EP0880787A1 - Control device for an internal combustion engine - Google Patents
Control device for an internal combustion engineInfo
- Publication number
- EP0880787A1 EP0880787A1 EP96945993A EP96945993A EP0880787A1 EP 0880787 A1 EP0880787 A1 EP 0880787A1 EP 96945993 A EP96945993 A EP 96945993A EP 96945993 A EP96945993 A EP 96945993A EP 0880787 A1 EP0880787 A1 EP 0880787A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- coil
- current
- signal
- value
- control
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01H—ELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
- H01H47/00—Circuit arrangements not adapted to a particular application of the relay and designed to obtain desired operating characteristics or to provide energising current
- H01H47/22—Circuit arrangements not adapted to a particular application of the relay and designed to obtain desired operating characteristics or to provide energising current for supplying energising current for relay coil
- H01H47/32—Energising current supplied by semiconductor device
- H01H47/325—Energising current supplied by semiconductor device by switching regulator
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F01—MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
- F01L—CYCLICALLY OPERATING VALVES FOR MACHINES OR ENGINES
- F01L9/00—Valve-gear or valve arrangements actuated non-mechanically
- F01L9/20—Valve-gear or valve arrangements actuated non-mechanically by electric means
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F7/00—Magnets
- H01F7/06—Electromagnets; Actuators including electromagnets
- H01F7/08—Electromagnets; Actuators including electromagnets with armatures
- H01F7/18—Circuit arrangements for obtaining desired operating characteristics, e.g. for slow operation, for sequential energisation of windings, for high-speed energisation of windings
- H01F7/1844—Monitoring or fail-safe circuits
Definitions
- the invention relates to a control device for an internal combustion engine according to the preamble of claim 1.
- a control device (EP 04 00 389 A) comprises an actuator with a coil, a core and an armature, an actuator and a control unit.
- the coil In order to attract the armature to the core, the coil is acted upon by a pull-in current which has such a high amplitude that the magnetic flux provides the force required to accelerate and move the armature. If the armature lies against the core, the current through the coil is limited to a holding current, the amplitude of which is so low that at least one holding force required to hold the armature on the core is applied by the magnetic flux.
- the current through the coil is tracked by a two-point controller to the respective target value of the pull-in current or the holding current, the pulse / pause ratio of the actuating signal being dependent on the reaching of an upper and a lower threshold value of the current.
- the control unit detects the duration of the pulses of the control signal and uses it as an indirect measure of the inductance of the coil, which increases as the distance between the core and the armature decreases. Accordingly, the holding current is specified as the setpoint if the detected time period exceeds a limit value lies. It is very disadvantageous here that the time of impact of the anchor cannot be determined exactly. If the armature hits the core shortly before the current reaches its lower threshold value, the impact can only be detected after the following pulse of the control signal. Accordingly, there are high losses in the coil since the current is limited to the holding current too late. These can only be reduced if the starting current has a correspondingly low amount. However, this increases the time required for the armature to reach the core from a rest position to the stop. The actuator can therefore no longer be activated as quickly, which is particularly the case with injection or injection / Exhaust valves of an internal combustion engine is disadvantageous.
- the invention is based on the knowledge that the inductance of the coil changes during the movement of an armature and, however, remains constant from when the armature strikes a core until the armature is released. By detecting a change in the inductance, a precise time of impact of the armature on the core can thus be determined.
- the control device has a measuring device from which the inductance of the coil is detected and from which a first control signal is generated as a function of the inductance, by means of which the desired value is set to a holding value.
- the measuring device comprises one Signal generator that generates a test signal that is applied to the coil.
- the test signal advantageously has a low amplitude.
- a narrow-band test signal is also advantageous, the frequency of which is significantly higher than that of the current through the coil.
- the first control signal is preferably generated when the inductance changes by less than a lower threshold value in a predetermined time interval.
- the time interval can be chosen so small that the time of impact is determined with sufficient accuracy. It is extremely advantageous that the point of impact can be determined independently of the effects of temperature and aging.
- a second control signal is preferably generated if the inductance changes in the time interval by more than a predetermined upper threshold value. In this way, a time of detachment of the armature from the core can also be recorded precisely.
