[0001] The invention relates to a system for reducing detonation phenomena in a combustion
chamber of an endothermic engine.
[0002] As is known, a detonation, i.e. an explosion due to anomalous combustion of the air/fuel
mixture, takes place in a combustion chamber in the presence of elevated temperatures
at particular hot spots in the chamber and in the presence of high internal pressure
levels. The detonation is particularly damaging in that it leads to high thermal and
metallurgical fatigue of the material of which the chamber is made and the components
(such as the valves) installed in the combustion chamber.
[0003] The object of the invention is to produce a system which permits the detonation phenomena
to be reduced so as to prevent the above-mentioned disadvantages.
[0004] On the basis of the invention a system is produced for reducing detonation phenomena
in a combustion chamber of an endothermic engine of an engine assembly which comprises
an air intake manifold, a multiplicity of cylinders, a first pipe for conveying exhaust
gases from the said cylinders, a system for electronic ignition and a system for electronic
injection, characterized in that it comprises :
means for detecting the detonation phenomenon; means for conveying exhaust gases from
the said first pipe to the said combustion chamber; and means connected to the said
means for detecting and controlling the said means for conveying exhaust gases to
determine the inflow of exhaust gases in the said combustion chamber in order to reduce
the possibility of a recurrence of the conditions which trigger the detonation phenomenon.
[0005] A preferred embodiment will now be described in order to provide a better understanding
of the invention, purely by way of non-exhaustive example and with reference to the
accompanying drawings, in which :
Fig. 1 is a diagrammatic view of the system to which the invention relates; and
Fig. 2 shows a functional flow chart of the system of Fig. 1.
[0006] Fig. 1 partially illustrates an engine assembly denoted in its entirety by 1 and
comprising : an endothermic engine 2 having a block 3 and a multiplicity of cylinders
4, only one of which is partially illustrated;
an air intake manifold 5 provided with a throttle-valved body 6 for controlling the
amount of air conveyed towards the cylinders 4;
a sensor 7 capable of detecting the angular position of the throttle valve with which
the body 6 is provided;
a sensor 8 capable of detecting the temperature of the air taken in along the manifold
5;
a sensor 11 capable of detecting the flowrate of the air taken in along the manifold
5;
a sensor 12 capable of detecting the number of engine revolutions;
a fuel manifold 13;
a pipe 14 for conveying exhaust gases from the cylinders 4;
a lambda probe 15 capable of detecting the amount of oxygen present in the exhaust
gases; and
an electronic unit 16 to which the sensors 7, 8, 11 and 12 and the lambda probe 15
lead.
[0007] The unit 16 is provided with an electronic injection system 19 capable of controlling
electronic injectors 17, only one of which is shown, which from the manifold 13 inject
fuel into the final section of the manifold 5 where the air/fuel mixture is produced.
Via an intake valve 18 this final section of the manifold 5 opens into the combustion
chamber 21 defined in the cylinder 4. The unit 16 is also provided with an electronic
ignition system 20 capable of controlling the sparking of the arc between the plug
electrodes 22, electrodes located inside the combustion chamber 21 between the valve
18 and an exhaust valve 23 from which the exhaust gases are introduced into the pipe
14.
[0008] With reference to Fig. 1, in its entirety 31 denotes a system which permits the reduction
of the detonation phenomena which may occur in the chamber 21 as a result of anomalous
combustion. As will be seen more clearly below, the system 31 prevents the recurrence
of the conditions which trigger the detonation phenomenon; conditions which chiefly
consist of the elevated temperature at particular points of the chamber 21 and of
the high internal pressure. To prevent the succession of detonation phenomena, once
the presence of detonation phenomena has been ascertained the system 31 controls the
introduction into the manifold 5 of an amount of exhaust gas taken from the pipe 14.
