Internal-combustion engines – High tension ignition system – Having dwell control
Reexamination Certificate
2001-12-10
2003-06-03
Kwon, John (Department: 3747)
Internal-combustion engines
High tension ignition system
Having dwell control
C123S679000
Reexamination Certificate
active
06571783
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates to an ignition control device and a corresponding ignition control method.
Although usable on any ignition control, the present invention and the set of problems on which it is based is explained with reference to an engine control unit located on board a motor vehicle.
BACKGROUND INFORMATION
Ignition control devices for controlling ignition events for ignition coil ignition systems or devices have essentially two control functions: the control of a desired ignition energy throughout the energization period or charging time of the ignition coil and the correct angle control of an ignition pulse via the deenergization point or the end of charging time of the ignition coil.
The ignition energy that is supplied in coil ignition systems over the course of an ignition coil charging time is of varying duration corresponding to the vehicle electrical system voltage applied to the electrical circuit of the coil and the time constant of the electrical circuit.
Typically, the particular setpoint values are stored in the control unit as a function of the engine speed and other possible engine parameters as a field of characteristics.
The setpoint values of “charging time” and “ignition angle” create a conflict of goals when engine speed dynamics come into play. The angular position of the beginning of the charging phase, thus the start-of-dwell angle, must be selected such that the ignition angle is reached after the end of the charging time. That means that at the instant the ignition event is calculated, the timing-angle curve of the crankshaft movement must be known in advance.
Extreme engine speed dynamics and low engine speed sampling rate, especially during engine cranking, cause a non-negligible estimation error of this timing-angle curve in standard ignition control devices.
Standard control units are equipped with a phase-angle sensor wheel, which supplies angle-equidistant pulses to the ignition-control device, for the output of angle signals. For reasons of computing time, the calculation of the ignition events in most ignition control device architectures, however, can be achieved only in segments, a segment being the angular interval of 720° of the crankshaft divided by the number of cylinders, thus 180° for a four-cylinder engine. Therefore, although the angular positions of the ignition events determined in the calculation can be measured with sufficient accuracy by the phase-angle sensor wheel and the timer/counter circuits typical for ignition control systems, the calculation itself assumes a detected engine speed that no longer exists at the location of the ignition when there are engine speed dynamics.
To explain the problems,
FIG. 2
shows a schematic diagram of the firing sequence in a four-cylinder internal combustion engine.
In
FIG. 2
the crank angle KW is recorded in degrees on the x-axis and the ignition curve ZZ, which has the sequence . . . −2−1−3−4−2 . . . , is recorded on the y-axis. One complete cycle is 720° of crank angle KW, corresponding to one cycle time of t
ZYK
. One segment is 720° KW/4=180°, corresponding to one segment time of t
SEG
.
FIG. 3
shows a schematic diagram of the ignition control functional sequences in the segment of the first cylinder of a four-cylinder internal combustion engine with respect to the triggering of the ignition coil current I
Z
.
At 0°, the engine speed N is detected and immediately thereafter the charging time t
L
, and the ignition angle w
Z
(approximately equal to the end-of-dwell angle) are derived from a field of characteristics B.
Next, the start-of-dwell or start-of-charging angle w
LB
from the relation
W
LB
=W
Z
−t
L
·&ohgr;
is determined assuming a uniform movement, &ohgr; being the angular speed corresponding to the engine speed N. For reasons of computing time, this time and angle position of the ignition event is calculated only once per firing interval.
In the case of charging time output mode, the angle w
LB
is detected via the crankshaft sensor signal KWS using a counter C
1
starting from 0°, and upon reaching the angle w
LB
, the ignition coil driver stage is triggered. Then the charging time t
L
is controlled using a timer, and after expiration of the charging time t
L
, the drive signal is interrupted.
In the case of ignition angle output mode, the angle w
LB
is detected via the crankshaft sensor signal KWS using a counter C
1
starting from 0°, and upon reaching the angle w
LB
, the ignition coil driver stage is triggered. The angle w
Z
is detected via the crankshaft sensor signal KWS using a counter C
2
starting from 0°, and upon reaching the angle w
Z
, the drive signal is interrupted.
Since the error calculation of the engine speed curve is not negligible, e.g., in the case of engine cranking, the control targets of charging time and ignition angle are typically prioritized for ignition control devices. If the exact output of the charging time—so-called charging time output mode—via the timer/counter circuit is desired, then this causes a retarding of the ignition angle during starting acceleration (engine speed increase). If, on the other hand, the ignition angle is output exactly—so-called ignition angle output mode—then the charging time, and with it the energy in the ignition coil, is reduced in the starting dynamics. Consequently, this can cause misfires.
Typically, the output method, i.e. charging time output or ignition angle output, is therefore permanently set as a function of the characteristics of the target system, or else the output method is switched at a limit engine speed. Typical in this context is a charging time output during cranking and a switch to ignition angle output beginning at a limit engine speed at which the engine speed sampling is frequent enough that the dynamics error becomes negligible, and at which, on the other hand, the sensitivity of the torque also increases sharply via the ignition angle.
In charging time mode, as explained above in reference to
FIG. 3
, the charging time cycle runs through after reaching the start-of-charging angle and ignition is triggered in the coil when the setpoint energy is met exactly. In this way sufficient energy is guaranteed at a minimal power loss. At low engine speed and high acceleration, the ignition angle is retarded as a function of the dwell period and the position of the setpoint ignition angle. Therefore, in the application of the ignition angle, a dynamic phase lead is appropriately added in the advancing direction when the engine speed is on the order of magnitude of the starter speed.
In ignition angle output mode, as explained above with reference to
FIG. 3
, the ignition angle is sized independent of the start-of-charging angle. When an acceleration starts, ignition occurs before expiration of the charging time. In the application under these circumstances a dynamic phase lead is appropriately applied in the retarding direction precisely when there is high acceleration and low engine speed.
Larger dynamic phase leads than absolutely necessary are applied as a rule , and this results in power loss also in the ignition components in charging time output mode and the danger of reverse rotations in ignition angle output mode. The greatest deviation from the setpoint value always occurs during the second ignition firing. In this case the engine speed is still low and the acceleration is typically already very high.
The selection of the output mode is typically also a function of how large the errors, and thus the necessary phase leads on the energy or the ignition angle side, can become. However, with new ignition applications, the case can now arise, wherein when the engine is cold and the fuel mixture is lean, the ignition angle sensitivity increases; i.e., ignition angle output mode should be selected. However, since ignition driver stages of the newer generation are mounted directly on the cylinder head, the dissipation of power loss becomes problematic primarily when the engine is hot. This would neve
Denz Helmut
Haussmann Martin
Kenyon & Kenyon
Kwon John
Robert & Bosch GmbH
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