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| United States Patent | 4885658 |
| Link to this page | http://www.wikipatents.com/4885658.html |
| Inventor(s) | Buchl; Josef (Lenting, DE) |
| Abstract | The invention relates to solid-state circuitry, including a freewheeling
circuit, for controlling the operation of an electromagnetically actuated
fuel intake or exhaust valve of an internal combustion engine by
alternatingly energizing, by way of a current switching element, the coil
of the electromagnet at a high level of current for attracting the
armature of the electromagnet into engagement with the stator, thus
driving the valve into its open or closed position, and maintaining, by
way of a transistor, lower level current pulses in the coil sufficient to
maintain the engagement. |
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Title Information  |
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Drawing from US Patent 4885658 |
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Apparatus for controlling the operation of an electromagnetic fuel
intake or exhaust valve of an internal combustion engine |
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| Publication Date |
December 5, 1989 |
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| Filing Date |
November 23, 1987 |
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| Parent Case |
REFERENCE TO RELATED APPLICATION
This application is a continuation-in-part of application Ser. No.:
855,896, filed Apr. 24, 1986 (now U.S. Pat. No. 4,706,619), and discloses
subject matter generally related to that of U.S. Pat. No. 4,544,986 issued
Oct. 1, 1985, U.S. Application Ser. Nos.: 856,032 filed Apr. 25, 1986,
937,406 filed Dec. 3, 1986, and 937,408 filed Dec. 3, 1986. |
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| Priority Data |
Apr 25, 1985[DE]3515041 |
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Title Information  |
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Description  |
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BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates generally to controls for electromagnetically
actuated valves. More particularly, the invention relates to electric
circuitry, including a novel switching arrangement, for controlling the
operation of an electromagnetically actuated fuel intake or exhaust valve
of an internal combustion engine by energizing a coil of an electromagnet
at a high level of current for attracting an armature of the electromagnet
into engagement with a stator and thus drive the valve into one of its
terminal, i.e. open or closed positions and by thereafter feeding current
pulses reduced to a level sufficient to maintain the engagement for a
predetermined time.
2. Statement of the Prior Art
The use of electromagnetically actuated fuel intake or exhaust valves in
lieu of conventional cam-operated valves for controlling the fuel intake
or exhaust emission cycles of internal combustion engines is known. For
instance, west German Patent Specification DE-A 30 24 109 discloses an
engine in which fuel intake and exhaust valves actuated by electromagnets
are normally spring biased into a position intermediate their open and
closed positions. The valves may be driven to either of their terminal,
i.e. open or closed, positions by energizing coils of the electromagnets
with electric current of a level sufficient to pull an armature of the
electromagnets into engagement with a stator. Subsequently de-energizing
the coils causes the armatures to disengage from the stators and the
valves to move to their intermediate positions under the bias of their
springs. Actually, the bias of the springs causes the valves to overshoot
their intermediate positions and to propel them into the vicinity of the
other of their terminal positions into which they may then be drawn by
appropriate energization of electromagnetic coils.
Such arrangements, while functioning satisfactorily, suffer from a very
high consumption of electrical energy.
OBJECTS AND SUMMARY OF THE INVENTION
It is an object of the invention to provided apparatus of the kind referred
to which functions at significantly reduced energy consumption.
Another object of the invention resides in providing novel circuitry for
operating electromagnetic fuel intake and exhaust valves of internal
combustion engines in an energy efficient manner.
It is also an object of the invention to provide control circuitry capable
of reducing the high current level required for attracting an armature
into engagement with a stator to a lower level sufficient to maintain the
engagement for a predetermined time.
A further object of the invention is to provide circuitry, including a
freewheeling circuit, for energizing an electromagnet at a high current
level to pull its armature into engagement with its stator and for
thereafter maintaining current pulses reduced to a level sufficient to
keep the armature in engagement with the stator.
Yet another object of the invention is to provide novel circuitry for
controlling the operation of electromagnetically actuated fuel intake and
exhaust valves, including solid state switching elements for providing an
initially high level energizing current followed by a reduced level
holding current.
It is also an object of the invention to provide control circuitry of the
kind referred to in which at least one of the switching elements is a low
cost transistor and another switching element is a thyristor.
Another object of the invention resides in the use of a transistor in a
circuit of the kind referred to for switching off a thyristor by
momentarily absorbing a current load in excess of its normal capacity.
It is also an object of the invention to provide means for simulating
current decay in the coil of the electromagnet when the thyristor and
transistor are in their non-conductive states.
Still another object resides in the provision of means responsive to a
signal corresponding to the level of current flowing in the electromagnet
and having an output connected to the transistor.
