[0001] This invention relates to a lighting circuit for an electric discharge lamp such
as a fluorescent lamp, a rare gas electric discharge lamp for near infra-red rays,
and other low pressure electric discharge lamps. More particularly, the present invention
is concerned with a lighting circuit for such electric discharge lamp which causes
it to operate by application of a high frequency voltage having a pause-time period
for every half cycle.
[0002] First of all, explanations will be given as to the conventional technique for operating
the low pressure electric discharge lamp by application of a voltage having a pause-time
period.
[0003] Japanese unexamined utility model publication No. 4779/1973 discloses a lighting
circuit of a construction, in which use is made of a turn-off thyrister provided in
parallel with a fluorescent lamp to thereby convert a lamp voltage V
L in a sinusoidal waveform into a plurality of pulse voltage as shown in Figure l(a)
of the accompanying drawing. This lamp voltage V
L, however, is of commercial frequency, the purpose of which is to reduce a size of
a choking coil as a current limiting impedance, hence the prior right invention differs
from the present invention.
[0004] In the above-described conventional technique, the pulse voltage in the half cycle
of the commercial frequency is in one and the same direction. However, Japanese unexamined
patent publication No. 36786/1976 discloses an improved technique, wherein the pulse
voltage is made in an alternate direction. This prior right invention also aims at
size-reduction of the choking coil, the frequency band for use of which is different
from that of the present invention, hence no improvement can be attained in the operating
efficiency of the low pressure electric discharge tube to be mentioned later.
[0005] Further, Japanese unexamined patent publication No. 115078/1976 discloses a lighting
circuit for a fluorescent lamp having a capacitive current limiting impedance composed
of a serial connection of a capacitor 1 and a choking coil 2 as shown in Figure l(b),
wherein a switching device 4 is provided in parallel with a lamp 3 to effect short-circuiting
of the switching device once every half cycle at the trailing part (those hatch-lined
portions in Figure l(c)) of the lamp current I
- in a sinusoidal waveform of a commercial frequency. This disclosed art is, however,
to facilitate restrike of the electric discharge lamp by increasing a charging voltage
V
c of the capacitor 1 at the time of the restriking.
[0006] U.S.P. 3789266, which is the closest prior art to the present invention, discloses
improvement in efficiency of the abovementioned electric discharge lamp, wherein a
high frequency interrupted current having a conduction period T
1 and a breaking period (hereinafter called "pause-time period") T
0, and the current direction of which reverses at every changing of the conduction
period and the pause-time period. A device for flowing electric current such as mentioned
above is limited to a circuit shown in Figure 2(b). This circuit is constructed with
a bridge circuit, in which transistors 5, 6, 7 and 8 are arranged on four sides and
an electric discharge lamp 9 is connected across the diagonal line; another transistor
10 provided in series with the input side of the bridge circuit; and a control device
11 which performs controls of opening and closing of the transistors 5, 6, 7, 8, and
10 to thereby cause electric current to flow as shown in Figure 2(a).
[0007] In such device, however, the voltage to be applied to the transistors 5, 6, 7 and
8 is in a rectangular waveform, at a high voltage portion of which the pause-time
period TO is formed by the transistor 10 with the consequent disadvantages such that
the capacity of the device should essentially be made larger, and that the radio noise
is also high. As the results of various studies and experiments made on the operating
of the low pressure mercury-vapor electric discharge lamp such as fluorescent lamp
with a high frequency voltage having the pause-time period as disclosed in Japanese
unexamined patent publication No. 196497/1982 and Japanese patent application No.
110369/1981,-the present inventors have discovered that the lamp efficiency can be
further improved from the values as shown in the above-discussed U.S.P. 3789266.
[0008] It is therefore an object of the present invention to provide a lighting circuit
having much higher utility than those lighting circuit disclosed in the above-described
published applications filed by the present inventors.
[0009] It is another object of the present invention to provide a lighting circuit for an
electric discharge lamp which has improved the abovementioned various disadvantages
inherent in the conventional device, wherein use is made of a high frequency inverter
to energize a low pressure electric discharge lamp, the inverter having a characteristic
such that its output voltage take a substantially sinusoidal waveform. In such high
frequency inverter, a pause-time period TO is formed at least at a rising part of
its sinusoidal output voltage where an instantaneous value is small, and the electric
power is supplied to the abovementioned low pressure electric discharge lamp at a
portion where the instantaneous value of the abovementioned output voltage is large,
thereby increasing efficiency of the abovementioned low pressure electric discharge
lamp, and improving the radio noise with the lighting circuit of a relatively small
capacity.
[0010] According to the present invention, in one aspect of it, there is provided a lighting
circuit for an electric discharge lamp, which comprises: a high frequency inverter
having a characteristic of rendering its output voltage to be in a substantially sinusoidal
waveform and for energizing a low pressure electric discharge lamp; a switching device
provided at an output terminal of said high frequency inverter; and a control device
for said switching device, said control device stopping its output to said low pressure
electric discharge lamp at the time of its operating at a rising part at every half
cycle of said output voltage and supplying the output to said low pressure electric
discharge lamp in the vicinity of the maximum instantaneous value at said half cycle.
[0011] According to the present invention, in another aspect of it, there is provided a
high frequency lighting circuit, which comprises: an inverter having a leakage type
output transformer and generating in said output transformer a high frequency output
voltage in a substantially sinusoidal waveform; a high pressure cable way provided
at the secondary side of said output transformer and with which a low pressure electric
discharge lamp is connected; a low pressure cable way provided at the secondary side
of said output transformer and with which a switching device is connected; and a conctrol
device which renders said switching device conductive at the time of operating of
said low pressure electric discharge lamp at a rising part of said high frequency
output voltage of every half cycle thereof, and interrupts said switching device in
the vicinity of the maximum instantaneous value of said high frequency output voltage.
[0012] According to the present invention, in still another aspect of it, there is provided
a lighting circuit for an electric discharge lamp, which comprises: an inverter which
functions to convert a direct current voltage to a high frequency output voltage in
a substantially sinusoidal waveform and operates the low pressure electric discharge
lamp with reactive current limiting impedance; a switching device provided at an output
side of said inverter to supply discharge current to said low pressure electric discharge
lamp at the time of interruption thereof and a control device which detects an output
current of said inverter and instantaneous value of the output current.
[0013] According to the present invention, in yet another aspect of it, there is provided
a lighting circuit for an electric discharge lamp, which comprises: a high frequency
inverter which functions to generate an output voltage in a substantially sinusoidal
waveform and with which the low pressure electric discharge lamp across output terminals
thereof; a switching device which is opened to supply output current to said low pressure
electric discharge lamp in the vicinity of the maximum instantaneous value of the
output current at every half cycle of said inverter; and a control device to open
and close said switching device, characterized in that said control device renders
a voltage analogous to a voltage across the terminals of said low pressure electric
discharge lamp to be an input signal thereto, and controls to open and close said
switching device by comparing the input signal with a set value.
[0014] According to the present invention, in other aspect of it, there is provided a lighting
circuit for an electric discharge lamp, which comprises: an inverter which functions
to convert a direct current voltage into a high frequency voltage in a substantially
sinusoidal waveform and to operate the low pressure electric discharge lamp with a
current limiting impedance of inductive reactance; a switching device provided at
an output side of said inverter to supply discharge current to said electric discharge
lamp at the time of its interruption; and a control device which interrupts said switching
device during a period including therein a peak value or its vicinity of an instantaneous
value of every half cycle of the output current from said inverter at the time of
operating of said electric discharge lamp, characterized in that there is further
provided at the output side of said inverter a surge absorbing circuit which absorbs
a surge voltage to be generated at the time of interruption of said switching device,
and that the charging operation of said surge absorbing circuit is set at a time constant
which terminates at substantially 3 µS or shorter at every half cycle of the high
frequency voltage.
[0015] According to the present invention, in still other aspect of it, there is provided
a lighting circuit for an electric discharge device, which comprises: an inverter
which functions to convert a direct current voltage to a high frequency output voltage
in a substantially sinusoidal waveform and operates the low pressure electric discharge
lamp by means of reactive current limiting impedance; a switching device provided
at the output side of said inverter to supply discharge current to said electric discharge
lamp at the time of interruption thereof; and a control device which interrupts said
switching device during a period including therein a peak value or its vicinity of
an instantaneous value at every half cycle of the output current of said inverter
at the time of operating of said electric discharge lamp, characterized in that length
of the interruption period of said switching device is made variable so that variations
in the power of said electric discharge lamp at every half cycle may be smaller than
variations in the peak value of the instantaneous value at every half cycle of the
output current from said inverter.
[0016] According to the present invention, in yet other aspect of it, there is provided
a lighting circuit for an electric discharge lamp, which comprises: an inverter which
functions to convert a direct current voltage to a high frequency output voltage in
a substantially sinusoidal waveform and operates the low pressure electric discharge
lamp by means of reactive current limiting impedance; a switching device provided
at an output side of said inverter and supplying discharge current to said electric
discharge lamp at the time of interruption thereof; and a control device which interrupts
said switching device during a period including a peak value and its vicinity of an
instantaneous value at every half cycle of the output current from said inverter at
the time of operating of said electric discharge lamp, characterized in that length
of the interruption period of said switching device is maintained substantially constant
during a normal operating time.
[0017] According to the present invention, in further aspect of it, there is provided a
lighting circuit for an electric discharge lamp, which comprises: an inverter which
functions to convert a direct current voltage to a high frequency output voltage in
a substantially sinusoidal waveform and operates the low pressure electric discharge
lamp by means of reactive current limiting impedance; a switching device provided
at the output side of said inverter and supplying discharge current to the electric
discharge lamp at the time of interruption thereof; a control device which interrupts
said switching device during a period including therein a peak value and its vicinity
of an instantaneous value at every half cycle of the output current from said inverter
at the time of operating of the electric discharge lamp; and detection means to detect
no discharge or asymmetrical discharge from the electric discharge lamp, characterized
in that said switching device is so maintained conductive for at least a certain predetermined
time in accordance with detection by said detection means.
[0018] The foregoing objects, other objects as well as specific constructions, functions,
and operating principle as of the lighting circuit for an electric discharge lamp
according to the present invention will become more apparent understandable from the
following detailed description of preferred embodiments thereof, when read in conjunction
with the accompanying drawing.
