DISCHARGE LAMP LIGHTING DEVICE

Abstract: The invention relates to a device for operating a fluorescent discharge lamp of the outer electrode type. As claimed in the invention a switching device is turned on and off by driver signals with a stipulated frequency, by which on the secondary side of a transformer the periodic voltage waveform shown at A in Figure 1 is produced. This voltage waveform is applied to the fluorescent discharge lamp of the outer electrode type, and thus operation is effected. For the above described periodic voltage waveform, with respect to repetition period t 2 W o < t, if the width at a voltage of the waveform of 0 V which has a single maximum peak value within one period is labelled W o , its full width at half maximum (the width between a and b in Figure 1) being set to a stipulated value (for example, to a value of less than or equal to 2.5 µsec). This makes it possible to maintain stable emission even if the pressure of the gas filled in the discharge lamp is increased. In this way high illumination intensity can be obtained.

Description: Background of the Invention Field of the Invention The invention relates to a device for operating a fluorescent discharge lamp according to the preamble of claim 1. Such a fluorescent discharge lamp is described in WO 94/23442 A and EP 781 078 A. EP 0593312 A discloses a fluorescent light source having a twin tube and inner filament cathodes at opposite ends. Description of Related Art A fluorescent discharge lamp of the outer electrode type is known as a fluorescent lamp which is used for document scanning illumination of an office automation device and for back light of a liquid crystal display of an office automation device and the like. In the above described fluorescent discharge lamp of the outer electrode type, on the outside of a glass tube there is a pair of line-like or strip-like outer electrodes to which an uninterrupted high frequency voltage or a pulse-like high frequency voltage is applied to operate the lamp. Figure 12 is a schematic of an arrangement of the above described fluorescent discharge lamp of the outer electrode type. Figure 12 (a) shows a cross section of the fluorescent discharge lamp of the outer electrode type which corresponds to the direction perpendicular to the direction of the tube axis. Figure 12 (b) is a side view hereof. As becomes apparent from Figure 12, fluorescent discharge lamp of the outer electrode type 1 consists of discharge vessel 3 which consists of a dielectric such as glass or the like, a pair of strip-like or line-like electrodes 2, 2', and layers of fluorescent material 4 which are formed on the inside of discharge vessel 3. Electrodes 2, 2' are located on the side of discharge vessel 3 in the direction of the tube axis roughly over the entire length and consist of aluminum or the like. Conventionally, above described fluorescent discharge lamp of the outer electrode type 1 has been operated by applying a high frequency voltage to the outer electrodes as in a cold cathode fluorescent discharge lamp of the inner electrode type. That is, high frequency main circuit 5 as shown in Figure 13 is connected to the pair of electrodes 2, 2' of fluorescent discharge lamp of the outer electrode type 1. For example, a waveform high frequency AC voltage according to Figure 14 is applied to electrodes 2, 2'. In this way a high frequency voltage is applied in the discharge space within discharge vessel 3 which is present between outer electrodes 2, 2' via the side discharge vessel 3, forming a discharge. This approach is disclosed in the patent disclosure document of Japanese patent application HEI 3-225745 (US Patent 5, 117, 160). In the above described conventional operation method there is a process with which the illuminance of the fluorescent discharge lamp of the outer electrode type is increased even more. In this process the gas pressure of the rare gas which is filled within discharge vessel 3 is increased. In the above described case of increasing the filling pressure however the current required for discharge is not sufficient if the voltage applied to the fluorescent discharge lamp of the outer electrode type is not increased. In this case a stable discharge cannot be obtained. In the following the shape of the discharge within discharge vessel 3 is detailed in the case of increasing the filling pressure: In this discharge, over the entire region of the lamp a plurality of locations at which emission is concentrated is formed. This plurality of local sites at which the emission is concentrated furthermore changes their positions over time. The emission state in discharge vessel 3 is observed in the form of a strip. Figure 15 schematically shows this strip-like discharge phenomenon. Fluorescent discharge lamp of the outer electrode type 1 shown in Figure 12 can be called a capacitor which consists of outer electrodes 2, 2' and discharge vessel 