As a result the combustion chamber 21 will be supplied with an amount of air/fuel
mixture and an amount of exhaust gas which is, as we will recall, an inert gas which
takes no part in the combustion process taking place in the chamber 21. The exhaust
gases introduced into the chamber 21 reduce the pressure values inside the chamber
21 and remove energy derived from the combustion insofar as these exhaust gases perform
the function of a "thermal sponge" which absorbs some of the calories derived from
the combustion. This function of the exhaust gases determines the reduction of the
maximum peak of the combustion temperature and hence discourages the creation of particularly
hot spots inside the chamber 21. In short, the presence in the chamber 21 of exhaust
gases prevents the recurrence of the conditions which trigger the detonation phenomenon;
conditions which, we will recall, chiefly consist of the high temperature at particular
spots in the chamber 21 and of the high internal pressure.
[0009] The system 31 comprises :
a pipe 32 which originates from the pipe 14 and which opens into the manifold 5 downstream
of the throttle-valved body 6;
a solenoid valve 33 installed along the pipe 32; a sensor 34 capable of detecting
the detonation; and
an electronic device 35 to which the sensor 34 leads and which is capable of controlling
the solenoid valve 33.
[0010] The device 35 may form part of the unit 16 or it may be a separate device which nonetheless
"talks" to the unit 16. In a preferred embodiment shown in Fig. 1, the sensor 34 is
fitted to a wall of the cylinder 4 and is constituted by an accelerometer capable
of detecting the vibrations to which this wall of the cylinder 4 is subjected in the
course of the operation of the engine 2. The intensity of the vibrations to which
the cylinder 4 is subjected is regarded as an indicator of the detonation phenomenon
insofar as experimental trials have shown that in the presence of detonations, peak
values of the intensity of the vibrations are detected at certain frequencies.
[0011] The device 35 manages the functioning of the system 31 according to a functional
flow illustrated in Fig. 2 and comprising a starting block 51 from which one passes
to a block 52 in which the signals received from the sensor 34 are filtered. This
filtering consists of eliminating the signals corresponding to the vibrations which
are regarded as typical of a correct operation of the engine 2 and therefore a correct
combustion of the air/fuel mixture. Essentially the signals which are outside a frequency
band of predetermined width are eliminated and the only signals considered valid are
the +Vfilt and -Vfilt signals which occur inside that band on the positive and negative
side. From the block 52 we reach a block 53 in which the absolute value IVfiltl of
the + Vfilt and -Vfilt signals considered valid in the block 52 is calculated. From
block 53 we pass to a block 54 in which the integral of the absolute values processed
in the block 53 is calculated between two angular positions of the drive shaft using
the equation JIVfiltlda, where a is the engine angle. Preferably the integral is calculated
for a 90
° rotation of the drive shaft from a pre-determined point such as the top dead centre
for example. From the block 54 we reach a block 55 in which the value produced by
the integration calculated in the block 54 is converted into a digital value Vdet.
[0012] From the block 55 we pass to a block 56 in which the value Vdet and a threshold value
Vsol are compared. If the engine 2 is operating for the first time a pre-determined
magnitude set on the basis of laboratory experiments is allocated to the value Vsol.
If the value Vdet is greater than the value Vsol it is assumed that there is a detonation
phenomenon, for which reason we pass from the block 56 to a block 57, whereas if the
value Vdet is not greater than the value Vsol it is assumed that there is no detonation
phenomenon, for which reason we pass from the block 56 to a block 58.
[0013] In the block 58 an assessment is made as to whether the engine 2 is in the first
operating cycle and thus whether a value Vmed is stored in a memory block of the device
35 which is not illustrated. If the engine 2 is in the first operating cycle we pass
from the block 58 to a block 61 whereas otherwise we reach a block 62 from the block
58. Vmed = T is fixed in the block 61, where T is a pre- determined magnitude set
on the basis of laboratory experiments. From the block 61 we pass to the block 62
in which a new value Vmed is calculated, which we can call Vmedn using the equation
Vmedn = Vmed + KxVdet/Vmed where Vmed relates to the preceding cycle and K is a pre-
determined constant. In the case of first operation, of course, the value set in the
block 61 is taken as the value Vmed. Still in the block 62 but following the calculation
of Vmedn, Vmed = Vmedn is assumed in order to use the new value Vmed in the next operating
cycle.