[0019] In the accompanying drawing:
Figures l(a), l(b) and l(c) are explanatory diagrams of a conventional device;
Figures 2(a) and 2(b) are explanatory diagrams of another conventional device and
its circuit construction;
Figure 3 is a circuit diagram showing the first embodiment of the lighting circuit
according to the present invention;
Figure 4 is a diagram of the main part of the circuit shown in Figure 3;
Figures 5(a), 5(b), 5(c), 5(d) and 5(e), and Figures 6(a), 6(b), 6(c), 6(d) and 6(e)
are respectively explanatory diagrams of the lighting circuit shown in Figure 3;
Figure 7 is a circuit diagram showing the second embodiment of the present invention;
Figure 8 is a diagram showing the main part of the circuit shown in Figure 7;
Figure 9 is a diagram showing the third embodiment of the circuit according to the
present invention;
Figure 10 is a diagram showing a main part of the fourth embodiment of the circuit
according to the present invention;
Figure 11 illustrates waveform diagrams for explaining the fifth embodiment of the
circuit according to the present invention;
Figure 12 is a diagram showing a main part of the sixth embodiment of the circuit
according to the present invention
Figure 13 illustrates waveform diagrams for explaining the circuit shown in Figure
12;
Figure 14 is an explanatory diagram of the seventh embodiment of the circuit according
to the present invention;
Figure 15 is a diagram showing the eighth embodiment of the circuit according to the
present invention;
Figure 16 is an explanatory diagram for the circuit shown in Figure 15;
Figure 17 is a diagram showing the ninth embodiment of the circuit according to the
present invention;
Figure 18 is a diagram showing the tenth embodiment of the circuit according to the
present invention
Figure 19 is a diagram showing the eleventh embodiment of the circuit according to
the present invention;
Figure 20 is a diagram of the main part of the circuit shown in Figure 19;
Figure 21 is an explanatory diagram for the device shown in Figures 19 and 20;
Figures 22(a), 22(b), 22(c), and 22(d) are waveform diagrams for explaining necessity
for the twelfth embodiment of the circuit according to the present invention;
Figure 23 is a diagram showing the twelfth embodiment of the circuit according to
the present invention;
Figure 24 is a diagram showing the main part of the circuit shown in Figure 23;
Figures 25(a), 25(b), 25(c), and 25(d) are waveform diagrams for explaining the thirteenth
embodiment of the circuit according to the present invention;
Figires 26(a), 26(b), and 26(c) are diagrams for explaining operations of the fourteenth
embodiment of the circuit according to the present invention for its necessity in
relation to the first embodiment thereof;
Figures 27 and 28 are the circuit diagrams for the fourteenth embodiment of the circuit
according to the present invention;
Figures 29 and 30 are respectively the diagrams showing the fifteenth and sixteenth
embodiments of the circuit according to the present invention;
Figures 31(a), 31(b) and 31(c) are diagrams for explaining the operations of the sixteenth
embodiment of the circuit according to the present invention;
Figures 32(a), 32(b), 32(c), 32(d), and 32(e) are the diagrams for explaining the
operations of the seventeenth embodiment of the circuit according to the present invention
for its necessity in relation to the twelfth embodiment thereof;
Figure 33 is a diagram of the seventeenth embodiment of the lighting circuit for an
electric discharge lamp according to the present invention;
Figure 34 is a diagram showing the eighteenth embodiment of the lighting circuit according
to the present invention;
Figure 35 is a diagram showing a control device for the lighting circuit for the electric
discharge lamp according to the nineteenth embodiment of the present invention;
Figures 36(a), 36(b), and 36(c) are the diagrams for explaining the operations of
the lighting circuit for the electric discharge device according to the nineteenth
embodiment of the present invention;
Figure 37 is a diagram of the twentieth embodiment of the lighting circuit according
to the present invention;
Figures 38(a), 38(b), 38(c), 38(d), 38(e), and 38(f) are operating waveform diagrams
of the lighting circuit according to the twentieth embodiment of the present invention;
Figure 39 is a diagram showing the twenty-first embodiment of the lighting circuit
according to the present invention;
Figure 40 is a diagram for a control device relative to the twenty-first embodiment
of the lighting circuit according to the present invention; and
Figure 41 is a diagram for explaining the operation of the circuit according to the
twenty-first embodiment of the present invention.
[0020] In the following, the present invention will be described in detail with reference
to preferred embodiments thereof shown in the accompanying drawing.
[0021] Referring first of Figure 3 showing a circuit diagram of the lighting circuit for
an electric discharge lamp according to the first embodiment of the present invention,
a reference numeral 12 designates a commercial alternating current power source, a
numeral 13 refers to a rectifying device for the full-wave rectification of the power
source 12, a numeral 14 refers to a smoothing capacitor, and a reference numeral 15
denotes a high frequency inverter to energize a fluorescent lamp 16 as a low pressure
electric discharge lamp. In this embodiment, there is used a self-excited, constant
current type push-pull transistor inverter.
[0022] The inverter 15 is constructed as mentioned in the following: a high frequency choking
coil 17 provided at the input terminal of the inverter 15; an output transformer 18;
the primary windings 18a, 18b, at the connetion of which the high frequency choking
coil 17 is connected; a feedback winding 18c; a secondary winding 18s; pre-heating
windings 18f, 18f to preheat those preheating type electrodes 16f, 16f of a lamp 16;
a power source winding 18d of a control device 19 to be described later; a resonating
capacitor 20 connected in parallel with the primary windings 18a, 18b; a pair of transistors
21a, 21b as the active components connected between the primary windings 18a, 18b
and the negative terminal of the capacitor 14; a pair of base resistors 22a, 22b;
and a choking coil 23 which functions as a current limiting impedance to the electric
current flowing through the lamp 16. A reference letter A designates a switching device
provided in parallel with the lamp 16 at the output terminal of the inverter 15, and
is constructed with a full-wave rectification circuit 24, the alternating current
terminal of which is connected in parallel with the lamp 16, and a transistor 25 disposed
at the direct current terminal of this rectification circuit 24.
[0023] Figure 4 is a circuit diagram showing one embodiment of the control device 19 for
the transistor 24. In the drawing, a reference numeral 18d designates a power source
winding provided in the transformer 18, a numeral 26 refers to a diode bridge which
performs the full-wave rectification of a high frequency of a low voltage induced
in the winding 18d, a reference numeral 27 represents a smoothing capacitor connected
with the output terminal of the diode bridge through a back-flow preventing diode
28, and a reference numeral 29 denotes a transistor connected in parallel with the
capacitor through a resistor 30, which is also disposed between the base and the emitter
of the transistor 25. Incidentally, a reference numeral 31 designates a constant voltage
diode connected with the base of the transistor 29 through a resistor 32.
[0024] In the lighting circuit of such construction as mentioned above, when a voltage is
applied to it from the power source 12, a smoothed direct current formed by the rectification
device rectifier 13 and the capacitor 14 is introduced as an input into the inverter
15, whereby the transistors 21a, 21b are opened and closed alternately by the actions
of the primary windings 18a, 18b, the resonating capacitor 20, the feedback winding
18c, and so forth, and the inverter 15 starts its self-oscillation. In this case,
the collector current of the transistors 21a, 21b is rendered to be in a substantially
rectangular waveform by the action of the high frequency choking coil 17, whereby
the voltage in the primary windings 18a, 18b assumes a substantially sinusoidal waveform.
As the result of this, there is generated in the power source winding 18d a high frequency
voltage of, for example, 20 kHz, in a substantially sinusoidal waveform, as shown
in Figure 5(a). This high frequency voltage is subjected to the full-wave rectification
by the diode bridge 26, from which a voltage as shown in Figure 5(b) is applied to
a constant voltage diode 31, the capacitor 27 is charged, and a smoothed direct current
is applied to a serial circuit of the resistor 30 and the transistor 29. Assume now
that the constant voltage diode 31 is interrupted in the hatch-lined portion and becomes
conductive in the white portion, as shown in Figure 5(b). A voltage across the collector
and the emitter of the transistor 29 takes a shape as shown in Figure 5(c), while
the transistor 25 becomes conductive at the trailing part T
01 and the rising part T
02 of the output voltage in the secondary winding 18s in a substantially sinusoidal
waveform (in general, a high harmonic component is superposed in it to some extent)
as shown in Figure 5(d) to thereby form the pause-time period T
0, and it is interrupted during a period T
1 in the vicinity of the maximum instantaneous value of the output voltage, whereby
a voltage as shown by a hatch-lined portion in Figure 5(d) is applied to the lamp
16.
[0025] On the other hand, the electrode 16f is preheated by a voltage in the sinusoidal
waveform which has been induced in the preheating winding 18f, and, as soon as the
electrode 16f is heated to a predetermined temperature level, the lamp 16 is lit.
In this case, the voltage to be applied to the lamp 16 (i.e., the voltage in the hatch-lined
portion in Figure 5(d)) lowers for a portion of a voltage drop in the choking coil
23, although it hardly changes during the time periods of T
1, T
01' T
02' and TO. The reason for this is that a starting voltage for the lamp 16 at its high
frequency operating is in general higher than in the case of the commercial frequency
operating, and the voltage for operating the lamp is low, on account of which the
inverter 15 has a constant current characteristic at the output side, and the output
current of the inverter 15 assumes a substantially continuous sinusoidal waveform
at the time of both conduction and interruption of the transistor 25. The output current
is in substantially the same waveform as that shown in Figure 5(d), the blank portion
indicating a short-circuit current flowing in the switching device A, and the hatch-lined
portion indicating a lamp current flowing in the lamp 16.
[0026] In the conventional circuit shown in Figure 2(b), and those circuit shown in the
afore-described Japanese unexamined patent publication No. 196497/1982 and Japanese
patent application No. 110369/1981, the output voltage as shown in Figure 2(a) is
only applied to the lamp 9, etc. through the current limiting impedance, so that no
lamp current as shown in Figure 2(a) cannot be obtained unless the current limiting
impedance is a resistor (even in this case, it is difficult to put this circuit construction
into practice so far as a complicated control circuit is added to it, since the power
loss is great). More specifically, in the case of the inductive impedance, the lamp
current takes a triangular waveform with gentle rising, while, in the case of the
capacitive impedance, the lamp current takes a triangular waveform with gentle trailing,
both cases not being able to afford sufficient lamp efficiency, and the efficiency
being particularly low in the former case. This is due to the fact that the improvement
in the lamp efficiency by the provision of the pause-time period TO owes very much
to the effect such that the electron density at a high temperature level becomes higher
than at the time of direct current operating and commercial frequency operating by
causing a current with a steep rising part to flow in the lamp which has been cooled
during the pause-time period T
0.
[0027] Unlike the conventional device as mentioned above, in the circuit construction of
this embodiment of the present invention, wherein the switching device A is provided
in parallel with the lamp 16, even if the constant current characteristic at the output
side of the inverter 15, for example, is not so perfect as mentioned in the foregoing,
there can be obtained fair waveforms with steep rising part as shown by the hatch-lined
portions in Figure 5(d) for both voltage and current of the lamp 16 by the counter-electromotive
force of the current limiting impedance 23 due to the short-circuit current, irrespective
of whether the current limiting impedance 23 is resistance, inductance, or capacitance,
whereby the operating efficiency of the lamp 16 improves remarkably.
