US 6,935,311 B2Grant
Engine control with fuel quality sensor
Issue Date:2005-08-30
•15 Claims
•13 Drawing Sheets
Abstract
A system is described using a fuel quality sensor for controlling various aspects of engine operation. In particular, an acoustic wave sensor is utilized to measure viscosity and density of gasoline fuels. This measurement is utilized to predict engine combustion quality during an engine start. Based on the prediction, the method adjusts engine operating parameters (such as fuel injection amount and ignition timing) to achieve improved vehicle driveability and engine combustion.
Metadata
Assignee
- Ford Global Technologies, LLC
Inventors
- Jacobus Hendrik Visser
- Allan Joseph Kotwicki
- Allan J. Lippa
- Carina Eva Irene Bjornsson
- Carol S. Smith
- Daniel Lawrence Meyer
- John D. Russell
- Michael Howard Parsons
- Philip William Husak
Application Information
Application Number:US 10/065,362
Filing Date:2002-10-09
Priority Date:2002-10-09
Art Unit:3747
Patent Drawings (13 sheets)
Description
Background of Invention
[0001] To ensure good cold-start driveability, the engine is fuelled to compensate for poor quality fuels, such as “hesitation fuel” (fuels with a high DI, or “driveability index”). Such a fuel can result in combustion that is leaner than expected given the amount of injected fuel. This can result in reduced engine speed during engine starting.
[0002] To reduce such speed drops, the engine control system can monitor engine speed. If engine speed drops too low after start-up, the fueling to the engine is increased to reduce the effects of such hesitation fuels. Such a system is described in U.S. Pat. No. 5,875,759.
[0003] However, the inventors herein have recognized several disadvantages with the above approach. In particular, for normal fuel types, of fuels with a low DI, the engine is still fueled too much since the basic calibration is for an “average” fuel. In addition, if the high DI fuels cause a decrease in engine speed (since the combustion is richer than expected), added fuel exacerbates the speed drop. Further, for hesitation (high DI) fuels, the system is reactive. I.e. the engine speed has already dropped and then action is taken. In some cases this action comes too late and the customer experiences a degraded starting or tip-in behavior.
Summary of Invention
[0004] The above disadvantages are overcome by various aspects of the present invention as defined in the claims.
[0005] In one example, the present invention can determine the fuel volatility and combustion characteristics based on a sensor. In this way, it can correct the amount of injected fuel commensurate with the fuel quality data.
[0006] An advantage of the present invention is improved cold-start emissions and driveability.
Brief Description of Drawings
[0007] FIG. 1 is a block diagram of an embodiment wherein the invention is used to advantage;
[0008] FIGS. 2A-C are schematic diagrams of an example acoustic wave fuel quality sensor;
[0009] FIGS. 3-4 are graphs illustrating sensor output for use with the present invention;
[0010] FIGS. 5-6 show experimental data illustrating the relationship between viscosity, density, and DI;
[0011] FIGS. 7-14 are high-level flow charts of various operations;
[0012] FIG. 15 is a graph illustrating transmission of the acoustic wave;
[0013] FIG. 17A is a graph showing operation according to one embodiment of the invention; and
[0014] FIG. 17B is a high level flow chart for learning fuel quality.
Detailed Description
[0015] Internal combustion engine 10 comprises a plurality of cylinders, one cylinder of which is shown in FIG. 2. Electronic engine controller 12 controls Engine 10. Engine 10 includes combustion chamber 30 and cylinder walls 32 with piston 36 positioned therein and connected to crankshaft 13. Combustion chamber 30 communicates with intake manifold 44 and exhaust manifold 48 via respective intake valve 52 and exhaust valve 54. Exhaust gas oxygen sensor 16 is coupled to exhaust manifold 48 of engine 10 upstream of catalytic converter 20.
[0016] Intake manifold 44 communicates with throttle body 64 via throttle plate 66. Throttle plate 66 is controlled by electric motor 67, which receives a signal from ETC driver 69. ETC driver 69 receives control signal (DC) from controller 12. Intake manifold 44 is also shown having fuel injector 68 coupled thereto for delivering fuel in proportion to the pulse width of signal (fpw) from controller 12. Fuel is delivered to fuel injector 68 by a conventional fuel system (not shown) including a fuel tank, fuel pump, and fuel rail (not shown).
[0017] Engine 10 further includes conventional distributorless ignition system 88 to provide ignition spark to combustion chamber 30 via spark plug 92 in response to controller 12. In the embodiment described herein, controller 12 is a conventional microcomputer including: microprocessor unit 102, input/output ports 104, electronic memory chip 106, which is an electronically programmable memory in this particular example, random access memory 108, and a conventional data bus.
[0018] Controller 12 receives various signals from sensors coupled to engine 10, in addition to those signals previously discussed, including: measurements of inducted mass air flow (MAF) from mass air flow sensor 110 coupled to throttle body 64; engine coolant temperature (ECT) from temperature sensor 112 coupled to cooling jacket 114; a measurement of throttle position (TP) from throttle position sensor 117 coupled to throttle plate 66; a measurement of turbine speed (Wt) from turbine speed sensor 119, where turbine speed measures the speed of shaft 17; and a profile ignition pickup signal (PIP) from Hall effect sensor 118 coupled to crankshaft 13 indicating and engine speed (N).
[0019] Continuing with FIG. 1 , accelerator pedal 130 is shown communicating with the driver's foot 132. Accelerator pedal position (PP) is measured by pedal position sensor 134 and sent to controller 12.
[0020] In an alternative embodiment, where an electronically controlled throttle is not used, an air bypass valve (not shown) can be installed to allow a controlled amount of air to bypass throttle plate 62. In this alternative embodiment, the air bypass valve (not shown) receives a control signal (not shown) from controller 12.
[0021] Continuing with FIG. 1 , a fuel tank 140 is shown for containing fuel used to operate engine 10. Pump 148 is shown inside the fuel tank 140 for pressurizing liquid fuel in fuel line 142. Fuel line 142 delivers pressurized liquid fuel to fuel injector 68 which, as described above herein, is controlled by a signal (fpw) received from controller 12. Fuel pressure regulator 152 is also shown for regulating pressure in fuel line 142. Regulator 152 is a mechanical pressure regulator valve.
