[0001] The present invention relates to a dimmable or controllable electronic ballast for
a low-pressure discharge lamp, especially a fluorescent lamp, whose operation is based
on regulating the light output of a lamp by varying the frequency of voltage supplied
to the lamp. The invention relates to a method and a circuit system for accurately
measuring the power supplied by such a ballast to a lamp load so as to find out the
proportional share of power consumed by the lamp cathodes.
[0002] The structure of electronic ballasts for low-pressure discharge lamps is prior known
from the Applicant's patent No. 64478 as well as the theoretical foundations from
the Applicant's patent No. FI 63314. On the other hand, the Applicant's patent No.
FI 63146 discloses the structure and operation of a low-voltage controlled electronic
ballast for gaining a light output proportional to an external control signal.
[0003] The structure and operation of a controllable or dimmable ballast prior known from
the Applicant's patent No. FI63146 will be described in more detail with reference
to fig. 1 of the attached drawings, depicting one preferred embodiment for such a
ballast. In order to simplify the representation, fig. 1 only illustrates the structural
components that are most essential in terms of understanding the operation.
[0004] The ballast shown in fig. 1 includes a rectifier V1 connected to a supply voltage
UV, a smoothing capacitor C1, a high-frequency oscillator A1, as well as transistors
TR1 and TR2 constituting a semi- or half-bridge circuit. A lamp LL is connected as
part of a resonance circuit, constituted by a capacitor C2 and a winding L2 and supplied
by the push-pull transistors TR1 and TR2. A filament pre-heating current for the cathodes
of the lamp LL at a switch-on stage of the lamp is passed via a capacitor C3. The
oscillator Al is provided with a control connection CO1 - CO2, wherethrough the control
signal influences the oscillating frequency of the oscillator. The electronic ballast
must generally be fitted with a separate safety feature for against certain special
circumstances, such as over- or undervoltage in an electric network supplying the
ballast, overheating of the device, a missing lamp, or breaking of the lamp cathodes,
as described e.g. in the Applicant's patent application FI 955695.
[0005] It is general knowledge that heating the cathodes of low-pressure discharge lamps
during the switch-on sequence of a lamp has a positive contribution to the service
life and operating characteristics of the lamp. The appropriately dimensioned filament
power can be used for prolonging the service life of a lamp by reducing a stress applied
to the lamp cathodes and especially to the emission material layer serving as a coating
therefor. At the same time, this enables a lamp to be switched on without flicker
with a voltage across the lamp that is lower than what is required when pre-heating
is not used. The requirements set on electronic ballasts regarding the heating of
cathodes during the ignition of a lamp are set forth in the International standard
IEC 929. The purpose of these requirements is to make sure that fluorescent lamps
according to standards IEC 81 and IEC 901 reach the service life specified therefor.
Deviation from the requirements of said standards may cause also other adverse effects,
such as blackening of the glass bulb of a lamp in areas next to the cathodes, as material
emitting from the cathodes accumulates on the internal surface of the glass bulb.
[0006] It is also prior known that said heating of the lamp cathodes is necessary whenever
it is desirable to regulate the light output of the lamp. Sufficient cathode incandescence
is used to make sure that a sufficient number of charge carriers are emitted from
the cathodes to sustain discharge in a lamp as the current passing therethrough is
diminishing. An optimal heating level is again necessary for maintaining the service
life of a lamp at an acceptable level. Fig. 2 of the drawings depicts one preferred
embodiment for heating of the cathodes of a lamp LL. In this circuit, a coil L2 includes
two secondary windings for supplying the cathodes of the lamp LL with filament heating
energy of a desired magnitude via capacitors C5 and C6. Circuit elements R4 and V5
are used for a measuring purpose in a manner explained in more detail in connection
with the description of the characterizing features of the invention.
