Technology field
[0001] This invention relates to the technology of igniting fuel mixtures, more specifically
to processes for ion-plasma combustion (ignition), providing an increase in volume
in the initial combustion region (space ignition).
Prior art
[0002] There is a known process for the ignition of fuel-air mixture in an internal combustion
engine (USSR Authorship Certificate No. 1464274), consisting of the preliminary combustion
of a small quantity of fuel in a limited-volume cavity around the spark plug electrodes
and the subsequent ejection of a plasma-flame jet through a small aperture in the
plug into the combustion chamber.
[0003] This ignition process is energy-consuming. The design of the plug is complex and
fuel consumption is increased.
[0004] There is a known process for the ignition of fuel-air mixture in an internal combustion
engine, consisting of the action of an electric pulse on the fuel-air mixture in the
plug electrode zone to decrease electric strength, after which the amplitude of the
electric pulse is decreased and the mixture is ignited under the effect of the energy
produced by the pulse. Fig. 1 shows the dependence of voltage at the spark plug electrodes
obtained in implementing this process (Ross Tveg, Ignition systems for cars. - Moscow:
"Za rulyom" Publishing House, 1998, fig. 2, page 5).
[0005] The problem with this process is the relatively low volume of ignition of the mixture
and the presence of parasitic detonations, impairing the reliability of the ignition.
[0006] There is a known process for the ignition of fuel-air mixture in an internal combustion
engine (USSR Authorship Certificate No. 1368936), consisting of creating a current-conducting
medium containing charged particles between the spark plug electrodes, imparting directed
motion to the charged particles to create a spark discharge and then igniting the
fuel-air mixture. Space ignition in this process is created by increasing the number
of charged particles in the combustion chamber by using an electron source with auto-electronic
emission, containing a piezo-ceramic resonator and an Austin emitter.
[0007] This ignition process is ecologically cleaner, since the introduction of an additional
quantity of charged particles into the combustion chamber improves the ignition process
and the subsequent combustion of the mixture in the engine cylinder is more complete.
The presence of additional charged particles improves conditions for the combustion
of the mixture in the cylinder, which reduces the quantity of toxic substances and
decreases the amount of energy consumed by the process.
[0008] The problem with this process is the relatively low volume of initial combustion,
which increases toxicity and reduces ignition efficiency.
Substance of the invention
[0009] The main problem to be solved by this invention is the creation of a process and
system for the ignition of fuel-air mixture which provide improved economy and reduced
toxicity by a more uniform ignition process and more complete combustion of the fuel-air
mixture.
[0010] In accordance with this invention, the fuel-air mixture ignition process comprises
the following successively implemented stages:
(a) increasing the intensity of the electrical field in the spark plug electrode gap
until an electric spark passes across it;
(b) decreasing the intensity of the electrical field in steps to a set level;
(c) fixing (maintaining) this level of intensity for 2.5-25 µsec until high-frequency
radiation appears in the plug electrode gap;
(d) inverting the direction of the electrical field;
(e) increasing the intensity of the electrical field in the plug electrode gap until
an electric spark passes across it;
(f) decreasing the intensity of the electrical field in steps to a set level;
(g) fixing (maintaining) this level of intensity for 2.5-25 µsec until high-frequency
radiation appears in the plug electrode gap;
(h) taking the electrical field away from the spark plug.
[0011] It is advisable to repeat stages (d) to (g) several times until the fuel-air mixture
ignition cycle is complete.
[0012] Stage (a) is implemented in an alternating electrical field, using a harmonic alternating
field with the duration of each half-wave in turn greater than the preceding one.
[0013] The electrical field is taken away gradually, using an alternating electrical field.
[0014] The solution of the problem is also achieved by the fact that the current in the
spark plug electrode gap is fixed at stages (b) and (f).
[0015] The gradual increase in the intensity of the electrical field at stage (a) over several
hundred microseconds enables a sufficient concentration of free radicals to form in
the spark plug electrode gap, which makes it easier for a discharge to take place
between the spark plug electrodes and makes it more stable.