[0022] A fuel vapor management system is also shown in FIG. 1 coupled to fuel tank 140 and engine 10. In particular, fuel vapor line 154 couples the fuel tank to the intake manifold 44. A purge control valve 156 is also shown receiving a signal from controller 12. As described below herein, controller 12 adjusts purge valve 156 to control air and fuel vapor entering manifold from the fuel system based on engine operating conditions. Continuing with the fuel vapor system, the fuel tank is shown coupled to a first and second carbon canister 144 and 146. Fuel vapors entering the engine 10, from fuel tank 140 first pass through the first fuel vapor carbon canister 146. Carbon canister 146 absorbs fuel vapors and desorbs fuel vapors depending on vapor concentration. The second carbon canister 144 is coupled downstream of the fuel tank via line 150.
[0023] Finally, fuel quality sensor 160 is shown in fuel tank 140. In this particular embodiment, sensor 160 is in fluid contact with liquid fuel stored in fuel tank 140. Sensor 160 provides a signal (FQ) to controller 12. As described below and with particular reference to FIG. 2 , sensor 160 is a surface acoustic wave device operating at approximately 100 megahertz. In general terms, this sensor provides a signal related to viscosity and density of the liquid fuel stored in tank 140.
[0024] According to the present invention, fuel quality sensor 160 can be located in various different positions on the fuel system/engine system. As an example, fuel sensor 160 can also be coupled to fuel line 142. The sensor can be located either upstream or downstream of pressure regulator 152. Sensor location depends upon various factors, such as, for example, measuring the fuel near the point of fuel delivery, measuring fuel with minimal changes in fuel temperature, and various others.
[0025] In addition, a dielectric sensor 162 is shown for measuring liquid fuel in tank 140. The dielectric sensor output is typically utilized to detect the ethanol content of gasoline fuels. Further, intake air temperature sensor 119 is shown coupled to intake manifold 44 for measuring a temperature of the intake air and providing a signal (ACT) to controller 12.
[0026] Referring now to FIG. 2 , details of sensor 160 are described. Sensor 160 is a surface acoustic wave device, operating at approximately 100 megahertz. The acoustic wave generated by the device interacts with the liquid fuel in which is contacting the device. The more viscous the liquid fuel, the more the propagation speed is changed and the more the acoustic wave is attenuated. By placing an electronic amplifier between input and output of the surface acoustic wave delay line, an oscillator is obtained. The oscillation frequency and electronic gain needed for oscillation on both measures for the viscosity (related to propagation, velocity and attenuation, respectively).
[0027] In addition, the surface acoustic wave device is covered by a thin layer of silicon dioxide. The wet cell (with liquid fuel) is placed on top of the delay lines, thereby allowing a leak-free connection secured with a 14 millimeter viton o-ring. The sensor output, (a frequency signal in megahertz in this particular example) provides an indication of dynamic viscosity times density.
[0028] According to the present invention, this signal (related to dynamic viscosity times density) correlates to fuel quality of liquid fuel contained in the fuel system coupled to the engine. In other words, the sensor output can be correlated to the “drivability index (DI)” typically utilized to characterize fuel quality for engine combustion. Various forms of the sensor output can be used, as described below, including frequency, phase, amplitude, or propagation velocity.
[0029] Sensor 160, in one embodiment, can be based on a micro-acoustic (LOVE) waves the property through a thin wave guide material deposited on a piezoelectric substrate. One example of the device is described in “Viscosity Sensing Using LOVE wave devices” by B. Jakoby and M. J. Vellekoop in Vol. A68 of Sensors and Actuators (1998) pgs 275-281. When the sensor is in contact with liquid fuel, the propagation losses and the phase velocity of the LOVE wave change as a function of the viscosity-density product of the fuel. The sensor size is typically approximately 8×4 millimeters. Since viscosity is dependent on temperature, the sensor measures and corrects for this temperature. Alternatively, a separate temperature sensor can be used and the correction performed in controller 12. In other words, the device can be temperature compensated by measuring the temperature and compensating for this measurement. Alternatively, or in addition, a dual delay line can be used, where only one is exposed to the liquid and the other not, but both are exposed to the same temperature. Besides the device temperature dependence, there is also a temperature dependence in the viscosity-density of the liquid. Here, the temperature can be measured and the measurement can be compensated as described above. Alternatively, or in addition, the device can be heated to a constant temperature and the liquid probed by the device is heated to that same temperature. If measurements are always performed at the same temperature, no further compensation would be used.
[0030] The sensor 160 can have various outputs including a shift in oscillation frequency, or a change in acoustic attenuation as measured by the electronic gain required for the oscillation.
[0031] As indicated, various types of acoustic waves can be generated on or in a piezoelectric material. This acoustic wave propagating in or on the substrate then interacts with a liquid adjacent to the substrate to “probe” the properties of that liquid. These include, but is not limited to: thickness shear mode resonator, flexural plate wave device, acoustic plate mode device, and Love wave sensors. The LOVE wave sensor is a described in detail since it has a simple and rugged design.
[0032] Referring now to FIGS. 2A through 2C , and specifically to FIG. 2A ; a schematic diagram of a viscosity sensing LOVE-wave device is shown. In this example of sensor 160, an isotropic guiding layer of silicon dioxide (210) is deposited on a substrate 212. A piezoelectric ST quartz is the substrate material 212, where the propagation direction is chosen to be orthogonal to the crystal X direction. Interdigital transducers (IDTs) 214 enable electrical excitation and reception of the LOVE-wave. The interdigital transducers 214 are embedded at the interface between the layer 210 and the substrate 212. The IDTs convert an electric signal into an acoustic wave.
