Title of Invention

A METHOD OF AND DEVICE FOR OPERATING A GAS DISCHARGE LAMP

Abstract

A method of operating a gas discharge lamp which is fed with an alternating voltage or an alternating current, the instantaneous power of the lamp being increased at given time intervals, characterized in the following steps: continuously or discontinuously measuring the values of at least one operational datum of the lamp which varies in time, and selecting the frequency of the alternating voltage or the alternating current (operating frequency) in dependence of the measured values.

Full Text

The invention relates to a method of and a device for operating a gas discharge lamp which is fed with an alternating voltage or an alternating current, the instantaneous power of the lamp being increased (pulsed mode of operation) at given time intervals. The invention also relates to apparatus equipped with such lamps and devices as well as to methods of treating an electrode which are based on said mode of operation. Such modes of operation and devices are known, for example, from WO 96/14724 or from US 5,608,294. The cited WO publication discloses a device with an energy supply circuit for operating a gas discharge lamp wherein the energy supply circuit provides an alternating voltage or an alternating current of predetermined period duration in order to feed the gas discharge lamp with a predetermined power in such a manner that, when the mean lamp power is reduced relative to the nominal power, the instantaneous power is increased with one half period duration directly prior to the reversal of polarity of the alternating voltage or the alternating current. This brief increase of the instantaneous power prior to the reversal of polarity ensures that the re-ignition voltage required after the reversal of polarity essentially need not be increased relative to the voltage in the nominal mode of operation. The cited United States patent describes a method of operating a gas discharge lamp with a short light arc; therein, the lamp receives an alternating current of a given period duration and a brief current pulse is superposed on the lamp current in each half period, which current pulse has the same polarity as the lamp current in the relevant half period so that the constancy of the light arc and the durability of the electrodes of the gas discharge lamp are essentially improved. The variation of the current intensity or the voltage, as known from the cited publications and referred to hereinafter as "pulsed operation" or "pulsed mode", has proven to be very effective in practice. It is to be noted that in this context the terms "pulsed operation" and "pulsed mode" are to be understood to cover all variations of the current strength or voltage in time where additional current or voltage pulses are superposed on the operating current or the operating voltage, notably for the purpose of stabilization of the lamp arc (in many publications (for example, see EP 0865210 A2, WO 97/247871 or US 5,428,408), however, the term "pulsed operation" is to be understood to mean exclusively a lamp mode of operation in which the lamp operates in quickly repeated, very short periods of time and does not output light during a large part of the time). Although pulsed operation can considerably improve the constancy of the light arc, the service life is not yet satisfactory; this is important notably in the case of high-pressure gas discharge lamps with a very short light arc, such as used, for example in data and video projectors with LC or mirror displays (deformable mirror device), but also for various other publications. The shorter the light arc required, the more severe the effects of burning off of e lamp electrodes and the accompanying extension of the light arc between the electrodes will be. It is not seldom that burning off of the lamp electrodes in gas discharge lamps with short and very short light arcs during the first 100 hours of operation already reduces the efficiency in, for example, a projection system, by 20%. Moreover, the manufacture of gas discharge lamps with a very short electrode gap is extremely difficult, since the electrodes are normally sealed in a quartz tube and are positioned, prior to the sealing into the tube, in such a manner that, due to the manufacturing process, their position deviates from the original setting after the finishing of the lamp, that is, both in respect of the gap as well as in respect of the lateral alignment with one another. The positioning tolerances of the electrodes can be reduced at great expense only. A further problem that can be solved with great difficulty only is posed by the geometrical shape of the electrodes themselves. Generally, it is possible to cut desired electrode geometries from a solid material, but for reasons of cost that the electrodes preferably consist of an electrode rod (drawn tungsten wire) with a tungsten spiral slid thereon, even though the geometry and the inner structure of the electrodes, ultimately defining the heat distribution, can be controlled to a lesser extent in such a construction. In lamps having short light arc the enormous thermal loading of the electrodes already causes fast transport of the electrode material (for example, evaporation of tungsten) which, within a few hours, completely change the electrode front face in high-pressure gas discharge lamps having arc length of approximately 1 mm. Even an ideally shaped electrode will usually retain its original functional properties for only less than 100 hours in such circumstances. Considering the foregoing, it is an object of the invention to provide a method and a device for operating a gas discharge lamp which make it possible to use the transport processes taking place during operation of a gas discharge lamp advantageously for the formation of the electrodes. The object is achieved by means of a method as disclosed in claim 1 and by means of a device as disclosed in claim 12. Advantageous versions and embodiments are