TECHNICAL FIELDThe present invention relates to an internal combustion engine control system for controlling an internal combustion engine and, more particularly, to an internal combustion engine control system for controlling intake air and fuel in an internal combustion engine.[0001]
BACKGROUND ARTGenerally, the timing of operations of the intake valve and the exhaust valve of engines including direct fuel injection engines is dependent only on the cam profiles of cams driven for rotation in synchronism with the rotation of the crankshaft of the engine. Accordingly, it is difficult to achieve optimum valve timing control in a wide range of operating condition. It is desirable to vary valve timing according to the operating condition to improve the output performance of the engine and the like. It is necessary to vary valve timing so that valve overlap period, i.e., a period in which both the intake and the exhaust valve are open, decreases to prevent the blowby of new charge while the engine is operating at a relatively low engine speed, and so that valve overlap period increases to supply new charge at a high charging efficiency by using exhaust gas pulsation while the engine is operating at a relatively high engine speed.[0002]
A technique relating to such a mode of control of valve timing is disclosed in JP-A No. 6-101508. This prior art technique controls negative pressure in the intake pipe minutely at an optimum value, and controls the timing of closing the intake valve on the basis of parameters indicating the operating condition of the engine including cooling water temperature, intake air temperature and time-dependent changes in the engine in addition to a map showing a function of engine speed and load to reduce pumping loss.[0003]
In an engine which is provided with a throttle valve disposed before an intake system to regulate the quantity of intake air and regulates the quantity of fuel to be injected according to the quantity of intake air, the pressure in the intake pipe is lower than the atmospheric pressure in an operating range in which the load on the engine is relatively low, energy necessary for lowering the piston, i.e., energy necessary to achieve a suction stroke (pumping loss) increases, the ratio of pumping loss to engine output increases and fuel consumption increases.[0004]
The prior art technique, however, keeps the lift of the intake valve and the opening angle fixed and does not control the same. Therefore, the quantity of intake air to be sucked into the combustion chamber of the engine must be controlled by a throttle valve or the like disposed above the intake valve. Therefore, a negative pressure prevails in the intake passage below the throttle valve and in the combustion chamber, causing pumping loss. Accordingly, this prior art technique is not fully satisfactory as regards the reduction of pumping loss and fuel consumption.[0005]
In a direct fuel injection engine in which the fuel is injected directly into the combustion chamber, fuel injection timing is set so that the fuel is injected in a period during the suction stroke and the compression stroke in which the exhaust valve is closed to avoid discharging the unburned fuel. Consequently, time available for the evaporation of the fuel, i.e., time from fuel injection to ignition, is short. Therefore, the fuel must be injected through a fuel injector in small particles to promote the evaporation of the fuel and the mixing of the fuel with air. As is generally known, the higher the fuel injection pressure, the smaller is the particle size of the fuel. Therefore, the fuel is pressurized at a very high pressure of about 5 MPa. However, the fuel injected at a high injection pressure has a very high spray penetration, impinges on the inner surface of the cylinder and the top of the piston, and part of the fuel adheres to the inner surface of the cylinder. The fuel adhering to the inner surface of the cylinder is exhausted without burning to increase the HC (hydrocarbon) content of the exhaust gas. The fuel injector for the direct fuel injection engine is required to inject the fuel in fine particles and to reduce the spray penetration in order that the foregoing problems are solved.[0006]
DISCLOSURE OF INVENTIONIt is an objective of the present invention to provide an internal combustion engine control system for controlling an internal combustion engine, capable of greatly reducing pumping loss while the engine is operating in a low-load range, of reducing fuel consumption, and of enabling satisfactory combustion without adversely affecting exhaust performance.[0007]
The foregoing objective is achieved by an internal combustion engine control system according to one aspect of the present invention for controlling an internal combustion engine, comprising: a fuel injection control means for controlling fuel injection quantity to be injected by a fuel supply system for supplying fuel to the internal combustion engine, and fuel injection timing; and a variable valve control means for continuously or gradually varying at least opening timing, closing timing or lift of a intake valve or an exhaust valve for sealing up a combustion chamber of the internal combustion engine; wherein the fuel injection control means controls at least fuel injection quantity or fuel injection timing on the basis of a value of a controlled variable provided by the variable valve control means.[0008]
The foregoing objective can be achieved by an internal combustion engine control system according to another aspect of the present invention for controlling an internal combustion engine, comprising: a fuel injection control means for controlling fuel injection quantity to be injected by a fuel injection system for directly injecting the fuel into a combustion chamber of the internal combustion engine, and fuel injection timing; and a variable valve control means for continuously or gradually varying at least opening timing, closing timing or lift of a intake valve or an exhaust valve for sealing up the combustion chamber of the internal combustion engine; wherein the fuel injection control means controls at least fuel injection quantity or fuel injection timing on the basis of a value of a controlled variable provided by the variable valve control means.[0009]
The controller of the foregoing construction exercises the following actions and effects. The variable valve control means regulates the opening timing, the closing timing and the lift of the intake valve and the exhaust valve to reduce pumping loss and fuel consumption while the engine is operating in a low-load operation range. The variable valve control means regulates the opening timing, the closing timing and the lift of the intake valve and the exhaust valve to increase charging efficiency and to enhance the output power of the engine while the engine is operating in a high-load operation range. The fuel injection control means controls fuel injection quantity and fuel injection timing according to changes in the variable valve control means to inject the fuel into the combustion chamber in satisfactory particles to enable stable combustion and to reduce the hydrocarbon concentration of the exhaust gas.[0010]
