[0001] The present invention refers to an ignition device for a flame burner or the like.
This device is realized in such a way to permit a limitation of radio interference.
[0002] As it is known, the present art includes appliances in which it is necessary to light
the fire for instance in a flame burner or the like. To this end, particular electron
devices may be used and may be equipped with capacitive discharge transformers. Such
transformers generate an electric discharge by using the energy accumulated by a condenser.
In other cases, such devices may be provided with transformers which use oscillatory
circuits in order to generate high-frequency electric discharges,for instance in the
range of a few kHz.
[0003] However, till today in the planning and manufacture of such circuits the problem
of the electro-magnetic compatibility and in particular the problem of the radio interference
has not been considered and therefore the users were often obliged to install suitable
filters, such filters being conceived and realized according to the known art by using
inductors and condensers.
[0004] Concerning the construction of the ignition device, the above mentioned filters are
sometimes integrated inside the ignition device itself. However, the results are not
satisfactory.
[0005] In the Figure 1, one of the possible realizations is shown and refers to a circuitry
of a known ignition device as actually realized. Its principle of working is the same
as almost all the ignition devices with capacitive discharge. This principle of working
is the following.
[0006] By supplying the circuit with the power, the charge of a condenser C1 starts through
a resistance R1. This charge is possible only when a diode D1 is in conduction (positive
half wave of input tension).
[0007] When the tension in the point common to resistors R2 and R3 is strong enough to reach
the threshold tension or voltage of a Zener Diode, the current passing through the
Zener diode permits a SCR to be conducted. The SCR discharges all the energy accumulated
in the condenser C1 on the primary of a transformer T which serves to raise the tension
of the primary according to the turns ratio between primary and secondary.
[0008] The transfer of energy between primary and secondary of transformer T causes the
formation of a spark which triggers the process of combustion. A diode D2 is therefore
a diode "flywheel". The repetition frequency of the spark, the tension in the secondary
of the transformer T and the generated energy depend on the frequency of the input
tension and on the dimensions of the used components.
[0009] Moreover, till today the constructors of ignition devices have always realized the
transformers by obtaining both windings on the same axis or by winding both windings
in a concentric way, the secondary being winded on the primary, without worrying about
problems of electromagnetic compatibility.
[0010] According to the described solution and according to all the known solutions, the
problem of radio interference has not been therefore solved till now unless conventional
filters are used. However, such filters are too cumbersome and do not offer satisfactory
results.
[0011] By using the present invention, the above mentioned inconveniences are removed, or
at least reduced. In particular, the present invention proposes a solution alternative
to the use of the conventional anti-interference filters in order to make the working
of the ignition device acceptable as concerns the electromagnetic compatibility in
relation to the radio interference.
[0012] The present invention permits to reach some practical advantages relative to the
fact that first of all the adopted measures are more economic than the knwon filters
and solutions and above all these measures permit to reduce the dimensions of encumbrance
to a minimum so that the same solution may be adopted also in those appliances in
which the available spaces are reduced to the simplest terms.
[0013] The above particular aims, functions and advantages are all reached according to
the present invention through an ignition device for a flame burner or the like permitting
a limitation or radio interference, characterized by the fact of consisting of a circuit
in which all or some of the following measures are provided: a SCR connection forms
a current ring between the SCR and the transformer; a resistance controlling the charge
of a condenser is divided in two parts, a resistance part being connected with a phase
and the other part being connected with a neutral; a control synchronizer is used
to prevent the formation of an electric discharge during the charge phase of the condenser;
a comb is grounded and is placed under an ignition transformer; the transformer is
realized by winding a primary on a secondary and in the inner part of both windings
there is a ferrite or the like for optimizing the energy transfer; utilization of
two condensers which discharge the generated radio disturbances to the ground and
above all, such condensers filter all the radio disturbances which are catched by
the primary winding; a direct connection of the ignition device or a direct connection
of only a part thereof with a starting electrode; the said command pulse may be sent
by a "diac" or "zener" or whatever component or electric circuit able to control the
conduction of the SCR whenever the voltage across the condenser reaches a wished value;
the said synchronizer may be for instance a "zero crossing" or other similar element
avoiding the formation of a discharge during the charge phase of the condenser.