[0028] Further, the output voltage from the bridge type inverter shown in Figure 2(b) is
in a rectangular waveform V
A as shown in the right half of Figure 5(d), in contrast to which the output voltage
from the inverter 15 is in a sinusoidal waveform as designated by V
s in Figure 5(d). In comparison with the rectangular waveform of the former, since
the sinusoidal waveform of the latter has its pause-time period TO formed at a relatively
small portion of the instantaneous voltage value, its output capacity can be smaller
than the former.
[0029] The transistors 10 and 25 both perform their respective switching operations at a
substantially same voltage and with a substantially same current, hence the switching
loss may be substantially equal between both transistors. However, in contrast to
that the transistors 5, 6, 7 and 8 perform their switching operations at a high voltage
and with a current in the rectangular waveform, the collector current of the transistors
21a, 21b is in a rectangular half waveform as shown in Figure 6(a), but their voltage
betwen the collector and the emitter is in a sinusoidal half waveform as shown in
Figure 6(b), so that their switching loss is theoretically non-existent. Accordingly,
the overall efficiency of the lighting circuit as a whole remarkably improves along
with improvement in the operating efficiency of the lamp 16.
[0030] Further, in the bridge type inverter, the output voltage, the output current, and
the collector current and the collector-emitter voltage of the transistors 5, 6, 7
and 8 are all in the rectangular waveform. In contrast to this, in the inverter 15
of the present invention, only the collector current of the transistors 21a, 21b is
in the rectangular waveform, while the output voltage, the output current, and the
collector-emitter voltage of the transistors 21a, 21b are all in the sinusoidal waveform
with the consequence that the lighting circuit of the present invention has a lower
radio noise than that in the conventional device.
[0031] The reason for the collector current of the transistors 21a, 21b taking the rectangular
waveform as mentioned above is as follows. It is now assumed that the output current
from the inverter 15 is in the sinusoidal waveform as shown in Figure 6(c), in which
the hatch-lined portion denotes the current flowing in the lamp 16, and the blank
portion indicates the short-circuit current produced by the switching device A. If
the high frequency choking coil 17 is not present, the output powers produced during
the periods of T
01 and
T02 for the abovementioned short-circuit current are almost reactive powers, except for
the preheating power for the electrode 16f in the inverter 15, with the consequence
that the collector current in any one of the transistors 21a, 21b is small during
the periods T
81 and T
02 as shown in Figure 6(d) and is large during the period T
l. The passage of a constant base current relative to such remarkably changing collector
current not only increases the switching loss in the transistors 21a, 21b, when they
are conductive, but also renders the operations of the inverter 15 instable. However,
by the provision of the high frequency choking coil 17 having an appropriate inductance,
the collector current is smoothed and takes a rectangular waveform as shown in Figure
6(e). Therefore, by stably operating the inverter 15 by means of a simple base drive
circuit composed of the feed-back winding 18c and the base resistors 22a, 22b, the
operating efficiency of the inverter 15 can also be improved. The abovementioned smoothing
operation may not be perfect as depicted in Figure 6(e). Incidentally, the choking
coil 17 has an effect of eliminating the high harmonic component to occur in the collector
current. While such function may take place in a separately excited inverter, it is
particularly effective in the self-excited inverter.
[0032] When a leakage type transformer is used as the output transformer 18, the power source
winding 18d had better be provided to the side of the primary windings 18a, 18b.
[0033] Figure 7 is a circuit diagram showing the second embodiment of the lighting circuit
according to the present invention in which a reference numeral 33 designates a smoothing
direct current power source same as that shown in Figure 3, and a numeral 15 refers
to a self-excited, constant current type push-pull transistor inverter also same as
that shown in Figure 3 with exception of using a capacitor 23 as the current limiting
impedance. A reference letter A designates a switching device provided in series with
the lamp at the output terminal of the inverter 15. This switching device A is constructed
with the full-wave rectification circuit 24 with its a.c. terminal being serially
connected with the lamp 16, and the transistor 25 provided at the d.c. terminal of
this full-wave rectification circuit 24. A numeral 19 refers to the control device
for the switching device, the details of which are shown in Figure 8. The control
device 19 is constructed mostly same as that shown in Figure 4, with the exception
that a signal reversing circuit comprising a serial connection of the resistor 34
and the transistor 35 is provided at the rear stage of the serial circuit composed
of the transistor 29 and the resistor 30. By the way, in Figure 7, the electrode 16f
and the preheating winding 18f are omitted from illustration.
[0034] In the glow starter circuit of the above-described construction, when the power source
33 is closed, the transistor 29 generates the signal as shown in Figure 5(c) by the
same operations as has been explained with reference to Figure 4. Accordingly, the
transistor 35 generates a signal, in which the periods of its conduction and interruption
are reversed from those in Figure 5(c) with the result that the transistor 25 is interrupted
during the period T
0 and conducted during the period T
1, whereby a voltage as shown in the hatch-lined portion of Figure 5(d) is applied
to the lamp 16, as is the case with the first embodiment of the lighting circuit shown
in Figure 3. Since, after starting of the lamp, the current limiting impedance is
the capacitor 23, both voltage and current having steep rising part can be obtained
for starting the lamp 16, whereby its operating efficiency increases.
[0035] In this second embodiment, too, the pause-time period T
0 is formed with the periods T
01 and T
02, during which the instantaneous value of the ouput voltage in the sinusoidal waveform
is small, the operating efficiency of the lamp 16 is seen to be improved with the
current limiting impedance of a capacity smaller than that shown in Figure 2.
[0036] Also, since the switching conditions of the transistors 21a, 21b are the same as
that of Figure 3, the switching loss of the transistor is substantially nil.
[0037] In view of the fact that the output current from the inverter 15' is as shown by
the hatch-lined portion in Figure 5(d), the radio noise increases more than that shown
in Figure 3, but it is less than that shown in Figure 2.
[0038] Incidentally, the load applied to the inverter 15 during the pause-time period T
0 is only the preheating load of the electrode 16f, hence the effectiveness of the
high frequency choking coil 17 as has been explained with reference to Figure 6 is
equally applicable to this
second embodiment.
[0039] In this embodiment, the variations in the load applied to the inverter during the
pause-time period T
0 and the period T
l for supplying power to the lamp 16 are greater than the load variations in the first
embodiment as shown in Figure 3, more stable operations can readily be obtained with
the inverter 15 of the separately excited type.
[0040] By the way, the capacitor 23 may be provided between the rectification circuit 24
and the lamp 16 to obtain the same resulting effect.
[0041] Figure 9 is a circuit diagram showing the third embodiment of the lighting circuit
according to the present invention, in which the same reference numerals as those
in the previous figures of drawing designate the identical or corresponding parts.
The characteristic feature of this third embodiment resides in that the switching
device A is connected to the output terminal of the inverter 15 through the electrodes
16f, 16f in parallel with the lamp 16. Incidentally, the control device 19 is the
same as that shown in Figure 4, using the power source winding 18d as the power source.
[0042] The thus constructed lighting circuit operates in the substantially same manner as
that shown in Figure 3, with the exception that current flows through the electrodes
16f, 16f during the pause-time period TO at the time of starting and lighting of the
electric discharge lamp. Such device can also be operated in the same manner as that
shown in Figure 3 without provision of the preheating winding 18f.
[0043] In each of the above-described three embodiments of the lighting circuit for an electric
discharge lamp, the inverter 15 is constructed with the constant current type push-pull
transistor inverter, but it may be replaced by a serial type transistor inverter as
used in the fourth embodiment shown in Figure 10. This serial type transistor inverter
15 comprises a pair of transistors 36a, 36b and another pair of resonating capacitors
37a, 37b, these pairs of transistors and capacitors constructing the four sides of
a bridge circuit, and a resonating choking coil 38 and an output transformer 18, both
being connected in series and disposed at the diagonal line in the bridge circuit.
To the secondary winding 18s of the transformer 18, there are connected the switching
device A, the control device 19, and the lamp 16 in any one of the arrangements shown
in Figures 3, 7, and 9.
[0044] In the device of such construction, when the transistors 36a, 36b are alternately
opened and closed in the base drive circuit 39 such as, for example, an integrated
circuit (IC) for a switching regulator, there flows in the primary winding 18e a substantially
sinusoidal vibrating current with its direction being reversed alternately, whereby
a substantially sinusoidal output voltage is obtained in the secondary winding 18s.
Consequently, the operating efficiency of the lamp 16 can be increased with the inverter
15 of a small capacity as is the case with the above-described embodiments. The radio
noise is also low, since at least the output voltage and the collector current are
in the sinusoidal waveform.
[0045] It should be noted that the abovementioned effect can be obtained with any type of
the lighting circuit of a construction, in which the power supply to the lamp 16 is
interrupted at least at the rising part of the voltage in the sinusoidal waveform
for its half cycle, and the power supply to the lamp 16 is done in the vicinity of
the maximum instantaneous value in the abovementioned half cycle.
[0046] Further, while the collector-emitter voltage in the transistors 36a, 36b is in the
rectangular half waveform, its collector current is in the sinusoidal half waveform.
In this case, too, the switching loss is theoretically nil. Furthermore, when at least
any one of the voltage and the current in the active elements of the inverter 19 is
in the sinusoidal waveform, the effect as mentioned above can be obtained with other
inverter 15.
[0047] Although, in the above-described embodiments, the input into the inverter 15 is the
smoothed direct current, those devices having the smoothing capacitor 14 incorporated
therein is low in the power factor. Therefore, in the ordinary high frequency operation,
there is a practice of using a pulsating voltage obtained by full-wave rectification
of the a.c. voltage from the power source 12 as the input voltage for the inverter.
Figure 11 shows the output voltage and the output current of the inverter in that
case, in which the voltage is an alternating current voltage containing beats therein.
However, if the frequency of the inverter is assumed to be, for example, 25 kHz, there
exists in the half wave of 50 kHz a high frequency voltage of 250 cycles, whereby
the output voltage is in the substantially sinusoidal waveform, when taken in a short
period of time.
[0048] While such lighting circuit reduces its lamp efficiency to some degree on account
of the lamp current becoming quiescent during a time period TO starting from the zero
volt condition in the power source 12. However, when the fifth embodiment of the present
invention is applied to such lighting circuit, the operating efficiency of the lamp
16 can be increased to a considerable degree, hence its power factor can be made high.
[0049] With a view to eliminating the current pause-time period T
0 as mentioned above, it has usually been a practice in the high frequency operation
to provide an auxiliary power source, with which the output voltage from the inverter
can be obtained even at the zero voltage level in the power source 12. Figure 12 illustrates
the circuit construction for one example of such auxiliary power source. The auxiliary
power source 44 as illustrated is constructed with a step-down transformer 40, a full-wave
rectification circuit 41 to perform the full-wave rectification on the output voltage,
a capacitor 42 connected to the d.c. terminal of the rectification circuit, and a
diode 43. By the way, both terminals of the capacitor 42 are connected with the input
terminal of the high frequency inverter 15 through the diode 43.