BRIEF DESCRIPTION OF DRAWINGSFIG. 1 is a typical view illustrating the configuration of a first embodiment of the present invention;[0011]
FIG. 2 is a typical view of assistance in explaining a variable valve timing mechanism according to the present invention;[0012]
FIG. 3 is a graph showing the relation between valve lift and fuel injection quantity in the first embodiment;[0013]
FIG. 4 is a graph showing the variations of fuel injection quantity and intake air quantity with valve lift in the first embodiment;[0014]
FIG. 5 is a graph showing the relation between valve lift and pressure in a combustion chamber in the first embodiment;[0015]
FIG. 6 is a view of assistance in explaining a principle of shock wave generation;[0016]
FIG. 7 is a typical sectional view of assistance in explaining fuel atomization by a shock wave in a combustion chamber;[0017]
FIG. 8 is a block diagram showing the flow of control signals in the first embodiment;[0018]
FIG. 9 is a diagrammatic view of a map for determining the operating mode of an engine in the first embodiment;[0019]
FIG. 10 is a block diagram showing the flow of control signals in the first embodiment;[0020]
FIG. 11 is a diagram of assistance in explaining the relation between the state of the intake valve and fuel injection timing;[0021]
FIG. 12 is a graph showing the variations of the lift of a valve, fuel injection quantity and air/fuel ratio with the stepping-on measurement of an accelerator pedal;[0022]
FIG. 13 is a block diagram showing the flow of a control signal in a second embodiment;[0023]
FIG. 14 is a graph of assistance in explaining a third embodiment of the present invention;[0024]
FIG. 15 is a graph of assistance in explaining a fourth embodiment of the present invention;[0025]
FIG. 16 is a graph of assistance in explaining a fifth embodiment of the present invention;[0026]
FIG. 17 is a typical view of a sixth embodiment of the present invention;[0027]
FIG. 18 is a graph showing the relation between the volume of a combustion chamber and pressure in the combustion chamber when compression ratio is equal to expansion ratio;[0028]
FIG. 19 is a graph showing the relation between the volume of a combustion chamber and pressure in the a combustion chamber when compression ratio is not equal to expansion ratio; and[0029]
FIG. 20 is a graph showing the dependence of compression ratio and expansion ratio on pressure in a suction pipe.[0030]
BEST MODE FOR CARRYING OUT THE INVENTIONFIG. 1 is a view showing the configuration of a first embodiment of the present invention and illustrating one of the cylinders of an engine in a sectional view. Referring to FIG. 1, an[0031]engine1 is provided with apiston2, afuel injector3, aintake valve4, anexhaust valve5, anignition plug6, a combustionchamber pressure sensor24 for sensing pressure in a combustion chamber, and aknocking sensor25. Aintake pipe18 is provided with anair flow sensor7, anair cleaner8 and a intakepipe pressure sensor23 for sensing pressure in theintake pipe18. Anexhaust pipe19 is provided with an air/fuel ratio sensor9, acatalytic unit10, and acatalyst temperature sensor26 for sensing catalyst temperature, i.e., the temperature of thecatalytic unit10. Signals provided by theair flow sensor7, the intakepipe pressure sensor23, the combustionchamber pressure sensor24, theknocking sensor25, the air/fuel ratio sensor9, thecatalyst temperature sensor26 and acrank angle sensor16 are given to anengine controller13. An operatingmode detecting unit27 detects an operating mode of theengine1 on the basis of the signals received by theengine controller13. A variablevalve control unit28 generates control signals for controlling the timing of operations of thesuction valve4 and theexhaust valve5 and the lift of thesuction valve4 and theexhaust valve5 on the basis of the result of determination made by the operatingmode detecting unit27 and gives the same to variablevalve timing mechanisms11 and12 to control theintake valve4 and theexhaust valve5. A fuelinjection control unit29 generates control signals specifying a fuel injection quantity and fuel injection timing on the basis of the control signals provided by the operatingmode detecting unit27 and the variable valvetiming control unit28 to control thefuel injector3. Thefuel injector valve3 operates according to the control signal given thereto by the fuelinjection control unit29 to inject thefuel20 into acombustion chamber17. An ignition control unit, not shown, generates an ignition signal on the basis of the control signals provided by the operatingmode detecting unit27, the variablevalve control unit28 and the fuelinjection control unit29 to drive the ignition plug for ignition to cause the combustion of the mixture in thecombustion chamber17 of theengine1.
When the[0032]engine1 is in a suction stroke, in which the piston is moving from the top dead center toward the bottom dead center, theintake valve4 is operated for an opening operation by the variablevalve timing mechanism11 for theintake valve4. In this state, air flowing through theair cleaner8 and theair flow sensor7 is sucked into theengine1. Theengine1 is not provided with any throttle valve and the quantity of intake air is controlled by the intake valve. The variablevalve timing mechanism11 keeps theintake valve4 closed while thepiston2 is moving near the bottom dead center. Thepiston2 moves upward to compress thecombustion chamber17. If theengine1 is a direct fuel injection engine, thefuel injector valve3 injects thefuel20 into thecombustion chamber17 while theengine1 is in a suction stroke and a compression stroke. The injectedfuel20 mixes with air in thecombustion chamber17, is compressed by thepiston2, and is ignited by theignition plug6 for combustion. Thepiston2 is caused to move downward by a high pressure generated by the combustion of the fuel. The movement of thepiston2 is transmitted through a connectingrod21 to acrankshaft22 to make the engine provide power through thecrankshaft22. Subsequently, the variablevalve timing mechanism12 for theexhaust valve5 opens theexhaust valve5 upon the arrival of thepiston2 moved by the expansion of a high-temperature combustion gas at a position near the bottom dead center to discharge the combustion gas from thecombustion chamber17. Then, thepiston2 moves from the bottom dead center to the top dead center to push out the gas staying in thecombustion chamber17.