[0007] It is essential for the operation of an electronic ballast as described above that
the power supplied to the lamp LL can be measured at a sufficient accuracy. This measuring
information is utilized in the operation of a control block Al, such that the lamp
LL can be supplied in a stable manner with a power proportional to a voltage between
control lines CO1 and CO2 for regulating the light output of the lamp. The power delivered
by the half-bridge connected transistor circuit TR1 and TR2 to the lamp load LL consists
of two components: an actual lamp power, which sustains a light-generating discharge
within the lamp, and a filament power, which is used for heating the lamp cathodes.
Especially at lower regulation levels, whereby the power consumed by the discharge
of a lamp is low, the power of cathode heating constitutes a substantial share of
the power of the entire circuit. A problem with the above-described ballast is the
measurement of a load power in such a fashion that the actual lamp power can be measured
at a sufficient accuracy without the power required by cathode heating having a significant
effect on the measuring result.
[0008] An object of this invention is to introduce a measuring circuit connection for a
ballast of the type defined in the preamble of claim 1, whereby the power of a low-pressure
discharge lamp, especially a fluorescent lamp, can be measured such that the proportion
of a power used for incandescence of the cathodes is compensated out of the measuring
result.
[0009] This object is achieved in the invention by means of the features set forth in the
annexed claim 1. The non-independent claims disclose preferred embodiments of the
invention.
[0010] In the drawings,
- fig. 1
- illustrates the prior art as described above;
- fig. 2
- shows one circuit configuration for the incandescence of a lamp cathode, said circuit
being provided with elements R4, V5 for measuring the proportion of a power used for
heating the cathodes; and
- fig. 3
- shows an electronic ballast, provided with a lamp power measurement of the invention
and including a circuit configuration slightly different from that of fig. 2 for heating
the cathodes and for measuring the proportion of a power used therefor.
[0011] The invention will be described in more detail in terms of its operation with reference
made to fig. 3, most of the functions thereof having already been explained by means
of fig. 1 of the drawings. An addition to this are so-called freewheel diodes V2 and
V3, which allow the forward passage of the current of an oscillating circuit whenever
a transistor TR1 or TR2 in parallel therewith has broken the circuit in the opposite
direction of the current.
[0012] The effective energy consumed by a half-bridge TR1 - TR2 is primarily transferred
into a load circuit C2, L2, LL, and C3. As a result of the symmetrical action of the
circuit, the current through either one of the half-bridge supplies is proportional
to the energy consumed by the load circuit, if the half-bridge supply voltage is maintained
constant.
P
load ~ I
halfbridge,supply
[0013] The load circuit is constituted by a coil or winding L2, a lamp LL, and capacitors
C2, C3. The lamp LL is the only one of these to use effective power. The energy spent
by the lamp LL is divided into the use of energy caused by the lamp discharge and
the energy consumed by filaments. In terms of light output, the energy of a lamp current
is interesting.
[0014] When the effective power of a load circuit or the light output produced by the lamp
LL is regulated by using the halfbridge supply current as a reference value, the regulation
functions well as long as the lamp power exceeds the filament power. When said powers
are equal or the lamp power is lower than the filament power, the regulation becomes
inaccurate. Depending on the type of lamp, this occurs between about 10...20 % light
level. When it is desirable to adjust this to a lower light level, the effect of the
filament power must be eliminated from the measuring signal. This can be effected
e.g. by measuring a voltage existing across one of the cathodes of the lamp LL. The
cathode voltage is a product of the cathode resistance and the square sum of a filament
current as well as a lamp current. It should be noted that the filament current and
the lamp current have a phase difference of about 90 degrees. At low light levels,
the filament voltage is constituted primarily by the filament current, as the lamp
current is low. Thus, a preferred compensating signal is obtained by simply subtracting
an appropriately dimensioned voltage proportional to the filament voltage from a voltage
proportional to the halfbridge supply current.
[0015] The compensation is dimensioned to be significant at lower light levels only. The
filament power can be calibrated, i.e. the effect of filament resistance fluctuations
between various individual lamps can be compensated for prior to the ignition of a
lamp by comparing the halfbridge current with the filament voltage.
