Abstract:
A current fed bipolar junction transistor (BJT) based inverter ballast includes base drive circuits configured to drive respective BJT switches, and high-speed drive reverse peak current limiting circuits, configured to operate in conjunction with the respective base drive circuits.

Description:
BACKGROUND OF THE INVENTION 
     The present application is directed to lighting devices, and more particularly to ballast circuitry for discharge lamps. Current fed bipolar junction transistor (BJT) based inverter ballasts are widely used in the lamp-lighting industry due to their inherent parallel lamp operation and output transformer isolation features. Providing transformer isolation permits parallel lamp operation and re-lamping of the lighting system to take place without requiring the shutdown of the power inverter of the entire system. Therefore, a lamp failure in the system can be replaced when it is needed while the remaining lamps are maintained in an “on” state. This therefore also reduces the maintenance and operational costs of such systems. 
     An example of a current fed inverter ballast having an instant program start configuration for use with parallel lamps has been described in U.S. Pat. No. 7,193,368, titled Parallel Lamps With Instant Program start Electronic Ballast, to Chen et al., issued Mar. 20, 2007. This ballast takes advantage of the beneficial aspects of a program start ballast (e.g., longer lamp life) and combines it with the advantages of an instant start ballast (e.g., quick start time) to produce an improved lamp ballast wherein parallel lamps are driven. Another circuit of this type is set forth in U.S. application Ser. No. 11/645,939, titled Switching Control For Inverter Startup And Shutdown, to Chen et al. filed Dec. 27, 2006, which describes a current fed BJT based inverter including a low cost shutdown circuit. Both U.S. Pat. No. 7,193,368 to Chen et al., and U.S. application Ser. No. 11/645,939 to Chen et al. are both hereby incorporated by reference in their entireties. 
     A drawback of existing current fed BJT based ballast systems which provide output transformer isolation is that they tend to have an efficiency which is relatively low compared to non-isolated lamp lighting ballasts due to the isolation transformer and operation mode of the BJTs. Therefore, a particular issue with such BJT based electronic ballasts has to do with the optimization of their base drive to improve the operational efficiency of these devices. Attempts to optimize the base drive signals commonly results in overdriving of the base-to-emitter junction of the BJT switches. This is a particular issue where the base of the BJT is driven by a parallel diode-resistor arrangement. In such configurations, when the base-to-emitter junction is overdriven, an undesirable increase in power dissipation takes place in the BJTs, and a higher circulating current exists in the ballast resulting in lower ballast efficiency. Another drawback which occurs due to overdriving is that dead-time, i.e., the overlap between the two transistor switching times, increases, leading to a higher current crest factor. Where current crest factor is the peak current divided by the root-mean-square (rms) current of lamp. ANSI standards require current crest factor to be less than 1.7. 
     Further, when current fed BJTs are used in conjunction with high efficiency lamp striations are known to occur even at room temperature. Striations manifest themselves as dark bands along the length of lamps and are particularly prevalent in lamps which use a high percentage of Krypton (Kr), which is employed as a buffer gas to improve the efficacy and usefulness of the lamps. For example, high efficiency lamps, may have a content of approximately 40 percent to 70 percent of Krypton (Kr). 
     Concepts of the present application are intended to address these and other outstanding issues as they relate to current fed BJT based inverter ballasts. 
     Prior art which may be of interest to the above-identified issues and others include U.S. Pat. No. 4,682,082, titled Gas Discharge Lamp Energization Circuit, to MacAskill et al., issued on Jul. 21, 1987; U.S. Patent Application Publication No. US2006/0103328, titled Striation Control For Current Fed Electronic Ballast, to Chen et al., published on May 18, 2006; U.S. Pat. No. 6,465,972, titled Electronic Elimination of Striations In Linear Lamps, to Kachmarik et al., issued on Oct. 15, 2002; and WO2006/051459, titled ANTI-STRIATION CIRCUIT FOR A GAS DISCHARGE LAMP BALLAST, to Fang, published May 18, 2006. 
     BRIEF DESCRIPTION OF THE INVENTION 
     A current fed bipolar junction transistor (BJT) based inverter ballast includes base drive circuits configured to drive respective BJT switches, and high-speed drive reverse peak current limiting circuits, configured to operate in conjunction with the respective base drive circuits. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  illustrates an existing electronic ballast type configuration in which the concepts of the present application may be used; 
         FIG. 2  illustrates the circuit of  FIG. 1 , implementing the concepts of the present application; and 
         FIG. 3  depicts a further embodiment of concepts related to the present application. 