disclosed in dependent claims. The secondary claims relate to processing methods and r devices bas n these methods and devices. The object is achieved notably by means of a method of the kind set forth wherein the values of at least one operational datum of the lamp which varies in time are continuously or discontinuously measured and the frequency of the alternating voltage or the alternating current (operating frequency) is selected in dependence on the measured values. The operating frequency is then advantageously selected in dependence on the measured values of at least one operational datum from the group of operational data which includes the overall ice life of the lamp, the operating voltage, the power taken up or given off, the arc length and the electrode gap, since all such data offer direct or indirect information concerning the state of the electrodes, notably the electrode gap (for example, even in the case of a new lamp having a service life, an idea of the approximate state of the electrodes, and hence of the necessity of selecting a given operating frequency, can be derived from the service life itself on the basis of experimental values). The invention is based on the novel insight that the magnitude of the structures growing on the electrodes during operation with alternating current or alternating voltage is proportional to the operating frequency of the current or the voltage. It has been found that the diameter of the structures grown is smaller as the fundamental frequency of the operating current or operating voltage is higher. Typical frequencies in high-pressure gas discharge lamps lie between approximately 40 and 600 Hz. For lamps of a given type (for example, in conformity with DE 38 13 421 A), for example, the following relation holds: approximate diameter of the structures grown D=a/f*/2, where f is the operating frequency in Hertz and a is a lamp-specific proportionality i fy constant of the unit [meter * Hertz ] which lies typically between approximately 2000 and 5000 \xm Hz , so that structures having a diameter of from approximately 200 to 500 |im are formed in the case of a fundamental frequency of 100 Hz.. Generally speaking, this constant may lie in a slot between 1000 and 10,000 jimHz . The height of the structures formed generally is smaller than their diameter and as a rule amounts to approximately from 0.4 to 0.8 time the diameter. The ratio, however, has been found to vary between 0.2 and 1.2. This relationship is used according to the invention so as to form projecting electrode tips in a controllable manner during operation of the lamp. The invention enables formation of the electrode during operation, independently within given limits) of the basic shape of the electrodes as imposed by the manufacturing process. The desired electrode gap, or the desired operating voltage, can be adjusted within given limits by utilizing the transport processes. When the desired voltage is reached, the conditioning process is interrupted and the lamp is operated at the frequency prevailing at instant. It is a special advantage of the method according to the invention that it can be applied time and again during the service life of the lamp, thus allowing to some extent a "regeneration of the electrodes so that outstanding results can be achieved over a very long service life. Because of the physical laws of the transport processes, the electrode structure formed during operation are situated practically exactly opposite one another, so that no lateral offset occurs. When the operation commences with sufficiently low" frequencies, the structure will be situated at the electrode center. To this end, the measured values are advantageously monitored in respect of the satisfying of predetermined boundary conditions and when a first boundary condition is satisfied (initial condition), the lamp is operated with a low operating frequency (initial frequency) until a second boundary condition is satisfied, after which the operating frequency is increased. Such start conditions may be, for example, the putting into operation of a new lamp for the first time or the building up of the necessary operating voltage beyond a given limit value. It is notably also possible to define different initial conditions with different initial frequencies so that, for example, successive structures of decreasing diameter can be built up on the electrodes when a new lamp is put into operation for the first time, a start being made with a comparatively low initial frequency, whereas in the case of electrodes whose shape is to be modified only slightly it may suffice to build up small structures immediately and to start with a comparatively high initial frequency. The operating frequency can be continuously increased for successively building up the structures, However, it has been found that it is particularly advantageous to increase the operating frequency in discrete steps until a predetermined interruption condition is reached. Such interruption conditions may be: the reaching of a predetermined operating frequency (maximum frequency), the reaching of a predetermined minimum operating voltage, constancy of the electrode gap over a predetermined period of time. A device which is arranged to achieve the described object in operating a gas discharge lamp is provided with measuring means for the continuous or discontinuous measurement of the values of at least one operational datum of the lamp which varies in time and with means for changing the frequency of the alternating voltage or the alternating current (operating frequency) in dependence on thp measured values. Such a device can also be simply use for or be provided in already manufactured gas discharge lamps and lighting devices used for gas discharge lamps of all types, notably projectors, lighting systems of trucks etc. A preferred embodiment of the device includes a compact evaluation and control unit which includes at least one microprocessor and is intended to control the