This application claims priority to Italian Patent Application No. RM2007A385, filed Jul. 12, 2007, which is incorporated herein by reference in its entirety.
The present invention generally relates to a method for estimating a pressure drop between two sections of an exhaust line of a diesel engine.
It is known that the pressure drop between any two sections of a fluid line is mainly a function of the mass flow rate of the fluid circulating in it. In case of an exhaust line, it is not convenient to measure directly the exhaust mass flow, but in most control strategies for diesel engines flow rates of fresh air and of fuel supplied to the engine are known, so that the exhaust gas mass flow can easily be calculated from these. Accordingly, it is suggested in EP 1 081 347 B1, for example, to estimate a pressure at a downstream side of a particulate filter using a function f(WDPF, Tb) of exhaust gas flow rate WDPF and exhaust gas temperature Tb, where WDPF is the sum of fresh air flow rate and fuel flow rate.
The function f is a polynomial, the coefficients of which are identified from experimental data. This method is rather tedious to implement, since a large quantity of experimental data is necessary to fit the polynomial f in the two variables WDPF, Tb. Further for estimating the pressure Pb downstream of the particulate filter, the temperature Tb at the downstream side of the filter has to be known. So, either a sensor must be provided for measuring Tb, or a mathematical model must be developed for calculating it.
In view of the foregoing, it is at least one object to provide a method for estimating a pressure drop between two sections of an exhaust line of a diesel engine which is easier and quicker to implement than conventional methods. In addition, other objects, desirable features, and characteristics will become apparent from the subsequent summary and detailed description and the appended claims, taken in conjunction with the accompanying drawings and this background.
The at least one object, other objects, desirable features, and characteristics, is achieved by a method comprising the steps of measuring a fresh air flow rate into the engine, measuring a fuel flow rate into the engine, calculating an exhaust gas flow rate from the fresh air and fuel flow rates, and determining an estimated pressure drop as a function of the exhaust gas flow rate, which is characterized in that the exhaust gas flow rate is calculated as a weighted sum of the fresh air and fuel flow rates, and a weighting factor of the fuel flow rate is higher than a weighting factor of the fresh air flow rate.
It appears that using such a weighting factor, temperature dependency of the pressure drop can be taken account of in a very simple and straightforward fashion.
Experiments have shown that the weighting factor of the fuel flow rate should be at least twice that of the fresh air flow rate, and that it should preferably be in a range between about 5 and 30 times that of the fresh air flow rate.
The function yielding the pressure drop preferably is a polynomial in the exhaust gas flow rate, and it may have the exhaust gas flow rate as its only variable.
If the method is applied to an exhaust line and one of the sections comprises a pressure sensor and the other section comprises a second sensor which gives pressure dependent readings, the method preferably further comprises the steps of calculating a pressure in the other section based on a pressure reading from the pressure sensor and the estimated pressure drop, and of compensating a reading from the second sensor based on the calculated pressure. Such a second sensor can be an oxygen sensor, for example.
Alternatively, one of the sections may be a downstream end of the exhaust line. Since the downstream end is necessarily always at ambient pressure, it is possible to calculate the pressure in any other section of the exhaust line without having to use a pressure sensor.
The present invention will hereinafter be described in conjunction with the following drawing figures, wherein like numerals denote like elements, and
The following detailed description is merely exemplary in nature and is not intended to limit application and uses. Furthermore, there is no intention to be bound by any theory presented in the preceding background or the following detailed description.
In order to estimate a pressure drop between any two points of the exhaust system or between a given point of the exhaust system and the outside environment, the mass flow through the exhaust system must be known. Conventionally, an airflow sensor 9 is provided in the intake manifold of the engine for detecting the fresh air flow into the cylinders, and the fuel supplied to the cylinders is metered and is thus known, too. vIt can therefore be concluded that the mass flow rate me of the exhaust gas expelled from the engine block 1 should be the sum {dot over (m)}e={dot over (m)}a+{dot over (m)}f of fresh air flow rate {dot over (m)}a and fuel flow rate {dot over (m)}f. vIt is found, however, that based on a thus calculated exhaust gas flow rate, a completely reliable prediction of a pressure drop in the exhaust system is not possible. This is not so surprising, because it is known that the pressure drop depends not only on the mass flow rate, but also on the temperature of the flowing gas, and this temperature may vary according to the operating conditions of the engine. Surprisingly, however, it was found that this influence can be taken account of by replacing the above algebraic mass flow by a weighted mass flow M given by {dot over (M)}={dot over (m)}a+k{dot over (m)}f, where k is a positive constant.
The optimum value of the weighting coefficient k may depend to a certain extent on the characteristics of the engine. However, the optimum weighting coefficient for a given engine may be obtained quite straightforwardly by obtaining experimental data of pressure drop Δp, fresh air flow rate {dot over (m)}a and fuel flow rate {dot over (m)}f, and carrying out a least-squares fit for polynomial coefficients a2, a1 and weighting factor k in formula Δp=a2({dot over (m)}a+k{dot over (m)}f)2+a1({dot over (m)}a+k{dot over (m)}f).
While at least one exemplary embodiment has been presented in the foregoing summary and detailed description, it should be appreciated that a vast number of variations exist. It should also be appreciated that the exemplary embodiment or exemplary embodiments are only examples, and are not intended to limit scope, applicability, or configuration in any way. Rather, the foregoing detailed description will provide those skilled in the art with a convenient road map for implementing an exemplary embodiment it being understood that various changes may be made in the function and arrangement of elements described in an exemplary embodiment without departing from the scope set forth in the appended claims and their legal equivalents.
Number | Date | Country | Kind |
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RM2007A385 | Jul 2007 | IT | national |