Method of determining distribution of vapors in the intake manifold of a banked engine

Information

  • Patent Grant
  • 6167877
  • Patent Number
    6,167,877
  • Date Filed
    Friday, January 15, 1999
    25 years ago
  • Date Issued
    Tuesday, January 2, 2001
    23 years ago
Abstract
A method is provided for accommodating the purge vapors from an evaporative emission control system of an automotive vehicle. The method includes a means of learning the bank-to-bank distribution of purge vapors within the engine manifold. As such, the fuel to air ratio delivered from various injectors can be selectively controlled to accommodate the purge vapor at that bank of the engine and maintain the desired fuel to air ratio.
Description




BACKGROUND OF THE INVENTION




1. Technical Field




The present invention relates generally to evaporative emission control systems for automotive vehicles and, more particularly, to a method of compensating for purge vapors from an evaporative emission control system for an automotive vehicle.




2. Discussion




Modern automotive vehicles typically include a fuel tank and an evaporative emission control system that collects volatile fuel vapors generated in the fuel tank. The evaporative emission control system includes a vapor collection canister, usually containing an activated charcoal mixture, to collect and store volatile fuel vapors. Normally, the canister collects volatile fuel vapors which accumulate during refueling of the automotive vehicle or from evaporation of the fuel. The evaporative emission control system also includes a purge valve placed between an intake manifold of an engine of the automotive vehicle and the canister. At certain times conducive to purging, the purge valve is opened by an engine control unit an amount determined by the engine control unit to purge the canister, i.e., the collected volatile fuel vapors are drawn into the intake manifold from the canister for ultimate combustion within a combustion chamber of the engine.




As one skilled in the art will appreciate, the entry of purge vapors into the combustion chambers of the engine change the combustion characteristics of the engine. More particularly, the presence of purge vapors in the intake manifold change the required amount of fuel injected from the fuel injectors to maintain optimum drivability. Injecting too much fuel in the presence of the purge vapors causes an improper fuel to air ratio which may result in incomplete combustion, rough engine operation and poor emissions.




Although prior art methods of accounting for purged volatile fuel vapors from the evaporative emission control system have achieved favorable results, there is room for improvement in the art. For instance, it would be desirable to provide a method of identifying the source of the vapors from within the evaporative emission control system based on source characteristics, anticipating variations in the level of purge vapors using learned information from the identified source, and adjusting the amount of fuel delivered from the fuel injectors in accordance with the variations and sources of the purge vapors to maintain a desired fuel to air ratio.




SUMMARY OF THE INVENTION




It is, therefore, one object of the present invention to provide a method of accounting for purge vapors in an evaporative emission control system of an automotive vehicle.




It is another object of the present invention to provide a method of learning the concentration of purge vapor, identifying the source of the purge vapor, and predicting variations in purge vapor concentrations as a function of purge flow.




It is yet another object of the present invention to provide a method of identifying the appropriate time to initiate a purge cycle, providing the appropriate flow conditions such that the concentration of purge vapor can be learned, and controlling the purge flow rate such that purge vapors are depleted from the system.




It is still yet another object of the present invention to provide a method for predicting the concentration of purge vapor at the purge valve of the evaporative emission control system as a function of purge flow and accumulated flow through the canister.




It is another object of the present invention to provide a method of learning changes in the mass of the canister such that a mass of purge vapor in the canister can be determined.




It is yet another object of the present invention to provide a method of learning the flow rate of purge vapors from the fuel tank such that the fuel delivered through the injectors can be controlled under varying air flow and purge flow conditions.




It is still yet another object of the present invention to provide a method of accounting for a predictable purge vapor surge from the canister to provide improved fuel to air control and emissions results.




It is another object of the present invention to provide a method of learning the distribution of purge vapors within the engine manifold such that the amount of fuel delivered from various injectors can be selectively controlled to accommodate the purge vapor at that location of the engine.




To achieve the foregoing objects, the present invention provides a method of accounting for purge vapors in an evaporative emission control system of an automotive vehicle. The method includes a purge compensation model for identifying the concentration of purge vapor entering the intake manifold of the engine, identifying the source of the vapor as from the vapor collection canister or the fuel tank, and using this information to predict variations in vapor concentrations as a function of purge flow. Preferably, predicting variations in vapor concentrations is accomplished by using a physical model of the mass of air flow through the purge valve (based on air density). The mass of air flow is then modified based on the density of hydrocarbon for the learned concentration of purge vapors in the system. The method also includes a purge control model which uses mode logic to identify an appropriate time to initiate a purge cycle, provides the flow conditions necessary for a learning portion of the purge compensation model and increases purge flow rates after the learning is complete to deplete the contents of the canister. The purge control model also manages the time spent with purge active (learning purge) and purge inactive (learning volumetric efficiency or EGR). Preferably, the mode logic initiates a sequence of purge-active/purge-inactive cycles based on the learned parameters of the system through oxygen-sensor feedback. The following sequence is performed to learn the required parameters: a) learn the volumetric efficiency of the engine; b) learn the concentration and stability of the purge vapor during a low flow condition to identify a level of canister loading; c) increase purge flow through the purge valve using the learned canister information and learn deviations from a canister surface (i.e., model) as a function of tank flow; and d) repeat (a) and (c) indefinitely for the remainder of the drive.