operating frequency, the operating voltage and the alternating current applied to the gas discharge lamp, as well as to evaluate and monitor the measured values in respect of the satisfying of predetermined or selectable boundary conditions; advantageous use can then be made of processors and units already provided in existing devices for the pulsed operation of gas discharge lamps. Further details and advantages of the invention will become apparent from the following, non limitative description, given with reference to the drawing and merely by way of example, of advantageous versions of the method according to the invention. Therein: Fig. 1 shows a typical variation in time of the operating current applied to a gas discharge lamp during pulsed operation, and Fig. 2 shows diagrammatically the lateral profile of an electrode formed by means of a method according to the invention. The cited US 5,608,294 describes an electronic ballast device which is capable current form as shown in Fig. 1 with an additional current pulse of the height 13 and thedur ion tp at the end of the relevant half- wave of overall duration tl/2 and the basic height 12. Preferably, this is realized by means of a microprocessor-controlled ballast device which is also capable of controlling the lamp operating frequency. It may also include a data carrier which contains a control program for executing the steps to be described hereinafter. There may also be provided a reading device whereby a machine-readable data carrier can be read so as to transfer its data to the ballast device. In order to build up an electrode having the desired shape as shown in profile in, Fig. 2, the lamp is operated with a slowly increasing frequency, starting from a low initial frequency, in the pulsed mode. A low frequency at the beginning of the sequence provides a wide structure 1 as a base on which continuously narrower structures 2 and 3 can be built, at higher frequencies. The transition may be continuous or take place in discrete steps. Practical results were obtained, for example, with an operation duration of each time a few hours at 45, 65, 90 and 130 Hz in this increasing sequence. Using this mode of operation it was found t be possible to reduce the electrode gap in a conventional high-pressure gas discharge lamp from 1.3 mm to 0.7 mm. During prolonged operation (some hundreds of hours) of the lamp thus conditioned at the highest frequency, the electrodes then gradually burn off to the initial state again, as can be readily observed on the basis of an increase of the operating voltage. When the operating voltage increases, the electrode according to the invention can be treated again with slowly increasing frequencies until the tip structures of the electrode have been almost completely rebuilt again. After every regeneration operation of this kind, the lamp can be operated at the highest selected frequency again for approximately 100 hours. The invention offers the major advantage that the light of the lamp can also be used during regeneration phases. Overall, the optical efficiency usually decreases as the electrode gap increases (for example, a decrease of the screen brightness in the case of video projection; this brightness is increased by the regeneration). Such a system efficiency, fluctuating over a time scale of 100 hours, in any case constitutes a major advantage which outweighs a continuously decreasing efficiency. The necessity of renewed regeneration can be readily deduced from the voltage rise of the lamp. When the operating voltage increases beyond a predetermined value, renewed regeneration is started. Hereinafter it will be described in detail, by way of example, how the method according to the invention can be carried out during operation of a gas discharge lamp of a video projector. First-time operation of the lamp is recognized by way of an hours of operation counter which is automatically reset when a lamp is replaced. This is already implemented in many commercially available projectors. The lamp is initially operated at an as low as possible frequency (for example, 45 Hz. Such operation can take place during a fixed time interval (for example, one hour of operation). Alternatively, the frequency can also be sustained until a significant voltage decrease (indicating growth of structures) can no longer be observed. This mode of operation is advantageous that individual differences can be taken into account better than in the case of operation during fixed periods of time. Subsequently, the frequency is increased. It has been found that an increase of the frequency to approximately from 1.2 to 1.8 times the respective preceding frequency is advisable. The operation at the new frequency can again take place for a fixed period of time or until a significant voltage decrease can no longer be detected. Overall, the frequency is increased until either a) a fixed frequency limit is reached, b) a fixed voltage is reached or c) a significant growth can no longer be observed after an increase of the frequency. The frequency thus determined is sustained and can be used, for example, until the voltage has considerably increased again, for example to the initial level. Preferably, however, the electrodes are "regenerated" anew before the rise to the initial level already; for this purpose lamp is operated again at an as low as possible frequency. The method according to the invention enables a substantial reduction of the operating voltage and the arc length or the electrode gap in gas discharge lamps. For example, in a gas discharge lamp of conventional construction, having electrodes of the previously described simple and economical construction, the operating voltage could be reduced from initially 85V to 52 V and the arc length from initially 1.3mm to 0.7 mm in the presence of a lamp current 12 for controlling the power and a pulse current 13 amounting to 2.8 A while utilizing a sequence of operating frequencies of 45,65,90 and 130 Hz; it is to be noted that this