The invention relates to improvements in and relating to UV (ultra-violet) gas discharge tubes. UV gas discharge tubes may be used in a variety of different applications where their response to ultra-violet radiation is used for detection and warning purposes, for example. Embodiments of the invention to be described in more detail below by way of example only are concerned with the detection of failure modes which are known to occur in such tubes. More specifically, a UV gas discharge tube can be used to monitor ultra-violet radiation emitted by the flame of a gas burner, so as to detect the absence or reduction of this radiation in the event of cessation of the flame (a “flame-out” condition), and thereupon shutting off the supply of gas to the burner. In such an application, it is necessary to detect failures in the detection process, particularly types of failure where the tube falsely continues to indicate the presence of UV radiation.
According to the invention, there is provided apparatus for detecting a condition in which an ultra-violet gas discharge tube becomes sensitive to radiation in another wavelength band, comprising means for temporarily directing radiation in the other wavelength band to the tube, and means for monitoring for any resultant increase in the output of the tube.
According to the invention, there is further provided an ultra-violet gas discharge tube arrangement, comprising means operative during each of a succession of periods (on periods) to apply an electric field to and within a UV gas discharge tube while the tube is exposed to a source from which ultra-violet radiation may be emitted so that conduction of the tube may take place during those periods, each on period being followed by a period (off period) in which the electric field is absent and during which in normal operation of the tube it returns to or maintains a quiescent state, control means responsive to any conduction of the tube during each of a plurality of the on periods for producing an output dependent on the mean value (mean lag value) of the lags within each of those on periods before any conduction takes place, first output means operative when the output indicates that the mean lag value lies within a predetermined range to indicate emission of the ultra-violet radiation from the source, second output means operative when the output indicates that the mean lag value is greater than the said range for indicating absence of emission of UV radiation from the source, and fault responsive means operative when the output indicates that the mean lag value is less than the predetermined range to indicate a fault condition in which conduction takes place within the tube without the presence of UV radiation.
According to the invention, there is also provided an ultra-violet gas discharge tube arrangement, comprising means operative during each of a succession of periods (on periods) to apply an electric field to and within a UV gas discharge tube while the tube is exposed to a source from which ultra-violet radiation may be emitted so that conduction of the tube may take place during those periods, each on period being followed by a period (off period) in which the electric field is absent and during which in normal operation of the tube it returns to or maintains a quiescent state, control means responsive to any conduction of the tube during each of a plurality of the on periods for producing an output dependent on the mean value (mean lag value) of the time lags within each of those on periods before any conduction takes place, first output means operative when the output indicates that the mean lag value lies within a predetermined range to indicate emission of the ultra-violet radiation from the source, second output means operative when the output indicates that the mean lag value is greater than the said range for indicating absence of emission of UV radiation from the source, and fault detecting means comprising means operative during a test duration to produce a predetermined and temporary increase in the length of the off periods and means operative in the event that the mean lag value increases during that test duration whereby to indicate the existence of a fault condition in which the normal length of the off periods is insufficient to allow the tube to return to the quiescent state.
According to the invention, there is still further provided a method for detecting a condition in which an ultra-violet gas discharge tube becomes sensitive to radiation in another wavelength band, including the step of temporarily directing radiation in the other wavelength band to the tube, and monitoring for any resultant increase in the output of the tube.
According to the invention, there is yet further provided a method of operating an ultra-violet gas discharge tube arrangement, comprising the steps of applying an electric field during each of a succession of periods (on periods) to and within a UV gas discharge tube while the tube is exposed to a source from which ultra-violet radiation may be emitted so that conduction of the tube may take place during those periods, each on period being followed by a period (off period) in which the electric field is absent and during which in normal operation of the tube it returns to or maintains a quiescent state, responding to any conduction of the tube during each of a plurality of the on periods for producing an output dependent on the mean value (mean lag value) of the time lags within each of those on periods before any conduction takes place, indicating emission of the ultra-violet radiation from the source when the output indicates that the mean lag value lies within a predetermined range, indicating absence of emission of UV radiation from the source when the output indicates that the mean lag value is greater than the said range, and indicating a fault condition in which conduction takes place within the tube without the presence of UV radiation when the output indicates that the mean lag value is less than the predetermined range.