[0033] As described above, the propagation direction is chosen to be orthogonal to the crystalline X direction. This orientation allows the excitation of sheer polarized modes by the interdigital transducers 214. The guiding layer 210 is deposited on the substrate by using plasma enhanced chemical vapor deposition. The acoustic energy associated with the propagating wave becomes concentrated in layer 210. This allows increased sensitivity with respect to surface mass loading. The top surface of layer 210 is in contact with the liquid fuel contained in tank 140, in one example. Additionally, shielding 216 can be placed over guiding layer 210. In one example shielding 216 is a metal layer. The delay line is used as a frequency determining element and an oscillator circuit. In other words, it changed in the delay time due to the sensing from the transducers can be observed by monitoring oscillation frequency as described below herein.
[0034] In addition, FIG. 2A shows a source 211 coupled to one of the transducers 214 and a load 213 coupled to the other of the transducers 214.
[0035] In general, the change in frequency as the viscosity-density of the liquid changes can be the sensor output. This change in frequency is related to the change in the propagation velocity of the acoustic wave. Alternatively, the change in damping of the acoustic wave can also be measured by the amount of electronic amplification that is needed to keep the device oscillating.
[0036] Referring now to FIG. 2B , a side view of the sensor 160 is illustrated using schematic diagrams. In particular, a wet cell 220 is shown mounted on the device, which allows the liquid fuel to contact only the region between the interdigital transducers 214. Wet cell 220 can be attached using adhesive and sealing materials such as silicon rubber. An alternate approach would utilize a micro machined wet cell attached using fusion bonding techniques.
[0037] Next, FIG. 2C shows the device coupled to analog circuitry to generate the sensor output. In FIG. 2C , the circuitry allows the determination of the affects of viscosity on the phase shift via measuring a corresponding change in frequency. Further, the control voltage of the automatic GAIN control is monitored for a constant output level. In particular, FIG. 2C shows the output delay line 230 from the interdigital transducers 214 coupled to a first amplifier 232. Further, a GAIN control amplifier 236 is used with a fixed reference level voltage. Further, the oscillator output is also fed to a DC/AC converter 238 and then to amplifier 236. The output of amplifier 236 is fed to amplifier 232. Further, the output of the GAIN control 242 provides the automatic GAIN control voltage readout which can be monitored. Further, the oscillator output is first buffered via amplifier 234 and then provides frequency readout 240 which can be used to determine fuel viscosity times density. The relation between the frequency change (ΔF/F) and the relative change in the wave number (ΔB/B) is given by the following equation:
ΔF/F=−Vg/Vp×ΔB/B
Where Vg and Vp denote the group and phase velocity of the LOVE wave.
ΔF/F=−Vg/Vp×ΔB/B
Where Vg and Vp denote the group and phase velocity of the LOVE wave.
[0038] ΔB/B is the relative wave number change evaluated at constant frequency. Complete details of calibration and calculations using the sensor in FIGS. 2A through 2C can be determined from the reference titled “Viscosity Sensing Using a LOVE-wave Device” by Bernard Jakoby and Michael J. Vellekoop, Vol A68 of journal Sensors and Actuators (1998) pages 275-281.
[0039] As described above, the details shown in FIGS. 2A to 2C show one example embodiment where acoustic energy (waves) are utilized to obtain information about the gasoline fuel fed to the engine. However, the present inventors have contemplated various other embodiments. For example, as described below here with particular reference to FIGS. 11-14 , and 17, one could also estimate fuel quality, or volatility, or viscosity, using estimates based on other sensors in the engine/vehicle system. Further, different sensor types could be used where different energy types are introduced into the fuel, such as light energy.
[0040] Referring now to FIG. 3 , the graph shows output of sensor 160 versus output of sensor 162 for various different fuels. The first grouping labeled “normal” fuels illustrates variation and sensor output across fuels that typically result in normal engine cold starts. The graph illustrates the different fuels both with and without ethanol. The graph also illustrates type 1 fuels on the lower left hand side indicating a low sensor output from sensors 160 and 162. These fuels are sometimes known as “hesitation” fuels in that they result in a lean combustion during engine cold starting compared with the normal fuels. Finally, FIG. 3 illustrates a type 2 fuel which typically results in a rich combustion compared to the normal fuels. For these type 2 fuels, sensor 160 provides an increased sensor output. As illustrated in FIG. 3 , in one embodiment when controller 12 receives a signal (FQ) from sensor 160 during an engine start, the controller adjusts the amount of fuel delivered via injector 68 based on the output of sensor 160. When the sensor 160 provides an output indicative of a normal fuel, controller 12 simply provides the scheduled amount of fuel via injector 68 during the engine start. However, if sensor 160 provides an output greater than approximately 110.202 megahertz, the routine reduces the amount of scheduled fuel to be delivered via injector 68 thereby preventing an overly rich mixture. Similarly, when sensor 160 provides an output lower than approximately 110.913 megahertz, controller 12 adds additional fuel during the cold start to be delivered by injector 68, thereby preventing the combustion from being too lean. In this way, more consistent engine cold starting can be achieved even when large variations in the fuel are experienced. This method, along with alternative embodiments, are described more fully with regard to the routines described below.
[0041] Referring now to FIG. 4 , the graph illustrates sensor output of sensors 160 and 162 with different levels of ethanol. In particular, the graph illustrates that sensor 160 provides a high sensor output for hydrocarbon and fuels containing approximately 10% ethanol. However, for methanol fuels (approximately 85% ethanol) sensor 160 provides a relatively low sensor output. In this way, sensor 160 can be used to detect the type of fuel in vehicle. In particular, according to the present invention, controller 12 can determine whether the vehicle is operating with methanol based on sensor 160.
[0042] As described above, output from sensor 160 can be utilized as an indication of the drivability index (DI). The drivability index is typically determined based on the following equation:
DI=1.5×T10+3×T50+T90
Where Tx is based on the ASTMD-86 distillation curve.
DI=1.5×T10+3×T50+T90
Where Tx is based on the ASTMD-86 distillation curve.
[0043] When oxygenates are present in the fuel the correction to the DI is as follows:
DI=1.5×T10+3×T50+T90+20*(weight % 02)° F.
DI=1.5×T10+3×T50+T90+20*(weight % 02)° F.