     
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     Turning to  FIG. 1 , illustrated is a particular circuit in which the concepts of the present application may be employed. It is to be appreciated, however, the concepts described herein are not intended to be limited only to such a circuit, and may be employed in other lamp lighting control circuits. That having been said,  FIG. 1  is a half-bridge current fed ballast  10  which includes a first or upper switching configuration  12 , and a second or lower switching configuration  14 . These switching configurations include BJT switches Q 1  and Q 2 , respectively. BJT switch Q 1  is driven by a first or upper BJT control or base drive circuit  16 , and BJT switch Q 2  is driven by second or lower BJT control or base drive circuit  18 . First or upper BJT control circuit includes zener diode D 3 , capacitor C 4 , diode D 4 , diode D 5 , diode D 6 , resistor R 4 , and transformer winding T 2 - 2 . Second or lower BJT control circuit  18  is comprised of diode D 7 , resistor R 5  and transformer winding T 2 - 3 . 
     An output transformer system  20 , including capacitor C 5  and output winding T 2 - 1 , provides output signals to lamp network  22 , which includes lamp connector winding T 2 - 4 , and lamp capacitors C 6 , C 7  and C 8 . Additionally, circuitry such as power zener diodes D 1  and D 2  and voltage input network including resistors R 1 , R 2  and R 3 , capacitor network C 1 , C 2  and C 3  and windings T 1 - 1  and T 1 - 2  are further incorporated in the circuit, to provide a pulsed DC current signal to the BJT control or base drive control circuits  16 ,  18 , which in turn selectively supplies a drive signal to the BJT switches Q 1 , Q 2 . 
     For a more detailed discussion regarding operation of a comparable circuit, reference may be made to commonly assigned U.S. Pat. No. 6,989,637, titled Voltage Controlled Start-Up Circuit for Electronic Ballast, to Chen et al., issued Jan. 24, 2006, hereby incorporated by reference in its entirety. 
     An issue with circuit  10  of  FIG. 1 , and similar circuit designs, is that overdriving of BJT switches Q 1  and Q 2 , causes increased power dissipation on Q 1 , Q 2  and increased circulating current within the circuit, resulting in lowering the efficiency of the inverter. Also an increase in dead time switching occurs leading to an increased crest factor of the lamp current. On the other hand, underdriving of the BJT switches will result in excessive temperatures on the BJTs (such as measured in the high temperature ALT tests), resulting in potential failure of the ballast. 
     The concepts of the present application allow an optimization of the base drive to the BJT switches by provision of a high-speed drive with peak current limiting circuit which is shown and will be described in connection with  FIG. 2  as being incorporated into the BJT control or base drive circuits  16 ,  18 . The high-speed drive with peak current limiting circuit acts to not only reduce switching and inverter magnetic losses, but also improve the crest factor by increasing the turn-on/off time of the BJTs. 
     The newly added changes to the circuit can also be implemented to control the switching speed of BJT switches Q 1 , Q 2  to provide a rich, even harmonic voltage waveform to the lamp or lamps. This even harmonic waveform acts to diminish or eliminate visible striations that may otherwise be found on the lamp or lamps controlled by the new ballast. 
     Turning more particularly to ballast circuit  10  of  FIG. 2 , the first or upper BJT control or base drive circuit  16  is redesigned to incorporate a resistance by resistor R 6  and a capacitance by capacitor C 9  in series with each other, and the base of BJT switch Q 1 , as its high-speed drive peak current limiting circuit. Further, second or lower BJT control or base drive circuit  18  is redesigned to include a resistor R 7  and a capacitor C 10  in series with each other and the base of BJT switch Q 2 , as its high-speed drive peak current limiting circuit. 
     Incorporation of capacitors C 9  and C 10  makes it possible to reduce the value of the resistance provided by resistor R 4  of the first control circuit  16 , and the value of the resistance provided by resistor R 5  of second control circuit  18 . By inclusion of capacitors C 9  and C 10 , and thereby a reduction of the values of resistors R 4  and R 5 , the on/off time of the BJT switches Q 1  and Q 2  are increased, thereby achieving higher inverter efficiency by approximately 1 to 3 percent of inverter operation. 
