[0001] The present invention refers to an electronic circuit for supplying high-frequency
power to fluorescent lamps of different types and powers.
[0002] Electronic ballasts are apparatuses which allow high-frequency power supply (in the
order of tens of kHz) to fluorescent lamps with undoubted advantages in terms of efficiency
and performance, such as protection against working anomalies, no flickering, etc.
[0003] Nevertheless, all of the types of electronic "ballast" currently on the market can
only supply a single type of lamp, of a certain power, or groups of lamps having electrical
characteristics (lamp current and voltage) which are similar between the individual
lamps, with the consequent drawbacks given by low performance which, in many cases,
is not congruous with the type of lamp supplied, by low efficiency and by the relatively
short useful life.
[0004] The purpose of the present invention is therefore that of avoiding the aforementioned
drawbacks and, in particular, that of realising an electronic circuit for supplying
high-frequency power for fluorescent lamps which is capable of supplying fluorescent
lamps of different types and powers, overcoming the limitations of apparatuses available
up to now.
[0005] Another purpose of the present invention is that of realising an electronic circuit
for supplying high-frequency power for fluorescent lamps which is particularly reliable
and which is capable of recognising the type of lamp connected to it, then supplying
it in the correct manner.
[0006] A further purpose of the present invention is that of indicating an electronic circuit
for supplying high-frequency power for fluorescent lamps which is also simple to realise,
safe and relatively economic, also concerning the low management and maintenance costs,
with respect to the electronic "ballasts" of the conventional type.
[0007] These and other purposes are achieved, in the invention, by realising an electronic
circuit for supplying high-frequency power for fluorescent lamps according to claim
1, to which we refer for the sake of brevity.
[0008] Further characteristics and advantages of an electronic circuit for supplying high-frequency
power for fluorescent lamps, according to the invention, shall become clearer from
the following description, given as an example and not limiting purposes, referring
to the attached drawings, in which:
- figure 1 shows a circuit diagram relative to the topology of the power stage of the
power supply device, according to the present invention;
- figure 2 shows a circuit for measuring the power absorbed by each lamp, which is used
in the power supply device, according to the present invention;
- figures 3 and 4 show a block diagram of a discriminator circuit of the power absorbed
and a circuit for changing the frequency of oscillation, which are present in a power
supply device, according to the present invention;
- figure 5 represents a circuit for comparing and varying the frequency used in the
power supply device, according to the present invention;
- figure 6 shows an example overall embodiment of the electronic circuit for supplying
high-frequency power for fluorescent lamps, according to the present invention.
[0009] As can be seen clearly in the aforementioned figure 1, the topology of the power
stage of the power supply circuit for fluorescent lamps object of the invention is
a half-bridge with series resonant load, consisting of the capacitor CRES and of the
inductor LRES, and has the fluorescent lamp LF connected in parallel to the resonance
capacitor CRES.
[0010] Two power MOSFETs, indicated with QHIGH and QLOW in figure 1, are connected to the
series resonant load and are supplied with power by a supply line or high voltage
bus HVB (about 400 Volts) . Moreover, the power MOFSETs QHIGH and QLOW are driven
by a suitable integrated command circuit ("half-bridge driver") - indicated with HBD
in figure 1.
[0011] Connecting to the mains, the power supply circuit or "ballast" starts to oscillate
at a frequency value far from the value of the resonance frequency of the mains comprising
the capacitor CRES and the inductor LRES, allowing the cathodes or filaments of the
lamp to be preheated, without switching it on.
[0012] The voltage at the ends of the lamp LF is, indeed, kept below a predetermined value
which is shown on the specific lamp. Such a value is the lowest from all of the lamps
which can be supplied.
[0013] Moreover, during the preheating step, recognition of the lamp LF is stopped and the
power supply circuit oscillates at the same frequency independently of the lamp LF
connected.
[0014] With the preheating of the filaments of the lamp LF completed, the frequency of oscillation
of the supply circuit gradually decreases moving closer to the resonance value of
the mains L-C formed by the capacitor CRES and by the inductor LRES. The voltage at
the ends of the lamp LF increases allowing it to be switched on.
[0015] With the lamp LF switched on, the supply circuit or "ballast" functions at the minimum
frequency of oscillation corresponding to the maximum power.
[0016] The procedure with which the electronic power supply recognises the lamp LF consists
of measuring the average power absorbed by it and of varying the frequency of oscillation
of the half-bridge circuit to adapt the current and voltage values to that which is
requested by the lamp LF.