As described in greater detail below, the present invention characterizes purge valve flow by using a surface for determining air mass flow rate as a function of vacuum at the purge valve and purge valve current. The flow through the valve is used to compute instantaneous flow rate and accumulated flow rate. A tactical adaption routine provides short term purge compensation (i.e., a tactical error term) through use of oxygen sensor feedback using proportional-integral control on an oxygen sensor integral error to tactically account for the purge concentration at the intake manifold. This term eventually forms the basis for all learning within the purge system.




The tactical adaption routine allows the system to maintain control and stability in the oxygen sensor feedback part of the methodology by extracting the integral error and learning it as representing purge concentration. By regulating the learning rate of the tactical adaption routine (O


2


rate/10) and a strategic adaption routine described below (O


2


rate/100), the learning of a quasi-steady state purge vapor concentration is made possible. Also, due to the controlled learning rate, the ability to disseminate the level of short term purge compensation (i.e., the tactical error term) into the appropriate source (canister loading or tank flow rate) is made possible without losing control stability.




The strategic adaption routine is performed to direct the tactical error term to a canister model for learning canister loading or to a fuel tank model for learning tank vapor flow rates. The strategic adaption routine also combines the tactical error term and the contribution from the canister and fuel tank models to yield a total purge concentration at the manifold.




The canister model uses the output of the strategic adaption routine to learn the loading of the canister. Thereafter, the canister model uses the learned tank flow rate from the tank model to compute the mass balance of purge vapor exiting and entering the canister. Based on the current loading of the canister, an open loop surface of canister concentration as a function of flow rate and accumulated flow is used to predict how the concentration will change as the flow rate through the canister changes.




The fuel tank model uses the output of the strategic adaption routine to learn the tank vapor flow rate. This flow rate is used to maintain fuel to air control under varying air flow and purge flow conditions especially under return-to-idle situations. Fuel tank flow rate is important because it can contribute to large variations in purge concentrations at the purge valve, and thus the entry to the manifold. This occurs when the tank vapor flow rate approaches the flow rate of the purge valve during low airflow conditions such as during idle, low load situations. Since the concentration of vapor from the tank is about 100%, as the purge valve flow approaches the tank flow, large variations in purge concentration at the manifold can be observed. Prior art methods of control which use a single adaptive cell to learn purge concentration typically exhibit rich fuel/air excursions on return to idle conditions resulting in HC emissions, and lean excursions on accelerations from idle resulting in NOX emissions. Learning the tank flow rate properly reduces these occurrences and, when coupled with closed loop feedback, these occurrences can be virtually eliminated.




A purge transport delay in the form of a first-in-first-out shift register is used to account for the delay that occurs in flow as the purge valve position is changed. Each position in the register is identified by a time and loaded from one side with the instantaneous flows as they occur at the valve. A table consisting of transport delays controls the delay time used per flow rate. Generally, low flows are given long delays and high flows are given shorter delays as measured on the system. The transport delay provides part of the timing required to determine when to compensate for a flow of purge vapors into the manifold by reducing the amount of fuel injected into the port. The remaining delay time is accounted for by the filling of the Intake Manifold. By timing the compensation correctly, the desired fuel/air ratio can be maintained for improved emissions and drive quality.











BRIEF DESCRIPTION OF THE DRAWINGS




In order to appreciate the manner in which the advantages and objects of the invention are obtained, a more particular description of the invention will be rendered by reference to specific embodiments thereof which are illustrated in the appended drawings. Understanding that these drawings only depict preferred embodiments of the present invention and are not therefore to be considered limiting in scope, the invention will be described and explained with additional specificity and detail through the use of the accompanying drawings in which:





FIG. 1

is a schematic diagram of an evaporative emission control system according to the present invention;





FIG. 2

is a diagrammatic representation of a method of purging the evaporative emission control system of

FIG. 1

according to the present invention;





FIG. 3

is a more detailed view of the purge compensation model portion of the method of

FIG. 2

;





FIG. 4

is a more detailed view of the tactical adaption portion of the purge compensation of

FIG. 3

;





FIG. 5

is a more detailed view of the strategic adaption portion of the purge compensation model of

FIG. 3

;





FIG. 6

is a graphic illustration of a three-dimensional surface used for determining purge fuel concentration.