In the accomplishment of these and other objects the invention, in a
preferred embodiment thereof, provides for an energization circuit,
including a freewheeling circuit and current switching means by means of
which an electromagnet for driving a fuel intake or exhaust valve of an
internal combustion engine may initially be energized with a high level
current to pull its armature into engagement with a stator, and a
transistor for switching off the current switching means by briefly
absorbing its current and thereafter feeding to the electromagnet current
pulses reduced to a level sufficient to maintain the engagement between
the armature and the stator.
Preferably, the switching means comprises a thyristor for supplying high
level energization current to the electromagnet and, connected in parallel
therewith, a transistor for selectively rendering the thyristor
non-conductive and maintaining reduced level current pulses in the free
wheeling circuit and the coil of the electromagnet.
In a preferred embodiment of the invention means are provided for
maintaining the resistance of the transistor in its conductive state lower
than the resistance of the thyristor in its conductive state.
Preferably, means for raising the resistance of the thyristor may be series
connected with its anode and cathode path.
The means for increasing the resistance of the thyristor may comprise an
ohmic resistor, a diode, or a positive temperature coefficient (PTC)
element.
Also, means are provided for simulating current decay in the coil of the
electromagnet for selectively rendering the current switching element and
the transistor conductive.
The principle of energizing an electromagnetic load by means of a
freewheeling circuit is known from west German Patent Specification DE-A
28 28 678. Typically, the current required for maintaining the engagement
between an armature and a stator is less than 20% of the current required
for pulling the armature into engagement with the stator.
For rapidly switching on the current and for thereafter generating current
pulses a switching element is needed which is capable of absorbing or
withstanding the highest operational currents. For this reason DE-A 28 28
678 proposes the use of a transistor designed to withstand such high
current levels. The cost of such a transistor is, of course,
correspondingly high.
Obviously, it would be desirable to manufacture a low cost circuit of the
kind known from the west German specification.
In accordance with the invention the coil of an electromagnet is initially
energized with high level current by way of a current switching element,
and thereafter a transistor provides lower level current pulses. The
current switch used for applying energization current once in every
operational cycle may, for instance, be a relay which while capable of
withstanding the high current levels would be cheaper than a transistor
suited for handling similarly high level currents.
Reduced level current pulses are subsequently provided by a transistor, and
since the current required in the freewheeling circuit to maintain the
armature in engagement with the stator, may be noticeably lower than the
energization current required to bring about this engagement, the
transistor may be much smaller and, hence, less expensive, than would
otherwise be possible.
Preferably, the current switching element is a semiconductor element such
as a thyristor. The use of a thyristor may pose problems for while a
thyristor may be rendered conductive by an external signal it can be
switched off only by briefly interrupting the current flowing through it.
It has been found that this current may be briefly fed through the
transistor. Preferably, the transistor is connected in parallel to the
thyristor. In such an arrangement, means may be necessary for ensuring
that the resistance of the thyristor path when in its conductive state is
in excess of the resistance of the transistor path when it is conducting
so that current may briefly be diverted from the thyristor to the
transistor to turn off the thyristor.
To provide for such higher resistance, a resistance such as a diode, an
ohmic resistor or a positive temperature coefficient (PTC) element may be
provided in the conductive path of the thyristor.
In this respect the invention is based upon the recognition that a
transistor can, without being damaged, absorb or withstand current of a
level significantly higher than the level under which it may operate
continuously without being damaged as long as it is subjected to it only
momentarily. Thus, current for energizing the electromagnetic load is
provided by way of a thyristor; however, to turn off the thyristor its
entire current is diverted to the transistor for several milliseconds.
Subsequently current pulses of a level about 10-20% as high as the
energizing current may be provided solely by the transistor. Therefore,
the transistor may be dimensioned correspondingly smaller than would
otherwise be possible.
While, as mentioned, means may be provided in the conductive path of the
thyristor for raising its resistance, this may not be absolutely necessary
as in normal circumstances the saturation voltage of the transistor in its
collector-emitter path is lower than in the thyristor. Nevertheless, where
an ohmic resistance is provided its resistance value may be less than one
ohm.
Instead of an ohmic resistance in the conductive path of the thyristor a
diode, for instance a silicon diode may be utilized which at a voltage
drop of about 0.7 volt would insure that the thyristor is turned off as
soon as the transistor is conducting.