The[0033]engine controller13 determines the operating condition of theengine1 on the basis of the engine speed of theengine1, the intake air quantity, the stepping-on measurement of anaccelerator pedal14, the suction pipe pressure, i.e., the pressure in the intake pipe, the combustion chamber pressure, i.e., the pressure in thecombustion chamber17, a combustion mode with or without knocking, the air/fuel ratio and the catalyst temperature, i.e., the temperature of the catalytic unit. The engine speed of theengine1 is measured by thecrank angle sensor16 attached to an end of thecrankshaft22, the quantity of intake air is measured by theair flow sensor7 disposed in theintake pipe18, the stepping-on measurement of theaccelerator pedal14 is measured by apotentiometer15 connected to theaccelerator pedal14, the pressure in the intake pipe is measured by the intakepipe pressure sensor23 disposed in theintake pipe18, the pressure in the combustion chamber is measured by the combustionchamber pressure sensor24 disposed in thecombustion chamber17, the knocking operation of theengine1 is detected by the knockingsensor25 disposed near thecombustion chamber17, the air/fuel ratio is measured by the air/fuel ratio sensor9 disposed in theexhaust pipe19, the temperature of the catalytic unit is measured by thecatalyst temperature sensor26 attached to the catalytic unit, and the temperature of cooling water is measured by a water temperature sensor, not shown.
The variable valve timing mechanisms of the present invention are of a direct hydraulic drive system as shown in FIG. 2.[0034]Pistons202 and203 are in contact respectively with aintake valve stem200 and anexhaust valve stem201. Twoselector valves205 and206 for valve opening control and valve closing control are disposed in aline204 connected to thepistons202 and203. When opening theintake valve4 and theexhaust valve5, theselector valve205 is opened by supplying a high-pressure working fluid through aline207 to thepistons202 and203. After theintake valve4 and theexhaust valve5 have been lifted by predetermined valve lifts, theselector valve205 is closed to seal the working fluid in a portion of the line on the side of thepistons202 and203 so that thevalves4 and5 are held at the predetermined valve lifts. When closing thevalves4 and5, theselector valve206 is opened to discharge the working fluid sealed in the portion of the line on the side of thepistons202 and203 to flow through adrain line208 so that the valves are closed by valve springs209 and210. The valves may be directly driven by electromagnetic forces.
FIG. 3 is a graph showing the relation between the valve lifts of the[0035]intake valve4 and theexhaust valve5, and fuel injection quantity in the first embodiment of the present invention. Theengine controller13 determines timing for opening theintake valve4, timing for closing theintake valve4 and a lift by which theintake valve4 is lifted. When theengine1 is operating at a high engine speed under a high load, theintake valve4 starts opening before the piston reaches the top dead center TDC and the crankshaft is at a crank angle a so that an open state of theintake valve4 and an open state of theexhaust valve5 indicated by avalve lift curve50 overlap greatly, and theintake valve4 is lifted by a large lift A to increase the quantity of intake air. Timing for closing theintake valve4 is determined so that theintake valve4 is closed at a crank angle a′ after the bottom dead center BDC for the utmost utilization of the effect of inertia supercharging. When theengine1 is operating under a low load, theintake valve4 is opened at a crank angle c corresponding to a position of the piston after the top dead center to prevent discharging a new charge taken into the stepping-on measurement through theintake valve4 through theexhaust valve5, theintake valve4 is closed at a crank angle corresponding to a position of the piston before the bottom dead center to shorten valve opening period, and theintake valve4 is lifted by a small lift C to reduce the quantity of intake air. Theintake valve4 can be opened at a crank angle b, can be lifted by a lift B and can be closed at a crank angle b′ by continuously varying the opening timing for opening theintake valve4, the closing timing for closing theintake valve4 and the lift of theintake valve4.
Fuel injection timing is determined so as to be synchronized with opening timing for opening the[0036]intake valve4 and the closing timing for closing theintake valve4. In the embodiment shown in FIG. 3, the fuel is injected in synchronism with the opening of theintake valve4. When the fuel is thus injected into the combustion chamber, fuel droplets injected into the combustion chamber immediately after the opening of theintake valve4 and flying in the combustion chamber are torn off, blown and atomized by rapid air currents flowing into the combustion chamber immediately after the opening of theintake valve4. The atomized fuel is mixed satisfactorily with air in the combustion chamber to produce a mixture which can be easily ignited, so that the mixture ignites surely, misfire does not occur and stable combustion is achieved. In the direct fuel injection engine, the fuel is liable to adhere in a liquid state to portions of the engine around the fuel injector, the fuel adhering to walls in a liquid state does not mix with air satisfactorily, and hence misfire or abnormal combustion is liable to occur. The rapid air currents exerts an effect of separating the liquid fuel from the wall to improve combustion.