[0017] If an average power value greater than a certain threshold is measured this means
that the lamp LF with the highest power is connected and the "ballast" continues to
function at the lowest frequency corresponding to the maximum power.
[0018] If, on the other hand, an absorbed power value lower than the aforementioned threshold
is detected, this means that a lamp LF with the lowest power is connected and, in
this case, the "ballast" increases the frequency of oscillation reducing the power
supplied to the lamp LF.
[0019] The measurement of the power absorbed by the lamp LF is carried out through a resistance,
indicated with RS in figure 2 connected in series to the "SOURCE" of the MOSFET with
power QLOW. The average value of the voltage signal at the ends of the resistance
RS is directly proportional to the average power absorbed by the lamp LF.
[0020] To obtain the average value of the voltage drop at the ends of RS, according to the
present invention, a low power filter R-C is used, generically indicated with LPF
in figure 3. Following on from such a low power filter LPF, a discriminator circuit
of the power absorbed is foreseen which, in preferred example embodiments of the present
invention, consists of a comparator CMP with output DO, of the open-drain type (see,
in particular, figure 3).
[0021] The signal coming from RS, mediated by the low power filter LPF, is compared with
a low voltage reference LVR.
[0022] When the signal S coming from the sensing circuit and, therefore, coming from the
resistance RS is greater than the reference LVR the output DO of the comparator circuit
CMP is forced to ground. Vice-versa, when the signal S is lower than the reference
LVR the output DO of the comparator CMP is an open circuit.
[0023] A second comparator circuit PI ("preheat inhibit") is used to inhibit the recognition
of the fluorescent lamp LF during the preheating step of the filaments. In practice,
until the voltage VCPH is less than a high voltage reference HVR, the output OUT of
the comparator PI is low and forces to ground the low voltage reference LVR of the
comparator CMP.
[0024] As can be seen in figure 4, the output DO ("open-drain output") of the comparator
CMP relative to the power signal is connected to the pin 6 (capacitor CT) of an integrated
circuit which functions as a half-bridge driver circuit. In particular, in preferred
but not limiting embodiments of the present invention, the integrated circuit IR2156
is used as a half-bridge driver HBD.
[0025] The output DO of the comparator CMP is also connected to the pin 4 (resistance RT)
of the integrated driver circuit HBD, respectively, through a signal diode DS (usually
a 1N4148 diode is used) and a resistance RSH.
[0026] When the output DO of the comparator CMP is low (practically at ground level), i.e.
in maximum power conditions, the resistance RSH is disconnected from the pin 6 (capacitor
CT) of the driver circuit HBD, since the diode DS is inversely polarised, the voltage
at the pin 6 (and therefore the voltage taken at the ends of the capacitor CT) always
being greater than 4.8 Volts.
[0027] If, on the other hand, the output DO of the comparator CMP is high (circuit open),
i.e. in minimum power conditions, the resistance RSH is connected in parallel to the
resistance RT, unless there is a drop in potential on the diode DS. In such conditions,
the capacitor CT is charged faster and the frequency of oscillation of the half-bridge
is higher.
[0028] The value of the resistance RT, together with the value of CT, set the minimum value
of the frequency of oscillation (and a corresponding maximum power value), whereas
the value of the resistance RSH sets the frequency of oscillation relative to the
minimum operating power condition.
[0029] For the discriminator stage of the power absorbed schematised in figure 3, according
to the invention, a double comparator CMOS with output DO ("open-drain") is used,
indicated with CDO in figure 5.
[0030] In particular, in the case of the present invention, the comparator TS393 was used,
in which the two voltage thresholds LVR (threshold of the power comparator CMP of
figure 3) and HVR (threshold of "inhibit" of Figure 3) are obtained by a partition,
formed by the resistances RDV1, RDV2, RDV3 of figure 5, of the supply voltage VCC
of all of the integrated circuits, the typical value of which is 15.6 Volts.
[0031] These two references LVR and HVR are respectively connected to the non-inverting
input of the power comparator CMP (pin 3 of the comparator CDO) and to the inverting
input of the inhibit comparator PI (pin 6 of the comparator CDO).
[0032] The inverting input of the power comparator CMP (pin 2 of the comparator CDO) is
connected to the signal S coming from the resistance RS, mediated by the low-power
filter R-C, whereas the inverting input of the inhibit comparator PI (pin 5 of the
comparator CDO) is connected to the capacitor CPH (pin 7 of the driver circuit HBD
of figure 5), with which the preheating time of the fluorescent lamp LF is set.