In accordance with another advantageous embodiment of the invention a
positive temperature coefficient (PTC) element may be series connected
with the thyristor for influencing the flow of current therethrough. In
its cold state such a PTC element would initially provide for a high level
current to flow through the thyristor after it has been turned on. As
current flows through the PTC element, its resistance increases and,
following the brief period of high level energizing current flow through
the thyristor, the current will be reduced as a result of the steadily
increasing resistance of the PTC element. At the end of the energizing
current phase the level of current will already have decreased so that the
transistor, at the time it is turned on, need no longer divert the maximum
energization current from the thyristor but, rather, current of a markedly
lower level.
BRIEF DESCRIPTION OF THE DRAWINGS
Several preferred embodiments of the invention are illustrated in the
drawings and will be described in greater detail in the following
description with reference to the drawings, in which
FIG. 1 is a schematic diagram of a first embodiment of a circuit in
accordance with the invention for controlling the operation of an
electromagnetic fuel intake or exhaust valve of an internal combustion
engine;
FIG. 2 is a schematic diagram of an alternate embodiment of a circuit in
accordance with the invention;
FIG. 3 is a diagram of current flow in the circuit of FIG. 1;
FIG. 4 is a diagram of current flow in the circuit of FIG. 2;
FIG. 5 is a schematic diagram of a circuit in accordance with the
invention, including a switch control unit;
FIG. 6 is a schematic diagram of a circuit for the control unit shown in
FIG. 5; and
FIG. 7 is a diagram depicting the sequence in which the switches of the
circuits in accordance with the invention may be actuated.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
FIG. 1 depicts a circuit which at its terminal 10 is connected to a
positive voltage source. At another terminal 12 the circuit is grounded.
An electromagnetic load 14, depicted as a coil of an electromagnet (not
shown) of the kind useful for driving fuel intake or exhaust valves
(schematically shown at 14a in FIG. 5) of internal combustion engines
(also not shown) between their open and closed positions, is connected
between the positive and negative terminals 10 and 12. Hereinafter those
valves may be collectively referred to as gas exchange valves. A
freewheeling circuit, shown as a diode 16, is connected in parallel to the
electromagnetic load 14. The freewheeling circuit 16 serves to maintain a
freewheeling current flow in the coil 14 when current flow from the
positive terminal 10 through the coil 14 to ground 12 has been turned off.
The freewheeling current decays in time at a predetermined rate.
The coil 14 is connected to ground 12 by way of two parallel circuit
branches 28 and 40 which are joined at junctions 42 and 44 to the coil 14
and ground 12, respectively. A current switching element 34 depicted as a
thyristor is provided in branch 40. The anode of the thyristor 34 is
connected to the coil 14 while the cathode is connected to ground 12. The
gate 36 of the thyristor 34 is connected to a terminal 38 for receiving
pulses or signals in a manner to be described. While a thyristor is the
currently preferred switching element, it will be appreciated by those
skilled in the art that a relay may be substituted for it.
Circuit branch 28 includes a transistor 18 the collector 20 and emitter 22
of which at times provide a connection between the coil 14 and ground 12.
The base 24 of the transistor 18 is connected to an external control to be
described by way of a terminal 26.
The circuit of FIG. 2 is in many respects similar to that of FIG. 1. To the
extent possible its elements have, therefore, been depicted with identical
but primed reference characters. The circuit differs from that of FIG. 1
in a resistance 46 connected in series with the thyristor 34'. The
resistance 46 may be an ohmic resistor, a diode, or a positive temperature
coefficient (PTC) element. It will be appreciated that other elements may
be used instead, provided they yield the desired effects to be described.
The function of the circuits in accordance with the invention will now be
described with reference to the current flow diagrams of FIGS. 3 and 4. It
should be noted, however, that where the resistance 46 in the circuit of
FIG. 2 is a PTC element, a somewhat different function described in
connection with FIG. 4 results.
In FIG. 3 curve a depicts current at terminal 38 (38'), curve b depicts
current at terminal 26 (26'), and curve c depicts current flowing in the
coil 14 (14'). That is to say, curves a and b represent current pulses
applied to gate 36 (36') of the thyristor 34 (34') and base 24 (24') of
the transistor 18 (18'), respectively. Curve c is, therefore, a
representation of the influence those current pulse exert upon the flow of
current in the coil 14 (14').
For purposes of explaining the function of the circuits it is assumed that
the voltage applied at terminal 10 (10') is positive and that both
semi-conductor switches, i.e. the thyristor 34 (34') and the transistor 18
(18") are initially in their non-conductive states.
Assuming a pulse as depicted in curve a in FIG. 3 is applied at terminal
38' (38") of the thyristor 34' (34"), the thyristor will commence
conducting, and current will, therefore, flow in the coil 14 (14').