FIG. 7

is a more detailed view of the canister model portion of the purge compensation model of

FIG. 3

;





FIG. 8

is a more detailed view of the fuel tank model portion of the purge compensation model of

FIG. 3

;





FIG. 9

is a more detailed view of the purge transport delay portion of the purge compensation model of

FIG. 3

; and





FIG. 10

is a diagrammatic illustration of the bank-to-bank distribution correction portion of the method of the present invention.











DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS




Referring now to the drawing figures,

FIG. 1

illustrates an evaporative emission control system


10


for an automotive vehicle. The evaporative emission control system


10


generally includes a fuel tank


12


connected to a vapor collection canister


14


by a vapor conduit


16


. As can be appreciated, this is merely a representative example of several possible means by which the fuel tank


12


may be connected to the canister


14


. An intake manifold


18


is connected to the canister


14


by a conduit


20


. A purge valve


22


is mounted along the conduit


20


. The control system


10


also includes an engine control unit (not shown) connected to and operative for controlling the purge valve


22


.




In operation, a supply of volatile liquid fuel for powering an engine of the automotive vehicle is placed in the fuel tank


12


. As fuel is pumped into the fuel tank


12


, or as the fuel evaporates, vapors from the fuel pass through the conduit


16


and are collected and stored in the canister


14


. Although the purge valve


22


is normally closed, under certain vehicle operating conditions conducive to purging, the engine control unit operates the purge valve


22


such that a certain amount of engine intake vacuum is applied to the canister


14


. The intake vacuum draws the collected vapors from the canister


14


through the conduit


20


and the purge valve


22


. From the purge valve


22


, the vapors flow into the intake manifold


18


for combustion in the combustion chambers. As such, the vapors are purged from the system.




Turning now to

FIG. 2

, a diagrammatic representation of a method for depleting the purge vapors from the evaporative emission control system


10


of

FIG. 1

is illustrated. The method generally includes two primary routines referred to as the purge control model


24


and the purge compensation model


26


. The purge control model


24


begins by receiving a number of input parameters generally indicated at


28


. The purge control model


24


uses the input parameters


28


to set a flag such that a preselected mode of operation is commanded based on the given environmental, operational, and feedback indicators available to the system. The input parameters


28


which are presently preferred include:




a) An oxygen sensor integral value which provides feedback information regarding the level of fuel control error (i.e., tactical error) present in the system. If purge is disabled this is viewed as a volumetric efficiency error or an EGR error. If purge is enabled this is viewed as purge concentration error.




b) An airflow value of the level of air flowing into the manifold as measured by a mass airflow sensor or calculated using a manifold pressure sensor. This provides a target flow that the purge valve attempts to match a fraction of when enabled. Tracking a continuous fraction of airflow yields a quasi stead-state ratio of HC from purge to air which simplifies the fuel compensation task.




c) A coolant temperature value which is used to identify the thermal conditions required for volumetric efficiency learning to occur and initiates a timer for a volumetric efficiency learn window at the end of which purge will initiate.




d) A closed loop flag is used since oxygen sensor feedback is relied upon for initially learning the purge concentration. This flag, which indicates that closed loop feedback is available, is required for enabling a purge event.




e) An RPM value (Engine Speed in Revolutions Per Minute) is used to indicate a start or stall condition under which the mode logic described below is reset.




f) A purge percent value, which is the calculated purge percent from the last pass through the purge model, and is used to determine the desired fraction of engine airflow to match at the purge valve and when to disable purge if the purge percentage falls below a calibrated threshold. This threshold indicates a clean canister.




g) A DFSO flag (Deceleration Fuel Shut Off) is used to indicate when purging is to be temporarily disabled. Since the flow of injected fuel is stopped during DFSO, the purge flow must be stopped or incomplete combustion will occur resulting in poor emissions.




Depending upon the values of the input parameters


28


, the methodology uses mode logic


29


to command the automotive vehicle engine to operate in one of three modes


30


,


32


, or


34


. In mode


0


, generally indicated at


30


, the purge feature of the present invention is disabled and the methodology learns the volumetric efficiency or EGR of the automotive vehicle engine. If the automotive vehicle is operating in mode


1


, generally indicated at


32


, the purge flow is relatively low. As such, the methodology learns the level of canister loading. If the automotive vehicle is in mode


2


, generally indicated at


34


, a high flow of purge vapor is available. As such, the methodology depletes the stored vapor from the evaporative emissions control system.




The following OR conditions determine that the vehicle should be commanded to operate in mode


0


:




a) RPM is below a calibrated lower limit value (or fuel delivery mode is not in run mode);




b) Fuel control is in open loop;




c) DFSO is active;




d) Purge percentage is less than a calibrated lower limit value for a calibrated time;




e) Modeled canister mass is less than a calibrated lower limit value for a calibrated time; OR




f) Oxygen sensor integral value is exceeding a calibrated upper limit value for a calibrated time (indicating lack of control).