3 as the dielectric. The lamp current which is supplied to this fluorescent discharge lamp of the outer electrode type 1 is determined by the magnitude of electrostatic capacity which is formed between outer electrodes 2, 2' and discharge vessel 3 which consists of the dielectric. Current must be supplied to increase the illuminance of fluorescent discharge lamp of the outer electrode type 1 even more. This means that the voltage applied to outer electrodes 2, 2' and the high frequency of the voltage must be increased. When the applied voltage was increased however the disadvantages of the danger of formation of creeping discharge on the surface of the dielectric between outer electrodes 2, 2' and the danger of formation of an insulation breakdown in the circuit arose. Summary of the Invention The invention is devised to eliminate the above described disadvantage. Therefore the object of the invention is to devise a device for operating a fluorescent discharge lamp of the outer electrode type in which even when the pressure of the filled gas is increased in the discharge vessel a stable discharge can be maintained and in which at the same time higher illuminance can be obtained. In the conventional operation method in which a sine curve is applied the phenomenon shown above in Figure 15 occurs when the pressure of the rare gas filled within discharge vessel 3 and the voltage applied to discharge lamp 1 are increased, as was described above. Therefore a stable discharge cannot be maintained. As the result of various experiments and tests it has been shown that by operating discharge lamp 1 by applying a periodic voltage waveform with a steep start-up and maximum peak waveform in which the width with respect to repetition period t is less than or equal to a stipulated value, a stable discharge can be maintained even when the pressure of the filled gas increases. This means that it was found that by applying a periodic voltage waveform to discharge lamp 1 in full width at half maximum lies within a stipulated value, even when the pressure of the filled gas increases, a stable discharge can be maintained and the illuminance intensity can be increased, when for a voltage waveform measured at the two ends of the lamp (voltage between P and Q in Figure 1) the width between two points a and b is defined as full width at half maximum. The voltage at two points a and b has a value (H/2 in the Figure) which, proceeding from the position in which a waveform with a maximum peak value of the voltage within the above described one period intersects voltage OV has half the maximum peak value (H in the figure) as is illustrated in Figure 1A. The object is achieved in accordance with the features of claim 1. This makes it possible to maintain a stable discharge even when the pressure of the gas filled in the discharge lamp is increased, and to increase the illuminance more than in the conventional operation method in which the sine curve is applied. (2) In the above described device for operating a discharge operating a discharge lamp, discharge lamp 1 is operated by applying a voltage with a periodic waveform, in which full width at half maximum of a waveform with a maximum peak value at the operating lamp voltage satisfies condition W < Wx, if with respect to the repetition period t of the voltage waveform 2 W o < t, if the width at a voltage of the waveform of 0 V which has a single maximum peak value within one period at the periodic waveform of the lamp voltage is labeled W o , if furthermore the maximum illuminance is labeled L, which in the case of operation of the above described lamp is obtained by a sine curve, if the same lamp wattage as in this case is supplied under the aforementioned conditions, and if the full width at half maximum of a waveform with a maximum peak value at which the above described illuminance L can be obtained is designated Wx. (3) For (1) and (2) full width at half maximum of the waveform with the maximum peak value is fixed in the range of W ≤ 2.5 µ sec. (4) For (1) and (2) period t of the periodic voltage waveform is fixed in the range from 5 µsec to 70 µsec. (5) For (1) and (2) a fluorescent discharge lamp of the outer electrode type is operated in which within the glass tube a gas with a partial pressure of the Xe gas of greater than or equal to 80 torr and a total pressure of the filled gas of less than or equal to 760 torr is filled. (6) For (1) and (2) an oscillation wave which follows the maximum peak voltage is supplied with an effective power which contributes to emission. (7) For (1) and (2) the periodic waveform of the lamp voltage is produced by a circuit of the flyback type. In the invention the arrangement described above in (1) to (7) makes it possible to maintain a stable discharge even when the pressure of the gas filled in the discharge lamp is increased, and to further increase the illuminance more than in the conventional