Depending upon the inductance of the coil 14 (14') and the applied
voltage, the current rises more or less rapidly, and it would approach a
saturation current in an asymptotic fashion. The rise of the current is
depicted by curve c of FIG. 3. However, upon reaching a predetermined
maximum level I.sub.max the energizing current required for pulling the
armature of the electromagnet into engagement with its stator has been
reached; thereafter the current is to be reduced to a lower level
I.sub.halt sufficient to maintain the engagement.
To accomplish this the thyristor 34 (34') has to be turned off. However,
this cannot be accomplished by means of its gate 36. Instead, all current
must be diverted from the thyristor 34 (34'), a function which in
accordance with the invention is assumed by the transistor 18 (18'). A
brief pulse is applied to the base 24 (24') of the transistor 18 (18') by
way of its terminal 26 (26') to switch the transistor 18 (18') from its
non-conductive state to saturation, so that the current from the thyristor
34 (34') may briefly flow through the transistor. Since the saturation
voltage of the collector-emitter path of the transistor 18 (18') is lower
than that of the thyristor 34 (34') the current, during the brief period
of turning on the transistor 18 (18'), does indeed flow through branch
circuit 28, and the thyristor 34 (34') is turned off. The same result
would be obtained if for the purpose of increasing its resistance the
thyristor circuit branch 40 (40') had resistance elements 46 connected to
it. As soon as the thyristor 34 is non-conducting the transistor 18 (18')
may also be switched off again, and current freewheeling in the coil 14
(14') will decay in accordance with the characteristics or parameters of
the circuit.
It is important to note that while for longer periods the transistor 18
(18') is capable of withstanding only currents which more or less
correspond to the holding current (considering also a safety margin), it
is not damaged by a current surge of short duration. Accordingly, the
transistor 18 (18') used in accordance with the principles of this
invention may be a relatively inexpensive one; that it to say, it may be a
transistor which normally would be structurally unsuitable for controlling
the entire energizing current.
Curve b of FIG. 3 depicts the energizing pulse at base 24 (24') of the
transistor 18 (18') at time t.sub.2 ; during the interval t.sub.2 to
t.sub.3 current flow through coil 14 (14') gradually decays to level
I.sub.halt. At time t.sub.3 the transistor 18 (18') passes a pulse lasting
until time t.sub.4, and at times t.sub.5 and t.sub.7 it may pass further
pulses lasting until times t.sub.6 and t.sub.8, respectively. The interval
between these pulses determines the upper and lower limits of the holding
current I.sub.halt.
Where the resistance 46 of the circuit of FIG. 2 is provided by a positive
temperature coefficient (PTC) element the resulting current flow is as
shown in FIG. 4. At time t.sub.1 a pulse as depicted by curve a of FIG. 4
is applied to the gate 36' of thyristor 34'. Thus, the thyristor is
rendered conductive and current builds up until time t.sub.2 as shown by
curve c of FIG. 4. At time t.sub.2 current begin to drop because of the
increasing resistance of the PTC element 46 as it heats up. The shape of
the energization current curve is thus not determined by the turning on of
the thyristor 34' and the subsequent firing of the transistor 18', but,
rather, by the turning on of the thyristor 34' and the influence the PTC
element 46 subsequently exerts on the current flow.
At time t.sub.3 current flowing through thyristor 34' is seen to have
dropped to a value substantially corresponding to the holding current
I.sub.halt. In order to maintain the holding current at its predetermined
level, a pulse as shown by curve b of FIG. 4 is applied to the base 24' of
transistor 18' at time t.sub.3 ; this pulse opens up the collector-emitter
path of the transistor 18' to provide for current to flow through the
electromagnetic load 14'. When transistor 18' conducts at time t.sub.3,
current flow through the thyristor 34' ceases. The thyristor 34' is thus
turned off. Pulses of holding current I.sub.halt may be applied to the
coil in the manner described above.
The circuit of FIG. 5 is substantially similar to that of FIG. 1 and
schematically depicts a control unit 52 into which data relating to the
current flowing between the terminals 10 and 12 and through the
electromagnetic load 14 is fed. The data is collected at a low value
resistor 50 (much less than 1 ohm) connected in a line leading from the
junction 44 to ground 12. The control unit 52 monitors any voltage drop
across the resistor 50, and may thus measure the current.