The following AND conditions determine that the vehicle should be in mode


1


(purge enabled in low flow mode—learning canister loading):




a) Fuel control is in closed loop;




b) DFSO is not active;




c) RPM is above a calibrated lower limit threshold (or fuel delivery mode is in run mode);




d) Oxygen sensor integral value is below a calibrated threshold for entering mode


1


(meaning volumetric efficiency is learned in the current cell);




e) A calibrated time has elapsed while conditions were present for learning volumetric efficiency (as defined by the coolant temperature and closed loop inputs); AND




f) Mode


1


has not been completed during this drive cycle.




The following AND conditions determine that the vehicle should be operating in mode


2


(purge enabled in high flow mode—learning tank flow):




a) Fuel control is in closed loop;




b) DFSO is not active;




c) RPM is above a calibrated lower limit threshold (or fuel delivery mode is in run mode);




d) A minimum volume has been purged from the canister as calculated in an accumulated mass variable routine in the purge model below. This is to ensure that a sufficient portion of the canister surface (i.e., model) which is suitable for learning the canister loading is has been sampled;




e) Purge percentage is not below a calibrated lower limit threshold for a calibrated amount of time; AND




f) Modeled canister mass is not less than a calibrated lower limit value for a calibrated time.




After commanding the proper mode of operation at block


24


, the methodology continues to a flow control system


35


. The system


35


includes a control block


36


wherein limits and ramp rates are applied. Limits are applied to the commanded flow through the purge valve in modes


1


and


2


based on the desired type of control. In mode


1


, the rate of purge flow is limited to a calibrated low flow level to ensure that enough flow is available for learning the level of purge concentration but is also limited to avoid large fuel/air deviations due to the presence of purge vapors in the intake manifold that have not yet been learned. In mode


2


, the rate of purge flow is limited to a calibrated maximum flow level for high flow mode (depending on the tolerance of the engine to purge, i.e., cylinder to cylinder distribution characteristics etc.). This may be done to prevent drive issues, or more commonly to limit the commanded purge flow to that level at which the purge valve can flow under the give pressure delta across the part. From block


36


, the methodology advances to block


38


and calculates a desired purge flow rate through the purge valve as a percentage or fraction of the rate of air flow through the engine. From block


38


the methodology advances to block


40


and looks-up the appropriate proportional purge solenoid current for the desired flow through the purge valve.




The result of blocks


36


,


38


, and


40


are sent to the purge valve


22


of

FIG. 1

as a commanded proportional purge solenoid current, generally indicated at


42


, to allow a given rate of purge flow to pass therethrough. In addition to the commanded proportional purge solenoid current


42


, a commanded proportional purge solenoid flow value (i.e., the amount of purge flow) results from blocks


36


,


38


, and


40


. The commanded proportional purge solenoid flow value, generally indicated at


44


, is sent to the purge compensation model


26


for further processing.




In the purge compensation model


26


, the commanded purge flow value


44


is used as feedback such that the correct purge flow, purge concentration and corresponding HC mass can be calculated. These values are then used to anticipate the amount of fuel compensation required at the fuel injectors to accommodate the change in purge flow into the manifold. Further, the commanded proportional purge solenoid flow value


44


is combined with an oxygen sensor integral error


46


(i.e., the tactical error or short term purge concentration value) at a vapor adaptive calculation routine


48


of the purge compensation model


26


. The oxygen sensor integral error is used to fine tune the value of the actual concentration of purge vapors and ultimately to adjust fuel compensation for any errors that are not comprehended by the purge compensation model


26


.




As described, the vapor adaptive calculation routine


48


provides a short term purge compensation value (i.e., tactical error) to account for the purge concentration at the manifold. The short term purge compensation value is provided through use of oxygen sensor feedback in the form of the oxygen sensor integral error. The purge compensation value is used to vary the amount of fuel delivered through the injectors to maintain a desired fuel to air ratio in the presence of the purge vapors. Further, the short term purge compensation value forms the basis for all learning within the purge compensation model


26


.




From the vapor adaptive calculation routine


48


, the methodology advances to a strategic or purge adaption routine


50


. The purge adaption routine


50


directs the vapor adaption calculation result (i.e., the short-term purge compensation value) to a canister model


52


for learning the level of canister loading or to a fuel tank model


54


to learn tank vapor flow rate. The short term purge compensation value, the level of canister loading, and fuel tank flow rate are used to yield a total purge concentration. This total purge concentration is then used in a purge transport delay routine


56


.