amazing reduction was not achieved in a separate process but during "normal" use of the lamp, for example, in the projection mode. Many any alternative versions and further elaborations are feasible within the scope of the invention; such alternatives relate, for example, to the boundary conditions at which the operating frequencies are increased or decreased, or to the selection of the operating frequencies. It is an essential aspect that the method enables treatment of the electrodes during operation of the gas discharge lamp in that transport phenomena are used to deposit mat on the electrodes by controlled variation of the operating frequency. WE CLAIM: 1. A method of operating a gas discharge lamp which is ted witn an alternating voltage or an alternating current, the instantaneous power of the lamp being increased at given time intervals, characterized in the following steps; continuously or discontinuously measuring the values of at least one operational datum of the lamp which varies in time, and selecting the frequency of the alternating voltage or the alternating current (operating frequency) in dependence of the measured values. 2. The method as claimed in claim 1, wherein the operating frequency is selected in dependence on the measured values of at least one operational datum from the following group of operational data: overall service life of the lamp, operating voltage, power taken up or given off, arc length, and electrode gap. 3. The method as claimed in claim 1 or 2, comprising the following steps: monitoring the measured values in respect of the satisfying of predetermined boundary conditions, operating the lamp with a low frequency (initial frequency) when a first boundary condition is satisfied (initial condition), and increasing the operating frequency of the lamp when a second boundary condition is satisfied. 4. The method as claimed in claim 3, comprising the following step: increasing continuously or preferably in discrete steps the operating frequency after satisfying of the initial condition and starting from the initial frequency, until a predetermined third boundary condition (interruption condition) is reached. 5. The method as claimed in claim 3 or 4, wherein the initial condition is considered satisfied when a given service life occurs or has been reached and/or the necessary operating voltage has increased to a predetermined value and/or the electrode gap has increased to a predetermined value. 6. The method as claimed in any one of the claims 3 to 5, wherein the second boundary condition is considered satisfied when the lamp has been operated at the initial frequency for a given period of time or when changes can no longer be observed during the direct or indirect measurement of the electrode gap over a predetermined period of time. 7. The method as claimed in any one of the claims 4 to 6, wherein the interruption condition is considered satisfied when a predetermined operating frequency (maximum frequency) has been reached or when the necessary operating voltage has decreased to a predetermined minimum value, or when changes can no longer be detected during the direct or indirect measurement of the electrode gap over a predetermined period of time. 8. The method as claimed in any one of the claims 3 to 7, comprising the following step: choosing the initial condition and the initial frequency in dependence on the operating state of the lamp. 9. The method as claimed in any one of the claims 1 to 8, comprising the following step: selecting the operating frequencies between approximately 40 and 600 Hz. 10. The method as claimed in any one of the claims 1 to 9, comprising the following step: increasing the operating frequency in discrete steps, wherein the frequency is increased with each step to approximately from 1.2 to 1.8 times the preceding frequency. 11. The method as claimed in any one of the claims 1 to 10, comprising the following step: selecting the operating frequency f according to the relation D = a/f in order to achieve structures having a diameter of D grown on the electrode, where a is a lamp-specific constant of the unit [meter * Hertz ] which is dependent notably on the electrode material and the electrode geometry, and f is the frequency in Hertz. 12. A device for operating a gas discharge lamp with an alternating voltage or an alternating current so that the instantaneous power of the lamp is increased at given time intervals, characterized in: measuring means for the continuous or discontinuous measurement of the values of at least one operational datum of the lamp which varies in time and means for changing the frequency of the alternating voltage or the alternating current (operating frequency) in dependence on the measured values. 13. The device as claimed in claim 12, wherein the device is provided with at least one monitoring unit which is coupled to the device, in order to monitor the measured values as regards the satisfying of predetermined or selectable boundary conditions. 14. The device as claimed in claim 12 or 13, wherein it is provided with at least one compact evaluation and control unit which comprises at least one microprocessor for controlling the operating frequency, the operating voltage and the alternating current applied to the gas discharge lamp, as well as for evaluating and monitoring the measured values in respect of the satisfying of predetermined or selectable boundary conditions. 15. A projector provided with a device for operating a gas discharge lamp as claimed in any one of the claims 12 to 14.

Documents:

357-mas-2001 description (complete) duplicate.pdf

357-mas-2001 abstract duplicate.pdf

357-mas-2001 claims duplicate.pdf

357-mas-2001 drawings duplicate.pdf

357-mas-2001-claims.pdf

357-mas-2001-correspondnece-others.pdf

357-mas-2001-correspondnece-po.pdf

357-mas-2001-description(complete).pdf

357-mas-2001-drawings.pdf

357-mas-2001-form 1.pdf

357-mas-2001-form 18.pdf

357-mas-2001-form 26.pdf

357-mas-2001-form 3.pdf

357-mas-2001-form 5.pdf