[0044] Typically, a high DI is indicative of a poor drivability fuel (poor cold-start), resulting in combustion too lean of stoichiometry. Conversely, an low DI can indicate poor driveability in that the combustion is too rich of stoichiometry.
[0045] This Driveability Index (DI) in one method to characterize fuel quality. DI correlates well with the cold-start driveability.
[0046] FIGS. 5 and 6 illustrate DI data versus dynamic viscosity times density for various hydrocarbon fuels contained in the American Automobile Manufacturer's Association 1996 survey data. Also note that a correction for ethanol fuels and methanol fuels can be used. Typically, a 10% EtOH results in a correction of approximately 70 points in DI. Further, a 10% MTBE typically results in a correction of approximately 35 points in the drivability index.
[0047] As shown in FIGS. 5 and 6 , a relatively consistent correlation between the drivability index and the dynamic viscosity times density measurement is obtained. As shown in FIG. 6 , this correlation is also true including both summer and winter hydrocarbon fuels.
[0048] The following is a potential explanation of why such measurements correlate to drivability index and, thereby, to combustion quality. Drivability can be affected by the degree of fuel atomization during the combustion process. The more effective the fuel atomization is, the smaller the mean fuel drop in size can be and the higher the rate of evaporation and mixing with the combustion air can be. For a fixed geometry of the fuel injector and a constant fuel pressure and air flow and density, the atomization is influenced by properties of the liquid fuel such as, for example: fuel density, fuel viscosity and surface tension. In addition to atomization, the spray angle can also be influenced by the density and viscosity of the fuel. Thus, measuring fuel viscosity and density can give an indication of the fuel quality.
[0049] Referring now to FIG. 7 , the routine is described for controlling fuel injection during an engine start based on the fuel quality sensor. First, in step 710, the routine determines whether the engine is currently starting. In particular, in step 710, the routine determines whether the engine is in either the crank mode, or the initial run-up mode where engine speed increases rapidly to the desired idle rpm speed. When the answer to step 710 is “no”, the routine continues to step 712 where injected fuel is controlled based on the desired idle speed and measured idle speed.
[0050] When the answer to step 710 is “yes”, the routine continues to step 712 to determine a base fuel amount (fuelb) based on the engine coolant temperature (ect), times since engine start, and intake air temperature (act). This base fuel amount is stored in lookup tables and calibrated over various engine conditions to achieve a reliable engine start. However, variations in fuel quality can cause degraded engine starts using this base fuel amount. In particular, variations in the fuel type can cause engine combustion to be either too lean or too rich, thereby creating poor engine startability and degraded drivability.
[0051] Note that the base amount of fuel can also be determined based on a desired torque. The desired torque can be determined from the operator of the vehicle, or from a controller. Further, the desired torque can be based on the pedal position.
[0052] Continuing with FIG. 7 , in step 714, the routine reads the sensor output (FQ) from sensor 160, which is indicative of fuel viscosity and density. Note, that in an alternate embodiment, the routine can simply measure either fuel viscosity or fuel density individually, or can simply measure fuel viscosity alone to provide an indication of fuel quality. Next, in step 716, the routine determines whether the parameter FQ read from sensor 160 is between a lower limit (L1) and an upper (L2).
[0053] When FQ is less than or equal to L1, the routine continues to step 718. When FQ is between L1 and L2, the routine continues to step 720. Finally, when FQ is greater than or equal to L2, the routine continues to step 722.
[0054] In step 718, the routine increases scheduled fuel amount by Δ2. Alternatively, in step 722, the routine decreases a scheduled fuel amount by Δ1. Finally, in step 720, no adjustment to the fuel delivered based on sensor 160 is used. From either 718, 720 or 722, the routine continues to step 724 to adjust the ignition timing based on the signal FQ. In one embodiment of step 724, the routine adjusts the location of borderline spark based on the fuel viscosity.
[0055] In this way, the routine adjusts the injected fuel amount to account for variations in the fuel quality and thereby achieve improved engine starting. Specifically, when the signal FQ indicates a high signal (for example greater than 110.202 megahertz), the routine decreases injected fuel since the sensor indicates that combustion may be too rich. Conversely, when sensor 160 indicates a low output (for example less than 110.193 megahertz) the routine increases the scheduled fuel amount since the sensor indicates that the fuel may provide combustion that is too lean.
[0056] Note that there are various alternative embodiments to the present invention. For example, the routine may continue the adjustment of fuel based on sensor 160 even after an engine start. For example, the adjustment can be continued for a predetermined number of seconds after an engine start, or after a predetermined number of throttle tip-in maneuvers by the driver. Also note that adjustment of the injected fuel and ignition timing based on the sensor 160 can be used for other engine operating modes than engine starting, such as, for example: during fuel vapor purging, or adaptive learning of the engine sensors 16 and 110.
[0057] Note also that in addition to adjust the fuel amount injected, the timing of the fuel injection can be adjusted based on sensor 160. For example, by changing the timing of the fuel injection, it is possible to change the amount of fuel injected and/or inducted into the engine. Furthermore, depending on the fuel quality, it may be beneficial to inject the fuel at an earlier or later time to reduce emission generation during the combustion process. This is especially true for engines utilized direct injection, where injector 68 is located to inject fuel directly into combustion chamber
[0058] In an alternative embodiment, both sensor 160 and dielectric sensor 162 are utilized to determine fuel volatility (or viscosity) as indicated in FIG. 3 , for example. As an example, sensor 160 provides an indication of the fuel DI (or volatility, or stoichiometric air-fuel ratio, etc.) while sensor 162 provides an indication of the ethanol content of the fuel. Then, both the indicated volatility and alcohol content can be used to determine the amount of fuel to be injected during engine starting. Further, the ignition timing can also be set based on this determination from both sensors 160 and 162. Experimental testing with different fuels and ignition timing values can provide the calibration data for such an approach.
[0059] Referring now to FIG. 8 , an alternative embodiment for adjusting injected fuel based on sensor 160 is described. In step 810, the routine determines whether the engine is in the starting mode. Specifically, the routine determines whether the engine has exited engine cranking. When the engine has exited engine cranking, the answer to step 810 is “yes” and the routine continues to step 812. In step 812, the routine determines an expected engine speed (RPM) based on engine coolant temperature (ECT) and times since engine starting.