The purge transport delay routine


56


accounts for the delay that occurs in flow as the purge valve position (and thus the purge flow rate) is changed. As such, changes in the amount of fuel injected are not made until the new purge flow concentration reaches the intake manifold of the engine. From the purge transport delay routine


56


, the methodology advances to a manifold filling routine


58


. In the manifold filling routine


58


, the injectors along each bank of the automotive vehicle engine are selectively adjusted to accommodate the amount of purge vapor present in that bank.




Referring now to

FIG. 3

, a more detailed view of the purge compensation model


26


is illustrated. Although not illustrated, one skilled in the art will appreciate that the purge compensation model


26


, as well as the remainder of the present invention, is performed in a controller of the automotive vehicle within which it is implemented, such as the engine control unit. Initially, the average of both banks' oxygen sensor integral error


46


, which is representative of the purge vapor concentration, is fed into a tactical adaptive routine


48


, formerly referred to in

FIG. 2

as the vapor adaptive calculation routine


48


. In the tactical adaptive routine


48


, the methodology learns the unlearned concentration of vapor required to drive the integral error


46


to zero. That is, an integral error


46


which is not zero indicates that the fuel to air ratio within the injectors is not optimum due to the presence of purge vapors. By learning the concentration of vapors, the fuel delivered by the injectors may be adjusted (i.e., reduced) such that the desired fuel to air ratio is achieved. This will be indicated when the integral error


46


equals zero.




Referring momentarily to

FIG. 4

, a more detailed illustration of the tactical adaptive routine


48


is illustrated. The average oxygen sensor integral error


46


is sent to an integral error calculation block


60


and to a proportional error calculation block


62


of a proportional-integral controller. The results of the integral error calculation


60


and the proportional error calculation


62


are summed at block


64


and the result is the vapor adaptive error term


66


(formerly referred to as the tactical error or short term purge compensation value). The vapor adaptive error term


66


forms the basis for all learning within the purge system. That is, the vapor adaptive error term


66


represents the purge vapor concentration level that has not yet been properly accounted for in the canister and/or tank models. The goal of the system is to drive this error to “zero” by properly learning the unaccounted for purge concentration into the appropriate canister or tank model.




Referring again to

FIG. 3

, the vapor adaptive error term


66


is sent to the strategic adaptive routine


50


, formerly referred to in

FIG. 2

as the purge adaption routine


50


, for directing the vapor adaptive error term


66


to the appropriate model (i.e., canister model or fuel tank model). The direction of the vapor adaptive term


66


depends upon the purge mode (i.e., mode


0


, mode


1


, or mode


2


) within which the vehicle is operating as described above. The strategic adaptive routine


50


also slows the learning rate of the system for stability. The goal of the strategic adaptive routine


50


is to drive the vapor adaptive error term


66


to zero. The criteria for redirecting the learning from canister mass (in Mode


1


) to Tank Flow Rate (Mode


2


) is made by the mode logic routine


29


described above. The main criteria for this transition is based upon the amount of flow that has passed through the canister (i.e., accumulated canister flow) in mode


1


.




Referring momentarily to

FIG. 5

, a more detailed view of the strategic adaptive routine


50


is illustrated. The vapor adaptive error term


66


is applied to a gain at


68


and is then sent as a concentration correction value


70


to the canister/tank flow learning logic


72


. In the canister/tank flow learning logic


72


, the concentration correction value


70


is combined with an accumulated canister purge mass value


74


at a time when a purge active indicator


76


is set. The accumulated canister purge mass value


74


is calculated by integrating the calculated instantaneous purge valve mass flow rate minus the calculated tank mass flow rate and using this value to indicate when the system is “viewing” a portion of the canister surface (SEE

FIG. 6

) with a reduced slope (the larger the slope, the more difficult the learning). The resulting output of the canister/tank flow learning logic


72


is a canister mass correction value


78


and a fuel tank mass flow rate correction flag


80


.




Referring again to

FIG. 3

, from the strategic adaptive routine


50


, the canister mass correction value


78


is forwarded in mode


1


to the canister model


52


. Similarly, the fuel tank mass flow rate correction flag


80


is outputted from the strategic adaptive routine


50


in mode


2


to the fuel tank model


54


.




Referring momentarily to

FIG. 6

, a three-dimensional surface for use in conjunction with the canister model


52


is illustrated. The surface includes a purge fuel fraction input along the z-axis, purge flow rate (or % duty cycle applied to the purge valve depending on the type of device) along the x-axis and accumulated purge flow along the y-axis. The open loop canister surface is the central mechanism around which purge concentration learning occurs. By using the output of the surface as a baseline of what should occur from a system with canister input only, any deviations from these predictions can be attributed to tank vapor flow rate which is the only other possible input to the system.