[0016] The stepped (by nanosecond units) reduction in the intensity of the electrical field
to a set level determined by the minimum current magnitude in the electrode gap, and
the subsequent fixing of this level, enable the current in the spark plug electrode
gap to be maintained at not less than a certain magnitude, and the fuel-air mixture
to flow into the region bounded by the spark plug electrode gap from the peripheral
regions of the combustion chamber to support the discharge for 2.5-25 µsec.
[0017] The stepped inversion of the electrical field, with the subsequent stepped rise (in
steps of the order of one microsecond) in the intensity of the electrical field to
spark-over level and the stepped reduction in intensity to the set level at which
it was fixed, alters the gradient of concentration of free radicals in the spark plug
electrode gap, improving conditions for the combustion of the fuel-air mixture between
the spark plug electrodes and making the combustion process virtually continuous.
[0018] The multiple repetition of stages (d) to (g) (a hundred times or more) over the whole
ignition cycle makes it possible to burn the fuel-air mixture more efficiently and
to raise the efficiency of the engine and its ecological characteristics by increasing
the duration of the continuous discharge by a factor of two or more.
[0019] The use of an alternating electrical field at stage (a) generates free radicals in
the spark plug electrode gap. Due to the alternation of the electrical field, the
radicals are injected into the combustion chamber, thus ensuring more efficient ignition
of the fuel-air mixture due to a reduction in the activation energy. Increasing the
duration of each of the half-waves of the harmonic electrical field in succession
at stage (a) makes it possible to generate the free radicals and inject them into
the combustion chamber with greater efficiency.
[0020] The gradual reduction in the intensity of the electrical field at the end of the
ignition cycle (combustion completion stage) makes it possible to prolong the period
of existence of the free radicals in the spark plug electrode gap and to ensure the
more complete combustion of the fuel-air mixture. The alternating nature of the electrical
field at this stage enables more free radicals to be injected into the combustion
chamber and provides more efficient completion of the combustion of the fuel-air mixture.
[0021] The fixing of the current in the spark plug electrode gap enables the process of
combustion of the fuel air mixture to be stabilised if its parameters and combustion
conditions change.
[0022] The high-frequency radiation occurring in the spark plug electrode gap at stages
(c) and (g) is due to the thermodynamic instability caused by the presence of a gradient
of concentration of positively and negatively charged free radicals, creating screened
regions close to the spark plug electrodes, thus preventing the combustion process.
The fixing of the set level of intensity before the moment when high-frequency radiation
occurs with subsequent stepped inversion of the electrical field alters the gradient
of concentration of the free radicals and thus stops the high-frequency radiation,
so that the screened regions created by the, three-dimensional discharge close to
the spark plug electrodes can be eliminated.
[0023] The fuel-air mixture ignition system in accordance with this invention includes a
generator with switching-on and switching-off input and a piezo-transformer, with
its input connected to the output of the said generator. Unlike known ignition systems,
it contains a reorientation resonator, combined in the design with a piezo-transformer,
and forming with it a single piezo-element, the output of which is connected to the
spark plug electrode. In accordance with the invention, the generator of the ignition
system may also contain a synchronisation input and a discharge current control input,
in which case the system has two feedbacks from the piezo-element to the generator,
one of which is connected to the said synchronisation input and the other to the said
discharge current control input.
[0024] The inclusion in the ignition system of a reorientation resonator combined in the
design with the piezo-transformer and forming with it a single piezo-element enables
an internal feedback to be created in the piezo-element to bring about the inversion
of its output signal when high-frequency radiation occurs in the spark plug ignition
gap.
[0025] The introduction of two feedbacks from the piezo-element to the generator, one of
which is connected to the synchronisation input and the other to the discharge current
control input, makes it possible to synchronise the frequency of the generator with
the moments of inversion of the output signal of the piezo-element and to fix the
current in the spark plug electrode gap.
Description of drawings
[0026] Fig, 1 shows the dependence of the voltage at the spark plug electrodes in the known
process.
[0027] Fig. 2 is a time diagram, illustrating the proposed process in accordance with the
invention.
[0028] Fig. 3 is a block diagram of the ignition system in accordance with this invention.
[0029] Fig. 4 shows graphs of the controlling pulse voltages and the excitation voltage.