[0014] From the block 62 we pass to the block 63 in which the value Ks is calculated on
the basis of an equation which takes account of the number of engine revolutions and
the engine load and essentially the engine conditions. These data are taken from the
unit 16 which, as is known, carries out a whole series of processing operations of
the findings of the above-mentioned sensors and is capable of supplying all the data
available in it on request. From the block 63 we reach a block 64 in which a new threshold
value Vsol is calculated using the equation Vsol = VmedxKs. From the block 64 we pass
to a block 65 in which the value Vsol calculated in the block 63 is stored and this
value Vsol replaces the previous threshold value in the block 56.
[0015] From the block 65 we pass to a block 66 in which a check is made as to whether there
is a correction phase of the fluid conveyed towards the chamber 21 and thus whether
a pre-determined amount of exhaust gas is currently being conveyed into the chamber
21, through the pipe 32 and the manifold 5, in addition to the air/fuel mixture. Essentially,
in the block 66 a check is made as to whether the solenoid valve 33 is in the opening
phase. If there is a correction phase we pass from the block 66 to a block 67 whereas
if there is not, we return to the block 52 from the block 66.
[0016] According to the equation Corn = Cor - Kzn%, in the block 67 a calculation is made
of the amount of exhaust gas to be introduced into the chamber 21. The value Cor relates
to the amount of exhaust gas currently being introduced into the chamber 21 whereas
the value Kzn% is a percentage value, deduced on the basis of laboratory experiments,
which is subtracted from the value Cor so as to define a new value Cor denoted by
Corn and relating to a lower amount of exhaust gas than the amount of exhaust gas
currently being introduced into the chamber 21 and calculated in a preceding cycle
of the operational flow. Essentially, once it has been ascertained in the block 56
that there is no detonation phenomenon and ascertained in the block 66 that a correction
phase still exists, the amount of exhaust gas to be introduced into the chamber 21
will reduce, cycle by cycle and gradually (-Kzn%). From the block 67 we pass to a
block 68 in which the value Corn just calculated is assumed and stored as the new
value Vcor so that in the next cycle the value Kzn% is subtracted from the new value
Vcor.
[0017] From the block 68 we then reach a block 71 in which the new value Vcor is compared
with zero. If the new value Vcor is not greater than zero we pass from the block 71
to a block 72 whereas otherwise we move to a block 73 from the block 71. Essentially,
in the block 71 a check is made as to whether, following a series of cycles in each
of which the amount of exhaust gas introduced into the chamber 21 has gradually decreased
because of the persistent absence of detonation phenomena, a new value Vcor equal
to zero or negative has been calculated, a new value Vcor corresponding to the closure
position of the solenoid valve 33. In the block 72 the value Vcor = 0 is fixed insofar
as the correction phase has been concluded. From the block 72 we now pass to the block
73 in which the control of the solenoid valve 33 is actuated to determine the passage
of exhaust gas according to an amount corresponding to the new value Vcor set in the
block 67, in the block 72 or in other blocks which will be described below. Finally,
from the block 73 we pass to the block 52.
[0018] As already indicated, from the block 56 we pass to the block 57 if detonation phenomena
are present or persist. The amount of exhaust gas to be introduced into the chamber
21 is calculated in the block 57 according to the equation Corn = Cor + Kz%. The value
Cor relates to the amount of exhaust gas currently being introduced into the chamber
21 whereas the value Kz% is a percentage value, deduced on the basis of laboratory
experiments, which is added to the value Cor in order to define a new value Cor indicated
as Corn and relating to a larger amount of exhaust gas than the amount of exhaust
gas currently being introduced into the chamber 21 and calculated in a preceding cycle
of the operational flow. Essentially, once it has been ascertained in the block 56
that there is a succession of the detonation phenomenon, the amount of exhaust gas
to be introduced into the chamber 21 will increase, cycle by cycle, and gradually
(+Kz%). Following the calculation of the value Vcorn, still in the block 57 the value
Vcorn just calculated is assumed and stored as a new value Vcor so that the value
Kz% is added to the new value Vcor in the next cycle.