operation method in which the sine curve is applied. In the following the invention is described using several embodiments shown in the drawings. Fig. 1 shows a schematic of one arrangement of a basic circuit of the flyback type of one embodiment of the device as claimed in the invention for operating a discharge lamp; Fig. 2 shows a schematic of an arrangement of a circuit of the flyback type of another embodiment of the operation device as claimed in the invention; Fig. 3 shows a schematic of one arrangement of a MOSFET circuit intrinsically including one diode; Fig. 4 shows a schematic of one arrangement of an experimental circuit of the flyback type which is used in the invention; Fig. 5 shows a schematic of the relation between the full width at half maximum and the illuminance of the discharge lamp (with 8 mm diameter); Fig. 6 shows a schematic of the relation between the full width at half maximum and the illuminance of the discharge lamp (with 6.5 mm diameter); Fig. 7 (a) through Figure 7 (d) each show one schematic of the lamp voltage waveform in operation of the discharge lamp; Fig. 8 shows a schematic of the relation between the lamp wattage and the illuminance with different waveforms; Fig. 9 shows a schematic of the relation between the operation period and the illuminance; Fig. 10 shows a schematic of the relation between the partial pressure of the Xe gas and the relative luminance fluctuation; Fig. 11 shows a schematic of the relation between the mixing ratio of Ne and the illuminance; Fig. 12 (a) shows a schematic cross section of one arrangement of a fluorescent discharge lamp of the outer electrode type as disclosed in US 5117 160 A; and Fig. 12 (b) shows a schematic side view of the arrangement according to Figure 12 (a); Fig. 13 shows a schematic of a circuit of a conventional operation type using a sine curve high frequency of a fluorescent discharge lamp of the outer electrode type; Fig. 14 shows a schematic of a voltage waveform for operation of a conventional fluorescent discharge lamp of the outer electrode type; and Fig. 15 shows a schematic of a pnenomenon of unstable discharge which occurs at a high pressure of the filled gas. Detailed Description of Preferred Embodiments Figure 1 is a schematic of an arrangement of a basic circuit of one embodiment of the device as claimed in the invention for operating fluorescent discharge lamp 1 of the outer electrode type (hereinafter called a discharge lamp). Furthermore, reference number 6 labels a DC source, reference number 7 a driver circuit, reference number 8 a switching device, and reference number 9 a transformer. This figure shows the arrangement of a basic circuit of the fly-back type. Switching device 8 is turned on and off by driver signals with a stipulated frequency which is delivered by driver circuit 7. If switching device 8 is turned on by the above described driver signals, current flows via a line from DC source 6 via the primary winding of transformer 9, switching device 8 to ground G, and energy is stored in transformer 9. When switching device 8 is turned off, the current flowing through transformer 9 is turned off. The above described energy stored in transformer 9 is therefore released. On the primary side and secondary side of transformer 9 this yields the voltage waveform shown at A in Figure 1 with a steep rise. This voltage waveform is attenuated with an attenuation constant which corresponds to the line constant. If switching device 8 is turned on and then turned off successively a voltage waveform with a steep rise is formed again in the above described manner. As was described above, each time switching device 8 is turned on/off with a stipulated frequency by the driver signals output by driver circuit 7, the voltage waveform with a steep rise is formed repeatedly on the secondary side of transformer 9, as is illustrated at A in Figure 1. This voltage waveform is applied to discharge lamp 1. In the above described device for operating a discharge lamp, as was described above, by fixing full width at half maximum of the above described voltage waveform within a stipulated value and by application thereof with the stipulated repetition period t to discharge lamp 1, a stable discharge can be maintained, even if the pressure of the gas filled in discharge lamp 1 is increased. One conceivable reason for this is the following: If a voltage with a short starting time, i.e., a voltage which contains a high percentage of high frequencies, is applied to discharge lamp 1, discharge vessel 3 consisting of glass or the like does not in fact act as a dielectric, and thus an approximation to a state is achieved in which a voltage is applied directly to the gas filled inside. That is, in the discharge lamp which is operated via the glass, the latter is a dielectric. If a voltage is applied to the lamp, this glass surface is therefore electrified and discharge begins if a breakdown