[0060] Next, in step 814, the routine measures actual engine rpm based on sensor 118. Then, in step 816, the routine calculates the difference (RPM_dif) between the expected engine speed and the measured actual engine speed. Then, in step 818, the routine determines whether the engine speed difference is greater than a limit (L3). Specifically, limit L3 represents a hysteresis band allowing small changes in engine speed without control action. When the answer to step 818 is “yes”, the routine continues to step 820. In step 820, the routine reads signal (FQ) from sensor 160 indicative of the fuel quality. As described above, sensor 160 can provide an indication of fuel viscosity, fuel density, the product of fuel viscosity and density, dynamic fuel viscosity times density, or static fuel viscosity times density. In this particular example, the sensor 116 provides an indication of dynamic viscosity times density.
[0061] Then, in step 822, the routine determines whether the signal of Q is greater than a limit L4. In one example, limit L4 is set to 110.199 megahertz when using the acoustic wave device described in FIG. 2. When the answer to step 822 is “no”, the routine continues to step 824 and sets the control parameter (K) equal to minus GAIN. Alternatively, when the answer to step 822 is “yes”, the routine sets the control parameter (K) equal to plus GAIN in step 826. Next, in step 828, the routine calculates an adjustment Δ3 based on the feedback parameter K times the rpm difference (RPM_DIF). Then, in step 830, the routine adjusts the new fuel injection amount (fueln) based on the base fuel amount minus the calculated adjustment Δ3. This value is then used to adjust the fuel injector 68 to deliver the requested fuel amount to the engine.
[0062] In still another aspect of the present invention, the desired air-fuel ratio can be adjusted based on the fuel quality (sensor 160 or a corresponding estimate). For example, the combustion air-fuel ratio is typically feedback controlled based on exhaust gas oxygen sensors, such as sensor 16, for example. In this case, the amount of injected fuel is adjusted to maintain the desired air-fuel ratio. Thus, according to one aspect of the present invention, this desired air-fuel ratio can be adjusted to compensate for changes related to changes in the fuel quality. In this way, it is possible to obtain improved combustion and reduced emissions by setting the desired air-fuel ratio closer to the actual stoichiometric ratio of the fuel. Further, the air-fuel ratio of the combustion gasses can be limited to certain air-fuel ratio ranges to prevent combustion instability. In yet another aspect of the present invention, this air-fuel limit (typically the lean air-fuel limit) can be adjusted based on the fuel quality, viscosity, and/or volatility. Such a system is described in FIG. 8B.
[0063] In particular, in step 810, the routine determines the desired air-fuel ratio set-point based on the fuel quality. Then in step 812, the routine controls the injected fuel quantity and/or timing to maintain the desired value based on the exhaust gas oxygen sensor 16. Then, a limit air-fuel ratio is determined in step 814 based on the fuel quality. Then, steps 816 and 818 prevent the desired value for surpassing the limit value.
[0064] Referring now to FIG. 9 , the routine is described for adjusting the lost fuel calculation based on the fuel viscosity. Lost fuel refers to the fuel does not participate in engine combustion and past the piston rings of the engine 10. First, in step 910, the routine calculates a base lost fuel parameter based on engine operating conditions as is known in the art. Then, in step 912, the routine adjusts this lost fuel calculation based on a function of the signal FQ received from sensor 160. The lost fuel parameter (LOST_FUEL) is used to control engine fuel injection and ignition timing during engine starting and other operating conditions.
[0065] Also note that other fuel calculations can be adjusted based on the fuel quality sensor 160. In particular, transient fuel models can adjust the fuel puddle size and time constant values based on the fuel quality sensor 160.
[0066] Referring now to FIG. 10 , the routine is described for performing default operation in the case when sensor 160 has degraded. In this way, the engine can provide acceptable combustion even if sensor 160 is degraded. First, in step 1010 the routine monitors sensor 160 as described herein with respect to FIGS. 11 through 13 . Next, in step 1012, the routine determines whether sensor 160 is degraded. When the answer to step 1012 is “no”, the routine returns to step 1010.
[0067] When the answer to step 1012 is “yes”, the routine continues to step 1014 and sets the signal FQ received from sensor 160 to a default value (for example 110.193 megahertz) which can then be used in the fuel starting control routines described above herein. In other words, the routine ignores the actual sensor output and replaces this actual sensor output with a predetermined default value. Further, in step 1016, the routine lights an indicator light to notify the driver of the degraded sensor.
[0068] In this way, it is possible to continue acceptable engine combustion even when the fuel quality sensor provides a degraded output. The default value selected to be used in this case represent values that are least likely to result in degraded engine combustion irrespective of the fuel quality actually in tank 140.
[0069] Referring now to FIG. 11 , the routine is described for determining the degradation of sensor 160. In general terms, the routine uses estimates of combustion air-fuel ratio during cold and warm engine operating conditions to determine an estimated fuel quality value which is then compared to the sensor reading to determine whether the sensor has degraded.
[0070] First, in step 1110, the routine determines whether engine coolant temperature is less than a threshold (L5) and whether the engine speed and load are in a first predetermined range (R1). When the answer to step 1110 is “yes”, the routine continues to step 1112 and saves the adaptive air-fuel ratio term as AT1. The adaptive air-fuel term is based on long term adaptive learning via sensor 16.
[0071] Next, in steps 1114 and 1116, this is repeated for warm engine operating conditions (ECT greater than L6) and this time the adaptive term is saved as AT2. Next, in step 1118, the routine determines whether both AT1 and AT2 have been updated via steps 1112 and steps 1116. When the answer to step 1118 is “no”, the routine returns to the start. When the answer to step 1118 is “yes”, the routine continues to step 1120.