[0050] In the thus constructed auxiliary power source, when the instantaneous value of the
pulsating voltage which has been subjected to the full-wave rectification by the rectification
device 13 becomes lower than the charged voltage of the capacitor 42, the input voltage
of the inverter 15 is supplied from the capacitor 42, and the output voltage and the
output current from the inverter 15 are as shown in Figure 13, wherein the current
pause-time period TO is abscent, with the consequence that the lamp efficiency improves.
When the present invention is applied to such construction, there can be obtained
various effects as mentioned above, and the lighting circuit with high power factor
and a extremely high general efficiency. This is the sixth embodiment of the lighting
circuit according to the present invention.
[0051] In the above-described embodiments of the present invention, the switching device
A is constructed with a combination of the rectification circuit 24 and the transistor
25. It should however be noted that the same effect can also be obtained by use of
other switching elements such as a turn-off thyrister, etc..
[0052] Although the control device 19 changes its characteristics by the kind of the switching
element used for the switching device A, there may be contemplated various kinds of
control device such as, for example, the one using a combination of a comparator IC
and the drive circuit of the switching element, the one using clock pulses, the one
using an integrated circuit (IC) for the switching regulator, or various others.
[0053] For example, when the control device using the clock pulses is employed as the control
device 19, it become possible to carry out the power supply to the lamp 16 for twice
or more of the time periods T11 and T
12 in the half cycle of the high frequency output voltage. Even with such control device,
the operating efficiency of the lamp 16 can be improved, as shown in Figure 14 which
is the seventh embodiment of the lighting circuit of the present invention.
[0054] In the preceding description, no particular mention has been made as to the frequency
of the inverter 15. However, by the provision of the pause-time period T
0 as disclosed in detail in Japanese patent application No. 110369/1981, the improvement
in the resulting lamp efficiency is recognized from a frequency of 1 kHz or its vicinity,
and, even at the frequency of 80 kHz, considerable improvement could still be obtained.
However, from the standpoint of preventing disagreeable audible noises, the frequency
of about 17 kHz and above is preferable. Further, when a bipolar type transistor is
used for the transistor 25, the frequency of 100 kHz or below is preferable for reducing
the switching loss.
[0055] In the above-described embodiments, the lamp 16 used is single, although the same
effect can be resulted, even when two or more serially connected lamps 16 are used.
[0056] Further, in the above-described embodiments, the low pressure electric discharge
lamp used is the fluorescent lamp 16. However, the improvement in the lamp efficiency
due to provision of the pause-time period TO could be recognized in other types of
the rare gas electric discharge lamp such as a neon lamp 16, a krypton lamp 16, etc.,
hence the lighting circuit of the present invention can be equally applied to these
low pressure electric discharge lamps 16.
[0057] Figure 15 is a circuit diagram showing the eighth embodiment of the lighting circuit
according to the present invention. In the drawing, those reference numerals same
as those in Figure 3 designate the identical or corresponding parts. In this embodiment,
unlike the device shown in Figure 3, the output transformer for the inverter 15 is
constructed with a leakage type transformer 18, and an auxiliary winding 18R wound
in subtractive polarity at its secondary side is connected with the secondary winding
18S to form a low pressure cable way E. To this low pressure cable way E, there is
connected the switching device A same as that shown in Figure 3. On the other hand,
the secondary winding 18S forms a high pressure cable way F, to which the fluorescent
lamp 16 is connected. By the way, the control device 19 in this eighth embodiment
of the present invention is exactly same as that of Figure 4, with the exception that
the power source winding 18d thereof is wound at the primary side. It should be noted
also that the preheating circuit for the electrodes 16f, 16f in the lamp 16 is omitted
from the illustration.
[0058] In the lighting circuit of the construction as described above, when the power source
11 is closed, the inverter 15 commences its oscillation in the same manner as that
in Figure 3, and the control device 19 introduces into the transistor 25 an input
signal same as that shown in Figure 5(c). As the result of this, the transistor 25
becomes conductive during the period TO. However, since the transformer 18 is of the
leakage type, the voltage applied to the lamp 16 also assumes substantially zero volt.
On the other hand, in the time period T
1, the transistor 25 is interrupted and a voltage in the vicinity of the maximum instantaneous
value of the winding 18S is applied to the lamp 16, whereby it is lit. in this case,
if the number of winding turns of the windings 18S and 18R is set n
S and n
R, respectively, and a no-load peak voltage of the winding 18S is represented by V
SO, there is applied to the transistor 25 a voltage V
SO. n
S - n
R. After the operation, the lamp 16 is
n S kept lighting with a voltage as shown in the hatch-lined portion in Figure 5(d),
and the same effect as that of Figure 3 can be obtained.
[0059] In this case, it should be noted that a diode of low voltage withstand and high speed
response can be used for the transistor 25 and the rectification circuit 24, hence
it becomes possible not only to construct the device with high reliablity and at a
reduced manufacturing cost, but also to further increase the general efficiency of
the device.
[0060] However, in the above-described construction of the circuit, since the windings 18S
and 18R are wound in the subtractive polarity, the electric current I
s at the time of conduction of the transistor 25 becomes greater than the lamp current
I
L as shown in Figure 16 with the consequence that there take place problems such that
not only a switching element of a large current capacity need be used as the switching
device A, but also the power loss thereof becomes great. Figure 17 is a circuit diagram
showing the ninth embodiment of the lighting circuit according to the present invention,
in which the abovementioned point is improved. In Figure 17, the control device 19,
etc. are omitted from the illustration. In this embodiment, the choking coil 33 as
the current limiting impedance is added in series with the switching device A in the
low pressure cable way shown in Figure 15.
[0061] In the circuit of such construction, the current IS at the time of conduction of
the switching device A can be reduced to thereby improve the abovementioned problem.
However, when the impedance value of the choking coil 33 is made too large, the voltage
to be applied to the lamp 16 at the time of conduction of the switching device A becomes
large. When this voltage value becomes higher than a discharge maintaining voltage
at the time of restriking of the lamp 16, the lamp commences its discharge before
the switching device A is interrupted, and the rising in the voltage and the current
for the lamp 16 are no longer steep, thereby hindering improvement in the lamp efficiency.
[0062] Further, in the lighting circuit, wherein the inverter 15 is of the self-excited
type, as in the above-described embodiments, if a difference between the current IS
and the current I
L is too large, the oscillation of the inverter tends to become instable. The choking
coil 33 has the effect of stabilizing the oscillation by reducing the current IS.
[0063] Figure 18 is a circuit diagram showing the tenth embodiment of the lighting circuit
according to the present invention. This embodiment performs the same operations as
that shown in Figure 15 and attains the same effect, even if both low pressure cable
way E and high pressure cable way F are individually provided at the secondary side
of the transformer 18. In this case, the polarity of the windings 18S and 18R has
no bearing on the operation of the transformer 18.
[0064] Figure 19 is a diagram showing the eleventh embodiment of the lighting circuit according
to the present invention, in which a tap T is provided at the intermediate point of
the secondary winding 18S to form the low pressure cable way E. A reference numeral
46 designates a current transformer provided in the high -pressure cable way F, the
signal of which is input into the control device 19.
[0065] Figure 20 is a circuit diagram showing details of the control device 19 for the eleventh
embodiment, in which a starting auxiliary means C to be explained hereinbelow is added
to the circuit shown in Figure 4. In the drawing, a reference numeral 47 designates
a transistor connected in parallel with the capacitor 27 through the resistor 48,
a numeral 49 refers to a transistor arranged in parallel with the transistor 29, a
numeral 50 refers to a diode bridge which performs the full-wave rectification of
the output signal from a current transformer 46, a reference numeral 51 denotes a
smoothing capacitor, a numeral 52 indicates a base resistor of the transistor 47,
and a reference numeral 53 designates a diode interposed between the collector of
the transistor 49 and the base of the transistor 25. A capacitor 54 and a resistor
55 are connected in series between the positive polarity of the capacitor 27 and the
base of the transistor 25 to thereby form a time constant circuit. By the way, in
this case, the power source winding 18d of the control device 19 and the preheating
winding 18f of the electrode 16f (not shown) is provided at the primary side of the
transformer 18.
[0066] In the device of such construction, when the power source 11 is closed, the base
current flows in the transistor 25 through the abovementioned time constant circuit.
On the other hand, since no signal has yet been generated in the current transformer
46, the transistor 47 is in an interrupted condition, hence there is no possibility
of current flowing into the transistor 49 from the time constant circuit due to presence
of the diode 53, even if the transistor is in a conductive state. Further, while the
transistor 29 performs the same operations as that shown in Figure 4, its signal does
not flow into the transistor 49 to be input into the transistor 25.
[0067] That is to say, during the initial period of from to to t
1 at the start of the lamp 16 shown in Figure 21, the electrode 16f is preheated by
the winding 18f. However, since the switching device A continues its conductive state,
substantially no voltage is applied to the lamp 16, hence it is not operateed.
[0068] After lapse of a predetermined time instant t
1, when the capacitor 54 is sufficiently charged and the base current of the transistor
25 is rendered substantially zero, the transistor 25 is brought to an interrupted
state. However, since no signal is generated in the current transformer 46, the transistor
49 maintains its conductive state and the transistor 25 also maintains its interrupted
state during a period of from t
1 to t
21 on account of which a no-load voltage of the secondary winding 18S is applied, as
it is, to the lamp 16. The electrode 16f is sufficiently preheated during a period
of from t
0 to t
1, and still continues its preheating even during a period of from t
1 to t
2. Therefore, a time interval is required more or less for the lamp 16 to shift from
its glow discharge to its arc discharge, although this time period of from t
1 to t
2 is a relatively short time interval.
[0069] When the lamp 16 starts at a time instant t
2, a signal is generated in the current transformer 46, and the transistor 47 becomes
conductive. On account of this, the transistor 49 is interrupted and the signal generated
in the transistor 29 is input into the transistor 25. As the result of this, the lamp
16 is operated with a voltage having its pause-time period of T
0 and its voltage applying period of T
1.
[0070] As mentioned in the foregoing, by making the conduction period of the switching device
A at the initial stage of the lamp starting longer than the conduction period at the
time of operating of the lamp to sufficiently preheat the electrode 16f without starting
the lamp 16, and then by making the interruption period of the switching device A
longer than the interruption period at the time of the operating of the lamp 16, it
becomes possible not only to start the lamp 16 without shortening the service life
of the lamp, but also to set the secondary no-load voltage of the transformer 18 to
be low, whereby the capacity of the lighting circuit can be made much smaller and
the loss in the device can be further reduced.
[0071] Incidentally, when the transistor 47 becomes conductive with a signal to be generated
in the current transformer 46 when the lamp 16 is in its glow discharge condition
during a period of from t
1 to t
2, there is a possibility such that the lamp 16 remain in its glow discharge condition,
or, if not remaining in this glow discharge condition, a time is taken for the lamp
to shift from the glow discharge to the arc discharge, thereby shortening the service
life of the lamp. In order to avoid such awkward situation to take place, it is preferable
that an element such as, for example, a constant voltage diode, etc. which does not
operate with a signal at the time of the glow discharge, but operate with a signal
at the time of the arc discharge be provided in the base circuit of the transistor
47.