The open loop surface describes the concentration level that can be expected based on the current purge valve mass flow rate and the accumulated canister purge mass flow. This surface is calibrated in a controlled environment by setting the valve flow rate constant and measuring the concentration obtained from the canister device (measurement can be achieved through feedback calculation or by direct sensor measurement). Accumulated canister flow is calculated during this process and concentration is mapped against this axis.




Since this surface is generated using a canister that is loaded to maximum capacity, the maximum concentration from the canister at any given flow condition is known. By learning what fraction of that maximum concentration is being measured (through feedback) an estimate of the loading (a fraction of a fully loaded canister) can be learned in mode


1


. Once the canister loading is learned in mode


1


, the trajectory or path to be followed through the surface is known if the canister is the only source of vapor. This is achieved by multiplying the canister loading fraction by the output of the canister surface. Since the majority of driving conditions result in tank flows that are a minor contributor of purge vapors in relation to the canister, this method results in a very feasible approach to the problem. That is, deviations from the learned path are the result of another source of vapor. Since there is only one other source, it must be the tank flow rate. It should be noted that the level of canister loading represents the ratio of the mass in grams of HC present in the canister relative to the maximum measured mass of the HC content under a 1.5× canister load on a loading bench.




Referring now temporarily to

FIG. 7

, a more detailed view of the canister model


52


is illustrated. The purge valve mass flow rate


84


is used with the fuel tank mass flow rate


88


at block


92


to yield a net mass flow to the canister


94


. The net mass flow to the canister


94


is used with the canister mass correction value


78


at block


96


in a canister conservation of mass calculation. The canister mass


98


is used to determine the duration of purge in the purge mode logic.




The canister conservation of mass calculation


96


is performed by the following equation:




Net Mass Flow from Canister


94


=Purge Valve Mass Flow Rate (HC)


84


—Fuel Tank Mass Flow Rate;




Mass depleted from the canister this software cycle=Net Mass Flow from Canister


94


* Interval Time (sec.); and




Canister Mass


98


=Previous Canister Mass—Mass Depleted from the canister this software cycle.




If the Mode=


1


(meaning canister learning is occurring):




Canister Mass=Previous Canister Mass—Mass Depleted from the canister this software cycle+Canister Loading Adapt


78


(Note that this also allows large tank flow rates to increase the canister mass under low flow conditions.)




Else:




Canister Mass=Previous Canister Mass—Mass Depleted from the canister this software cycle;




Canister Loading Fraction


100


=Canister Mass


98


/Maximum Calibrated Canister Mass; and




Modeled Concentration from the Purge Canister


90


=Canister Loading Fraction


100


*Open Loop Canister Surface value of concentration (as a function of flow and accumulated flow).




The canister loading fraction


100


is used with the purge valve mass flow rate


84


and the accumulated canister purge mass flow


82


at block


102


to yield a model concentration value


90


from the purge canister. For example, if 10% concentration is learned and the outer limit surface has a maximum value of 20% for the current flow and accumulated flow, then the load faction is {fraction (10/20)} or 0.5 such that from that point forward the outer limit value *0.5 gives the actual concentration as the canister is depleted. If the canister is the only source of vapor, the job is done for the drive.




Referring again to

FIG. 3

, the fuel tank model


54


determines a flow rate of vapor from the fuel tank based on a learned value and a transient purge compensation value. That is, the fuel tank model


54


looks for the fuel tank mass flow rate correction flag


80


in order to combine the vapor adaptive error term


66


and the purge valve mass flow rate


84


to yield the fuel tank mass flow rate


88


. When in mode


2


, the vapor adaptive term


66


is used to learn the tank mass flow rate term up or down in order to drive the vapor adaptive term


66


to “zero”.




Referring momentarily to

FIG. 8

, the fuel tank model


54


is illustrated in greater detail. When the tank flow rate adapt flag


80


is set, the purge valve mass flow rate


84


and vapor adaptive error term


66


are combined with a gain term


104


at block


106


and then sent to a tank flow rate calculation block


108


. At block


108


, the difference between the purge valve mass flow rate


84


(i.e., the amount of purge vapor from the canister) and the vapor adaptive error term


66


. The tank flow rate calculation block


108


yields a fuel tank mass flow rate


88


which is fed back to the canister model


52


(see

FIG. 3

) as well as to a lookup surface block


110


for combination with the accumulated canister purge mass flow value


112


to yield a transient additive concentration value


114


.




Based on the level of tank flow rate present, the surface provides an additive amount of concentration over time following a purge valve shut off condition such as a long deceleration with purge off (in DFSO). This additive concentration represents the buildup of vapor in the dome of the canister and the upper regions of the carbon in the canister as the tank flow saturates these areas while the valve flow is stopped. Without this feature, purge vapor surges would occur due to this buildup resulting in increased HC emissions and possible drive problems.