[0072] Continuing with FIG. 11 , in step 1120 the routine calculates the difference of (ΔT) between the first and second saved adaptive terms. This represents a change in combustion air-fuel ratio between cold and warm engine coolant temperatures within a defined engine speed range R1. Next in step 1122 the routine estimates a sensor reading (FQ_EST) based on the calculated difference ΔAT. Then, in step 1124, the routine compares the estimate with the sensor reading and indicates whether degradation has been detected. In particular, the routine determines whether the difference between the estimate and the actual sensor reading is greater than a predetermined amount for a predetermined duration. When this occurs, the routine provides an indication to the driver via an indicator light.
[0073] Referring now to FIG. 12 , an alternate embodiment for determining degradation in sensor 160 is described. First, in step 1210 the routine monitors the rpm difference from step 816 of FIG. 8. In particular, the routine monitors the rpm difference over numerous engine starts and averages this value with a predetermined averaging filter rate. Then in step 1212, the routine estimates the sensor output (FQ) based on the average rpm difference over these monitored engine cold starts. In one example, the routine monitors between 15 to 20 engine cold starts to provide an estimate of the sensor output. Alternatively, more or less engine starts can be utilized depending on the required accuracy. Then, in step 1214, the routine compares the estimate with the actual sensor reading as described above herein with particular reference to step 1124.
[0074] Referring now to FIG. 13 , yet another alternative embodiment for determining degradation in sensor 160 is described. In particular, this routine monitors the sensor output over time and detects suspiciously constant sensor output, or suspiciously large changes in sensor output.
[0075] First, in step 1310, the routine monitors the signal sensor output (FQ) over various engine starts. Next, in step 1312, the routine determines whether the sensor reading has changed by less than a threshold (L7) over these engine starts. As above, approximately 10 to 15 engine starts can be utilized. As above, more or less engine starts can be utilized based on the required accuracy. In particular, in step 1312, the routine monitors the sensor reading over several fuel tank refills. If the sensor reading has not changed over various starts and refills, the routine determines that the sensor has degraded in step 1316 as described above herein with particular reference to 1124 indicates this to the driver via an indicator light.
[0076] When the answer to step 1312 is “no”, the routine continues to step 1314. In step 1314, the routine determines whether the sensor reading has changed by greater than a predetermined amount (L8) over various engine starts. If the sensor reading changes greater than this amount, the routine indicates degradation in step 1316 as described above.
[0077] Still another alternative embodiment, that can be used alone or in addition to the above described approaches, would use a purposeful disturbance of the amount of injected fuel during idle conditions. There should be no effect if the sensor is measuring accurately. If the sensor output is degraded, then a further deviation will result in an rpm fluctuation.
[0078] Note that the estimates in FIGS. 11-14 (as well as in FIG. 17B ) can be used in place of the sensor reading in an alternative embodiment.
[0079] Referring now to FIG. 14 , a routine is described for adjusting fuel vapor purging estimation and control based on sensor 160. First, in step 1410, the routine determines whether the engine is currently purging fuel vapors from the fuel system. When the answer to step 1410 is “Yes”, the routine continues to step 1412 and estimates the vapor concentration based on various sensors, such as for example: oxygen sensor 16, mass air flow sensor 110, command signal (PRG), and command signal (FPW). Various methods are known for estimating fuel vapor concentration and can be used in step 1412.
[0080] Next, in step 1414, the routine adjusts the estimate based on the fuel quality signal FQ from sensor 160. In particular, the routine adjusts the amount of fuel vapors estimated by shifting the assumed stoichiometric combustion air-fuel ratio to account for the output from sensor 160. In this way, the routine can re-calculate the fuel vapor quantity using this additional information. Then, in step 1416, the routine can adjust the fuel pulse with and purge control valve based on this adjusted estimate of fuel vapor concentration to more accurately control engine combustion.
[0081] In addition, an estimate of the fuel vapor concentration coming from the tank (before feedback information becomes available) can be determined based on the fuel quality.
[0082] FIG. 15 shows in detail how the liquid fuel interacts with the acoustic wave, the amplitude of which is shown as 1510. This illustrates how the wave generated by the oscillator circuit propagates into the liquid, thereby creating the basic sensing ability of the device. This interaction is influenced by the liquid density and viscosity.
[0083] FIG. 16 shows a routine for adjusting the engine fuel control depending on whether the fuel used is methonal (M85), or gasoline fuel. As shown in FIG. 4 , sensor 160 can be used (alone or in conjunction with sensor 162) to indicate such fuel type information. First, in step 1610, the routine measures the sensor output (FQ). Then, in step 1612, the signal (FQ, or viscosity density depending on the type of sensor used) is compared with a value (Limit, 110.16 MHz in this example). When the answer to step 1614 is YES (i.e., FQ is less than the Limit), the routine indicates methanol fuel in step 1614. Alternatively, in step 1616, the routine indicates gasoline fuel. Then, in step 1620, the routine controls the injected fuel based on the indicated fuel type. Furthermore, the routine can adjust the ignition timing based on the fuel type, if desired.
[0084] Referring now to FIGS. 17A and 17B , yet another embodiment of a method for estimating fuel quality is illustrated. In particular, FIG. 17B shows a method utilized fuel vapor learning to estimate fuel volatility. In FIG. 17B , the routine first enables purge compensation and disables adaptive learning in step 1710. In other words, the routine assigns all of the air-fuel error to determining the concentration of fuel vapors (pcomp) in the purge flow. Typically, pcomp is the learned concentration for the MAF sensor, fpw, and exhaust gas oxygen sensors, as is known in the art.
[0085] Next, in step 1712, the routine ramps open the purge valve. Step 1714 continues the ramping until the valve is fully open. When fully open, the routine continues to step 1716 to determine whether a timer (time) has run (i.e., reached limit time T2). If not, the routine continues to step 1718 to monitor the learned concentration value (pcomp) over this initial time period. In particular, in step 1720, the routine calculates the rate of change (R) of the purge concentration and estimates (in step 1722) the fuel quality/volatility (FQ_est) based on the calculated rate (R).
[0086] As shown in FIG. 17A , this calculated rate is taken during a fixed volumetric flow since the purge valve is fully open at time t1. This rate provides an indicate of fuel desorption or vaporization from the fuel tank and therefore can be correlated to volatility.