[0072] In the above-described embodiment of the present invention, the switching device
A is constructed with a combination of the rectification circuit 24 and the transistor
25, although the same resulting effect can be obtained with those switching devices
using other switching elements such as a field-effect transistor 25, and so on. Further,
the control device 19 varies its function by the switching element used, and there
are contemplated various kinds of such switching elements other than those used in
the above-described embodiments.
[0073] Furthermore, in the above-described embodiment, the inverter 15 is a self-excited,
constant current type push-pull transistor inverter. Besides this, there may also
be used a serial inverter 15, for example, provided that the leakage type transformer
18 can be used as the output transformer, in which a substantially sinusoidal output
voltage can be obtained.
[0074] Moreover, in the above-described embodiments, a smoothed d.c. voltage is used for
the power source 11. However, there may also be used a pulsating d.c. voltage obtained
by the full-wave rectification of an a.c. voltage and a pulsating d.c. voltage obtained
by supplying a voltage from the auxiliary power source in the vicinity of the zero
volt.
[0075] In the following, the twelfth embodiment of the lighting circuit according to the
present invention will be explained. This embodiment is concerned with further improvement
in the afore-described first embodiment. By the way, the following fact has become
evident as the result of detailed studies and researches on the operation of the device
according to the first embodiment of the present invention.
[0076] Figure 22(a) indicates an output voltage V
DB of the diode bridge 26 of the control device 19 and a Zener voltage V
z of the constant voltage diode 31 of the same. Figure 22(b) shows an interrupted period
T
1a of the transistor 25 in the switching device. Figure 22(c) shows an output current
from the inverter 15. Due to presence of the choking coil 23, the output current from
the inverter has its phase delayed from the output voltage from the inverter 15, i.e.,
the output voltage V
DB from the diode bridge 26. This output voltage V
DB is clipped by the constant voltage diode 31 to form the period T
1. However, since the output voltage from the inverter 15, i.e., the output voltage
from the diode bridge 26 is at a high frequency level, if the switching speed of the
transistor 29, the transistor 25, and so forth is not so high, the interrupted period
T
1a of the transistor 25 is delayed by td from the conduction period of the constant
voltage diode 31. However, since the output current from the inverter 15 has also
its phase delayed by e
l from the power source winding 18d, there flows in the lamp 16 the output current
from the inverter 15 in the vicinity of its maximum instantaneous value as shown by
the hatch-lined portion in Figure 22(c). In such a device, however, when a phase difference
between the output current from the inverter 15 and the voltage of the power source
winding 18d is very large, or when a high speed component is used for the transistors
25, 29, and so on in the control device 19 and the switching device A with a delay
time being different from a predetermined value, there takes place such an apprehension
that no current can be supplied to the lamp 16 with a desired phase. It has therefore
been discovered that, in such case, there flows in the lamp 16 a current.portion of
a low instantaneous value in the output current, on account of which a capacity of
the device becomes inevitably large for supplying a predetermined power to the lamp
16, and the operating efficiency of the device decreases due to flow of current in
the vicinity of the maximum instantaneous value of the output current through the
transistor 25.
[0077] With the abovementioned situation in mind, there has been devised the twelfth embodiment
as shown in Figure 23, which serves to supply appropriate electric current to the
lamp, even when the phase difference between the output current and the output voltage
from the inverter is great, by detection of the output current from the inverter and
by on-off controls of the switching device by this signal.
[0078] Figure 23 is the circuit diagram showing the twelfth embodiment of the present invention,
wherein the same reference numerals as those in Figure 3 designate the identical or
equivalent parts. Further, Figure 24 illustrates one embodiment of the control device
19 for use in the device according to the twelfth embodiment of the present invention.
[0079] In Figure 23, a reference numeral 33 designates a current transformer which detects
the output current from the inverter 15 and inputs the current into the control device
19. In Figure 24, a numeral 33 refers to the same current transformer as mentioned
above, a reference numeral 34 designates an output resistor for the current transformer
33, 35 a full-wave rectifier to rectify the output from the current transformer 33,
31 a constant voltage diode, and 36 a d.c. power source for driving the device, which
can be constructed by, for example, rectifying and smoothing an output from the auxiliary
winding provided in the transformer 18 of the inverter 15. This circuit construction
is substantially same as that shown in Figure 4 with the only differences in that
the input signal for the constant voltage diode 31 is derived from the full-wave rectification
of the output from the current transformer 31, and that a signal reversing circuit
consisting of a transistor 37 and a resistor 38 is added. Moreover, the graphical
representation in Figure 22(d) indicates the output voltage from the current transformer
33, the output having a substantially same phase as, and analogous waveform to, those
of the output current from the inverter 15, as a matter of course.
[0080] In the device of a construction as described above, the current transformer 33 does
not produce an output voltage before the lamp 16 starts its electric discharge, and
the transistor 25 maintains its interrupted conditions, on account of which the output
voltage from the inverter 15 is applied to the lamp 16 as it is to facilitate commencement
of its discharge. In the next place, when the lamp 16 starts its electric discharge,
the current transformer 33 generates an output voltage. At this instant, the transistor
29 becomes conductive during the period T
1a including the maximum instantaneous value of the output current from the inverter
15 by means of the constant voltage diode 31 as shown in Figure 22(d), to thereby
interrupt the transistor 25. As the consequence of this, the discharge current flows
through the lamp 16 during this period T
la as shown by the hatch-lined portion in Figure 22(c).
[0081] In this manner, when a current in the vicinity of the maximum instantaneous value
of the output current from the inverter 15 is made to flow in the lamp 16, the capacity
of the device can be made smaller than in the case wherein such current does not flow,
and the operating efficiency of the device increases.
[0082] In the following, the thirteenth embodiment of the lighting circuit according to
the present invention will be explained. In the twelfth embodiment as shown in Figure
23, the explanations have been given as to a case, wherein ripples are less in the
input d.c. voltage for the inverter 15. In this embodiment, however, explanations
will be made as to applications to those cases where a pulsating d.c. voltage containing
more ripples in the input d.c. voltage is used, i.e., a pulse current obtained by
simply rectifying the commercial a.c. power source as shown in Figure 25(a) is used;
or where an auxiliary d.c. voltage having a low peak is superposed on the commercial
a.c. power source as shown in Figure 25(c). In such instances, the current flowing
in the lamp 16 takes its waveform as shown in Figures 15(b) and 25(d) when no switching
device A is provided. Here, it is assumed that, in the control device 19 same as that
shown in Figure 22, a level for detecting the output voltage from the current transformer
33 by means of the constant voltage diode 31 is set at a predetermined value A
L as shown in Figures 25(b) and 25(d). Then, at a portion where the peak value is higher
than the predetermined value A
L, the control device performs the same operation as has been explained with reference
to Figure 22, but, at a portion where the peak value is lower than the predetermined
value A
L, the switching device A maintains its interrupted condition. By constructing the
control device as such, i.e., by providing the pause-time period for only a period
where the maximum instantaneous value of the lamp current is greater than the predetermined
value A., and by flowing a current having no pause-time period for a period where
the instantaneous value of the lamp currrent is low, it is possible to further improve
the operating efficiency of the lamp 16.
[0083] In the foregoing, the explanations have been given as to an example of using the
current transformer 33 for the control device 19. However, the other expedients such
as, for example, one which detects the current by use of resistors, etc. may be used.
Further, the constant voltage diode 31 is used for detection of the instantaneous
value of the output current, which can also be replaced by a comparator IC, or the
like for obtaining the same effect. Furthermore, in this embodiment, the switching
device A is constructed with combination of the rectifying circuit 24 and the transistor
25, which can also be replaced by a field-effect transistor or other switching elements
for obtaining the same effect.
[0084] The inverter 15 may be such one as, for example, a serial inverter, etc. provided
that a substantially sinusoidal output voltage can be obtained at the output terminal
thereof. Also, the current limiting impedance 23 to set the lamp current at a predetermined
value may not be inductance of the inductive reactance, but a capacitor of capacitive
reactance. Further, in the foregoing, explanations have been given as to a case, wherein
the choking coil is used at the output terminal of the inverter 15, although the transformer
18 of the inverter 15 may be constructed as the leakage transformer.
[0085] Various arrangements of the switching device A are possible other than that in the
embodiment. For instance, an additional winding in the opposite poilarity as that
of the secondary winding 18S of the transformer 18 is provided, through which the
switching device A is connected; or when the transformer 18 is the leakage type transformer,
an intermediate
'tap is provided in the secondary winding and the switching device A is connected with
a low pressure cable way to be formed in this intermediate tap; or it may be feasible
that an impedance is connected in series with the switching device A to reduce the
current flowing through the switching device A. Furthermore, the switching device
A is connected in parallel with the lamp 16 through the electrodes 16f, 16f thereof,
and the preheating current is caused to flow at the time of conduction of the switching
device A. Moreover, it may be feasible that, at the start of the lamp 16, the switching
device A be maintained without operating the same for a certain period of time for
stabilizing it even after commencement of the electric discharge.
[0086] In the following, the fourteenth embodiment of the present invention will be described.
This embodiment is a furtehr improvement in the first embodiment.
[0087] Incidentally, in the device, wherein the inverter 15 varies its output voltage in
substantial correspondence to variations in the input d.c. voltage thereof as the
device of the first embodiment shown in Figure 3, the voltage in the control winding
18d also varies in accordance with the input d.c. voltage of the inverter. Accordingly,
when the input d.c. voltage of the inverter 15 is of a voltage waveform having large
ripples, i.e., if a difference between the maximum value (E
max) and the minimum value (E . ) of the input d.c. voltage as in the example shown in
Figure 24(a), the voltage variations in the control winding 18d is remarkable (E
min /E
max < 0.8 or so), hence the output signal from the control device 19 to be generated with
the voltage of this control winding 18d as the input signal for it also varies. On
account of this, the pause-time period T
0 varies greatly to possibly cause inconveniences in carrying out stable control of
the device as well as in improving efficiency of the circuit. With this in mind, therefore,
the circuit in this fourteenth embodiment is so constructed that the stable control
of the circuit can be effected with a voltage obtained by use of this type of inverter
as the input signal for the control device, which does not vary so remarkably even
when the ripples in the input d.c. voltage become fairly large.
[0088] Figure 27 illustrates the fourteenth embodiment of the lighting circuit according
to the present invention, and Figure 28 shows a concrete embodiment of the control
device therefor. It is to be noted that explanations will be made with reference to
Figure 27 only for those parts which are different from those in the circuit of the
Figure 3 embodiment.