To render the thyristor 34 conductive the control unit 52 sends a pulse to
the gate 36 of the thyristor 34 by way of line 54 and contact 38. The
pulse which turns the thyristor on may, for instance, be generated on the
basis of engine parameters fed into the control unit 52 as indicated by
arrow EP. Once the thyristor 34 is conducting current flows and increases
to the level I.sub.max. When level I.sub.max is detected by the control
unit 52 the latter, by its other output 56, applies a short pulse to the
base 26 of the transistor 18. The transistor 18 is thus rendered
conductive and all the current from the thyristor 34 is dumped through it.
This turns off the thyristor 34, and substantially immediately thereafter
the transistor 18 is also turned off. The current in the coil 14 may now
decay by way of the freewheeling diode 16.
To maintain the holding current I.sub.halt between its upper and lower
limits depicted at times t.sub.3 and t.sub.4, respectively, the transistor
18 is periodically turned on and off by the control unit 52 in order to
provide current pulses. When the transistor 18 is conducting the level of
current flowing through the electromagnetic load 14 and the transistor is
rising; when the transistor 18 is turned off current gradually decays
depending upon the constant of the freewheeling circuit. As stated above,
the freewheeling circuit may in its simplest form consist of the
electromagnetic load 14 and the diode 16. The holding current I.sub.halt
will be established by the cycling of the transistor 18 as determined by
the control unit 52.
The transistor 18 (18') could, of course, be provided with a current
limiter so that during the current phase the transistor could be pulsed at
currents up to the I.sub.max level; however, because of such a current
limiter (not shown) current could not begin to flow until it has decayed
to the I.sub.halt level.
As stated above, current is freewheeling in the coil 14 and the diode 16
when both the thyristor 34 and the transistor 18 are in their
non-conductive states. Of course, this current cannot be detected by the
control unit 52 at the resistor 50.
As shown in FIG. 6, the control unit 52 may be provided with a current
decay simulator, such as an RC unit 58. The pulses applied at terminals 26
(26') and 38 (38') and required for periodically turning on the thyristor
34 and for cycling the transistor 18 on and off to provide pulses of
holding current I.sub.halt are generated by the decay simulator. After a
pulse has been applied to terminal 38 (38') current may thus increase to
level I.sub.max at which point it is turned off by the transistor 18 (18')
in the manner described. Since the rate of decay of the freewheeling
circuit is determinable on the basis of operating parameters, decay
simulation may be carried out with sufficient accuracy to ensure safe
operation of the circuit and its electromagnetic coil 14. Any error
occurring from the simulated pulses may in the event be compensated by the
ensuing current monitoring across the transistor 50.
When the simulation indicates that the freewheeling current has decayed, at
t.sub.3, to the lower limit of I.sub.halt current flow through the coil
14 from the positive terminal 10 to ground 12 may be resumed by triggering
transistor 18 into conduction by a pulse applied to its base 24 from the
control unit 52. The current will rise to the upper limit of I.sub.halt at
time t.sub.4. As has been stated above, at this point the transistor 18 is
turned off by the control unit 52 on the basis of the voltage monitored at
resistance 50, and it remains turned off until the simulated current again
reaches the lower limit of I.sub.halt at which time the transistor
repeates its cycle.
The function of the circuit depicted in FIG. 6 will only be described
briefly as this circuit forms no part of the present invention. Actual
current I.sub.ist as measured across the resistance 50 and, applied by way
of a diode 60, is compared at a comparator 58 with a desired current
I.sub.soll determined, for instance, by engine performance parameters as
schematically indicated by arrow EP in FIG. 5. Based on the result of the
comparison, a pulse is generated at the output of the comparator 58 which
is fed to the gate 36 of the thyrisrtor 34 by way of line 54 and terminal
38. Current level I.sub.ist may either be derived from measuring the
voltage across the resistor 50 or, when no current is flowing through the
resistor 50, from the RC unit 68. The RC circuit 68 includes a variable
resistor 62 and a capacitor 64 and simulates the decay of the freewheeling
current, i.e. the discharge rate of the capacitor 64 resembles the rate of
decay of the freewheeling current. Adjustments in the slope of the
discharge curve relative to the slope of the current decay curve may be
made by the variable resistor 62.
The output of the comparator 58 is also applied to a monoflop 66 for
feeding a pulse to the base 24 of the transistor 18 (18') when the
energizing current curve has reached I.sub.max to turn on the transistor
18 for taking over the entire current from the thyristor 34 for a period
sufficiently brief to prevent damage to the transistor 18 even though it
is overloaded, but long enough to turn off the thyristor 34 (34').
The resulting relationship between the pulses for turning on the thyristor
34 and the transistor 18 have been depicted in FIG. 7.
Thus, a novel contro has been devised for effectively curtailing the energy
requirements for actuating electromagnets for gas exchange valves of
internal combustion engines.
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Description  |
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