Lamp driving topology

Information

  • Patent Grant
  • 6559606
  • Patent Number
    6,559,606
  • Date Filed
    Tuesday, October 23, 2001
    23 years ago
  • Date Issued
    Tuesday, May 6, 2003
    21 years ago
Abstract
A lamp driving system that includes a first impedance and a second impedance coupled to the secondary side of a transformer, where the second impedance has a phase shifted value compared to the first impedance. Two lamp loads are connected in series together, and in parallel to the first and second impedances and to the transformer. The phase shift between the impedances ensures that the transformer need not supply double the striking voltage to strike the series-connected lamps. A difference in the resistance between the first and second impedances ensures that the lamps ignite in a specified sequence.
Description




BACKGROUND OF THE INVENTION




1. Field of the Invention




The present invention relates to a system and method for driving multiple loads. More particularly, the present invention relates to a system and method for driving two lamp loads connected in series.




2. Description of Related Art




CCFLs (cold cathode fluorescent lamps) are widely employed in display panels. CCFLs require approximately 1500 Volts (RMS) to strike, and require approximately 800 Volts (RMS) for steady state operation. In displays where two CCFLs are required, a conventional technique is to couple the lamps in parallel with the secondary side of step-up transformer. In multiple lamp systems, the conventional technique for driving the lamps is to couple the lamps together in parallel with one another to the transformer. While this ensures voltage control during striking, this topology also requires impedance matching circuitry for the lamps. Also, current control in this topology is difficult since the current conditions of each lamp must be monitored.




Accordingly, it is desirable to couple lamps in series since current control for series-connected lamps is idealized. However, connecting lamps in series requires the transformer to deliver a multiple of striking voltage for each lamp. This, obviously is untenable since most transformers are incapable of providing 3000 Vrms for striking, or are prohibitively expensive. Thus, there is a need to provide a lamp driving system that can drive two lamps coupled in series without straining the transformer to develop double the striking voltage.




SUMMARY OF THE INVENTION




Accordingly, the present invention provides a load driving system, comprising a transformer; a first impedance network coupled in series to a second impedance network, said second impedance network being phase-shifted with respect to the first impedance network, the first and second impedance networks coupled in parallel to a power source. A first load is coupled in series to a second load, the first and second loads are coupled in parallel to said first and second impedance networks.




In another embodiment, the present invention provides a circuit, comprising a first impedance network coupled in series to a second impedance network, said second impedance network being phase-shifted with respect to said first impedance network, said first and second impedance networks coupled in parallel to a power source; and a first load coupled in series to a second load, said first and second loads coupled in parallel to said first and second impedance networks.




In the present invention, the phase difference between the first and second impedance networks ensures that the power source deliver significantly less voltage the loads connected in series. Also, in other exemplary embodiments, the resistance difference between the first and second impedances ensures a desired load striking sequence.




It will be appreciated by those skilled in the art that although the following Detailed Description will proceed with reference being made to preferred embodiments, the present invention is not intended to be limited to these preferred embodiments. Other features and advantages of the present invention will become apparent as the following Detailed Description proceeds, and upon reference to the Drawings, wherein like numerals depict like parts, and wherein:











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

is a block diagram of one exemplary lamp driving system according to the present invention; and





FIG. 2

is an exemplary circuit diagram of the system of FIG.


1


.











DETAILED DESCRIPTION OF EXEMPLARY EMBODIMENTS




FIG.


1


. is a block diagram of one exemplary load driving system


10


according to the present invention. More specifically, the system


10


is an exemplary lamp driving system. The loads in this exemplary embodiment comprise two lamps, Lamp


1


and Lamp


2


, connected in series, however the present invention is to be broadly construed to cover any particular load. The transformer


12


delivers a stepped-up power source for the loads, Lamp


1


and Lamp


2


. In the following description, the transformer will be generically referred as a power source, and should be broadly construed as such. Those skilled in the art will recognize that conventional inverter topologies may be used to drive the primary side of the transformer


12


. Such inverter topologies include push-pull, Royer, half bridge, full bridge, etc., and all such inverters may be used with the lamp driving system


10


of the present invention. As an overview, the system


10


depicted herein permits two lamps to be connected in series without requiring double the voltage output of the secondary side of the transformer. The exemplary embodiments will be described herein with reference to cold cathode fluorescent lamps (CCFLs), however the present invention is applicable to any type of load.