[0089] A reference numeral 14 designates an auxiliary d.c. power source having a peak value
lower than the peak value of the output voltage from the smoothing capacitor or the
rectifying circuit 13. The output transformer 18 contains therein the current limiting
impedance constructed with a leakage type transformer. To the switching device A,
is connected an impedance 26 (in this embodiment, a choking coil) in series. This
choking coil 26 is set at such an inductance value that no current may flow in the
lamp 16 during a period when the switching device is in a conductive state.
[0090] In Figure 28, a reference numeral 18d represents a control winding; a numeral 28
refers to a resistor; 29 a constant voltage diode; 30 a transistor; 31 a resistor;
and 32 a control d.c. power source, which can also be obtained by rectifying and smoothing
an output from the control winding provided at the primary side of the output transformer
18.
[0091] In the device as constructed in the abovementioned manner, it is assumed that the
input d.c. voltage for the inverter 15 is as shown in Figure 26(a). As is the case
with the circuit of the Figure 3 embodiment,
the inverter 15 carries out the self-oscillation to generate a high frequency voltage,
thereby operating the lamp 16. Here, the output transformer 18 is the leakage type
transformer, wherein the control winding 18d wound around the magnetic circuit at
the secondary side of this transformer generates a voltage analogous to the voltage
from the secondary winding 18s, i.e., a voltage analogous to the voltage appearing
across the terminals of the lamp 16. In the illustrated circuit, the impedance 26
functions to generate in the control
winding 18d a voltage above the minimum required level when the switching device A
becomes conductive.
[0092] Now, with variations in the input d.c. voltage for the inverter 15, the output current
from the inverter varies as shown in Figure 26(b). However, since the lamp voltage
does not change so remarkably even if the lamp current values change, it does not
change so remarkably as shown in Figure 26(c). Accordingly, the voltage in the control
winding 18d does not change so remarkably, whereby the constant voltage diode 29 of
the control device 19 causes electric current to flow for a substantially same period
of time at every half cycle of the high frequency voltage to render the transistor
30 conductive. On account of this, even if the input d.c. voltage for the inverter
15 varies, the transistor 25 of the switching device A is brought to its conductive
state for a substantially constant period TO as shown by the hatch-line in Figure
5(b). In this way, it is possible to provide an appropriate pause-time period.
[0093] Figure 29 illustrates the fifteenth embodiment of the lighting circuit according
to the present invention, in which the control device 19 is further provided with
resistors 35, 37, a constant voltage diode 33, a capacitor 34, and a transistor 36.
Before start of the electric discharge in the lamp 16, the transistor 36 is rendered
and maintained in a conductive state in utilization of the phenomenon that the voltage
in the secondary winding 18s and the control winding 18d is higher during this period
than at the time of operating of the lamp, thereby keeping the switching device in
an interrupted state and facilitataing start of the lamp.
[0094] In the above explanations, a choking coil is used as the impedance 26, although it
goes without saying that a capacitor may also be used for the purpose. From the standpoint
of obtaining a quick rising of the current to be supplied to the lamp 16, this latter
component is preferred. In the case of using the choking coil, it may be connected
to the output side of the full-wave rectifying circuit.
[0095] In the foregoing explanations, the impedance is connected in series with the switching
device A to thereby generate a required voltage in the control winding 18d even when
the switching device is in a conductive state. When no impedance is connected, the
winding provided in the magnetic circuit at the secondary side does not produce a
voltage in the leakage transformer during conduction of the switching device. The
following is an embodiment of the circuit which is applicable to such case.
[0096] Figure 30 shows the sixteenth embodiment of the lighting circuit according to the
present invention, wherein the construction is the same as that shown in Figure 25
with the exception of the control device 19 (also no impedance 26 is provided). The
point of difference in this embodiment from that shown in Figure 26 is that the capacitor
38 is connected with the output terminal of the control device 19.
[0097] In the following, operations of the circuit in this embodiment will be explained.
Figures 31(a), 31(b) and 31(c) are diagrams for explaining the operations of the circuit
according to the sixteenth embodiment of the present invention, wherein the solid
line in Figure 31(a) indicates an output current from the secondary winding 18s of
the inverter, and a hatch-lined portion denotes the current flowing in the lamp 16;
the solid line in Figure 31(b) indicates an output voltage from the full-wave rectifying
circuit 27 of the control device; and Figure 31(c) shows a voltage to be applied across
the base and the emitter of the transistor 25.
[0098] During the operating of the lamp, the output voltage from the control winding 18d
lowers, and when it goes down below V
z in Figure 31(b), the transistor 30 is brought to an interrupted state, while the
transistor 25 is rendered conductive to stop the power supply to the lamp. However,
after a predetermined time to be set by a time constant of the resistor 31 and the
capacitor 38 (a period of T
0 in Figure 31(b)), the transistor 25 returns to its interrupted state and the current
begins to flow again in the lamp. An output voltage from the full-wave rectifying
circuit 27 at this time is represented by V . Then, a signal as shown in Figure 31(c)
is applied to the transistor 25. In the embodimental device, the relationship between
V
x and V
z can be arbitrarily established as: V > V
z, V
x - V , and V < V
z. by appropriate selection of the pause-time period T
0. The method for generating this pause-time period T
0 may be any one, other than that in the above-described embodiment, such as use of
an appropriate timer, use of a monostable multi-vibrator, and others.
[0099] It is further possible that the lighting circuit according to the sixteenth embodiment
shown in Figure 30 be used in combination with a device as shown in Figure 29 for
not generating the pause-time period at the time of starting the lamp.
[0100] It is also useful that the switching device is connected in parallel with the lamp
through its filament, the conduction period T
0 of the switching device is extended (or the interruption period T
1 is omitted) at the time of starting the lamp so as to sufficiently preheat the filament,
thereafter the conduction period TO is shortened (or T
0 may be omitted) to facilitate starting of the lamp discharge, and, after operating
of the lamp, the conduction period T
0 and the interruption period T
1 be set at their initial values.
[0101] In the foregoing explanations, use has been made of a voltage from the control winding
wound at the secondary side of the leakage type output transformer as an input signal
into the control device. However, when a voltage which is substantially analogous
to the voltage across the lamp terminals is used, the intended purpose can be achieved.
Therefore, it is feasible to connect a signal generating transformer in parallel with
the lamp so that a voltage from the winding provided on this transformer may be used
as the input signal for the control device, in which case the device with the impedance
23 being connected therewith may also be used. Next, when a phase difference exists
between the input signal and the voltage across the lamp terminals, it may suffice
that this phase difference be compensated and the switching device be subjected to
the on-off controls. This can also be realized, in the case of using the leakage transformer
according to this embodiment, as by appropriate adjustment of the winding position
of the control winding.
[0102] For the inverer 15, the self-excited, push-pull inverter is suited. Besides this,
any type of inverter, which is capable of stopping the power supply to the lamp at
least at the rising part of a substantially sinusoidal output current at every half
cycle thereof, and of performing the power supply to the lamp in the vicinity of the
maximum instantaneous value thereof. The output transformer may not necessarily be
the leakage type transformer.
[0103] For the auxiliary d.c. power source 14, there may be used a low d.c. voltage to be
obtained by use of a transformer, etc., or such voltage generated from voltage dividing
by the serial connection of a plurality of capacitors, and by other expedients. In
short, the d.c. voltage may contain therein the ripples, if only it is able to maintain
the lamp discharge.
[0104] In each of the above-described embodiments, the switching device A used is constructed
with the rectifying circuit 24 and the transistor 25. However, this switching device
may also be constructed with other switching elements, etc. having a required characteristic.
Furthermore, other connection decvice may be adopted, if the power supply stoppage
period to the lamp can be provided.
[0105] In the following, the fifteenth embodiment of the present invention will be described.
This embodiment is a further improvement of the afore-described twelfth embodiment.
[0106] In the afore-described twelfth embodiment, the lamp 16 is operateed by the circuit
construction shown in Figure 23; however, when the electric discharge becomes difficult
due to the service life of the lamp reaching its end, or no regular discharge can
be done in any longer due to progress in consumption of one if the electrodes to bring
about the asymmetrical discharge, etc., wherein the discharge is effected with only
one of the polarities, there inevitably occurs the phenomenon to be mentioned in the
following. That is to say, in case the switching device A is conductive during a period
including the phase 80 in Figure 5(c) and this conductive state is interrupted at
the phase θ
1, there will be no problem at all so far as the current flows through the lamp 16.
However, when no current flows in the lamp 16 for some reason, the choking coil 23
as the current limiting impedance is abruptly interrupted from its current flow to
generate a high pressure voltage due to the counter-electromotive force, which is
applied to the switching device A. On account of this, there is apprehension such
that a large stress is applied to the component parts constituting the switching device
to lower reliability of the device. This is also true with the case wherein the output
transformer 18 is constructed as the leakage transformer, and no choking coil 23 is
used.
[0107] In this embodiment, therefore, attempt is made as to improving reliability of the
switching device by providing a surge absorbing circuit having an appropriate response
time without impairment being caused to the lamp.. operation.
[0108] First of all, prior to the explanations of the fifteenth embodiment of the lighting
circuit according to the present invention, the basic principle of the present invention
will be explained.
[0109] The rising part of the current and voltage in the lamp 16 (a time instant t
1 or its vicinity shown in Figures 32(d) and 32(e)), when the lamp is operated with
the lighting circuit according to the twelfth embodiment shown in Figure 23, can be
shown in an enlarged waveform in these figures of drawing. When the neighboring area
of the time instant t
1 is observed in detail, it is seen that a current increase exists in the lamp current,
as shown by a broken line in Figure 32(d). This current increase varies in accordance
with magnitude of impedance in the choking coil 23. Also, the lamp voltage at its
rising part t
1 is at a lower value V
I than a value V
2 which can be anticipated from the locus of the original inverter output voltage,
as shown in Figure 32(e), and it becomes substantially coincident with the locus of
the original output voltage after the time instant t
2. A time required for this time period between t
1 and t
2 is approximately 2 µS (more accurately, longer than 1.5 µ S but not reaching 3 µ
S) with a fluorescent lamp of 40W capacity, for example. This phenomenon may be inferred
due to the current flowing in the vicinity of the tube wall of the lamp at the restriking
thereof for every half cycle, though the detailed reasons therefor is yet to be clarified.
[0110] The lighting circuit in this fifteenth embodiment of the present invention purports
to effectively utilize the voltage dropping phenomenon to occur at the rising part
of the lamp voltage as mentioned above, thereby reducing the voltage to be applied
to the switching device. In the following, the embodiment will be explained in reference
to the drawing.
[0111] Referring to Figure 33, a reference numeral 37 designates a surge absorbing circuit,
a numeral 38 refers to a diode, 39 and 40 refer to resistors, and 41 a capacitor.
The remaining construction of the device according to this embodiment are the same
as that shown in Figure 23, hence the corresponding parts are designated by the same
reference numerals and the explanations for them are dispensed with.