[0033] Finally, figure 6 schematically illustrates the overall circuit of the power supply
device or "ballast" object of the invention. For the sake of clarity, said circuit
has been divided into five blocks and, in particular, it is possible to identify an
interference filter F ("EMI filter"), a stage S1 for the active control of the power
factor ("PFC section"), a half-bridge driver circuit HBD, a discriminator circuit
CDO of the power absorbed ("power comparator") and a resonant load LR.
[0034] The interference filter F is not essential for the operation of the supply circuit,
but is obviously necessary to contain the interference within the limits set by the
current norms in the field.
[0035] The stage S1 allows the values of the power factor near to the unit to be obtained
and allows the harmonic content of the current absorbed by the mains to be limited
within the limits dictated by the norms.
[0036] The stage S1 also allows a virtually constant continuous regulated voltage (with
a low residual "ripple" at 100 Hz) to be obtained with which the half-bridge is to
be supplied.
[0037] From the description which has been made, the characteristics of the electronic circuit
for supplying high-frequency power for fluorescent lamps object of the present invention
are clear, just as the advantages are also clear.
[0038] Finally, it is clear that numerous other variants can be brought to the supply circuit
in question, without for this reason leaving the novelty principles inherent to the
inventive idea, just as it is clear that, in the practical embodiment of the invention,
the materials, the shapes and the sizes of the illustrated details can be whatever
according to requirements and they can be replaced with others which are technically
equivalent.
1. Electronic circuit for supplying high-frequency power for fluorescent lamps (LF),
characterised in that it comprises a command circuit (HBD) of a power stage, a resonant load circuit (LR)
and a discriminator circuit (CDO) of the active power absorbed by each lamp (LF),
which measures the power absorbed by each type of fluorescent lamp (LF), so that said
lamp (LF) is correctly supplied with consequent determined values of current and voltage.
2. Electronic power supply circuit according to claim 1, characterised in that it also comprises at least one interference filter (F) and at least one circuit stage
(S1) for actively controlling the power factor, in order to obtain power factor values
near to the unit and to limit the harmonic content of the current absorbed by the
mains, said circuit control stage (S1) also allowing a substantially constant continuous
regulated voltage to be obtained with which said power stage is to be supplied.
3. Electronic power supply circuit according to claim 1, characterised in that said power stage is of the half-bridge type and comprises a resonant load of the
series type with resonance capacitor (CRES) and inductor (LRES), said fluorescent
lamp (LF) being connected in parallel to said resonance capacitor (CRES).
4. Electronic power supply circuit according to claim 1, characterised in that power transistor devices (QHIGH, QLOW), which are supplied with power by a high voltage
ballast (HVB), are connected to said series resonant load, said transistor devices
(QHIGH, QLOW) being driven by said driver circuit (HBD) and said connection to the
supply line being used to operate a preheating step of the filaments of said lamp
(LF) during which said supply circuit oscillates at a predetermined frequency value,
independently from the type of fluorescent lamp (LF) connected.
5. Electronic power supply circuit according to claim 4, characterised in that following said preheating step of the filaments of the lamp (LF) there is a step
in which said frequency of oscillation gradually reduces moving closer to the resonant
frequency value of said resonant circuit (CRES, LRES), so that the voltage at the
ends of said lamp (LF), increasing, allows it to be switched on.
6. Electronic power supply circuit according to claim 5, characterised in that said frequency of oscillation of the half-bridge circuit is regulated so as to adapt
the voltage and current values applied to said fluorescent lamp (LF), according to
the average power values absorbed by the lamp (LF) with respect to a determined threshold
value.
7. Electronic power supply circuit according to claim 6, characterised in that one of the terminals of at least one of said power transistor devices (QLOW) is connected
to at least one resistive element (RS), suitable for measuring the power absorbed
by said lamp (LF), said resistive element (RS) being connected to a low-power filter
(LPF) which is, in turn, connected in cascade to said discriminator circuit (CDO)
of the power absorbed.
8. Electronic power supply circuit according to claim 7, characterised in that said discriminator circuit (CDO) comprises at least one first comparator device (CMP)
with output (DO) of the open-drain type, said first comparator (CMP) taking care of
comparing a signal (S) coming from said resistive element (RS) and mediated by said
low-power filter (LPF) with a low voltage reference (LVR), so as to force said output
(DO) to ground or to make it an open circuit, according to the value of said signal
(S) compared to said low voltage reference (LVR).
9. Electronic power supply circuit according to claim 8, characterised in that a second comparator device (PI) is used to inhibit the recognition of said fluorescent
lamp (LF) during the preheating step of the filaments, the output (OUT) of said second
comparator (PI) being connected to said low voltage reference (LVR).