voltage is achieved. This discharge immediately neutralizes the glass surface and then stops because there is no longer any potential gradient. When the next discharge begins, the glass surface is neutralized again and the discharge stopped in the same way. This process is repeated. This phenomenon arises depending on the condition of the glass surface and the respective electrification condition in each area of the glass surface.. When the voltage applied to the lamp is a sine curve, the voltage increases relatively gently, and a voltage waveform of this type occurs continually and repeatedly. These phenomena therefore always occur and it is conceivable that apparently a strip-like discharge would occur, as was described above. In the case of a conventional luminous operation process in which a sine curve is applied, therefore at a partial pressure of the Xe gas of greater than or equal to 10665,79 N/m 2 (80 torr), the above described phenomenon occurs and relative luminance fluctuation is acutely increased if the pressure of the gas encapsulated in the discharge lamp is increased to raise the illumination intensity, as is described below. If, on the other hand, a voltage waveform with a short rising time is applied to the lamp, a condition approximated in which the voltage is applied directly to the gas itself filled in discharge vessel 3, as was described above. The above described phenomenon of neutralization of the surface of the dielectric is therefore reduced. It is conceivable that a strip-like discharge would not occur and that a stable emission would be produced. Here the illumination intensity of the ultraviolet radiation which are emitted from the Xe gas of discharge lamp 1 decreases both at an overly high repetition frequency of the above described voltage applied to discharge lamp 1 (called the "operation frequency"), and also at an overly low operation frequency. The possible reason for this is as follows: (1) in the case of a reduction of the luminous frequency If the operation frequency is reduced with a constant input power, the energy per repetition of the lamp voltage waveform increases according to the reduction of the operation frequency. On the other hand, the radiant efficiency of Xe decreases when the input energy is increased. It is therefore conceivable that the lower the luminous frequency is made, the more the radiant efficiency and the illuminance decrease. (2) in the case of an increase of the operation frequency Based on the aforementioned explanation (1), the illuminance does increase up to a certain frequency when the operation frequency is increased. But if the frequency is increased even more, the next voltage waveform destroys the excitation species which produce the ultraviolet radiation, thus causing the illuminance to decrease. The conceivable reason for this is that in conjunction with the lifetime of the excitation species, still remaining excitation species are destroyed by the energy obtained during the next period and that emission with good radiant efficiency is no longer obtained from the excitation species if the next voltage waveform with an earlier period than the lifetime of the excitation species once produced is applied to the discharge lamp. As was described above, by fixing full width at half maximum of the voltage applied to discharge lamp 1 within a stipulated value and furthermore by selecting the repetition frequency of the voltage applied to discharge lamp 1 in a suitable range, the discharge lamp is operated in a stable emission condition even if the pressure of the filled gas is increased. Figure 2 is a schematic of an arrangement of a circuit of the flyback type of another embodiment of the operation device as claimed in the invention. In this embodiment diode D is located in series with switching device 8. If for example a MOSFET is used as switching device 8, conventionally with respect to an arrangement between the drain and the source electrode there is diode D1, as is shown in Figure 3. In the case of the circuit shown in Figure 2 therefore at the instant the input power is turned off on the primary side of transformer 9 an electromotive counterforce is formed, the current flowing in the direction of arrow in Figure 3 and the efficiency decreasing to a high degree. In Figure 2 therefore diode D is series connected to switching device 8 so that the above described current is hindered. Without a decrease of efficiency, this arrangement yields a voltage waveform with above described full width at half maximum within a stipulated value even if switching decive 8 which is shown in Figure 3 and which is provided with diode D1 is used. In the following the experimental result during operation of fluorescent discharge lamp of the outer electrode 1 using the above described operation device is shown. Figure 4 is a schematic of one arrangement of an experimental circuit of the flyback type which was