[0014] Further features and details of the present invention will better appear from the
following description of a preferred embodiment which is represented in the accompanying
drawings as an example not limiting the invention itself in which drawings:
Fig. 1 shows a diagram of one of the possible realizations of a known ignition device
as realized at present;
Fig. 2 shows a diagram of a circuit according to the present invention in which the
SCR connection forms a current ring between the SCR and the transformer when there
is the discharge;
Fig. 3 shows a diagram of a circuit according to the present invention in which the
resistance adjusting the charge of the condenser is divided in two resistances (R1
and R2);
Fig. 4 shows a diagram of a circuit according to the present invention in which a
synchronizer or the like is installed;
Fig. 5 shows a schematic view of an earthed element or comb under the ignition transformer;
Fig. 6 shows a schematic view of the transformer T, which is realized by winding the
primary on the secondary;
Figg. 7 and 8 show schematic views of two solutions of transformers, realized according
to the known art;
Figg. 9-12 show diagrams of possible connections of two condensers (C2 and C3), used
to discharge the generated radio interference to earth;
Figg. 13-15 show diagrams referring to the positioning of some possible components
generating a command pulse;
Fig. 16 shows a view of a whole electric diagram according to the present invention
referring to the solution of the problem of radio interference;
Fig. 17 shows a schematic view of a graph referring to the performances of the present
invention;
Fig. 18 shows a schematic view of a graph referring to the performances of an ignition
device of present production;
Fig. 19 shows a view of a diagram from which it appears the direct connection of the
ignition device on the electrode.
[0015] The aim of the present invention has been reached through the following measures.
Each of these single measures proved effective.
[0016] As it appears from Fig. 2, the first measure refers to the connection for the SCR
which is arranged in such a way to form a current ring between the SCR itself and
the transformer when there is the discharge. This permits to obtain a good reduction
in the generated radio interference, especially as regards the low- frequencies (lower
than 1 MHz).
[0017] The second measure as it appears from Fig. 3 refers to the resistance regulating
the charge of the condenser, which resistance is divided in two resistances, the former
being connected to the phase (R1) and the latter being connected to the neutral (R2).
This solution permits a better balance of the radio interference which occurs in the
phase and neutral. On the contrary, from the prior art it appears that the radio interference
coupled with the neutral is very higher than the radio interference coupled with the
phase.
[0018] A third measure refers to the use of a synchronizer as it appears from Fig. 4. This
synchronizer prevents the formation of an electric discharge during the charging phase
of the condenser C1 and during the whole period in which the diode D1 is directly
polarized. This measure prevents that a current source be generated when the device
is connected to the input voltage through the conduction of the diode D1. Moreover,
this measure permits that the radio interferences be generated only when the device
is decoupled from the supply mains through the diode D1 which is denied in this phase.
This measure is a further improvement as concerns the radio interferences, especially
in case of low-frequencies (lower than 1 MHz).
[0019] The fourth measure resulting from Fig. 5 concerns the use of a grounded comb A placed
under the ignition transformer B in order to absorb the generated radio interference
as much as possible.
[0020] Fig. 6 shows a fifth measure according to which the transformer T is realized by
winding the primary 1 on the secondary 2 so that the transformer T acts also as a
screening element. In this way, it is not necessary to insert screens realized in
conductive materials for screening the transformer according to the known art.
[0021] The more the primary winding includes the secondary, the higher the results are.
A suitable ferrite 3 is placed in the inside of both windings. This ferrite optimizes
the transfer of the energy. On the contrary, till today the constructors of ignition
devices have always realized the transformers by getting both windings on the same
axis as it is represented in Fig. 7 or by winding them in a concentric way, the secondary
being winded on the primary without worrying about the problems of the electromagnetic
compatibility (Fig. 8).
[0022] A sixth measure refers to the utilization of two condensers (C2 and C3) connected
as it results from Figg. 9-12 and used to discharge the generated radio interferences
to the ground. In particular, these condensers (C2 and C3) filter all the radio interferences
which are catched by by the winding of the primary, this winding having also a screening
function. These condensers may be connected both upstream and downstream in respect
to the resistors R1 and R2, as it is represented in Figg. 9-12. The connection assuring
the highest effectiveness is to be determined each time depend ing above all on the
arrangement of the components of the printed circuit or in the inside of the ignition
device.
[0023] Finally, a further effective measure for reducing the radio interferences consists
in directly connecting the ignition device 4 or only a part thereof to the ignition
electrode 5, as it is schematically represented in Fig. 19. This measure eliminates
the presence of a high-tension cable. This is advantageous since high - tension cables
as aerials irradiate electromagnetic waves in the atmosphere. Accordingly, this measure
cancels a part of the other measures.
[0024] The direct connection between the ignition device and the electrode offers the following
advantages:
a) the radio interferences are eliminated or reduced to the minimum since the connection
between the outer device and the apparatus does not take place any more through a
high-tension cable. The connection occurs through a usual cable;
b) the resistance, which has been used till today to reduce the high-frequency radio
interferences, is eliminated. This resistance was positioned near the ignition electrode;
c) there is the possibility of further reducing the dimensions of the apparatus since
there are no more high-voltage parts in the inner part of the apparatus itself.