Referring again to

FIG. 3

, the canister model


52


outputs the canister concentration value


90


to the purge transport delay


56


for further processing. The purge transport delay routine


56


calculates the total concentration of vapor at the purge valve


116


and a transport delay


118


from the purge valve to the manifold. The purge transport delay routine


56


receives the vapor adaptive error term


66


from the tactical adaptive routine


48


, the fuel tank mass flow rate


88


, and transient additive concentration value


114


from the fuel tank model


54


, the canister concentration value


90


from the canister model


52


, the commanded proportional purge solenoid flow


42


based on the mode of operation, and the purge valve mass flow rate


84


.




Referring momentarily to

FIG. 9

, the purge transport delay routine


56


is illustrated in greater detail. The purge canister mass flow rate


84


is combined with the fuel tank mass flow rate


88


and canister concentration value


90


at block


120


to calculate a total modeled concentration of vapor at the purge valve from the canister and tank. The modeled concentration


122


is combined with the transient additive concentration


114


and the vapor adaptive error term


66


at block


124


to yield a concentration of vapor value


116


at the entry of the manifold. Further, the commanded proportional purge solenoid flow


42


is sent to a block


126


to look up the appropriate amount of delay time from a table. The resulting delay time


128


is used with the commanded proportional purge solenoid flow


42


at block


130


to yield a transport delay


118


to delay the flow into the manifold.




Referring again to

FIG. 3

, the percentage concentration of vapor


116


at the entry of the manifold is sent at the delay time


118


to the manifold filling equations


58


. Referring momentarily to

FIGS. 1 and 10

, the manifold filling equations


58


will now be described in greater detail. As is known, V-type engines include two banks of cylinders. These banks of cylinders are illustrated in

FIG. 1

as bank


1


and bank


2


. Depending on the nature of the air flow through the manifold


18


, more or less of the vapor concentration could end up in either bank


1


or bank


2


. As such, a vapor distribution correction value


133


is used.




In order to define the nature of the air flow through the manifold


18


, an oxygen sensor is used in each bank. By comparing the oxygen sensor values to one another, a pattern of the flow through the manifold


18


is obtained. Thus, referring to

FIG. 10

, an oxygen sensor feedback integral value


134


for bank


1


is combined with an oxygen sensor feedback integral value


136


for bank


2


at block


138


to yield an oxygen sensor integral difference value


140


. The oxygen sensor integral difference value


140


is combined with a distribution gain value


142


at block


144


when a distribution correction enable flag


146


is set. The resulting distribution value


148


of the combined oxygen sensor integral difference value


140


and distribution gain value


142


is integrated at integrator


150


(like an integral controller) and forwarded to a limiter


152


. The limiter


152


forces the integrated distribution value


148


to be between −1 and +1.




The resulting integrated and limited distribution value


154


is forwarded to block


156


. In block


156


, the value


154


is added to the output of an open-loop distribution correction table


160


. The open-loop table


160


is a function of input airflow rate, as defined by the sum of idle bypass flow and throttle flow


158


. This open loop table


160


reduces the feedback instability of distribution correction


132


. After the addition, the corresponding distribution correction value


132


is calculated.




The bank-to-bank distribution correction value


132


, hereinafter labeled “d”, is used as follows:




If:




a


1


=purge fuel flow for bank


1


; then




a


1


=port gas flow rate (bank


1


) *manifold purge concentration;




and if:




a


2


=purge fuel flow for bank


2


; then




a


2


=port gas flow rate (bank


2


) * manifold purge concentration.




Thus, if d<0:




fuel flow (from purge) into bank


1


=a


1


−d * a


2


; and




fuel flow (from purge) into bank


2


=(1+d) * a


2


;




and if d≧0:




fuel flow (from purge) into bank


1


=(1−d) * a


1


; and




fuel flow (from purge) into bank


2


=a


2


+d * a


1


.




It is worthwhile to note that when the calculated distribution correction d equals zero, purge flow follows the volumetric efficiency and air flow prediction. When d equals −1, all purge flow goes to bank


1


as shown in FIG.


1


. Also, when d equals 1, all purge flow goes to bank


2


as shown in FIG.


1


. Moreover, for single bank engines, d equals 0.




For the Fueling effect to be correctly compensated, the Purge concentration/mass flow at the entry to the intake manifold has to be converted into a concentration/mass flow at the intake port. This transformation is performed as part of the Manifold Filling block. Referring again to

FIG. 3

, after performing the manifold filling equations at block


58


, the port purge percent concentration


162


is sent to the engine controller such that the amount of fuel delivered from the fuel injectors is adjusted to accommodate the additional presence of the volatile fuel vapor. As such, the proper fuel to air ratio is maintained and drivability is improved.