     An issue, however, which arises due to adding the caps C 9  and C 10  is the potential of a higher peak of the base to emitter current at turn-on of the BJTs Q 1  and Q 2 . Such a higher peak current can result in a failure of BJTs Q 1 , Q 2 . Therefore, to protect against this undesirable result, ballast circuit  10  is further designed with resistor R 6  in first control circuit  16  and resistor R 7  in second control circuit  18 . These resistors, placed in series with capacitors C 9  and C 10 , respectively, operate to reduce the peak current of the respective control circuits  16  and  18 , thereby protecting BJTs Q 1 , Q 2  from receiving destructively high peak currents at Q 1  and/or Q 2  turn-on/off. At the same time, inclusion of resistors R 6  and R 7  improves the inverter efficiency and lowers the current crest factor for the lamp. 
     In one embodiment of circuit  10  of  FIG. 2 , the values of capacitors C 9 , C 10  and resistors R 6 , R 7  are chosen to be equivalent to each other resulting in a balanced circuit operation. However, in an alternative embodiment, by intentionally selecting the values of capacitors C 9  and  010  to be different from each other and/or resistors R 6  and R 7  to be different from each other, an imbalance in the waveform generated by circuit  10  will occur. This intentional imbalance may be useful in generating high, even harmonic supply voltages for the lamp or lamps. Such high, even harmonic supply voltages are useful in diminishing or eliminating visible striations in lamps. Particularly, it is known to be desirable to create a high even harmonic content with respect to the fundamental waveform of the signal supplied to lamps to increase the striations&#39; frequency above the range in which a human eye is able to detect striation effects. Typically, this frequency is greater than approximately 40 Hz. 
     Turning to  FIG. 3 , ballast circuit  10  depicts yet a further embodiment of the present application. Particularly, in addition to incorporation of capacitors C 9 , C 10  and resistors R 6 , R 7 , a separate imbalancing resistor R 8  may be added between winding T 2 - 2  and the output line leading to output winding T 2 - 1 , placing resistor R 8  in series with base drive winding T 2 - 2 . Addition of imbalancing resistor R 8  provides an imbalance in the output of ballast circuit  10 , allowing for an improvement in the even harmonic voltage supplied to the lamps. Such an even harmonic voltage will, again, act to minimize or eliminate visible striations in the lamp or lamps. 
     It is to be appreciated in  FIG. 3 , resistor R 8 ′ may alternatively be inserted in series with base drive winding T 2 - 3  of the second or lower control circuit  18  and the emitter of BJT switch Q 2  (as shown in dotted line) to obtain the higher, even harmonic supply voltage for the lamps. Still further, if R 8  and R 8 ′ are used at the same time, R 6  and R 7  could be eliminated. 
     Addition of capacitors C 9  and C 10 , causes the current needed during turn-on and turn-off of the BJT switches to be provided when the sinusoidal drive winding (e.g., from drive windings T 2 - 2 , T 2 - 3 ) voltages are low, i.e., at crossover. Further, in addition to reducing the dead time when both BJTs are in an “on” state, this design also reduces switching losses. Such an arrangement reduces the circulating current, and therefore as a result the efficiency of the inverter increases. Because the peak of the lamp&#39;s current is directly related to the dead time, the smaller the overlap of the BJTs, the lower the crest factor. Increasing the ballast efficiency and, therefore, the lighting system efficiency. 
     While the values of specific components of the present newly described circuit will depend in part on particular implementations, including operating frequency of the ballast, in at least one embodiment, resistors R 4  and R 5  may be in the range of 30-100 ohms and particularly 40 ohms. Resistors R 6  and R 7  may be in the range of 1-10 ohms, particularly 5 ohms, and capacitors C 9 , C 10  may be in the range of 47 nanofarads to 0.22 microfarads. Imbalancing resistor R 8  may be in the range of 1-5 ohms. 
     As previously discussed,  FIGS. 1 and 2  illustrates the present concepts are suitable for current fed BJT inverter ballasts, including half-bridge ballast inverters. However, this is not intended to limit the present concepts to the circuit of  FIGS. 1 and 2 , but rather the concepts may be used in other BJT based circuits such as other current fed half-bridge and full-bridge ballast circuits, including push-pull current fed ballast inverters, as well as voltage fed series resonant ballasts. The design is also useful with high content Krypton mixture, or other appropriate gas mixture, lamps used in non-dimming or dimming applications. 
     The invention has been described with reference to the preferred embodiments. Obviously, modifications and alterations will occur to others upon reading and understanding the preceding detailed description. It is intended that the invention be construed as including all such modifications and alterations.