[0030] Fig. 5 shows another variant of block diagram of the ignition system in accordance
with this invention.
Examples of the implementation of the invention
[0031] Let us consider Fig. 2, showing: U - axis of voltage between spark plug electrodes;
t - time; U
init.o - initial spark-over voltage; U
break rep - repeat spark-over voltage; U
stab - stabilisation voltage; t
build-up - duration of gradual build-up of intensity of electrical field; t
red - duration of gradual reduction in intensity of electrical field.
[0032] Up to the moment when spark-over occurs, for time t
build-up, the intensity of the field in the spark plug electrode gap steadily increases to
U
init.o, this being an alternating electrical field. The intensity of the electrical field
is then reduced in steps to the set level U
stab and this level is fixed. After the occurrence of high-frequency radiation in the
spark plug electrode gap, the direction of the electrical field is inverted and the
intensity of the electrical field is again raised to the level at which spark-over
occurs in the spark plug electrode gap (U
break rep), U
break rep being less than U
init.o, and the intensity of the electrical field is again reduced in steps to the set level
U
stab, and this level is fixed. The process is then repeated many times until the end of
the ignition cycle. The electrical field is then gradually reduced over time t
red.
[0033] The block-diagram shown in Fig. 3 of an ignition system implementing the fuel-air
ignition process in an internal combustion engine in accordance with the invention
includes spark plug 5, piezo-transformer 2 and generator 1 with switching-on and switching-off
input 7, the output of which is connected to the input of piezo-transformer 2, and
also re-orientation resonator 3, combined in the design with piezo-transformer 2 and
forming with it a single piezo-element 4, as a result of which an internal feedback
6 is formed. The input of piezo-element 4 is connected to the electrode of spark plug
5.
[0034] The circuit operates as follows. Control pulses (Fig. 4a) of duration t
cont 2-5 msec with period T
cont = 20-200 msec, depending on the rate of rotation of the engine crankshaft, determining
the initial moment and the duration of the fuel-air mixture ignition cycle, are sent
to the switching-on and switching-off input 7 of the generator 1 and permit it to
operate. The sine curve signal (Fig. 4b), for the duration t
cont of the control pulse from the output of the generator 1, goes to the signal input
of the piezo-electric transformer 2 and on through the series-wired reorientation
resonator 3 forming the single piezo-element with the piezo-transformer 2, to the
electrode of the spark plug 5.
[0035] In connection with the high quality factor of the piezo-element 4, the amplitude
of the sine curve signal at its output will build up gradually in accordance with
the law [1 - exp(-t/
2)] for time t
build-up ~ 0.5 msec (see Fig. 2) to magnitude U
init.o ~ 10 kV, i.e. up to the moment that discharge formation begins. This ensures a gradual
rise in the intensity of the electrical field in the spark plug electrode gap (stage
a).
[0036] At the moment of commencement of the discharge, step reduction of voltage occurs
down to the set level U
stab ~ 650 V, at which it is maintained virtually up to the end of the current half-period
of the excitation voltage in stages (b) and (c) of the process. The set level is achieved
by selecting the amplitude of the build-up sine curve sent to the input of the piezo-element
4.
[0037] When high-frequency radiation occurs in the electrode gap, the internal feedback
in the piezo-element operates, causing the inversion of its output signal.
[0038] The presence of internal feed back is due to the fact that when high-frequency radiation
occurs in the in the electrode gap, there is a sharp change in the output impedance
of the spark plug 5. This causes reorientation of the polarisation vector of the surface
layers in the reorientation resonator (3), leading to a step change in the phase ratios
when acoustic waves are propagated in the piezo-transformer 2 (thus implementing internal
feedback 6 in the piezo-element 4), as a result of which inversion of the output voltage
of the piezo-element (in stage d of the process) takes place.
[0039] In the next half-period, the voltage builds up to spark-over level U
break rep ∼ 2 kV, which is only about a fifth of the initial spark-over level U
init.o, due to the presence of residual ionisation (free radicals) in the electrode gap of
the spark plug 5 (stage e of the process). After the formation of the discharge in
this half-period, the voltage again falls to the set level U
stab, at which it is maintained virtually up to the end of the current half-period of
the excitation voltage (stages c and g of the process).