According to the invention, there is also provided a method of operating an ultra-violet gas discharge tube arrangement, comprising the steps of applying an electric field during each of a succession of periods (on periods) to and within a UV gas discharge tube while the tube is exposed to a source from which ultra-violet radiation may be emitted so that conduction of the tube may take place during those periods, each on period being followed by a period (off period) in which the electric field is absent and during which in normal operation of the tube it returns to or maintains a quiescent state, responding to any conduction of the tube during each of a plurality of the on periods for producing an output dependent on the mean value (mean lag value) of the time lags within each of those on periods before any conduction takes place, indicating emission of the ultra-violet radiation from the source when the output indicates that the mean lag value lies within a predetermined range, indicating absence of emission of UV radiation from the source when the output indicates that the mean lag value is greater than the said range, producing a predetermined and temporary increase in the length of the off periods during a test duration, and indicating the existence of a fault condition in which the normal length of the off periods is insufficient to allow the tube to return to the quiescent condition in the event that the mean lag value increases during that test duration.
Apparatus and methods according to the invention for detecting and signalling the failure of a UV gas discharge tube will now be described, by way of example only, with reference to the accompanying diagrammatic drawings in which:
In the drawings, like elements are generally designated by the same reference numerals.
UV gas discharge tubes comprise a pair of electrodes (cathode and anode) enclosed within a housing, the housing being filled with a suitable gas. A voltage difference is applied across the electrodes to create a field within the tube. Upon irradiation of the tube by ultra-violet radiation, the incident energy can cause the emission of a surface electron from the cathode into the gas. In the presence of the applied electric field within the tube, the emitted photoelectron can cause electrical breakdown within the gas by collision with gas molecules, secondary emission from the cathode by UV radiation from the discharge, and ion bombardment, thereby creating a current flow in the tube from the cathode to the anode. The process is inherently very inefficient with only 1 in 104 incident photons causing photocell conduction. The probability is affected by the cathode material, the gas type, the gas pressure and the applied electric field.
Once in a conducting state, the tube will remain in conduction until the externally applied voltage is removed. After a certain period with the voltage removed, the charged species in the gas recombine and the gas becomes non-conducting again. Upon re-application of the voltage, the time elapsing from that re-application until conduction through the gas occurs again depends on the level of the ultra-violet radiation, the sensitivity of the gas discharge tube, and Poisson statistics (owing to the large number of photons involved in generating a single photoelectron). This elapsed time is known as the “statistical lag”, Ts.
In operation, a predetermined voltage is periodically applied between the electrodes 9 and 11. A control unit 13 detects whether a current flows between the electrodes after each application of the applied voltage and measures the elapsed time (the “statistical lag”, Ts) between each application of the applied voltage and the resultant conduction in the tube. After each application of the voltage, the voltage is then removed for a sufficient length of time so that (in normal operation of the tube) the charged species in the gas recombine and conduction stops, so that on re-application of the voltage no conduction occurs in the absence of UV radiation.
During operation, the control unit 13 produces an output signal representing the mean value of the statistical lag over a predetermined number of voltage applications. One method of carrying this out is to count the number of conductions of the tube which occur within a predetermined time period (e.g. 125 milliseconds). The reciprocal of the number of counts is thus representative of the mean statistical lag over this period. As shown in
In practice, various faults or failures can occur in the tube. One possible fault occurs when the tube becomes insensitive to UV radiation. This is often caused by partial or complete loss of gas within the envelope of the tube, normally caused by leakage. This stops the tube conducting in the presence of UV radiation. Clearly, in such a case the control unit 13 would respond by signalling a flame-out (because the mean value of the statistical lag Ts would become very high). This is a fail-safe fault.
However, other fault modes can occur which are “fail-dangerous”—that is, each such fault mode causes the tube to conduct or to continue to conduct even though incident UV radiation is absent. Various types of fail-dangerous faults can occur and the apparatus being described is arranged to detect them and signal a warning.
One such fault mode results in the tube becoming sensitive to longer wavelength radiation not specific to the presence of a flame (that is, sensitive to “room light”—the ambient light in the region of the tube). This fault is often caused by contamination of the cathode material, which lowers the work function of the material, causing the tube to conduct in the absence of the flame 3. Therefore, in such a case the control unit 13 would continue to assume that the flame 3 is present and thus continue to allow the supply of gas to the burner 16. This fault mode may be gradual, with the tube becoming more sensitive to longer wavelength radiation over an extended period of time.