The system


10


includes a high impedance network


14


coupled in series to a phase-shifted low impedance network


16


. These two networks together are coupled in parallel to the secondary side of the transformer


12


. Two lamps


18


and


20


(also referred to herein as Lamp


1


and Lamp


2


) are coupled in series to each other, and together in parallel across the impedance networks


14


and


16


. Lamp


1


is connected in parallel across the high impedance network


14


(with a return path across the low impedance network


16


as will be described below) and Lamp


2


is connected in parallel across the phase-shifted low impedance network


16


. Note that the “High” side of Lamp


1


is connected to the upper side of the transformer


12


, and Lamp


2


has the “High” side connected to the lower side of the transformer


12


. Voltage feedback circuitry


24


is coupled to the high impedance network


14


and the phase-shifted low impedance network


16


to generate a voltage feedback signal FB


V


indicative of the voltage appearing on Lamp


1


or Lamp


2


. The voltage feedback circuitry may comprise a peak detector or other type of circuitry as is known in the art. Current sense circuitry


22


is coupled to the Low side of Lamp


2


to generate a current feedback signal FB


C


indicative of power being delivered to Lamp


2


. The voltage and current feedback signals are generally utilized by the inverter (not shown) to adjust the voltage and power delivered by the transformer, as is understood in the art. The specific utilization of voltage and current feedback information for the present invention will be detailed below.




The present invention employs a high impedance network


14


and a low impedance network


16


. Additionally, network


16


is phase shifted with respect to network


14


. The network


14


comprises real components (resistance), and the network


16


is comprised of real and reactive components, or purely reactive components, provided that there exists an overall phase difference between network


16


and network


14


. Since network


16


is phase shifted with respect to network


14


, the total voltage (V


t


) developed across the combined network


14


and network


16


is given by the equation:








V




t


=(


x




2




+y




2


);  Eq. 1






where x is the voltage developed across the (real) high impedance network and y is the voltage developed across the phased (reactive) impedance network.




Lamp Striking and Operational Sequence




The operational characteristics of the lamp driving system


10


are described below. CCFLs require approximately 1500 Vrms for striking, and then approximately 800 Vrms for operating voltage. Initially, a striking voltage is applied to the secondary side of the transformer


12


. The high impedance network


14


receives a majority of this voltage because the resistance of network


14


is greater than the resistance of network


16


. Since two voltage drops are present (across network


14


and network


16


), the transformer delivers a voltage equal to the striking voltage of Lamp


1


, plus the voltage lost in network


16


. This voltage is dictated by the equation set forth above for V


t


. Lamp


2


does not have a return path until Lamp


1


strikes because the high impedance of Lamp


1


(before struck) and the high impedance of network


14


(compared to network


16


) which isolates Lamp


2


. Thus, Lamp


1


strikes first. Network


16


provides a return path for Lamp


1


.




The voltage required to strike Lamp


2


is approximately equal to the voltage to strike Lamp


1


, e.g., 1500 Vrms. Since Lamp


1


is already struck, there is an operational voltage of approximately 800 Vrms across the network


14


. Accordingly the controller needs to supply an additional striking voltage for Lamp


2


. This striking voltage is the voltage across networks


14


and


16


, i.e., the voltage is (1500


2


+800


2


), or approximately 1700V. The numerical examples provided above assume a purely reactive load in the phased low impedance network


16


. Thus, instead of needing to supply 3000 Vrms to strike lamps connected in series, the system


10


of the present invention significantly reduces the voltage requirements of the transformer and system components.