The fuel injection quantity is dependent on the valve lift of the[0037]intake valve4. A large quantity of air is sucked and hence the fuel injection quantity is α and theintake valve4 is opened at a crank angle a if theintake valve4 is opened in a mode represented by acurve51. A small quantity of air is sucked and hence the fuel injection quantity is and theintake valve4 is opened at a crank angle c if theintake valve4 is opened in a mode represented by acurve53. If the timing of opening theintake valve4, the valve lift and the timing of closing theintake valve4 are varied continuously and intermediate conditions (a intake valve opening crank angle b, a valve lift B, and a intake valve closing crank angle b′) are selected, a fuel injection quantity is β and theintake valve4 is opened at a crank angle b.
FIG. 4 is a graph showing the variations of fuel injection quantity and intake air quantity with valve lift in the first embodiment. In view of the controllability of the engine, it is desirable that the intake air quantity varies with valve lift linearly as indicated by a[0038]curve56a. However, intake air quantity varies with valve lift in a mode indicated by acurved section56bof thecurve56awhen valve lift is small. If air/fuel ratio is fixed at a set air/fuel ratio, such as 14.7, fuel injection quantity is dependent on valve lift as indicated by acurve55b. If the set air/fuel ratio is varied according to the operating condition of the engine, one ofcurves55ato55dis used selectively. A conventional method, which retrieves and determines a fuel injection quantity by an engine speed measured by the crank angle sensor and an air quantity measured by the air flow sensor from a fuel injection quantity map stored in theengine controller13, may be used.
FIG. 5 is a graph showing the relation between the respective valve lifts of the[0039]intake valve4 and theexhaust valve5, and the pressure Pc in the combustion chamber in the first embodiment. In FIG. 5, acurve40 indicates the variation of the valve lift of the exhaust valve. In this embodiment, control operation is executed so that the timing of opening the valve, the timing of closing the valve and the valve lift are fixed. A curve indicates the variation of the valve lift of the intake valve when the intake valve is operated according to conditions for high-load operation. In this operating state, the pressure Pc in thecombustion chamber17 is substantially equal to the atmospheric pressure Pa as indicated by acurve43 while theexhaust valve5 opens in a mode indicated by acurve40 for exhaust stroke. If theintake valve4 is opened at a crank angle a and theexhaust valve5 is closed at a crank angle b so that an open state of theintake valve4 and an open state of theexhaust valve5 overlap each other in an angular period between the crank angles a and b, the pressure Pc in thecombustion chamber17 varies as indicated by agray curve44 and becomes substantially equal to the pressure Pb in theintake pipe18 during suction stroke. In an engine provided with a throttle valve disposed above an intake system to control air flow, the pressure Pb is below the atmospheric pressure Pa. In the engine of the present invention not provided with any throttle valve, the pressure Pb is substantially equal to the atmospheric pressure. If theintake valve4 is not opened after theexhaust valve5 has been closed, the pressure Pc in thecombustion chamber17 will decrease as indicated by abroken curve45 and when the piston reaches the bottom dead center BDC,
Pc=Pa/ε (1)
where * is the compression ratio of the[0040]engine1. If theintake valve4 is opened at a crank angle c which makes the pressure Pc meet an inequality:
Pc<0.54*Pb
the pressure Pc in the[0041]combustion chamber17 increases sharply, thereby generating an accompanying shock wave.
A principle of shock wave generation will be briefly described with reference to FIG. 6. Suppose that a high-[0042]pressure chamber215 and a low-pressure chamber216 partitioned by apartition film217 contain a stationary gas, the pressure in the high-pressure chamber is P1 and the pressure in the low-pressure chamber is P2. If thepartition film217 is broken when
P2/P1<0.54 (3)
the gas flows at a high velocity from the high-[0043]pressure chamber215 into the low-pressure chamber216. The velocity of the gas is not lower than a sound velocity; that is the gas flows at a velocity higher than Mach number one. Shock waves are classified into compression waves which increase the pressure, temperature and density of a gas as they propagate, and expansion waves which reduce the pressure, temperature and density of a gas as they propagate. A compression wave propagates from the high-pressure chamber215 toward the low-pressure chamber216. Pressure, temperature and density change discontinuously at the wavefront of a shock wave; the same increases at the wavefront of a compression wave.