[0112] In the lighting circuit for the electric discharge lamp of the abovementioned construction,
the surge absorbing circuit 37, in its normal operation, performs its charging operation
to some extent at the rising part t
1 of the voltage at every half cycle of the lamp operation, although the main charging
operation thereby is set to be in a constant which terminates within 3 µS. Accordingly,
irrespective of presence of the surge absorbing circuit 37, the lamp 16 indicates
its lamp voltage at a substantiall equal level to that when no surge absorbing circuit
is provided.
[0113] In the following, explanations will be made as to a case when the lamp 16 is not
in a position to perform its normal discharging operation. If it is now assumed that
the lamp 16 is discharging from only one of the electrdoes 16f, 16f. In this case,
the lamp operation is not different during its half cycle in the normal polarity,
but, at the subsequent half cycle, the lamp 16 does not discharge, hence no current
flows therein, at an instant when the switching device A is interrupted (corresponding
to tl in Figure 32(e)), whereby a high voltage tends to be applied to the switching
device A. At this instant, a charging current flows in the surge absorbing circuit
37 to restrain this high voltage. While it is possible to contemplate various other
construction for the surge absorbing circuit 37, it should contain therein at least
a capacitor, a resistor serially connected with it, another resistor connected in
parallel with it, and a diode. In this manner, the application of the high voltage
to the switching device A can be prevented by means of the surge absorbing circuit.
[0114] In the case of the output transformer being the leakage type transformer, the surge
absorbing circuit 37 may be constructed as in the above-described embodiment with
respect to the secondary winding 18S; besides this, the circuit may be connected with
the secondary winding through a middle point as shown in Figure 34, or it may be connected
with another winding of the secondary winding which is furtehr provided at the secondary
side.
[0115] Further, the connection of the surge absorbing circuit 37 in parallel with the switching
device A as in the fifteenth embodiment shown in Figure 33.is effective not only in
the case of connecting the inductive impedance in series with the switching device
A (the device construction as shown in Figure 23), but also in the case of further
connecting an auxiliary choking coil, etc. in parallel with the lamp and in series
with the switching device A.
[0116] Besides the device shown in this embodiment, the inverter may be of such a construction
that it is able to generate a substantially sinusoidal output and to supply a high
frequency power having a pause-time period to the lamp, and that the main impedance
for limiting the lamp current in the inverter is constructed with the inductive reactance.
Moreover, the input d.c. voltage to the inverter may not necessarily be one which
has been rectified and smoothed by the smoothing capacitor as in the foregoing embodiments,
but it may be those such as pulsating current obtained without provision of the smoothing
capacitor 14 or its equivalent component, or one obtained by using an appropriate
auxiliary d.c. power source at this portion for the smoothing capacitor.
[0117] Furthermore, in the above-described fifteenth embodiment of the present invention,
there has been indicated use of the current transformer 33 as the method for setting
the pause-time period, but the invention may of course be applicable to the use of
other expedient for realizing the pause-time period.
[0118] The switching device A may utilize various switching elements such as, for example,
a field-effect transistor, etc.. The method for connecting the switching device A
may be of variety when the output transformer is the leakage type transformer, though
any type of the connecting method is possible, provided that a desired high frequency
power can be supplied. It is further feasible to combine it with an expedient for
properly controlling the switching device A and also performing starting and preheating
operations of the lamp.
[0119] In the following, explanations will be given as to the nineteenth embodiment of the
present invention in relation to the twelfth embodiment shown in Figure 23. Before
explaining the nineteenth embodiment, the operations of the lighting circuit according
to the twelfth embodiment will be explained in further details.
[0120] The circuit of this twelfth embodiment has such an advantage that the instantaneous
value A
1 of the lamp current when the current begins to flow in the lamp 16 remains to be
a constant value irrespective of variations in the power source voltage, etc., althoughn,
on the other hand, the circuit is supposed to have an inconvenience to be mentioned
as follows. That is to say, when it is considered that the input d.c. voltage of the
inverter 15 contains many ripples, for example, when the voltage as shown in Figures
25(a) and 25(c) is generated in the inverter 15, the peak value of the lamp current
is also high during a period wherein the peak value of the output voltage is high,
and the period T
la (refer to Figure 22) during which the current flows through the lamp 16 becomes also
long. On account of this, when the a.c. power source 12 increases, the power consumption
of the lamp 16 increases much higher than the power source to thereby deteriorate
the so-called "power source voltage variation characteristic"; and when the input
d.c. voltage of the inverter 15 contains many ripples, even if the a.c. power source
does not vary, the power consumption in the lamp at every half cycle of the high frequency
inevitably varies to a large extent, and some other problems.
[0121] Under such circumstances, there has further been contemplated the lighting circuit
as shown in Figure 35 paying attention to the abovementioned point.
[0122] Figure 35 illustrates the control device 19 for the lighting circuit for the electric
discharge lamp as the nineteenth embodiment of the present invention, the control
device being applicable to the lighting circuit such as, for example, shown in Figure
23. The control device as shown in Figure 35 is constructed with the current transformer
33, the resistor 34, the full-wave rectifying circuit 35, resistors 44, 45 for detecting
and dividing voltage of the inverter output current at every half cycle, the diode
39, the capacitor 40, the resistor 41, the constant voltage diode 42, the resistor
43, the voltage comparator 46, the resistor 47, the auxiliary d.c. power source for
driving 36, and the transistor 25 for the switching device A. Incidentally, the terminal
voltage of the capacitor 40 assumes a voltage analogous to an envelope of the peak
value of the output current from the inverter 15 or to the input d.c. voltage into
the inverter 15.
[0123] In the following, explanations will be given as to the operations of the control
device 19 of the above-described construction, when it is used for the lighting circuit
for the electric discharge lamp as shown in Figure 21. Assume now that the inverter
15 starts its operation, and the lamp 16 is operated. Then, there is applied to the
input terminal B of the voltage comparator 46 a varying voltage of the peak value
envelope of the output from the inverter as shown in Figure 36(a) by the signal produced
in the current transformer 33. Also, there is applied to the input terminal A of the
voltage comparator 46 a voltage analogous to the high frequency output current as
shown by a broken line in Figure 36(a). In this way, the voltage comparator 46 has
its output transistor rendered conductive during a period of the voltage at the input
terminal A becoming higher than the voltage at the input terminal B thereof, i.e.,
during the periods of Dl and D
2 as shown in Figure 36(b), and the output terminal C assumes a low voltage level (as
shown in Figure 36(c)). Accordingly, the transistor 25 becomes non-conductive during
the periods Dl and D
2, and the current flows to the side of the lamp 16. Here, as is apparent from the
state of the voltage at the terminal B, it is possible to prevent the period, during
which the current flows through the lamp 16, from extending, even when the peak value
of the output current from the inverter is large in comparison with a case wherein
the peak is small, i.e., a relationship of D
1 « D
2. Further, the period D
l during which the peak value is small and the period D
2 during which the peak value is large can be appropriately set by selection of a voltage
dividing ratio of the resistors 44, 45 and a zener voltage in the constant voltage
diode 42.
[0124] In the above-described embodiment, the control of the device is effected in correspondence
to the peak value of the output current from the inverter. It may howeve be feasible
to effect the control in accordance with the input voltage for the inverter 15 by
such means that, for example, a high frequency component is eliminated from the output
voltage in the winding provided on the transformer 18 for the inverter 15, and the
output voltage is rectified and applied to the input terminal B of the voltage comparator
46. It is also feasible that, in the state of the peak value of the output current
from the inverter being lower than a predetermined value, as, for example, in the
period during which the peak value is lower than the current value A
L in Figures 25(b) and 25(d), the lamp current be so set that no pause-time period
be provided therein.
[0125] In the foregoing explanations, use of the current transformer 33 in the control device
19 has been taken as an example, although other expedient may of course, be adopted,
such as, for example, detection of current by use of a resistor, etc.. Furthermore,
a period during which the current is supplied to the lamp is set by use of the voltage
comparator 46, which may also be carried out by other expedients. Moreover, in the
above-described embodiment, the switching device A is a combination of the rectifying
circuit 24 and the transistor 25, although the same effect can be obtained by use
of the field-effect transistor, and other switching elements.
[0126] The inverter 15 may be of any type that is able to obtain a substantially sinusoidal
output voltage at its output terminal, such as, for example, a serial inverter or
a bridge type inverter provided with an output transformer. The current limiting impedance
23 for setting the lamp currrent at a predetermined value may not only be the inductance
of the inductive reactance, but also the capacitance of the capacitive reactance.
[0127] In the above explanations, use of the choking coil 23 at the output terminal of the
inverter 15 is taken as an example. However, the transformer 18 of the inverter 15
may also be constructed as the leakage type transformer.
[0128] The arrangement of the switching device A is possible other than that shown in the
above-described embodiment. That is to say, an additional winding having an opposite
polarity to that of the secondary winding 18S of the transformer 18 is provided, by
way of which the switching device A is connected, or, in the case of the transformer
18 being the leakage type transformer, an intermediate tap is provided on the secondary
winding and the switching device A is connected with a low pressure cable way to be
formed by this intermediate tap. Or, it may also be feasible that an impedance is
connected in series with the switching device A to thereby reduce the current flowing
in the switching device. Furthermore, it may be feasible that the switching device
A is connected in parallel with the lamp 16 through the electrodes 16f, 16f and the
preheating current is caused to flow through it at the time of its conduction. Also,
with a view to stabilizing the switching device even after starting of the electric
discharge, when the lamp 16 is being operated, there may be added an expedient to
maintain the switching device A without its being operated for some length of time.
This can be realized by providing a timer circuit to maintain the output at the output
terminal C of the voltage comparator 46 in the embodiment shown in Figure 35 at a
low output level during a predetermined period after closure of the power source,
or by providing means for detecting the operating of the lamp 16 to control the output
at the abovementioned output terminal C.
[0129] Besides using the rectified and smoothed voltage as the power source for the device
as shown in Figure 1, the input d.c. voltage for the inverter 15 may also be the pulsating
d.c. voltage as shown in Figure 25(a), or the d.c. voltage as shown in Figure 25(c)
which is not perfectly smoothed, but obtained from the circuit constructed in combination
with an appropriate d.c. power source, and so forth.
[0130] In the following, the twentieth embodiment of the lighting circuit according to the
present invention will be described in reference to Figure 37. In this embodiment,
the period for supplying electric current to the lamp is maintained substantially
constant irrespective of magnitude of the output current from the inverter or instantaneous
variations in the input d.c. voltage for the inverter, thereby reducing variations
in the power consumption in the lamp at every half cycle.
[0131] In the following, the twentieth embodiment of the present invention will be explained
in reference to the drawing. In Figure 37, the control device 19 is constructed, in
addition to the full-wave rectifier 35 and the d.c. power source 36, the resistors
39 and 40, a transistor 41 having an output terminal L, monostable multi-vibrators
42, 43, each having an output terminal M and N and generating an output for a predetermined
time period, resistors 44, 45 and 46, capacitors 47 and 48, and a transistor 49, thereby
performing the drive-control of the transistor 25 in the switching device A.