[0019] From the block 57 we pass to a block 74 in which the new value Vcor is compared with
a pre- determined and stored value Vcormax relating to a maximum value of the amount
of exhaust gas that it is possible to introduce into the chamber 21. This maximum
value may depend, for example, on the maximum quantity that it is possible to convey
along the pipe 32 when the solenoid valve 33 is in the position of maximum opening.
If the new value Vcor is not less than the value Vcormax we pass from the block 74
to a block 75 and from there to the block 73, whereas otherwise we move directly to
the block 73 from the block 74. Essentially in the block 74 a check is made as to
whether, following a series of cycles in each of which the amount of exhaust gas introduced
into the chamber 21 has increased gradually because of the persistent presence of
detonation phenomena, a new value Vcor has been calculated which is not less than
the value Vcormax corresponding to the maximum amount of exhaust gases which it is
possible to introduce into the chamber 21. In the block 75 the value Vcor=Vcormax
is fixed insofar as beyond this limit it is not possible to increase the amount of
the exhaust gases which it is possible to introduce into the chamber 21.
[0020] The advantages achieved with the implementation of the invention will be evident
from the above description.
[0021] In particular a system has been produced which, in the event of detonation phenomena
being ascertained, introduces exhaust gases into the combustion chamber according
to a pre-determined law and which then, in the event of a persistent absence of detonation
phenomena being ascertained, reduces the amount of exhaust gases to be introduced
into the combustion chamber according to a pre-determined law. As will be apparent
the reduction of the possibility of the recurrence of the conditions which trigger
the detonation phenomenon relieves the material of which the combustion chamber is
made and the components installed inside it of excessive thermal and metallurgical
fatigue. Finally the structural simplicity of the system according to the invention
should be stressed; a structural simplicity which promotes a reduced production cost.
[0022] Finally it will be evident that modifications and variants may be made to the system
31 described and illustrated without departing from the scope of the invention.
[0023] In particular, the law which determines the amount and/or the variation in that amount
of exhaust gases to be introduced into the air intake manifold may be different from
that described with reference to Fig. 2. For example, the first occasion that a detonation
is detected, independently of the possible succession of detonations, an amount of
exhaust gas to be introduced for a pre-determined time or an amount of exhaust gas
which decreases in a pre-determined time according to a pre-determined method may
be pre-determined. The amount of exhaust gas may be equal for all the cylinders in
the engine or an amount of gas which is different for each cylinder may be introduced;
in this case a respective detonation detection sensor may be applied to each cylinder.
The duration of the correction phase may be correlated to the persistence of the detonation
and/or the engine conditions of the engine assembly such as number of engine revolutions,
engine load, temperature of air taken in, etc. It is then possible to provide the
engine assembly with an element by means of which the user can control the correction
and with a device capable of recording a series of engine parameters recorded before,
during and after the correction phase so that these parameters can be processed to
produce a diagnosis of the engine assembly.
[0024] In place of the solenoid valve 33 a different fluid interception device may be used
such as, for example, an on/off choking device or a choking device with proportional
control. Furthermore, in place of the solenoid valve 33, a battery of interception
devices, each strictly dedicated to a corresponding cylinder, may be installed. Finally
an interception device with pneumatic, mechanical, magnetic or optical control may
be installed in place of the solenoid valve 33.
[0025] The means of detecting the detonation may comprise a single sensor 34 installed in
correspondence with a cylinder or on the engine block, or they may comprise a multiplicity
of sensors 34 each installed in correspondence with a respective cylinder. The detection
means may comprise one or more sensors of a type different from that described. For
example, the sensor 34 may comprise a pressure sensor installed in one or in several
combustion chambers, an acoustic sensor which detects the acoustic waves generated
by the engine assembly, an element which analyzes the composition of the combustion
products, an element which analyzes the thermal and/or kinematic state of the combustion
products, or elements such as load cells installed on components of the engine assembly
which record the vibrations of the engine structure.