[0016] A measurement from the end of a lamp yields both the filament and lamp current. The
dynamic impedance of a fluorescent lamp is almost resistive over a wide frequency
range and the value of impedance is keenly dependent on the level of a lamp current
such that, on low currents, the effective resistance is very high and, on high currents,
it is respectively low.
[0017] Fig. 3 of the drawings illustrates one embodiment of the above-described measuring
principle. In this case, the total output of a load circuit is measured by using a
resistance R2, which produces a voltage proportional to the current of a halfbridge
TR1 - TR2, said voltage bing filtered by means of elements R3 and C4 and forwarded
to an oscillator block A1. Here, the oscillator block A1, in terms of its function,
is divided in two sections, whereby a sub-block II handles the processing of measuring
signals and a sub-block I the control of the halfbridge transistors TR1 and TR2.
[0018] The voltage proportional to a power used for the heating of the cathodes of the lamp
LL is developed by means of elements V4 and R1 and this measuring signal is likewise
forwarded into the sub-block II of the oscillator circuit A1. The difference between
said measuring signals is obtained here, whereby the control block has at its disposal
a real measuring signal proportional to the lamp power. By means of this and a control
signal fed into the lines CO1 - CO2, the control block II is able to conduct its control
function in such a manner that control of the halfbridge TR1 - TR2 by way of the sub-block
I guarantees a stable lighting regulation as designed for the ballast.
[0019] When the pre-incandescence of cathodes is carried out by using a circuit as set forth
in fig. 2, the voltage proportional to the filament power of the cathodes is obtained
across a resistance R4 and the measuring signal is delivered to the control block
by way of a diode V5.
[0020] It is evident for a skilled person that the invention is not limited solely to the
described embodiments but it equally well adaptable to numerous other frequency-regulation
based ballast circuits, e.g. to multiple-lamp ballast versions. Especially, the technology
of switching transistors used in the halfbridge bears no significance on the usefulness
of the described circuit, i.e. applicable in this context are a.o. a bipolar transistor
and various versions of field effect transistors. It is also obvious that the control
signal of the oscillator A1 in the circuit CO1 - CO2 can also be digital, in which
case the sub-block II includes necessary circuit elements for processing digital information,
e.g. by means of a programmable microcontroller.
1. A controllable or dimmable electronic ballast provided with a lamp power measurement
for a low-pressure discharge lamp, especially for a fluorescent lamp, said ballast
comprising
- at least one halfbridge inverter (TR1, TR2, V2, V3) or a corresponding AC-source,
which supplies power to a load circuit,
- a load circuit, which includes a current limiting inductance (L2) and a filament
current supplying capacitance (C3) as well as a discharge lamp (LL) connectable to
the ballast,
- a regulation or control block (A1/I, II) for controlling the frequency of the inverter
or a corresponding AC-source for regulating the light output of the lamp; and
- elements (R2, R3, C4) for measuring a current proportional to the load circuit power
and for delivering measurement information (Umeas.) to the regulation or control block,
characterized in that the device further includes elements (R1, V4; R4, V5) for measuring a voltage
proportional to a current passing through one or more filaments of the lamp and for
delivering measurement information to the regulation or control block (A1/I, II),
wherein the measurement information is used for compensating the effect of filament
power out of the measuring result of the load circuit power.
2. A ballast as set forth in claim 1, characterized in that from a voltage proportional to the load circuit current is subtracted a voltage
proportional to the filament current and the difference is used for controlling the
regulation of the light output of a lamp.
3. A ballast as set forth in claim 1 or 2, characterized in that said elements for measuring a voltage proportional to the filament current
include a resistance (R1, R4) connected to the end of a filament, and the elements
for delivering measurement information to the regulation or control block (A1/I, II)
include a diode (V4, V5) connected to one of the poles of the measuring resistance
(R1, R4).