used in this embodiment. In Figure 4 a MOSFET was used as switching device 8. Diode D was series connected to switching device 8, as was shown in Figure 2. On the primary side of transformer 9 snubber circuit 10 is connected; it consists of a series connection of resistor R1 of 50 ohms and capacitor C1 of 1000 pF. Furthermore, a 24 V DC source was connected to one of the terminals on the primary side of transformer 9, while switching device 8 was connected to the other terminal via diode D and was supplied with driver signals with a peak value of 12 V, as is shown in the drawing. Capacitor C2 of 440 µF was connected to the 24 V DC source. Transformer 9 with following properties (1) to (4) was used, the full width at half maximum of the periodic voltage waveform which is formed on the secondary side of transformer 9 having been changed. (1) at a full width at half maximum of 0.4 µs inductance on primary side 8.5 µH inductance on the secondary side 0.34 mH (2) at a full width at half maximum of 0.8 µs inductance on primary side 8.5 µH inductance on the secondary side 1.3 mH (3) at a full width at half maximum of 1.9 µs inductance on primary side 8.5 µH inductance on the secondary side 5.4 mH (4) at a full width at half maximum of 3.0 µs inductance on primary side 8.5 µH inductance on the secondary side 12.1 mH Figures 5 and 6 are schematics of the relation between the full width at half maximum which was obtained in the above described experimental circuit, and the illuminance of the discharge lamp. In Figure 5 a lamp with a tube diameter of 8 mm and a lamp length of 360 mm is used as a discharge lamp; it has two strip-like electrodes (one pair) with an electrode width of 8 mm. Figure 5 shows the relation between the full width at half maximum and the illuminance during operation of the discharge lamp under conditions A and B described below. In Figure 5 the "operation process as claimed in the invention" represents operation using the circuit shown in Figure 4, while the "conventional operation process" represents operation of the discharge lamp with a sine curve high frequency AC voltage. Condition A: lamp wattage 7 W Condition B: lamp wattage 13W Operation in the operation process as claimed in the invention was accomplished with a operation frequency of 40 kHz under condition A and with a operation frequency of 70 kHz under condition B. As is apparent from the drawing, in the conventional luminous operation process the illumination intensity under conditions A and B is essentially constant, regardless of the value of the full width at half maximum. In the operation process as claimed in the invention on the other hand the illuminance becomes higher according to a reduction of the full width at half maximum. Here the illuminance at a full width at half maximum of less than 2.8 µs to 3 µs becomes higher than in the conventional light operation process. In Figure 6 a lamp with a tube diameter of 6.5 mm and a lamp length of 360 mm is used as a discharge lamp; it has two strip-like electrodes (one pair) with an electrode width of 7 mm. Figure 6 shows the relation between the full width at half maximum and the illuminance during operation of the discharge lamp under the same condition as above described condition B, i.e., with a lamp wattage of 13 W. Here the "operation process as claimed in the invention" represents operation using the circuit shown in Figure 4, while the "conventional operation process" represents operation of the discharge lamp with a sine curve high frequency AC voltage, as in Figure 5. Here the operation frequency in the operation process as claimed in the invention was 70 kHz. In the case shown in Figure 6 for a full width at half maximum of less than 2.6 :s the illuminance becomes higher than in the conventional operation process. From the above described tests it was possible to state that even for changes of operation conditions and of the tube diameter of the discharge lamp the illuminance becomes higher than in the conventional operation process, if at least W ≤ 2.5 µs. Next, to study the relation between the voltage waveform applied to the discharge lamp and the illuminance, the circuit parameter of the circuit shown in Figure 4 was changed, voltages with waveforms 1 through 3 shown in Figure 7 (a) through (c) were produced and applied to the discharge lamp, and the relation between the lamp wattage and illuminance studied. In Figure 7 the oscillation waves which follow on the maximum peak voltages become smaller in the sequence of waveform 1 to waveform 2 to waveform 3. The lamp wattage for example at a peak voltage of 1400 V was 13.5 W for waveform 1, 12.7 W for waveform 2 and 11.0 W for waveform 3. This corresponds to 1.22 for waveform 1 and 1.14 for waveform 2 if the lamp wattage is designated 1 for waveform 3. These differences of lamp wattage are based on differences of the power which is supplied to the oscillation wave which