final determination of the quantity of fuel injected: adding a corrective term that is determined as a function of at least one of the two physical quantities characterizing the first (Pdrop.sub.1) pressure drop and the second (Pdrop.sub.2) pressure drop.
3. The determination method as claimed in claim 2, wherein the physical quantity selected characterizing the first (Pdrop.sub.1) pressure drop and the second (Pdrop.sub.2) pressure drop is the pressure variation.
4. The determination method as claimed in claim 3, wherein the corrective term is determined both as a function of at least one of the two pressure variations (Pdrop.sub.1, Pdrop.sub.2) and as a function of the total pressure variation (Pdrop.sub.tot), that is, the pressure variation between the start of injection and the end of injection.
5. The determination method as claimed in claim 1, wherein the physical quantity selected characterizing the first (Pdrop.sub.1) pressure drop and the second (Pdrop.sub.2) pressure drop is the duration of the pressure drop.
6. The determination method as claimed in claim 2, wherein the corrective term is determined both as a function of at least one of the two pressure drop durations and as a function of the time interval between the start of injection and the end of injection, that is between the start of the first (Pdrop.sub.1) pressure drop and the end of the second (Pdrop.sub.2) pressure drop.
7. The determination method as claimed in claim 1, wherein the filtering of the pressure measurement is analog hardware filtering.
8. The determination method as claimed in claim 1, wherein the temperature used for determining the quantity of fuel injected is an estimated temperature.
9. A device for controlling and managing an internal combustion engine, is the device being programmed to implement all of the steps of a method as claimed in claim 1.
10. A non-transitory computer-readable medium on which is stored a computer program containing instructions, which when executed by the device as claimed in claim 9, causes the device to execute the determination method.
11. The determination method as claimed in claim 1, wherein the physical quantity selected characterizing the first (Pdrop.sub.1) pressure drop and the second (Pdrop.sub.2) pressure drop is the pressure variation.
12. The determination method as claimed in claim 5, wherein the corrective term is determined both as a function of at least one of the two pressure drop durations and as a function of the time interval between the start of injection and the end of injection, that is between the start of the first (Pdrop.sub.1) pressure drop and the end of the second (Pdrop.sub.2) pressure drop.
13. The determination method as claimed in claim 2, wherein the physical quantity selected characterizing the first (Pdrop.sub.1) pressure drop and the second (Pdrop.sub.2) pressure drop is the duration of the pressure drop.
14. The determination method as claimed in claim 2, wherein the filtering of the pressure measurement is analog hardware filtering.
15. The determination method as claimed in claim 3, wherein the filtering of the pressure measurement is analog hardware filtering.
16. The determination method as claimed in claim 4, wherein the filtering of the pressure measurement is analog hardware filtering.
17. The determination method as claimed in claim 5, wherein the filtering of the pressure measurement is analog hardware filtering.
18. The determination method as claimed in claim 2, wherein the temperature used for determining the quantity of fuel injected is an estimated temperature.
19. The determination method as claimed in claim 3, wherein the temperature used for determining the quantity of fuel injected is an estimated temperature.
20. The determination method as claimed in claim 4, wherein the temperature used for determining the quantity of fuel injected is an estimated temperature.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0027] Further features, details and advantages of the invention will become apparent on reading the following detailed description and on analyzing the appended drawing, in which:
[0028]
[0029]
[0030]
[0031]
[0032]
DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0033] The drawings and descriptions below essentially contain elements of definite character. They can therefore not only be used to improve understanding of the present invention but also contribute to the definition thereof, as applicable.
[0034] Reference is now made to
[0035] Increasingly often, in an internal combustion engine, the fuel is injected at high pressure directly into the cylinders. In this case, the fuel is pumped out of the tank by a pump, also known as a booster pump, that can be immersed in the fuel tank or is otherwise located in immediate proximity to the tank. This pump makes it possible to pressurize the whole fuel circuit, from the tank to the cylinders of the engine. For the injection of the fuel into the cylinders, the pressure used is of the order of several hundred bar (1 bar=10.sup.5 Pa), for example approximately 200 bar. It is then known practice to pressurize fuel in an injection rail to a high pressure, for example using at least one other pump. The injection rail then supplies injectors so that when an injector opens, fuel from the injection rail is sent at high pressure into the corresponding cylinder.
[0036] The description below relates to the situation in which the high-pressure pump(s) is/are disabled. In this scenario, the pressure in the injection rail corresponds to the pressure supplied by the booster pump. In this case, the engine is working in a degraded operating mode.
[0037] In
[0038] It will be noted that when the control signal requests the opening of the injector, the pressure in the injection rail starts to drop. Surprisingly, it has been observed that after a first pressure drop, the pressure in the injection rail increases before falling again to reach a minimum pressure. This rise in the pressure in the rail can be explained by the vaporization of a portion of the fuel that is injected into the cylinder. This fuel is heated, part of it then vaporizes and the fuel vapor causes the pressure in the injection rail to rise.
[0039] Three pressure variations are illustrated in
[0040]
[0041]
[0042] It is known from the prior art to determine (or compute) a quantity of fuel injected as a function of the pressure variation measured. This determination depends on the characteristics of the injector and of the fuel, particularly the bulk modulus and temperature of the fuel. The bulk modulus of a given fuel is known. With regard to the temperature, a temperature sensor can provide the information but more often than not, this temperature is estimated on the basis of other measurements taken in the engine.
[0043] A person skilled in the art wishing to determine the quantity of fuel injected would thus do so on the basis of the value Pdrop.sub.tot. Here, it is proposed that the equivalent quantity of fuel injected corresponding both to Pdrop.sub.1 and to Pdrop.sub.2 be determined using the bulk modulus, and that these be added together. Let Qinj_eq.sub.1+2 be the equivalent quantity determined.