- Figure 1 a control device according to the invention
- Figure 2 the control device of Figure 1 with a
- FIG. 3 a block diagram of a measuring device from FIG. 2,
- Figure 4a-g waveforms in the control device according to
- Figure 1 Figure 1a: the course of a coil current plotted over the
- FIG. 4b the course of a control voltage plotted over time
- FIG. 4c the course of the amplitude of an output current plotted over time
- FIG. 4e the course of a first control signal plotted over time
- Figure 4f the course of a second control signal plotted over time
- Figure 4g the course of a pulse signal plotted over the
- a control device comprises an actuator 1, an actuator 2, a control unit 3 and a measuring device 4.
- the actuator 1 has a coil 10 which is wound around a core 11.
- a spring 12 is arranged on the core 11 in such a way that it prestresses an armature 13 against the direction of force of a magnetic force which acts when the coil 10 is energized.
- the actuator 2 has a spindle 21 and a cone 22. It is used in this design for an injection valve or an intake / exhaust valve of the engine.
- the special design of the actuator 2 is not essential to the invention. Accordingly, the actuator can also be designed such that it can be used, for example, for a common rail system or an exhaust gas recirculation system.
- the coil is connected to the control unit 3 as well as to the measuring device 4 via a first tap point 5 and a second tap point 6.
- the coil 10 can be represented as a series connection of a resistor 100 and an inductor 101 (FIG. 2).
- the structure of the control unit 3 is known per se and is not essential for the invention. Accordingly, it is not described further below. The operation of the control unit 3 is described with reference to Figures 4a, 4b.
- the measuring device 4 has a signal generator which is designed as an oscillator 40 and of which a test signal (in hereinafter referred to as test voltage) is generated.
- the oscillator 40 is connected to a first coupling device 41, which is connected to the coil 10 via the first tap point 5.
- the coupling device 41 is designed, for example, as a capacitor or as a bandpass filter, the bandwidth of which approximately corresponds to that of the test voltage.
- the coil 10 is thus subjected to the test voltage, which in this embodiment is a sinusoidal voltage with a significantly higher frequency than the highest occurring frequency in a control voltage with which the control unit 3 applies the coil 10.
- the test voltage which in this embodiment is a sinusoidal voltage with a significantly higher frequency than the highest occurring frequency in a control voltage with which the control unit 3 applies the coil 10.
- This ensures that an output current I A can be coupled out via a second coupling device 42, which in turn consists of a capacitor or a bandpass filter and which is connected to the coil 10 via the second tap point 6.
- the bandwidth of the bandpass filter is advantageously chosen so that it corresponds approximately to that of the test voltage.
- the amplitude of the test voltage is predetermined so that it is significantly smaller than that of the control voltage U s .
- a voltage meter 43 is arranged between the oscillator 40 and the first coupling device 41, from which the magnitude of the test voltage is detected and passed on to an evaluation device 44.
- a measuring device which is designed as an ammeter 45, is connected to the second coupling device 42 and detects the magnitude of the output current I A and forwards it as a measuring signal to the evaluation device 44.
- an inductance value L of the inductance 101 is determined by forming the ratio of the amount of the test voltage to the amount of the output current I A and taking into account the predetermined resistance 100. This process is carried out at predefined time intervals. If the inductance value L changes within a time interval by less than a predetermined lower one Threshold value, a first control signal S1 is generated. If, on the other hand, the inductance value L changes by more than a predetermined upper threshold value in a predetermined time interval, a second control signal S2 is generated. In the control unit 3, when the first control signal S1 is applied, a setpoint value for the coil current I s is reduced from a pull-in current 1 ⁇ to a holding current I H.
- FIG. 4a shows the course of the coil current I s plotted over time t.
- a pulse signal P (FIG. 4f) is generated at time t 0 .
- a control voltage U s is then applied by the control unit 3 and drops across the resistor 100 and the inductance 101.
- the amount of the control voltage U s corresponds to that of the pull-in voltage U A.
- the coil current I s increases approximately exponentially until the time t x , at which it reaches the value of a maximum starting current I AMAX .