[0132] Figures 38(a) to 38(f) respectively indicate signals corresponding to the output
terminals K to O shown in Figure 37. Figure 38(f) shows the output current from the
inverter 15, in which the hatch-lined portion designates the current flowing in the
lamp-16. Assume now that the inverer 15 generates a high frequency voltage and the
lamp 16 commences the electric discharge. The output current from the inverter 15
flows in either the switching device A or the lamp 16, and voltage resulted from the
full-wave rectification of the output voltage from the current transformer 33 is as
shown in Figure 36(a). During a period when the instantaneous value of this voltage
is low, the transistor 41 is interrupted, and a synchronous signal as shown in Figure
38(b) is obtained at the output terminal L. Here, the monostable multi-vibrators 42,
43 are of the type which is triggered by the trailing part (shown by an arrow ↓ in
the drawing) of the input signal and performs the time limiting operation. Accordingly,
the monostable multi-vibrators 42, 43 perform their predetermined time-limiting operation,
whereby the output voltages as shown in Figures 38(c) and 38(d) are generated at their
respective output terminals M and N. These voltages are reversed by the transistor
49, while the output from the output terminal O becomes as shown in Figure 38(e),
to drive the transistor 25 of the switching device A, whereby the current in the hatch-lined
portion of Figure 38(f) flows through the lamp 16. Since the period of this current
flow is determined by the time-limiting operation of the monostable multi-vibrator
43, it can be maintained at a substantially constant level irrespective of the output
current from the inverter 15.
[0133] Though, in the above-described embodiment, the synchronous signal is generated by
use of the current transformer 33, there may be used any other means which is capable
of operating the switching device A so that the current flowing in the lamp 16 may
include therein the peak value and its vicinity of the output current from the inverter
15, and of being operated for a substantially constant time period. Further, while
the switching device A according to this embodiment is a combination of the rectifying
circuit 24 and the transistor 25, the same effect can be obtained by use of a field-effect
transistor, or other switching elements. Furthermore, the connection of the switching
device A can be effected by other method than the above-described embodiment. For
instance, an additional winding having the opposite polarity to that of the secondary
winding 18S of the transformer is provided, by way of which the switching device A
is connected, or, in the case of the transformer 18 being constructed as the leakage
type transformer without use of the choking coil 23, an intermediate tap is provided
in the secondary winding 18S and the switching device A is connected with a low pressure
cable way to be formed by this intermediate tap, or other winding may be made the
low pressure cable way. Furthermore, it is also feasible to connect impedance in series
with the switching device A so as to reduce the current flowing in the switching device
A. It is moreover feasible that the switching device A is connected in parallel with
the lamp 16 through the electrodes 16t, 16f and the preheating current is caused to
flow at the time of its conduction. Also, with a view to preheating the electrodes
16f, 16f at the start of the lamp 16 and facilitating commencement of the electric
discharge, there may be added an expedient to differentiate the conduction and interruption
operations of the switching device A from those operations at the time of the normal
operating. Besides using the rectified and smoothed power source as in the above-described
embodiment, the input d.c. voltage for the inverter 15 may use a pulsating d.c. voltage
as shown in Figure 25(a), or a d.c. voltage obtained from a circuit constructed in
combination with an appropriate auxiliary power source of low peak value as shown
in Figure 25(c). It is also feasible that, in the case of a voltage contianing therein
many ripples as such, the switching device A is kept in the interrupted state with
the cycle having its peak value lower than a certain current value A
L as shown in Figure 25(d) by detecting the voltage level at the terminal K and controlling
the transistor 49, and that the device of the present invention is operated with the
cycle alone having the peak value higher than the current value A
L. Conversely, when the switching device A is operated only during a period of lower
peak value than the current value A-, the switching device may be of a low voltage
withstand. On the other hand, it may be sufficient that the inverter 15 is of such
a type that generates a substantially sinusoidal output voltage at the output terminal
thereof, and uses the capacitive or inductive reactance as the current limiting impedance
to set the lamp current. As an example, a serial inverter or a bridge type inverter
provided with the output transformer is also useful.
[0134] In the following, explanations will be made as to the twenty-first embodiment of
the lighting circuit according to the present invention in relation to the fourteenth
embodiment of the circuit shown in Figure 25. This embodiment is of such a construction
that, when the lamp does not perform its normal electric dischage, the switching device
connected in parallel with the lamp is conducted and maintained to thereby prevent
application of the surge voltage to the switching device or generation of excessive
inverter current.
[0135] Referring now to Figure 39, the lighting circuit according to the twenty-first embodiment
of the invention will be described. Figure 39 illustrates the construction of the
lighting circuit according to the present embodiment, in which a point of difference
from the fourteenth embodiment in Figure 27 resides in that no choking coil is provided.
Figure 40 shows the construction of the control device 19 for use in the circuit of
Figure 39, which comprises resistors 34, 37, 39, and 42, the constant voltage diode
35, the capacitors 33, 36, the thyrister 38, the diodes 40, 43, and the transistor
41.
[0136] In the above-described construction, when the lamp 16 is operating in its normal
condition, the voltage in the control winding 18d is as shown by a solid line in Figure
41. When the output voltage from the full-wave rectifier 27 becomes higher than a
set voltage V
29 in the constant voltage diode 29, the transistor 30 becomes conductive, and, after
a predetermined time to be decided by the resistor 31 and the capacitor 33, the transistor
25 is interrupted, whereby the output current in the inverter 15 flow through the
lamp 16. Also, when the output voltage from the full-wave rectifier 27 becomes lower
than the set voltage V
29' the transistor 30 is interrupted, the transistor 25 becomes conductive, and the current
does not flow through the lamp 16. On the contrary, when the lamp 16 is in an abnormal
condition such as, for example, no discharging or the asymmetrical discharging due
to the end of its service life, the voltage in the control winding 18d becomes higher
as shown by a dot line in Figure 41 than the voltage during its normal operation (shown
by the solid line); in particular, in its asymmetrical discharging, the voltage increases
from its normal voltage level at either positive or negative polarity in the waveform
as shown in Figure 41. In this way, when the output voltage from the full-wave rectifier
27 becomes higher than a set voltage v
35 in the constant voltage diode 35, the thyrister 38 becomes conductive and the transistor
41 is interrupted. On account of this, the base current continues to flow in the transistor
25 through the resistor 42, and the transister 25 maintains its conductive state,
whereby a high voltage is no longer applied to the lamp 16. As the result of this,
increase in current and voltage due to the asymmetrical discharging and generation
of the high surge voltage at the time of non-lighting of the lamp are prevented. The
capacitor 36 and the resistor 37 function to prevent the thyrister 38 from becoming
conductive at the time of the operating of the lamp 16, either at the initial stage
of its operating or until commencement of its operating.
[0137] Incidentally, in the above-described embodiment, when the thyrister 38 becomes once
conductive, this conductive state is maintained; however, after lapse of a predetermined
time periode using a timer, etc., the switching device A may be reinstated to its
interrupted state. The current to flow during maintenance of the switching device
A in its conductive state may be set at a value which is not very much different from
that during the operating of the lamp by setting the leakage inductance of the output
leakage transformer 18 in the inverter 15; however, it is also feasible to provide
the impedance 26 as has been done heretofore. As the preheating method of the lamp
electrode 16f, it is also useful that the switching device A is connected in parallel
with the lamp 16 through its filament; at the time of operating of the lamp, the conduction
period of the switching device A is extended (or the interruption period T, may be
eliminated) to sufficiently preheat the filament, thereafter, the period TO is made
shorter (or may be eliminated) to facilitate commencement of the electric discharge
in the lamp 16; and after the operating, the periods T
0 and T
1 are reinstated to their original set values. In the foregoing explanation, use is
made of the voltage in the control winding 18d wound at the secondary side of the
leakage type output transformer 18 as the input signal into the control device 19.
This object can be achieved by use of a voltage substantially analogous to the voltage
across the lamp 16: for example, a signal generating transformer is connected in parallel
with the lamp 16, and the voltage in the winding provided on this transformer is used
as the input signal into the control device 19, in which case there may also be used
a construction wherein the impedance 26 is connected. Next, where there is a phase
difference between the input signal and the voltage across the terminals of the lamp
16, this phase difference may be compensated to subject the switching device A to
the open and close controls. This can be realized, in the case of the leakage type
transformer as in this embodiment, by appropriate adjustment of the winding position
of the control winding 18d.
[0138] In this twenty-first embodiment of the present invention, the switching device A
is operated by the voltage in the control winding 18d for both its normal and abnormal
operations. However, it is also feasible that the normal operation is perfomed by,
for example, detecting the current flowing in the inverter 15 or the lamp 16 to provide
an appropriate pause-time period, and, at the abnormal operation, the switching device
A is operated by obtaining a voltage substantially analogous to the voltage across
the terminals of the lamp 16 as in this embodiment. Conversely, it is also feasible
that other means be provided to cause the switching device to perform the operations
in conformity to its normal operations and its abnormal operations by detection of
the current flowing through the lamp 16 or of the output current from the inverter
15.
[0139] For the inverter 15, the self-oscillating push-pull inverter as used in this embodiment
is suitable. Besides this, however, other types of the inverter may be used, which
is capable of stopping the power supply to the lamp 16 at the rising part of a substantially
sinusoidal output current at every half cycle thereof, and of supplying the power
to the lamp at the maximum instantaneous value of the current or in its vicinity.
The output transformer 18 may also not necessarily be of the leakage type. It is of
course possible that, depending on the kind of the current limiting impedance of the
lamp 16, when the impedance 26 connected in series with the switching device A is
to be provided, the transformer may be constructed with a capacitor. From the standpoint
of quicken the trailing of the current to be supplied to the lamp 16, the latter is
preferable. Furthermore, when the choking coil is used as the impedance 26, it may
be connected with the output side of the full-wave rectifying circuit 24.
[0140] For the auxiliary d.c. power source 14 to the inverter 15, there may be used a low
d.c. voltage to be obtained by use of a transformer, etc., besides a well known smoothing
circuit, or a d.c. voltage generated from a divided voltage due to the series connection
of a plurality of capacitors, or other means. In short, the power source may contain
therein the ripples, if only the required electric discharge of the lamp 16 can be
maintained.
[0141] Furthermore, in the above-described embodiment, the switching device A is constructed
with the rectifying circuit 24 and the transistor 25. However, it may be made up of
other switching elements having the required characteristic. The connection of the
switching device A can be done by other methods than the above-described one, provided
that a power supply stoppage period to the lamp 16 can be provided.
[0142] So far the present invention has been described with reference to particular embodiments
thereof, it should be noted that the present invention is not limited to these embodiments
alone, but any changes and modifications may be made by those skilled in the art within
the spirit and scope of the invention as recited in the appended claims.