The impedance difference between network


14


and network


16


ensures a desired striking sequence. In the exemplary system


10


described above, Lamp


1


strikes first, with a return path through network


16


. Thus, as a general statement, the impedance value of network


16


is selected to ensure a return path for Lamp


1


. The impedance value is also a function of operating frequency, and thus may be changed according to the frequency characteristics of the system


10


. To ensure a striking sequence between Lamp


1


and Lamp


2


, qualitatively the resistance values of the two networks is selected such that network


14


initially receives a majority of the voltage delivered by the transformer. The larger the majority (i.e., the larger the resistance values between networks


14


and


16


) means the less voltage that must be developed by the transformer initially. The phase difference between network


14


and network


16


permits the present invention to utilize Eq. 1 to operate two lamps connected in series without requiring double the voltage output from the transformer.




Best Mode Implementation





FIG. 2

is an exemplary circuit diagram


10


′ of the lamp driving system


10


of FIG.


1


. Certain component values are set forth below, however, these component values are merely exemplary and may be changed according to the principles set forth herein without departing from the scope of the present invention. The high impedance network


14


comprises a resistor R


1


. Resistor R


2


is provided for voltage feedback data indication of voltage feedback across Lamp


1


. R


1


>>R


2


, so that a negligible voltage drop appears across R


2


. The phase shifted low impedance network comprises capacitor C


1


. The impedance value of the capacitor C


1


(given by ½πfC) is chosen in accordance with the principles set forth above, and in the example of

FIG. 2

is approximately 600 kΩ (assuming a 5 pF. capacitor operating at 50 KHz). In other words, the resistance of the high impedance network is approximately 5 times greater than the impedance of the low impedance network. Capacitor C


2


is provided to generate a voltage feedback signal indicative of voltage in Lamp


2


, and the value of C


2


is larger than C


1


so that a complete path for Lamp


1


is provided through C


1


(and through diode D


2


), rather than a short to ground through C


2


. In the figure, C


2


is approximately an order of magnitude larger than C


1


. D


1


and D


2


operate as blocking diodes for the negative half cycles for the AC voltage appearing across R


2


and C


2


, respectively.




The operation of the system


10


′ is set forth in the above-description of the system


10


in broad terms. Specific operation of system


10


′, by inspection, is as follows. Network


16


is phase-shifted 90 degrees from network


14


, thereby reducing the total voltage required by the transformer. Before any lamp is struck, the secondary side of the transformer


12


develops a voltage across network


14


and


16


equal to V


t


=(X


2


+y


2


); where x is the voltage developed across R


1


and y is the voltage developed across C


1


. X also represents the voltage required to strike Lamp


1


, i.e., 1500 Vrms. Since the resistance of R


1


is approximately 5 times greater than the resistance of C


1


, y is approximately 300 Vrms, yielding a total voltage of approximately 1530 Vrms. Lamp


1


has sufficient voltage to strike, and is provided a return path to the transformer


12


through C


1


. Once struck, Lamp


1


only requires approximately 800 volts. However, Lamp


2


still requires 1500 Vrms to strike. Since 800Vrms is already appearing across Lamp


1


and R


1


, the inverter is controlled (via voltage feedback circuit


24


) to deliver 1500 Vrms to the secondary side of the transformer to Lamp


2


for striking. However, because of the phase difference between networks


14


and


16


, the transformer need only deliver a total of approximately 1700 Vrms. This again is dictated by the equation: V


t


=(x


2


+y


2


); where x is the voltage developed across R


1


(800 Vrms) and y is the developed across C


1


which represents the voltage necessary to strike Lamp


2


(1500 Vrms). Also, since Lamp


1


is already struck, its intrinsic impedance reduces significantly compared with R


1


, and thus a return path for Lamp


2


to the top side of the transformer is provided through Lamp


1


.




As shown in

FIG. 2

, there are two voltage feedback components that generate the voltage feedback signal: a first voltage feedback signal generated by network


14


(FBV


1


) and a second voltage feedback signal generated by network


16


(FBV


2


). More specifically, FBV


1


is taken from the anode of diode D


3


, as generated across R


2


, and FBV


2


is taken from the anode of D


4


, as generated across C


2


. Both signals combine at node


30


. This configuration ensures that the larger signal of either FBV


1


or FBV


2


dominates the sensed voltage of the voltage feedback block


24


. Before Lamp


1


strikes, FBV


1


is larger than FBV


2


, and thus the transformer voltage is controlled by FBV


1


. After Lamp


1


strikes, FBV


1


drops since Lamp


1


requires less operating voltage. The voltage appearing on network


16


increases (because Lamp


2


has not yet struck), and thus voltage is controlled by FBV


2


until Lamp


2


strikes. Accordingly, output voltage of the transformer is controlled by FBV


1


or FBV


2


. As is recognized to one skilled in the art, controlling transformer output voltage directly is difficult because the transformer