If such a shock wave is generated in the combustion chamber of the engine, the shock wave is reflected repeatedly by the wall defining the combustion chamber. It is the point of the present invention to atomize the fuel by vibrating a spray of the fuel injected into the combustion chamber by the pressure energy of the shock wave.[0044]
The foregoing effect is available if the start of fuel injection is timed so as to be synchronized with the opening timing of the suction valve to inject the fuel into the combustion chamber immediately after the generation of a shock wave or while a shock wave is being generated as shown in FIG. 3. Thus, the fuel can be effectively atomized simply by controlling fuel injection start timing and intake valve opening timing, and any special modification of the fuel injector and the like for the atomization of the fuel is not necessary.[0045]
The generation of a shock wave must be predicted or detected and fuel injection must be controlled to realize the foregoing effect on an actual engine. One of methods of realizing the foregoing effect on an actual engine uses a crank angle sensor disposed on an engine. The crank angle sensor measures crank angles through the measurement of angular positions of a gear or a disk attached to the crankshaft or the like at angular intervals of several degrees, and gives signals representing the angular positions to an operating mode detecting unit for detecting an operating mode of the engine. The pressure Pc in the combustion chamber of the engine is substantially equal to the atmospheric pressure Pa at a moment immediately after the exhaust valve has been closed as shown in FIG. 5. If the intake valve is not opened while the piston is moving downward after the exhaust valve has been closed, the pressure Pc in the combustion chamber decreases as indicated by the[0046]curve45 as mentioned above. The pressure Pc in the combustion chamber meet an expression:
Pc=0.54*Pc (4)
if the volume V of the combustion chamber meet an expression:[0047]
V=Vt/0.54 (5)
where Vt is the volume of the combustion chamber with the piston at the top dead center; that is, a shock wave is generated if the intake valve is opened when the volume ratio, i.e., the ratio of the volume of the combustion chamber to the volume of the same with the piston at the top dead center, is 1/0.54≈2 or above. Therefore, the engine controller is able to find the variation of the volume of the combustion chamber dependent on the bore of the combustion chamber and the stroke of the piston from the crank angle and is able to predict the generation of a shock wave on the basis of the variation of the volume of the combustion chamber.[0048]
Another method uses a intake pipe pressure sensor disposed in the intake passage of an engine to measure the pressure in a suction pipe. This method measures the pressure Pb in the intake pipe while the exhaust valve is closed, an operating mode detecting unit receives a pressure signal indicating the pressure Pb, and an arithmetic circuit included in an engine controller calculates a crank angle where the pressure Pc in the combustion chamber is expressed by:[0049]
Pc=0.54*Pb (6)
and intake valve opening timing is determined so that the intake valve is opened at the calculated crank angle. Then, as mentioned above, the fuel is injected in synchronism with intake valve opening timing. This method also is able to predict the generation of a shock wave. This method which employs the intake pipe pressure sensor for measuring the pressure in the intake pipe for predicting the generation of a shock wave is effective when a throttle valve is disposed above the intake system, when the engine is provided with a supercharger or when the atmospheric pressure changes because the engine is operated at a place in highlands, i.e., when the pressure in the intake pipe is changed.[0050]
A third method of sensing the generation of a shock wave employs a combustion chamber pressure sensor disposed in the combustion chamber of an engine to measure the pressure in the combustion chamber. This method measures the pressure Pc in the combustion chamber at a moment the exhaust valve is closed, the measured pressure Pc is read by an operating mode detecting unit to hold the pressure in an engine controller, the variable pressure in the combustion chamber varying with the downward movement of the piston is measured continuously and the intake valve is opened when the value of the pressure Pc meets an expression:[0051]
Pc=0.54*Pc (7)
As mentioned above the fuel is injected in synchronism with intake valve opening timing. This method is able to predict the generation of a shock wave, and is able to ascertain the generation of a shock wave through the measurement of the variation of the pressure in the combustion chamber after the generation of the shock wave.[0052]
FIG. 7 typically illustrates the condition of the interior of a combustion chamber when a shock wave is generated in the combustion chamber. A[0053]shock wave59 is generated upon the opening of theintake valve4 when one of the foregoing conditions for shock wave generation expressed by Expressions (1) to (5) is satified, thefuel20 injected simultaneously with the opening of theintake valve4 is vibrated and atomized by the pressure energy of the shock wave. Having a small mass, the atomized particles of the fuel are easily carried by air currents and disperse insprays57 and58.
In this embodiment, intake valve opening timing is varied by the variable valve timing mechanism to generate a shock wave in the combustion chamber, and the fuel is injected in synchronism with the generation of the shock wave to atomize the fuel as shown in FIG. 7.[0054]
FIG. 8 is a block diagram showing the flow of control signals in the first embodiment. Flow of control signals in the engine controller and prediction of generation of a shock wave will be described with reference to FIG. 8. In a[0055]block27, theengine controller13 for controlling theengine1 shown in FIG. 1 receives and holds data on engine speed, intake air quantity, stepping-on measurement of the accelerator pedal, pressure in the intake pipe, pressure in the combustion chamber, knocking, cooling water temperature and temperature of the catalytic unit, and determines the operating mode of the engine, i.e., a high-load operating mode, a medium-load operating mode or a low-load operating mode, from the data. For example, the operating mode detecting unit refers to a map of FIG. 9 defining operating condition of the engine by engine speed and the stepping-on measurement of the accelerator pedal, and decides that the engine is operating in the low-load, the medium-load or the high-load operating mode when the operating condition of the engine defined by engine speed and the stepping-on measurement of the accelerator pedal falls in a region L, a region M or a region H. In ablock28, the intake valve is controlled so as to generate a shock wave if it is decided in theblock27 that the engine is operating in a low-load or a medium-load operating mode. The generation of a shock wave is predicted or ascertained from signals provided by the crank angle sensor, the intake pipe pressure sensor and the combustion chamber pressure sensor, and fuel injection is started simultaneously with the generation of a shock wave. If it is decided that the engine is operating in a high-load operating mode, the engine output demanded by the driver is estimated from the stepping-on measurement of the accelerator, and the lift of the intake valve is increased and the open period of the intake valve is extended to increase intake air quantity so that the engine will provide the demanded engine output. Although any shock wave is not generated in such an operating mode, a spray of the fuel and air are mixed satisfactorily, stable combustion can be achieved and any problem does not arise because the flow of air in the combustion chamber is intensified by the increased intake air quantity and an increased engine speed.