[0025] The above-described measures may be utilized on the whole in order to reach the highest
reduction in the radio interferences. However, it is possible to utilize only some
of these measures according to the wished result. From Fig. 16 it results in detail
the whole circuitry concerning the solution of the problem of radio interference.
It is to be noted that the command pulse or signal shown in Fig. 4 may be generated
by using for instance a diac (Fig. 13), a zener (Fig. 14) or whatever electric component
or circuit which may control the conduction of the SCR whenever the voltage across
the condenser C1 reaches the wished value (Fig. 15).
[0026] Moreover, there are other solutions for the circuitry different from the solution
proposed to generate a synchronizing signal. One of these solutions is a "zero crossing"
or the like.
[0027] Now we shall briefly describe the principle of working of the ignition circuit according
to the present invention including the above described measures for limiting the radio
interferences.
[0028] By feeding the circuit it is possible to start charging the condenser C1 through
the resistors R1 and R2. The charge may occur only when the diode D1 is in conduction
(positive half wave in this case).
[0029] When the voltage in the point common to resistors R5 and R6 is strong enough to reach
the threshold voltage of the zener diode DZ near the half wave of the feed voltage
opposite to the charge half wave (negative half wave in the represented case), in
which phase the transistor TR is denied, the SCR discharges the energy which had been
previously stored in the condenser C1 on the primary of the transformer T. The diode
D2 is thus a "flywheel" diode.
[0030] During the discharge, a part of the generated radio interferences is absorbed by
the grounded comb under the transformer while the greater part of the radio interferences
is absorbed by the primary and discharged to the ground through the condensers C2
and C3.
[0031] The spark is generated during the half wave opposite to the charge half wave. In
this way the remaining radio interferences are eliminated, especially in case of frequencies
lower than about 1 MHz.
[0032] On the whole, the so-obtained solution permits to amply maintain the radio interferences
generated by this kind of ignition device within the limits provided for by the relevant
provisions. On the contrary, the radio interferences issued by the currently used
ignition devices always exceed the upper limit permitted by the provisions.
[0033] The above described difference will be better comprised from the accompanying graphs
which show the new solution in question (Fig. 17) and an igniter of present production
(Fig. 18) for a frequency field included between 150 KHz and 30 MHz; the broken line
indicates the upper limit permitted.
[0034] The present device for limiting the radio interferences in a capacitive discharge
igniter has been described and illustrated according to the preferred solutions. However,
there may be provided variants which are technically equivalent to the described parts
and components and are included within the scope of protection of the present invention.
1. An ignition device for a flame burner or the like for limiting the radio interferences,
characterized by the fact of comprising a circuit in which the connection of the SCR
forms a current ring between the SCR itself and a transforming element (T), and in
which the said transforming element (T) is realized by winding the primary (1) on
the secondary (2), a ferrite (3) or similar element being placed in the inner part
of the said windings for optimizing the transfer of energy; the said circuit is provided
with a resistance (R) for regulating the discharge of the condenser, the said resistance
being divided into two parts (R1, R2), the former being connected to the phase and
the latter being connected to the neutral; the said circuit comprises a control synchronizer
for avoiding the formation of an electric discharge during the charging phase of the
condenser and for the whole period in which the diode is directly polarized; a grounded
element or comb (A) is provided under the ignition transformer (B); at least two condensers
(C2 and C3) are provided to permit the discharge to ground of the generated radio
interferences and above all to filter all the radio interferences catched by the primary
winding; finally there is a direct connection for the ignition device (4) or only
a part thereof on the ignition electrode (5).
2. An ignition device for a flame burner or the like, as claimed in claim 1, characterized
by the fact that the said command signal may be transmitted by a "diac" or by a "zener"
or whatever electric component or circuit which may control the conduction of the
SCR whenever the voltage across the condenser (C1) reaches the wished value.
3. An ignition device for a flame burner or the like, as claimed in the foregoing claims,
characterized by the fact that the said synchronizer may consist for instance of a
"zero crossing" or the like avoiding the formation of the discharge during the charging
phase of the condenser.
4. An ignition device for a flame burner or the like, as claimed in the foregoing claims,
characterized by the fact that the devices as described in the foregoing claims may
all be inserted in the circuit in order to reach the highest level of reduction in
the radio interferences; otherwise it is possible to utilize only some of the described
components according to the wished results, the innovative concept of the ignition
circuit remaining the same.