follows on the maximum peak voltage and which contributes to emission. If in this way an effective power which contributes to emission can be supplied to the oscillation wave which follows on the maximum peak voltage, it becomes possible to obtain the required amount of light as the peak voltage drops, by which handling, such as insulation, pressure tightness and the like, are simplified in the luminous circuit lamp. Figure 8 schematically shows the relation between the lamp wattage and the illuminance if the above described waveforms 1 through 3 have been applied to the discharge lamp. In Figure 8 a lamp with a tube diameter of 8 mm and a lamp length of 360 mm is used as a discharge lamp, the operation frequency being 70 kHz. As shown in the drawing, it could be stated that essentially the same illuminance is obtained even if the voltage waveform applied to the discharge lamp does not change. Furthermore it is conceivable that not only for waveforms 1 through 3, in which the voltage peak value occurs in only one polarity, as is shown in Figure 7 (a) through (c), but also for voltage waveform 4 is the same effect obtained in which the voltage peak value occurs in two polarities, as is illustrated in Figure 7 (d). This means that in this way an invention action can be obtained in which the voltage waveform with full width at half maximum of less than or equal to a stipulated value (for example W ≤ 2.5 µs) is applied with stipulated time intervals to the discharge lamp. Figure 9 is a schematic of the relation between the operation period and the illuminance (lamp wattage is constant: 13 W). Here the "operation process as claimed in the invention" represents operation using the circuit shown in Figure 4, while the "conventional operation process" represents luminous operation of the discharge lamp with a sine curve high frequency AC voltage, as in Figure 5. Here a discharge lamp with a tube diameter of 8 mm and a lamp length of 360 mm was used. As is shown in the drawing, the illuminance decreases in the "operation process as claimed in the invention" when the operation period becomes longer. For a short operation period the illuminance also decreases. The conceivable reason for this is that at a low operation frequency (for a long operation period) the radiant efficiency and illuminance decrease and that for an overly high operation frequency (for a short operation period) emission with good radiant efficiency from the excitation species cannot take place, as was described above. On the other hand, in the "conventional operation process" up to a operation period of roughly 30 µs a constant illuminance is maintained and for longer than roughly 30 µs the illuminance decreases. From the above described test it became apparent that in the case of using the "operation process as claimed in the invention" for a operation period of roughly 5 to 70 µs a higher illuminance can be obtained than in the "conventional operation process". Next, the relation between the partial pressure of the Xe gas filled in the discharge lamp and relative luminance fluctuation was examined. As was described above, when the encapsulation pressure of the discharge lamp increases in the "conventional operation process" the emission state within discharge vessel 3 is observed as a strip, as is illustrated in Figure 15. Therefore, in the case of using the "operation process as claimed in the invention" and in the case of using the "conventional operation process" the relation between the partial pressure of the Xe gas and relative luminance fluctuation was examined, the effect of the invention having been confirmed. The relative luminance fluctuation is defined by maximum brightness "a" of the discharge lamp after n minutes have passed since starting of operation of the discharge lamp (the maximum value of brightness on the locations in Figure 15 at which emission is concentrated) and by minimum brightness "b" (the maximum value of brightness at the dark locations in Figure 15), and it can be computed using the following formula: Relative luminance fluctuation (%) = {(a - b)/(a + b)} x 100 Figure 10 is a schematic of the relation between the partial pressure of the Xe gas and the relative luminance fluctuation. Here the "operation process as claimed in the invention" represents operation using the circuit shown in Figure 4, while the "conventional operation process" represents operation of the discharge lamp with a sine curve, as shown in Figure 5. Here a discharge lamp with a tube diameter of 8 mm and a lamp length of 360 mm was used which was operated at lamp wattage of 13 W. Three minutes after starting operation relative luminance fluctuation was determined. As is apparent from the drawing, in the case of the "conventional operation process" relative luminance fluctuation is acutely increased if the partial pressure of the Xe gas is greater than or equal to 13332,24 N/m 2 (100 torr). In the "operation process as claimed in the invention", on the other hand, relative luminance fluctuation does not change even if the partial pressure of the Xe gas is increased. This confirms that at a partial pressure of the Xe gas of greater than or equal to 10665,79 N/m 2 (80 torr) in the invention the luminous condition can be kept stable. As was described above, the filling pressure of the Xe gas can be set to greater than or equal to 10665,79 N/m 2 (80 torr), at which a stable luminous condition could not be easily maintained in the "conventional operation process" due to high brightness control. As claimed in the invention, this enabled a higher illuminance to be maintained than in the "conventional operation process". As one of the processes for increasing the illuminance of a discharge lamp there is a process in which a mixed gas based on Xe-Ne is used as the gas filled in the discharge lamp. Figure 11 schematically shows the efficiency of the illuminance when the mixing ratio of Ne gas changes, the Xe gas pressure having been 13332,24 N/m 2 (100 torr) using the above described basis of gases. In Figure 11 a discharge lamp with a tube diameter of 8 mm, a lamp length of 360 mm, an operation frequency of 70 kHz and constant lamp wattage of 20 W was used. As is shown in the drawing the efficiency of the illuminance increases when the mixing ratio of the Ne gas is increased as the partial pressure of the Xe gas is kept at 13332,24 N/m 2 (100 torr). As was described above, it is confirmed here that the effect of the invention is obtained in which, when the "operation process as claimed in the invention" is used, even when the partial pressure of the Xe gas is increased, a stable discharge condition can be maintained, as in Figure 10, even if a mixed gas based on Xe-Ne is used. If the partial pressure of the Xe gas is 13332,24 N/m 2 (100 torr) and the mixing ratio of the Ne gas is 80%, the total pressure within the discharge lamp is 66661,20 N/m 2 (500 torr). If however the total pressure of filling in the discharge lamp is greater than or equal to 101325,02 N/m 2 (760 torr), the difficulty arises that when the discharge lamp is produced the lamp expands, making its manufacture difficult. It is therefore desirable that the total pressure of the gas encapsulated in the discharge lamp be less than or equal to 101325,02 N/m 2 (760 torr). Commercial Application As was described above, the device for operating a discharge lamp can be used for document scanning illumination of an information processing device, such as a fax machine, a copier, an image reader and the like, and for a background light device of a liquid crystal display.

Claims: Device for operating a fluorescent discharge lamp for document scanning illumination of an information processing device and for a background light device of a liquid crystal display, in which within a glass tube (3) at least one of the rare gases He, Ne, Ar, Kr, or Xe is hermetically sealed in a stipulated amount, in which fluorescent material is applied to the inside of the glass tube (3), and in which in the axial direction on the outside of the glass tube (3) there are at least two strip-shaped electrodes (2) over the entire length of the glass tube (3), and with a lamp voltage with a cyclic voltage waveform, controlled by a driver circuit(7), characterized in that the driver circuit (7) is of the fly-back type, in the cyclic voltage waveform the zero-level width W o of the waveform having the maximum peak voltage in one period is set to 2 W o < t with respect to the cycle period t, whereby a half-value width W is set to a predetermined value of a waveform in the range of 10 µs ≤ t ≤ 30 µs, all electrodes (2)are arranged on the outside of the glass tube (3) and there are no inner electrodes (Fig.1). Device for operating a fluorescent discharge lamp according to claim 1, wherein in the cyclic voltage waveform the half maximum level width W of the waveform having the maximum peak value is set in the range of W ≤ 2.5 µs (Fig.5). Device for operating a fluorescent discharge lamp according to claim 1 or 2, wherein the glass tube (3) of the fluorescent discharge lamp of the outer electrode type (1) comprises a gas with a partial pressure of the Xe gas of greater than or equal to 10 665,79 N/m 2 (80 torr) and a total pressure of the filled gas of less than or equal to 101 325,02 N/m 2 (760 torr). Device for operating a fluorescent discharge lamp according to one of the proceeding claims, wherein an oscillation wave which follows the maximum peak voltage is supplied with an effective power which contributes to emission.

Inventors: HIRAOKA TATUHIRO, IGARASHI TATUSHI, INOUE MASAKI, YOKOKAWA YOSHIHISA, YOSHIOKA MASAKI, HIRAOKA, TATUHIRO, IGARASHI, TATUSHI, INOUE, MASAKI, YOKOKAWA, YOSHIHISA, YOSHIOKA, MASAKI
Applicants: USHIO ELECTRIC INC, USHIO DENKI KABUSHIKI KAISHA
Application year: 1997
Main classification: H05B41
IPC codes: H05B41