Thus, the present invention provides a means for compensating for the presence of purge vapor in the combustion chambers of an automotive vehicle engine. More particularly, the amount of fuel delivered through each fuel injector is modified depending on the purge flow through a proportional purge solenoid of an evaporative emission control system of the vehicle. Depending on the source of the purge vapor and its flow, different modifications to the fuel to air ratio are implemented.




Those skilled in the art can now appreciate from the foregoing description that the broad teachings of the present invention can be implemented in a variety of forms. For example, the distribution correction and accompanying fuel flow calculations can be identically replicated for EGR (Exhaust Gas Recirculation) systems. Therefore, while this invention has been described in connection with particular examples thereof, the true scope of the invention should not be so limited since other modifications will become apparent to the skilled practitioner upon a study of the drawings, specification, and following claims.



Claims
  • 1. A method of learning bank-to-bank distribution of a desired gas within an intake manifold of an engine in an automotive vehicle comprising:determining an airflow condition in a first bank of said intake manifold through first oxygen sensor feedback; determining an airflow condition in a second bank of said intake manifold through second oxygen sensor feedback; obtaining a ratio of said airflow condition in said first bank to said airflow condition in said second bank to yield an airflow distribution value representing a distribution of airflow through said intake manifold; and delivering a first amount of fuel to said first bank and delivering a second amount of fuel to said second bank in accordance with said distribution value.
  • 2. The method of claim 1 wherein said distribution value represents a distribution of airflow through said first and second banks of said intake manifold.
  • 3. The method of claim 1 wherein said distribution value represents a distribution of said desired gas through said first and second banks of said intake manifold.
  • 4. The method of claim 1 further comprising:determining a flow rate of said desired gas at a valve of a gas system; looking up a delay time corresponding to said flow rate; and adjusting said delivery of fuel at said delay time.
  • 5. The method of claim 1 wherein said desired gas further comprises purge vapors of an evaporative emissions control system.
  • 6. The method of claim 1 wherein said desired gas further comprises exhaust gas from an exhaust gas recirculation system.
  • 7. A method of learning a distribution of a desired gas within an intake manifold of a banked engine in an automotive vehicle comprising:determining a first oxygen sensor feedback integral value for a first bank of said intake manifold; determining a second oxygen sensor feedback integral value for a second bank of said intake manifold; subtracting said first oxygen sensor feedback integral value from said second oxygen sensor feedback integral value to yield an oxygen sensor difference value; and independently adjusting a fuel delivery into said first and second banks of said intake manifold according to said difference value.
  • 8. The method of claim 7 wherein said oxygen sensor difference value represents a distribution of airflow through said first and second banks of said intake manifold.
  • 9. The method of claim 7 wherein said difference value represents said distribution of said desired gas through said first and second banks of said intake manifold.
  • 10. The method of claim 7 wherein said step of independently adjusting a fuel delivery to said first and second banks of said intake manifold further comprises changing an amount of fuel injected into said first and second banks at a ratio dictated by said difference value such that a desired fuel to air ratio is maintained in the presence of said desired gas.
  • 11. The method of claim 7 further comprising:determining a flow rate of said desired gas at a purge valve of an evaporative emissions control system; looking up a delay time corresponding to said flow rate; determining an intake port purge vapor concentration based on said flow rate of said desired gas; and adjusting said fuel delivery at said delay time.
  • 12. A method of learning a distribution of a desired gas within an intake manifold of a banked engine in an automotive vehicle comprising:determining a first oxygen sensor feedback integral value for a first bank of said intake manifold; determining a second oxygen sensor feedback integral value for a second bank of said intake manifold; comparing said first and second oxygen sensor feedback integral values to yield an oxygen sensor difference value; and independently adjusting a fuel delivery into said first and second banks of said intake manifold by changing an amount of fuel injected into said first and second banks at a ratio dictated according to said difference value such that a desired fuel to air ratio is maintained in the presence of said desired gas.
  • 13. The method of claim 12 wherein said step of comparing said first and second oxygen sensor feedback integral values further comprises subtracting said first oxygen sensor feedback integral value from said second oxygen sensor feedback integral value to yield an oxygen sensor difference value.
  • 14. The method of claim 12 wherein said oxygen sensor difference value represents a distribution of airflow through said first and second banks of said intake manifold.
  • 15. The method of claim 12 wherein said difference value represents said distribution of said desired gas through said first and second banks of said intake manifold.
  • 16. The method of claim 12 further comprising:determining a flow rate of said desired gas at a purge valve of an evaporative emissions control system; looking up a delay time corresponding to said flow rate; determining an intake port purge vapor concentration based on said flow rate of said desired gas; and adjusting said fuel delivery at said delay time.
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Entry
Pending patent application Ser. No. 09/079,706, filed May 15, 1998, entitled “Proportional Purge Solenoid Control System”, in the name of Blomquist et al.