In a[0056]block60 included in ablock29, an intake air quantity is estimated from the lift of the intake valve determined in theblock28 and determines a fuel injection quantity so that a mixture of the set air/fuel ratio can be produced. The fuel injection quantity may be determined from the map defining fuel injection quantities as a function of engine speed and intake air quantity stored in theblock27. If theblock27 decides that the engine is operating in a low-load or the medium-load operating mode, and a shock wave is to be generated, ablock61 determines fuel injection starting time so that fuel injection starting timing is synchronized with intake valve opening timing. If it is decided that the engine is operating in a high-load operating mode and any shock wave need not be generated, intake valve opening timing is advanced to increase an overlapping period in which both the intake valve and the exhaust valve are open to increase the charging efficiency by the agency of the pulsation of the negative pressure in the exhaust pipe. Control signals for controlling intake valve opening timing, intake valve closing timing, the valve lift, the fuel injection quantity and fuel injection start timing determined in theblocks28 and29 are given to the variable valve timing mechanism in ablock11, and to the fuel injector in a block3 and operations are timed by those timing signals.
Another method of accurately determining intake valve opening timing to generate a shock wave, which is a point of the present invention, will be described with reference to FIG. 10. FIG. 10 is a block diagram showing the flow of control signals between the[0057]blocks27 and28. Ablock64 calculates a crank angle at which the combustion chamber pressure Pc shown in FIG. 5 meets Expression (6) by using the signal indicating the intake pipe pressure Pb and received by theblock27, and ablock66 determines intake valve opening timing on the basis of the crank angle calculated by theblock64. A third method determines which one of Expressions (4), (6) and (7) is met by the combustion chamber pressure Pc by ablock65 when a signal indicating the combustion chamber pressure Pc is given to theblock27, and ablock66 decides a crank angle at that time as intake valve opening timing. Thus, intake valve opening timing can be accurately determined.
Another method of determining fuel injection starting time by the[0058]block61 of FIG. 8 will be described with reference to FIG. 11 showing the relation between stepping-on measurement of the accelerator pedal, and open state and fuel injection timing. For example, intake valve opening timing and intake valve closing timing vary alongcurves220 and221 according to the operating mode of the engine determined by theblock27 of FIG. 8. Valve lift varies along acurve78 shown in FIG. 12. If it is decided that the engine is operating in a low-load operating mode, an angular interval between intake valve opening timing and intake valve closing timing is small, the intake valve is open for a short time and valve lift is small. If it is decided that the engine is operating in a medium-load operating mode, intake valve opening timing is advanced and intake valve closing timing is delayed to increase the intake valve opening period, and valve lift is increased. In this case, the fuel injection start timing is set close to the intake valve opening timing as indicated by acurve222 to generate a shock wave. If it is decided that the engine is operating in a high-load operating mode, the overlap of the intake valve and the exhaust valve is further increased by further advancing the intake valve opening timing and further delaying the intake valve closing timing so that charging efficiency is increased by the pulsation of a negative wave in the exhaust pipe and the pulsation of a positive wave in the intake pipe to further increase the intake air quantity. If fuel injection start timing222 is advanced ahead of exhaustvalve closing timing223, it is possible that unburned fuel is discharged and the quality of the exhaust gas is deteriorated. Therefore, fuel injection start timing222 cannot be advanced ahead of exhaustvalve closing timing223 and hence any shock wave cannot be generated in this case. However, a spray of the fuel and air are mixed satisfactorily, combustion is not deteriorated and any problem does not arise because the flow of air in the combustion chamber is intensified by the increased intake air quantity and an increased engine speed.
If a lean burn operation using a mixture of a large air/fuel ratio is desired, an angular delay * of fuel injection timing[0059]224 behind intake valve opening timing may be increased so that fuel injection start timing224 is close to intake valve closing timing or fuel injection start timing may be delayed as indicated at225 behind intake valve closing timing. If fuel injection is started at such delayed fuel injection start timing, the fuel is not dispersed in a wide region and concentrated on regions around the ignition plug to produce the so-called stratified mixture suitable for lean burning.
FIGS. 12 and 13 show a second embodiment of the present invention. FIG. 12 is a graph showing the variations of valve lift, fuel injection quantity and air/fuel ratio with the stepping-on measurement of an accelerator pedal. A stepping-on measurement of the accelerator pedal represents an engine output demanded by the driver. It is considered that a high engine output is demanded when stepping-on measurement of the accelerator pedal is large, and it is considered that not a very high engine output is demanded when stepping-on measurement of the accelerator pedal is small. An engine like that of the present invention not provided with any throttle valve in the intake system needs to control intake air quantity to be sucked into the combustion chamber of the engine by the intake valve. Since the quantity of air flowing through the intake valve is roughly proportional to the area of an opening formed by lifting the intake valve, air quantity can be estimated from the lift of the intake valve. This method is able to estimate air quantity without delay and, if the engine is of a direct fuel injection type, the fuel may be injected into the combustion chamber after estimating air quantity by this method. Accordingly, the fuel injection quantity can be controlled according to air quantity which varies every cycle to avoid deteriorating the quality of the exhaust gas, to stabilize combustion and to reduce vibrations of the engine. A method of correcting the estimated air quantity by using a measured air quantity measured by an air flow sensor may be employed additionally.[0060]
In this embodiment, valve lift is controlled according to the variation of the stepping-on measurement of the accelerator pedal as indicated by a[0061]curve78 in FIG. 12, and a fuel injection quantity is determined as indicated by acurve77 on the basis of an estimated air quantity estimated on the basis of valve lift or a corrected air quantity determined by correction using a measured air quantity measured by the air flow sensor. When determining fuel injection quantity, a set air/fuel ratio for the stepping-on measurement of the accelerator pedal is taken into consideration. The engine controller decides that engine output demanded by the driver is low if the stepping-on measurement of the accelerator pedal is small, and reduces the valve lift of the intake valve to reduce intake air quantity. The estimation of intake air quantity is difficult, the accurate estimation of intake air quantity is impossible, the flow of air in the combustion chamber becomes sluggish and unstable combustion occurs if the valve lift is excessively small. Therefore, as shown in FIG. 13 in a block diagram, the valve lift is fixed when the stepping-on measurement of the accelerator pedal is not greater than a value X to keep intake air quantity constant, fuel injection quantity is reduced and air/fuel ratio is increased to control engine output. Thus, the deterioration of combustion is avoided. Fuel consumption is improved by the reduction of fuel injection quantity. With a direct fuel injection engine, in particular, response characteristic is excellent because the fuel is injected directly into the combustion chamber.