- the magnitude of the control voltage U s is then reduced to a zero voltage U 0 (for example 0 volts).
- the coil current I s then drops approximately exponentially until it has the magnitude of the minimum pull-in current I ft m H at time t 2 .
- a control voltage U s with the amount of the starting voltage U A is applied to the coil 10 until the coil current I s again reaches the value of the maximum starting current I ⁇ M ⁇ X at time t 3 . This process continues until the first control signal S1 is generated at time t 4 .
- the course of the amplitude of the output current I A has a kink over time.
- a sudden flattening of the course of the inductance value to an approximately constant value at point t 4 can be seen in FIG. 4d.
- the inductance value L changed less than a lower threshold value in the time interval from time t 3A to time t 4A .
- the first control signal S x (see FIG. 4e) is generated at time t 4 .
- the time intervals between two determinations of the inductance value L can be chosen to be as small as desired if the lower and the upper threshold value are adapted accordingly. As a result, the time of impact and the time of release can be determined as precisely as desired.
- the coil current I s by suitable circuit means, such as. B. a free-wheeling diode, reduced as quickly as possible to a holding current I H.
- the coil current I s reaches the value of the minimum holding current I HMIN - the control voltage U s is then set to a holding voltage U H.
- the coil current I s then reaches the value of a maximum holding current I HMAX - thereupon the control voltage U s is reduced again to the zero voltage U 0 until the coil current I s reaches the value of the minimum holding current I HMIN . This process is repeated until the pulse signal P is withdrawn at time t 7 .
- the control voltage U s is then set to the zero voltage U 0 and the current through the coil is reduced to a zero current (for example 0 amperes) by suitable switching means (for example a freewheeling diode).
- FIG. 4d shows a sharp drop in the inductance value L at time t 8 . Accordingly, the second control signal S 2 (FIG. 4e) is generated at this time.
- test signal has a very high frequency, the influence of the resistor 101 can be neglected.
- temperature and age-dependent changes in the resistance 101 can be detected by means of suitable resistance measuring means.
- pulse signal P is not present, a voltage can be impressed on the coil 10 by means of these resistance measuring means the stationary current through the coil 10 can be detected. The ratio of these two quantities then forms the value of the resistor 100.
- the control device accordingly enables precise detection of the time of impact of the armature 13 on the core 11. This makes it possible to set the coil current I s in the vicinity of the saturation limit of the coil 10 up to the point of impact of the armature 13, so that the armature 13 is accelerated as much as possible.
- the losses in the control device are kept very low by rapidly reducing the coil current I s from a value between the maximum starting current I ⁇ and the minimum starting current I HN to the minimum holding current I HMIN .
- the measuring device 4 has a second ammeter which detects the magnitude of the coil current I s and forwards it to the evaluation device 44.
- the measuring device 4 then has a map memory in which base values for the
- Position of the armature 13 in dependence on the amount of the coil current I s and the inductance L are stored.
- the position of the armature 13 can thus be determined in this embodiment of the invention.
- the measuring device 4 has means for detecting the phase difference between the test signal and the output signal.
- the inductance value L of the inductance 101 is determined from the phase difference, taking into account the predetermined resistance 100.