[0040] This process is repeated in each half-period up to the end of the action of the excitation
voltage at the input of the piezo-element 4.
[0041] At the end of the excitation action on the input of the piezo-element 4, the amplitude
of the sine curve signal at its output begins to diminish gradually in accordance
with the exponential law for time t
red ∼ 0.5 msec, which ensures a gradual reduction in the intensity of the alternating electrical
field.
[0042] When the next controlling pulse arrives, the process is repeated.
[0043] The block diagram of the ignition system shown in Fig. 5 differs from that shown
in Fig. 3 in that the generator 1 also contains a synchronisation input 8 and a discharge
current control input 9. There are two feedbacks from the piezo-element, one of which
is connected to the synchronisation input 8 and the other to the discharge current
control input 9 of the generator 1.
[0044] The introduction of a feedback via the generator synchronisation input 8 makes it
possible to synchronise the inversion of the output signal of the piezo-element 4
with the change of phase of the output signal of the generator 1, and the connecting
of the feedback to the discharge current control input 9 of the generator 1 makes
it possible automatically to maintain a fixed current level in the electrode gap of
the spark plug 5, e.g. by altering the output power of the generator 1.
[0045] Experiments carried out have shown that the characteristic values for the process
applied for are as follows: U
init.o - 8-14 kV; t
build-up - 0.4-0.6 msec; time for step reduction of intensity of electrical field after spark-over
- 3-10 nsec; step raising of intensity of electrical field during inversion - 0.5-1
µsec; U
break rep - 1-2 kV; U
stab - 400-800 V; duration of t
break - 10-14 µsec; t
red - 0.4-0.6 msec. The process achieved a fuel saving of 15-30% due to more complete
combustion, and a reduction in toxicity of 20-30%.
1. Ignition process for fuel-air mixture in an internal combustion engine,
characterised in that it includes the following sequence of stages being carried out:
(a) increasing the intensity of the electrical field in the spark plug electrode gap
until an electric spark passes across it;
(b) decreasing the intensity of the electrical field in steps to a set level;
(c) maintaining this level of intensity for 2.5-25 µsec until high-frequency radiation
appears in the plug electrode gap;
(d) inverting the direction of the electrical field;
(e) increasing the intensity of the electrical field in the plug electrode gap until
an electric spark passes across it;
(f) decreasing the intensity of the electrical field in steps to a set level;
(g) maintaining this level of intensity for 2.5-25 µsec until high-frequency radiation
appears in the plug electrode gap;
(h) taking the electrical field away from the spark plug.
2. Process in accordance with claim 1, characterised in that stages (d) to (g) are repeated several times up to the end of the fuel-air
mixture ignition cycle.
3. Process in accordance with claims 1-2, characterised in that stage (a) is carried out with an alternating electrical field.
4. Process in accordance with claim 3, characterised in that at stage (a), a harmonic alternating electrical field is used, the length
of each successive half-wave of which exceeds that of the previous one.
5. Process in accordance with claims 1-4, characterised in that the removal of the electrical field is implemented only with repeated change
of its sign.
6. Process in accordance with claims 1-2, characterised in that at stages (b) and (f), the current in the spark plug electrode gap is fixed.
7. Process in accordance with claims 1-2, characterised in that at stages (c) and (g), the maintenance of the set level of intensity proceeds
until high-frequency radiation occurs in the spark plug electrode gap.
8. Ignition system for fuel-air mixture in an internal combustion engine containing a
spark plug, a piezo-transformer and a generator with switching-on and switching-off
input with its output connected to the input of the piezo-transformer, characterised in that it includes a reorientation resonator, combined in the design with the piezo-transformer
and forming with it a single piezo-element, the output of which is connected to the
spark plug electrode.
9. Ignition system in accordance with claim 8, characterised in that the generator also includes a synchronisation input and a current discharge
control input, and in which two feedbacks from the piezo-element to the generator
are introduced, one of which is connected to the said synchronisation input, and the
other to the said generator discharge current control input.