[0044]
[0045] where Qinj_eq.sub.1+2_20 is the equivalent quantity of fuel injected at a temperature of 20° C.
[0046] It will be noted that in
[0047]
[0048] In
[0049] The signal transmitted by the pressure sensor during the measurement taken in step 100 is filtered during a step 200 of the method. Preferably, the filtering is carried out with an analog hardware filter.
[0050] Once the signal from the pressure sensor has been filtered, this signal is acquired during a step 300. This acquisition preferably takes place at a high frequency, for example at a frequency of several kHz such as, by way of non-limiting example, 10 kHz. During this step 300 of acquiring the signal, the voltage transmitted by the sensor (and filtered) is converted into a value representative of the pressure prevailing in the injection rail. Digital filtering can also be envisaged during this step 300 after the acquisition of the signal.
[0051] Step 300 thus makes it possible to provide a curve giving the pressure prevailing in the injection rail as a function of time. This curve is analyzed in step 400 during the open period of an injector, optionally also shortly after the closing of the injector. The aim of this analysis is to determine the maximum and minimum pressures of the curve. As stated above, it has been noted that the pressure curve falls on the opening of the injector to a relative minimum, then rises before falling again to a minimum. The pressure curve is analyzed at least until the detection of this minimum that follows the closing of the injector. In order to determine these extreme values, conventionally, the relative minimum and maximum points of the curve are sought.
[0052] The analysis of the curve carried out in step 400 makes it possible, during a subsequent step 500, to determine the pressure variations in the injection rail. Here, the pressure drops are determined. Reference is made here to
[0053] Pdrop.sub.1 is the pressure difference between the first maximum determined on the opening of the injector and the first minimum pressure,
[0054] Pdrop.sub.2 is the pressure difference between the maximum pressure detected after the first minimum pressure and the minimum pressure just after the closing of the injector.
[0055] On the basis of the pressure differences Pdrop.sub.1 and Pdrop.sub.2, a step 600 provides the computation of the equivalent quantity of fuel injected for each of these pressure differences. Here, the computation is carried out particularly using the temperature of the fuel in the injection rail and also the bulk modulus.
[0056] In a variant embodiment for steps 500 and 600, instead of working directly with pressure differences, seconds (or microseconds) could be used as a physical quantity, and not Pascals. Instead of considering the pressure differences, the duration of the pressure drop could be considered. On the basis of these durations, it is also possible to determine an equivalent quantity of fuel injected, mainly as a function of the characteristics of the injector, the temperature and the bulk modulus of the fuel.
[0057] During this step 600, both a first equivalent quantity of fuel injected Qinj_eq.sub.1 corresponding to Pdrop.sub.1 and a second equivalent quantity of fuel injected Qinj_eq.sub.2 corresponding to Pdrop.sub.2 are thus determined. The total equivalent quantity is determined on the basis of these two partial quantities: Qinj_eq.sub.1+2=Qinj_eq.sub.1+Qinj_eq.sub.2
[0058] The value thus determined gives a good approximation of the equivalent quantity of fuel injected during the injection under consideration. However, provision is advantageously made to apply a corrective term to this equivalent quantity. It has been assumed, and observed, that not only do the absolute values of the pressure drops have an influence, but that the ratio between these values also has an influence. In order to take this ratio into account, it is proposed that a corrective term Qcorr be added that can be a function of Pdrop.sub.1 and/or Pdrop2 and Pdroptot or of a variable such as for example
Pdrop.sub.1/Pdrop.sub.tot
or
Pdrop.sub.2/Pdrop.sub.tot
or
(Pdrop.sub.1+Pdrop.sub.2)/Pdrop.sub.tot
or
[0059] (Qinj_eq.sub.1+Qinj_eq.sub.2)/(Qinj_eq.sub.tot) where Qinj_eq.sub.tot is the equivalent quantity of fuel injected for the pressure drop Pdrop.sub.tot.
[0060] If the decision was taken above to work with the duration of the pressure drops and not directly with the pressures themselves, the corrective term can be a function of:
[0061] T.sub.1 the duration of the first pressure drop, and/or
[0062] T.sub.2 the duration of the second pressure drop, and
[0063] T.sub.tot the duration between the start of the first pressure drop and the end of the second pressure drop,
[0064] or one of the variables:
T.sub.1/T.sub.tot
T.sub.2/T.sub.tot
(T.sub.1+T.sub.2)/T.sub.tot
or in this case also (Qinj_eq.sub.1+Qinj_eq.sub.2)/(Qinj_eq.sub.tot).
[0065] A curve then makes it possible to give the value of the correction to be applied to the equivalent quantity injected found above.
[0066] The corrective value is thus determined as a function of the measurements (pressure or time) taken in step 500, that is, Qcorr=f(Pdrop.sub.1, Pdrop.sub.2, Pdrop.sub.tot) or Qcorr=g (T.sub.1, T.sub.2, T.sub.tot). There could also be a map that gives the corrective value to be applied directly as a function of Pdrop.sub.1 and/or Pdrop.sub.2 and Pdrop.sub.tot (or T.sub.1 and/or T.sub.2 and T.sub.tot).
[0067] Determining the equivalent quantity of fuel injected, preferably with the corrective value, makes it possible to know what quantity of fuel has been injected and it is then possible to adjust the control of the injectors if a drift is observed relative to the setpoint given. As a result, operation in degraded mode is improved. This satisfactory knowledge of the quantity injected makes it possible to avoid combustion misfires linked to the injection, improve the adjustment of the richness of the air/fuel mix and therefore also improve the control of polluting emissions.
[0068] Of course, the present invention is not limited to the preferred embodiment described above or to the variants mentioned, but also covers variant embodiments within the competence of a person skilled in the art.