[0087] As such, the learning based on the liquid injected fuel is disabled and the learning of the fuel quality based on vaporized fuel is enabled.
[0088] Also note that the learning of the fuel quality can be enabled after a second period (after the valve is fully open) to eliminate degraded reading from the stored vapors in the tank. By enabling learning of the fuel quality based on the rate of change after the stored vapors have been purged, a better reading of the fuel vaporization rate can be found.
[0089] As described above, the present invention uses a measurement of fuel volatility (viscosity in one example) to predict the combustion characteristics of the fuel during cold engine starting. This prediction can include compensation for various parameters, such as fuel temperature, engine temperature, barometric pressure, atmospheric temperature, intake air temperature, and others. In any event, the engine controller is able to adjust the amount of scheduled fuel (or scheduled air-fuel mass ratio) based on the sensed data. This allows for a tighter control of combustion air and fuel (thereby improving engine emissions even for “normal” fuels). In addition, it allows for improved engine startability and driveability, even when so called “fringe” fuels, such as high or low DI fuels are experienced in the engine. In this way, a feedfoward estimate of the fuel quality can be obtained without waiting for dips in engine speed.
[0090] Further, with a combination of a viscosity-density sensor and a dielectric sensor, one can measure both the DI and amount of ethanol present in the fuel.
[0091] In yet another aspect of the present invention, the method uses a viscosity-density sensor to measure large concentrations of alcohol as can be present in flex fuels (0-85% ethanol).
[0092] Note that various embodiments have been described for determining fuel quality, volatility, and/or viscosity. In one example, an acoustic wave sensor uses acoustic energy to determine fuel viscosity, which is then used to determine fuel combustion quality. In another embodiment, the fuel quality is estimated from adaptive parameters based on exhaust gas air-fuel ratio sensors. In still another embodiment, the rate of change of exhaust gas sensors is utilized to estimate fuel volatility, and thereby estimate fuel quality.
[0093] This concludes the detailed description of the invention.
Claims
Certificate of Correction present
The claims shown below may not include correction changes. Use the corrected PDF for authoritative text.
1. A method for controlling a spark ignited engine operated with fuels of varying volatility or viscosity, comprising:
generating an acoustic wave in proximity to the fuel;
providing a signal related to viscosity or volatility of the fuel, said signal being derived from alterations in said acoustic wave caused by said fuel;
providing a base ignition timing signal to the engine for predetermined engine operation;
adjusting said base ignition timing signal in relation to said signal; and
adjusting a fuel injection amount in relation to said signal.
2. The method recited in claim 1 wherein said generating further comprises at least one of propagating the wave into the fuel, or propagating the wave from a medium into the fuel.
3. The method recited in claim 1 wherein said alterations in said wave include at least alterations in frequency, phase, amplitude, or propagation velocity.
4. The method recited in claim 1 wherein said engine operation includes at least engine speed, engine load, throttle angle, or starting conditions.
5. A method for controlling a multi cylinder engine operated with fuels of varying volatility or viscosity, comprising:
generating a signal related to fuel viscosity;
inducting air into each of the cylinders;
delivering fuel to each of the cylinders in relation to said inducted air and a desired air/fuel ratio;
generating a minimum air/fuel ratio in relation to said viscosity indication;
preventing said delivered fuel from falling below a minimum amount corresponding to said minimum air/fuel ratio; and
adjusting ignition timing in relation to said signal.
6. The method recited in claim 5 wherein said minimum air/fuel ratio is selected to reduce combustion instability.
7. A method for controlling a multi-cylinder engine operated with fuels of varying viscosity, comprising:
generating an indication of fuel viscosity;
inducting air into each of the cylinders;
delivering fuel to each of the cylinders in relation to said inducted air to maintain an average desired air/fuel ratio;
adjusting said desired air/fuel ratio in relation to said fuel viscosity indication; and
adjusting ignition timing in relation to said signal.
8. The method recited in claim 7 further comprising feedback controlling injected fuel based on an exhaust gas sensor.
9. A method for controlling a multi-cylinder engine operated with fuels of varying viscosity, comprising:
generating a signal related to fuel viscosity;
inducting air into each of the cylinders;
delivering fuel to each of the cylinders in relation to said inducted air to maintain an average desired air/fuel ratio;
adjusting said delivered fuel in relation to feedback from an exhaust gas sensor;
further adjusting said delivered fuel in relation to said signal; and
adjusting ignition timing in relation to said signal.
10. A method for controlling a multi-cylinder engine operated with fuels of varying viscosity, comprising:
generating an indication of fuel viscosity;
delivering fuel to each of the cylinders in relation to a desired output torque; and
adjusting said delivered fuel and ignition timing in relation to said fuel viscosity to maintain said desired output torque.
11. The method recited in claim 10 wherein said desired output torque includes at least a desired engine torque, a desired torque from a vehicle operator, a desired torque from a controller, or a desired torque from a pedal position.
12. A method for controlling a multi-cylinder engine operated with fuels of varying viscosity or volatility, the engine inducting fuel vapors from a fuel system into an engine air intake, comprising:
generating an indication of fuel viscosity or volatility;
delivering injected fuel to each of the cylinders; and
adjusting said delivered injected fuel in relation to said inducted fuel vapors and said fuel viscosity or volatility indication.
13. The method of claim 12 wherein adjusting said delivered injected fuel in relation to said inducted vapors include adjusting said delivered injected fuel in relation to vapor flow and/or vapor density.
14. A method for controlling a multi cylinder engine operated with fuels of varying volatility or viscosity, comprising:
providing a signal related to viscosity based on a rate of change of an exhaust system sensor; and
adjusting fuel injection and ignition timing in relation to said signal.
15. A method for controlling a multi cylinder engine operated with fuels of carrying volatility or viscosity, comprising:
providing a signal related to viscosity or volatility of the fuel, said signal being derived from alterations in a source of energy directed into the fuel;
providing the fuel to at least one of the cylinders at a timing related to a predetermined engine operation;
adjusting said fuel timing to an earlier or later timing in relation to said signal; and
adjusting ignition timing in relation to said signal wherein said source of energy directed to the fuel is acoustic energy.