FIG. 14 is a graph of assistance in explaining a third embodiment of the present invention. Usually, engine output is increased by increasing intake air quantity to provide driving power for driving an engine accessory, such as an air conditioning system while an engine is operating under a very light load, i.e., while the engine is idling. In a conventional engine provided with a throttle valve, intake air quantity is regulated by opening and closing a bypass passage bypassing the throttle valve by a valve disposed in the bypass passage for the fine adjustment of air quantity without opening the throttle valve, which, however, increases the number of parts and increases the costs. In the[0062]engine1 illustrated in FIG. 1, the variable valve timing mechanism of the present invention keeps the open period and the valve lift of the intake valve constant and regulates intake valve opening timing and suction valve closing timing minutely to regulate the engine speed and the driving force of the engine. When the engine is in a suction stroke, the piston moves from the top dead center TDC toward the bottom dead center BDC and air is sucked accordingly into the combustion chamber. When the crankshaft is at crank angles a and b, the piston is near the top dead center and moves at a low speed, and hence intake air quantity is small. When the crankshaft is at a crank angle c, the piston is at a position past the top dead center and the speed of the piston is increasing, and hence intake air quantity increases even if the valve lift and the open period of the intake valve are kept constant. Therefore, if it is desired to provide driving force for driving, for example, an accessory, engine speed is increased by adjusting the intake valve opening timing so that the intake valve is opened at the crank angle c to increase engine output. If the intake valve opening timing corresponds to the crank angle a or b, engine speed is suppressed to prevent the increase of fuel consumption. Thus, the variable valve timing mechanism of the present invention is able to exercise the foregoing effects without requiring any additional parts.
FIG. 15 is a graph of assistance in explaining a fourth embodiment of the present invention. FIG. 15 shows the relation between crank angle and intake pipe pressure Pb. Pressure in the intake pipe of an engine pulsates when a intake valve is opened, and a positive pressure wave of a pressure above the mean intake pipe pressure and a negative pressure wave of a pressure below the mean intake pipe pressure propagate alternately. Therefore, an increased quantity of air greater than a normal quantity of air is sucked into the combustion chamber, effectively increasing engine output if a positive pressure wave portion of pressure pulsation enters the combustion chamber. If a negative pressure wave portion of pressure pulsation enters the combustion chamber, a reduced quantity of air smaller than the normal quantity of air is sucked into the combustion chamber and thereby engine output decreases. Therefore, a mechanism for changing the length of the intake pipe has been employed to make a positive pressure wave enter the combustion chamber regardless of engine speed. Most methods employing such a mechanism change the length of the intake pipe gradually, and thus the foregoing inertia supercharging effect is available only in a range of engine speed matching with the length of the intake pipe. A structure for changing the length of the intake pipe is necessary, which increases the number of parts and the cost. According to the present invention, in the[0063]engine1 shown in FIG. 1, theengine controller13 determines the intake pipe pressure on the basis of the output signal of the intakepipe pressure sensor23, and closes the intake valve instantaneously upon the entrance of a positive pressure wave of intake pipe pressure pulsation indicated by acurve90,91 or92 as shown in FIG. 15. Thecurves90,91 and92 indicate, for example, pulsations of intake pipe pressure Pb when engine speed is 1000, 2000 and 3000 rpm, respectively, and have different phases. Engine output can be enhanced by raising combustion chamber pressure, i.e., by increasing air quantity, by instantaneously closing the intake valve as indicated by acurve94,95 or96. Thus, the foregoing inertia supercharging effect is available in a wide range of engine speed. Thus, the variable valve timing mechanism of the present invention is able to exercise the foregoing effects without requiring any additional parts.
FIG. 16 is a graph of assistance in explaining a fifth embodiment of the present invention. FIG. 16 shows a mode of increase of catalyst temperature with the variation of exhaust valve opening timing. Catalyst temperature is low in a state immediately after the start of the engine and hence the exhaust gas cannot be purified at a high purification ratio. However, the engine discharges the unburned fuel due to imperfect combustion during operation immediately after the start of the engine. Since the purification power of the catalyst is low until its temperature rises beyond an activation temperature, the unburned fuel discharge from the engine during operation immediately after the start of the engine is discharged outside through the exhaust pipe, causing environmental pollution by the exhaust gas. A conventional method uses an electric heater to heat the catalyst quickly to a temperature above the activating temperature. However, the electric heater employed in this method needs much power, increases load on the vehicle for power generation and, consequently, air quantity is increased and engine speed is raised to increase power generated by the engine. Consequently, power consumption increases inevitably and cost increases. According to the present invention, in the[0064]engine1 shown in FIG. 1, the engine controller determines catalyst temperature on the basis of the output signal of the catalyst temperature sensor during operation immediately after the start of the engine, and advances normal exhaust valve opening timing EVO1 to advanced exhaust valve opening timing EVO2 as indicated by a curve111 if the measured catalyst temperature is lower than the activating temperature Tc to discharge the high-temperature exhaust gas from the combustion chamber during the expansion stroke to heat the catalyst as indicated by acurve110. The advanced exhaust valve opening timing EVO2 is delayed to the normal exhaust valve opening timing EVO1 after the catalyst has been heated to a temperature not lower than the activating temperature. The variable valve timing mechanism of the present invention which carries out this method is able to exercise the foregoing effects without requiring any special device.