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Power Engineering (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Electrical Control Of Air Or Fuel Supplied To Internal-Combustion Engine (AREA)
- Valve Device For Special Equipments (AREA)
- Measurement Of Resistance Or Impedance (AREA)
Abstract
Description
Claims
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE19605244 | 1996-02-13 | ||
DE19605244 | 1996-02-13 | ||
PCT/DE1996/002187 WO1997030462A1 (en) | 1996-02-13 | 1996-11-18 | Control device for an internal combustion engine |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0880787A1 true EP0880787A1 (en) | 1998-12-02 |
EP0880787B1 EP0880787B1 (en) | 2002-03-27 |
Family
ID=7785267
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP96945993A Expired - Lifetime EP0880787B1 (en) | 1996-02-13 | 1996-11-18 | Control device for an internal combustion engine |
Country Status (4)
Country | Link |
---|---|
US (1) | US6191929B1 (en) |
EP (1) | EP0880787B1 (en) |
DE (1) | DE59608979D1 (en) |
WO (1) | WO1997030462A1 (en) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6249418B1 (en) * | 1999-01-27 | 2001-06-19 | Gary Bergstrom | System for control of an electromagnetic actuator |
US6612322B2 (en) | 2000-08-09 | 2003-09-02 | Siemens Vdo Automotive Corporation | Method of detecting valve timing |
US6559654B2 (en) * | 2001-03-29 | 2003-05-06 | General Electric Company | Method and system for automatic determination of inductance |
DE102011076113B4 (en) * | 2011-05-19 | 2016-04-14 | Continental Automotive Gmbh | Determining the movement behavior of a fuel injector based on the time interval between the first two voltage pulses in a holding phase |
EP3125258B1 (en) * | 2015-07-31 | 2021-08-25 | Goodrich Actuation Systems Limited | Monitoring solenoid plunger position |
Family Cites Families (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2041659A (en) * | 1979-02-09 | 1980-09-10 | Lucas Industries Ltd | Sensing position of armature in an electromagnetic device |
DE3150814A1 (en) * | 1981-12-22 | 1983-06-30 | Herion-Werke Kg, 7012 Fellbach | Device for the contact-free determination of the switching position of the armature of an electromagnet |
JPS62225742A (en) | 1986-03-28 | 1987-10-03 | Hitachi Ltd | Engine controller |
US4970622A (en) * | 1986-12-03 | 1990-11-13 | Buechl Josef | Method and apparatus for controlling the operation of an electromagnet |
DE3741734C2 (en) * | 1987-12-09 | 1996-09-26 | Herion Werke Kg | Device for measuring the inductance of a coil, in particular for measuring the armature position of a coil / armature magnet system |
US5293551A (en) * | 1988-03-18 | 1994-03-08 | Otis Engineering Corporation | Monitor and control circuit for electric surface controlled subsurface valve system |
US4851959A (en) * | 1988-07-25 | 1989-07-25 | Eastman Kodak Company | Solenoid engagement sensing circuit |
US5053911A (en) | 1989-06-02 | 1991-10-01 | Motorola, Inc. | Solenoid closure detection |
US5172298A (en) * | 1990-01-09 | 1992-12-15 | Honda Giken Kogyo Kabushiki Kaisha | Electromagnetic actuator |
JP2800442B2 (en) | 1991-03-18 | 1998-09-21 | 国産電機株式会社 | Method and device for driving electromagnetic fuel injection valve |
US5196983A (en) * | 1991-10-07 | 1993-03-23 | Eastman Kodak Company | Solenoid engagement sensing circuit |
US5204633A (en) * | 1992-02-25 | 1993-04-20 | International Business Machines Corporation | Electromagnetic contactor with closure fault indicator |
US5347419A (en) | 1992-12-22 | 1994-09-13 | Eaton Corporation | Current limiting solenoid driver |
US5539608A (en) * | 1993-02-25 | 1996-07-23 | Eaton Corporation | Electronic interlock for electromagnetic contactor |
US5774323A (en) * | 1995-10-31 | 1998-06-30 | Eaton Corporation | Detection of contact position from coil current in electromagnetic switches having AC or DC operated coils |
US5668693A (en) * | 1996-06-25 | 1997-09-16 | Eaton Corporation | Method of monitoring a contactor |
-
1996
- 1996-11-18 WO PCT/DE1996/002187 patent/WO1997030462A1/en active IP Right Grant
- 1996-11-18 EP EP96945993A patent/EP0880787B1/en not_active Expired - Lifetime
- 1996-11-18 DE DE59608979T patent/DE59608979D1/en not_active Expired - Fee Related
-
1998
- 1998-08-13 US US09/133,705 patent/US6191929B1/en not_active Expired - Fee Related
Non-Patent Citations (1)
Title |
---|
See references of WO9730462A1 * |
Also Published As
Publication number | Publication date |
---|---|
US6191929B1 (en) | 2001-02-20 |
EP0880787B1 (en) | 2002-03-27 |
DE59608979D1 (en) | 2002-05-02 |
WO1997030462A1 (en) | 1997-08-21 |
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