Patent Citations (38)
| Patent | Date | Inventor | Cited By |
|---|---|---|---|
| US3307391(A) | 1967-03-01 | Parker | Applicant |
| US3556160(A) | 1971-01-01 | Link et al. | Applicant |
| US4252097(A) | 1981-02-01 | Hartford et al. | Applicant |
| US4893496(A) | 1990-01-01 | Bau et al. | Examiner |
| US4955345(A) | 1990-09-01 | Brown et al. | Applicant |
| US5233959(A) | 1993-08-01 | Kojima | Examiner |
| US5444627(A) | 1995-08-01 | Sandborg et al. | Applicant |
| US5499607(A) | 1996-03-01 | Tomisawa | Examiner |
| US5537854(A) | 1996-07-01 | Phillips et al. | Examiner |
| US5582157(A) | 1996-12-01 | Uchikawa | Examiner |
| US5586537(A) | 1996-12-01 | Tomisawa et al. | Examiner |
| US5701863(A) | 1997-12-01 | Cemenska et al. | Examiner |
| US5701868(A) | 1997-12-01 | Tomisawa | Examiner |
| US5706780(A) | 1998-01-01 | Shirakawa | Applicant |
| US5827952(A) | 1998-10-01 | Mansure et al. | Examiner |
| US5875759(A) | 1999-03-01 | Meyer et al. | Applicant |
| US5934255(A) | 1999-08-01 | Dalton et al. | Examiner |
| US5957994(A) | 1999-09-01 | Meyer et al. | Applicant |
| US6067965(A) | 2000-05-01 | Trumpy et al. | Applicant |
| US6102000(A) | 2000-08-01 | Shindoh et al. | Examiner |
| US6176222(B1) | 2001-01-01 | Kirwan et al. | Examiner |
| US6178949(B1) | 2001-01-01 | Kirwan et al. | Examiner |
| US6286360(B1) | 2001-09-01 | Drzewiecki | Examiner |
| US6304021(B1) | 2001-10-01 | Wolf et al. | Examiner |
| US6360726(B1) | 2002-03-01 | Javaherian | Examiner |
| US6460513(B1) | 2002-10-01 | Meyer et al. | Applicant |
| US6564624(B2) | 2003-05-01 | Lin et al. | Examiner |
| US6588253(B2) | 2003-07-01 | Lambert et al. | Examiner |
| US6679225(B2) | 2004-01-01 | Robertson et al. | Examiner |
| US6679226(B2) | 2004-01-01 | Burke et al. | Examiner |
| US2002/0152999(A1) | 2002-10-01 | Holder et al. | Examiner |
| US2003/0140715(A1) | 2003-07-01 | Burke et al. | Examiner |
| US2003/0213474(A1) | 2003-11-01 | Lambert et al. | Examiner |
| US2003/0217584(A1) | 2003-11-01 | Sato et al. | Examiner |
| EP1091111 | 2000-08-01 | Applicant | |
| JP158768 | 1997-06-01 | Examiner | |
| JP2001004605 | 1999-06-01 | Applicant | |
| JP132503 | 2001-05-01 | Examiner |
Non-Patent Literature (14)
- “Integration of Physical Chemosensors”, M.J. Vellekoop, invited, Proceedings of the 1998 Microsystem Symposium, Sep. 10-11, 1998, Delft, The Netherlands, pp. 117-122.Applicant
- “Characterization of Fuel Sprays in Spark Ignition Engines”, P.A. Williams, PH.D Thesis, Dept. of Mechanical Engineering, University College , London, UK, 1994, Thesis No. DX 188495, The British Library.Applicant
- “Viscosity sensing using a Love-wave device”, Jakoby et al., Elsevier Science S.A., Sensors and Actuators A 68 (1998), pp. 275-281.Applicant
- “A Love wave sensor for (bio)chemical sensing in liquids”, Kovacs et al., Sensors and Actuators A, 43 (1994), pp. 38-43.Applicant
- “The Emergence of Physical Chemosensors and Biosensors”, Vellekoop, Proc. Of Transducers '01, Munich, Germany, Jun. 2001.Applicant
- “Determination of Viscosity Changes of Cement Pastewith a Smart Lamb-Wave Sensor System”, Van Beek et al., Proc. Of the 2nd RILEM Workshop on Hydration and Setting, Dijon, France, Jun. 1997, pp. 329-338.Applicant
- “Microfabrication of acousitc-wave devices”, Vellekoop, Proc. of SPIE vol. 3224, Micromachined Devices and Components III, Austin, Texas, Sep. 1997, pp. 90-97.Applicant
- “Design of a Smart Microacoustic Liquid Sensor System, Part I: Microacoustic Device”, “Sensor Technology in the Netherlands: State of the Art”, van den Bert et al., ISBN0-7923-5010-3, 1998, pp. 165-170.Applicant
- “Design of a Smart Microacoustic Liquid Sensor System, Part II: Electronics”, “Sensor Technology in the Netherlands: State of the Art”, van den Bert et al., ISBN0-7923-5010-3, 1998, pp. 171-177.Applicant
- “Properties of Love waves: applications in sensors”, Jakoby et al., Special issue on SAW devices and their applications, Journal of Smart Materials and Structures, vol. 6, No. 6, Dec. 1997, pp. 668-679.Applicant
- “Acoustic wave sensors and their technology”, Vellekoop, Ultrasonics, vol. 36, 1998, pp. 7-14.Applicant
- “Substrates for Zero Temperature Coefficient Love Wave Sensors”, Jakoby et al., IEEE Transactions on UFFC, vol. 47, No. 3, May 2000, pp. 701-705.Applicant
- “Analysis of Viscous Losses in the Chemical Interface Layer of Love Wave Sensors”, Jakoby et al., IEEE Transactions on UFFC, vol. 47, No. 3, May 2000, pp. 696-700.Applicant
- “Analysis and Optimization of Love Wave Liquid Sensors”, Jakoby et al., IEEE Transactions on UFFC, vol. 45, No. 5, Sep. 1998, pp. 1293-1302.Applicant