1. System for reducing detonation phenomena in a combustion chamber (21) of an endothermic
engine (2) of an engine assembly (1) which comprises an air intake manifold (5), a
multiplicity of cylinders (4), a first pipe (14) for conveying exhaust gases from
the said cylinders (4), a system for electronic ignition (20) and a system for electronic
injection (19), characterized in that it comprises :
means (34) for detecting the detonation phenomenon;
means (32 and 33) for conveying exhaust gases from the said first pipe (14) to the
said combustion chamber (21); and
means (35) connected to the said means for detecting (34) and controlling the said
means for conveying (32 and 33) exhaust gases to determine the inflow of exhaust gases
in the said combustion chamber (21) in order to reduce the possibility of a recurrence
of the conditions which trigger the detonation phenomenon.
2. System according to Claim 1, characterized in that the said detection means comprise
at least one sensor (34) for detecting the vibrations to which a said cylinder (4)
is subjected.
3. System according to Claim 1, characterized in that the said detection means comprise
at least one sensor (34) for detecting the vibrations to which a structure of the
said engine (2) such as the engine block (3) is subjected.
4. System according to Claim 1, characterized in that the said detection means comprise
at least one sensor for detecting the pressure inside the said combustion chamber
(21).
5. System according to Claim 1, characterized in that the said detection means comprise
at least one acoustic sensor for detecting the acoustic waves generated by the said
engine assembly (2).
6. System according to Claim 1, characterized in that the said detection means comprise
at least one element which analyzes the composition of the combustion products.
7. System according to Claim 1, characterized in that the said detection means comprise
at least one element which analyzes the thermal and/or kinematic state of the combustion
products.
8. System according to any one of the preceding Claims, characterized in that the
said means (32 and 33) for conveying exhaust gas from the said first pipe (14) to
the said combustion chamber (21) comprise a second pipe (32) which originates from
the said first pipe (14) and which opens into the said manifold (5) and a flow interception
device (33) installed along the said second pipe (32) and controlled by said control
means (35).
9. System according to Claim 8, characterized in that the said interception device
comprises a solenoid valve (33).
10. System according to Claim 8, characterized in that the said interception device
comprises an on/off choking device.
11. System according to Claim 8, characterized in that the said interception device
comprises a choking device with proportional control.
12. System according to Claim 8, characterized in that the said interception device
comprises a choking device with pneumatic control.
13. System according to Claim 8, characterized in that the said interception device
comprises a choking device with mechanical control.
14. System according to Claim 8, characterized in that the said interception device
comprises a choking device with magnetic control.
15. System according to Claim 8, characterized in that the said interception device
comprises a choking device with optical control.
16. System according to any one of the preceding Claims, characterized in that the
said control means (35) comprise :
means for recognizing signals generated by the said detection means and relating to
the detonations;
means for processing the signals relating to the detonation;
means which on the basis of the result of the processing of the signals relating to
the detonations calculate the amount of exhaust gas to be introduced into the said
combustion chamber (21);
means for managing the said conveying means (32 and 33) to allow the passage of the
calculated amount of exhaust gas.
17. System according to Claim 16, characterized in that the said control means (35)
comprise means for comparing the result of the processing of the signals relating
to the detonations with a pre-determined threshold value above which the passage of
the calculated amount of exhaust gas towards the said pipework is controlled.
18. System according to Claims 16 and 17, characterized in that the said control means
(35) comprise means which, in the absence of a succession of detonations, control
the gradual reduction of the amount of exhaust gases to be introduced into the said
chamber (21) up to the closure of the passage of such gases along the said conveying
means (32 and 33).
19. System according to Claims 16 to 18, characterized in that the said control means
(35) comprise means which, in the event of a succession of detonations, control the
gradual increase in the amount of exhaust gases to be introduced into the said chamber
(21) up to a maximum quantity.