FIG. 17 shows a sixth embodiment of the present invention. A[0065]mechanical supercharger151 for enhancing the pressure of intake air is disposed in asuction duct18 of anengine1 to supply air of a pressure above the atmospheric pressure to theengine1. In the engine provided with thesupercharger151, knocking occurs due to an excessively high boost pressure. The supercharger may be a turbo charger, a supercharger or a motor-driven charger. FIG. 18 shows the theoretical relation between the volume of a combustion chamber and pressure in the combustion chamber on an assumption that combustion and gas exchange occur in a moment. Referring to FIG. 18, theengine1 sucks air pressurized by the supercharger in the suction stroke from apoint7 to apoint1 and compresses a mixture of air and the fuel in acombustion chamber17 in a time from thepoint1 to apoint2, the mixture is ignited and burns instantaneously and the pressure in the combustion chamber increases at thepoint2 to a pressure at apoint3. The high-pressure combustion gas depresses a piston in the expansion stroke from thepoint3 to apoint4 to deliver engine output. An exhaust valve is opened at thepoint4, exhaust pressure drops instantaneously in a time from thepoint4 to apoint5, and the gas is discharged from the combustion chamber in a time from thepoint5 to apoint6. Occurrence of knocking will be explained with reference to FIG. 18. Knocking, i.e., the generation of unpleasant sound and vibrations, occurs when boost pressure is excessively high, the temperature of the compressed mixture, i.e., temperature at thepoint2, is excessively high, and detonation other than normal flame propagation starts in a portion of the unburned mixture. A conventional knocking evasion method sets the engine at a low compression ratio. However, in the conventional engine in which valve opening timing and valve closing timing are fixed, expansion ratio is decreased if the compression ratio is decreased, and the efficiency of the conversion of thermal energy generated in the combustion chamber into engine output is reduced. In FIG. 18, a compression ratio * and an expansion ratio *′ are expressed by:
ε=ε′=1+Vs/Vc (8)
where Vc is the volume of the combustion chamber and Vs is the stroke volume of the[0066]engine1.
FIG. 19 shows the theoretical relation between the volume of a combustion chamber and pressure in the combustion chamber on an assumption that combustion and gas exchange occur in a moment. When the intake valve is closed by the variable valve timing mechanism of the present invention at a[0067]point8 during the suction stroke in which the piston is moving down, combustion chamber pressure Pc expands from thepoint8 to apoint1, changes from thepoint1 to thepoint8 as the piston moves up after passing the bottom dead center, and returns to thepoint8. Subsequently, substantial compression is started. Therefore, compression ratio is expressed by:
ε=1+Vs′/Vc (9)
The mixture is ignited at a[0068]point2 and burns. Expansion ratio in the expansion stroke from apoint4 to apoint5 is:
ε′=1+Vs/Vc
Since Vs′<Vs, (compression ratio)<(expansion ratio). In FIG. 19, a substantial suction stroke is carried out from a[0069]point7 to apoint8 and intake air quantity is small. Since the substantial compression ratio is low, the temperature of the compressed mixture, i.e., a temperature at thepoint2, is lower than the temperature of the compressed mixture when the compression ratio is high, i.e., a temperature at apoint2′ and, consequently, knocking can be evaded.
Although the compression ratio is low, the expansion ratio is high and hence thermal energy generated in the combustion chamber can be effectively converted into engine output. Accordingly, the substantial compression ratio can be changed by controlling the intake valve closing timing at the[0070]point8 to evade knocking. FIG. 20 shows the dependence of compression ratio and expansion ratio on boost pressure. When boost pressure is increased, the engine controller determines whether or not knocking has occurred on the basis of the output signal of the knocking sensor and, if knocking has occurred, advances intake valve closing timing to reduce the substantial compression ratio. However, the expansion ratio is kept constant to convert the thermal energy generated in the combustion chamber effectively into engine output.
In a supercharged engine in which the fuel is injected through a suction port, the ratio of specific heat of a mixture supercharged into the combustion chamber is affected greatly by the ratio of specific heat of the fuel and is in the range of 1.2 to 1.3. When supercharging a direct fuel injection engine, in which the fuel is injected directly into the combustion chamber, according to the present invention, the supercharger pressurizes only air, the pressurized air is supercharged into the combustion chamber, and then a quantity of the fuel determined on the basis of the quantity of air is injected. Therefore, the ratio of specific heat of a mixture thus produced is nearly equal to 1.4 times the ratio of specific heat of air and hence the quantity of air greater than that of air which can be charged into the intake port fuel injection engine can be charged into the intake fuel injection engine to enhance engine output.[0071]
Knocking can be easily evaded and, at the same time, engine output can be enhanced by the foregoing structure.[0072]