In order to detect such a fault mode, the apparatus of
It is also possible for the tube to enter a “field emission” state whereby free electrons are generated by the applied electric field, without the presence of UV radiation. This fault mode is also fail-dangerous because the tube reacts in the same way as it does in the presence of UV radiation. This fault mode can occur as a result of surface roughening of the cathode material caused by ion bombardment. The resultant high points on the cathode surface will experience electrical field enhancement, resulting in the field emission effect. This fault mode is commonly referred to as “runaway”.
Clearly, in the presence of a field emission fault, the tube will go into conduction substantially immediately the electric field is applied across the electrodes. Therefore, the mean value for the statistical lag Ts will be very short and will lie within region I as shown in
In situations in which the tube is being used to monitor a very intense flame 3, the emitted ultra-violet radiation will be correspondingly intense and will thus result in a correctly operating tube producing very short values for Ts. It could thus become difficult to distinguish between a tube with a field emission fault and a correctly operating tube detecting high values of UV radiation. In order to deal with this potential problem, the value of the voltage applied across the electrodes (and thus the strength of the electric field) is selected, during initial set-up, so that under all values of UV radiation likely to be produced by the flames being monitored, the mean value of Ts will lie within region II. This ensures that if the intensity of the flame increases significantly from that observed during scanner commissioning, the signal level is such that the mean Ts generated will not become too short to compromise checking the integrity of the tube.
Another type of fault mode which can occur is a “multiple counting” fault. Here, contamination of the gas within the tube causes the de-ionisation of the gas to be increased. In other words, the length of the “off” periods between the application of the voltage across the electrodes is no longer sufficient to ensure that all the charged species in the gas have dissipated after its conduction. Therefore, when the voltage is next applied across the electrodes, the tube immediately re-conducts even in the absence of UV radiation. This again is fail-dangerous. This fault mode can occur gradually, initially becoming evident when a single conduction of the photocell becomes recorded as two counts. This has the effect of increasing the number of conductions for the same level of UV radiation. As contamination of the gas increases, a single photo-conduction of the cell leads to multiple counts until, eventually, a continuous pulse train is produced, again being termed “runaway”. Thus, the effect again is that the mean statistical lag will lie within the region I (
In order to detect this fault mode, and to enable it to be distinguished over a field-emission fault, the control unit 13 not only measures the mean value of TS but also carries out interrogation of each individual conduction. This enables an abnormally high number of conductions with short Ts to be identified, and thus the potentially dangerous situation to be signalled as a fault.
Instead, however, a multiple-counting fault mode could be detected by periodically increasing the lengths of the periods for which the voltage applied across the tube electrodes is off. Such a time increase will reduce or eliminate the multiple counting effect (by providing sufficient time for the charged species in the gas to dissipate) and will thus increase the mean value of the statistical lag detected by the control unit 13. If such a reduced signal level is detected during the increased “off” periods, this will be indicative of a multiple counting fault and a suitable warning can be signalled. Of course, this increase in the lengths of the off periods will cause a corresponding decrease in the length of the periods for which the applied voltage is on, causing a corresponding reduction in signal level (even in the absence of a multiple counting fault). The control unit will be arranged to take this reduction in signal level into account.
If the control unit detects a multiple counting fault (by either of the methods described above), then it could be arranged to cause a re-setting of the lengths of the off periods (within a set limit or by a predetermined amount)—that is, not merely a period in increase in the lengths of the off periods for fault detection purposes but in continuing increase. This would then enable the tube to operate correctly (i.e. it will overcome the multiple counting fault), and safe operation would thus continue. The control unit could then indicate a non-critical fault condition so that the tube would be replaced at the next maintenance inspection. Testing for multiple counting would of course continue so as to detect a worsening situation in which the increase in the length of the “off” periods was insufficient to overcome the multiple counting fault.
In practice, the apparatus and the control unit 13 will be arranged to be able to detect the existence of any one or all of the three different types of “fail-dangerous” faults described.
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0419847.9 | Sep 2004 | GB | national |
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