12


exists in a floating state. However, in the present invention the relative voltage drops across networks


14


and


16


are known, and it is further known that the transformer voltage is approximately equal to the striking voltage of either Lamp


1


or Lamp


2


, as given by Eq. 1. After both lamps are turned on (struck), the output voltage of the transformer is lower than the striking voltage and the inverter controls lamp current via current feedback through Lamp


2


.




The present invention assumes the inverter connected to the primary of the transformer is capable of adjusting power delivered to the transformer based on the current and voltage feedback information, via an inverter controller. Such inverter controllers are well-known in the art, and generally use the feedback information to adjust a pulse width modulation switching scheme, such as provided by push-pull, Royer, half bridge and full bridge inverter topologies. Additionally, while the present invention makes specific reference to CCFLs, the present invention is equally applicable for driving many types of lamps and tubes known in the art, such as: metal halide lamps, sodium vapor lamps, and/or x-ray tubes.




Those skilled in the art will recognize numerous modifications to the present invention. For example, the feedback control circuitry


22


may also include time-out circuitry that generates an interrupt signal to the inverter controller to discontinue (or minimize) voltage appearing on the transformer if Lamp


1


and/or Lamp


2


does not strike within a predetermined time. Additional modifications are also possible. For example, the capacitive load representing the phase-shifted low impedance network


16


depicted in

FIG. 2

may be implemented with an inductive load without departing from the present invention. Also, the voltage feedback capacitor C


2


could be replaced with a resistor of similar resistance characteristics without significantly changing the operational characteristics of the exemplary embodiment depicted in FIG.


2


. Additionally, the resistance value of the low impedance network may be chosen to match or approximately match the resistance value of the high impedance network, however such an alteration would require the transformer to develop a higher voltage, and may require additional circuitry to ensure a desired lamp striking sequence. These and other modifications will be apparent to those skilled in the art, and all such modifications are deemed within the spirit and scope of the present invention, only as limited by the appended claims.



Claims
  • 1. A load driving system, comprising:a power source; a first impedance network coupled in series to a second impedance network, said second impedance network having a different impedance value and phase-shifted with respect to said first impedance network, said first and second impedance networks coupled in parallel to said power source; and a first load coupled in series to a second load, said first and second load coupled in parallel to said first and second impedance networks, respectively; wherein said impedance difference between said first and second impedance networks generating a selected sequence of initial voltage for said first and second loads.
  • 2. A system as claimed in claim 1, wherein said first impedance having a larger impedance value than said second impedance.
  • 3. A system as claimed in claim 1, said first impedance comprising a resistor and second impedance comprising a capacitor, wherein said first impedance having a larger impedance value than said second impedance.
  • 4. A system as claimed in claim 1, said first impedance comprising a resistor and second impedance comprising an inductor, wherein said first impedance having a larger impedance value than said second impedance.
  • 5. A system as claimed in claim 1, wherein said second impedance providing a return path for said first load to said power source.
  • 6. A system as claimed in claim 1, wherein said first load providing a return path for said second load to said power source.
  • 7. A system as claimed in claim 1, wherein the total voltage delivered by said power source, Vt, satisfies the equation Vt=(x2+y2); where x is the voltage developed across said first impedance network and y is the voltage developed across the phased impedance network.
  • 8. A system as claimed in claim 1, wherein said first load receiving a majority of initial voltage provided by said power source, thereafter said first load receiving an operational voltage less than said initial voltage.
  • 9. A system as claimed in claim 1, wherein said second impedance being approximately 90 degrees out of phase from said first impedance.
  • 10. A system as claimed in claim 1, further comprising voltage feedback circuitry coupled to said first and second impedances and generating a voltage feedback signal indicative of the voltage across said first and second impedances.
  • 11. A system as claimed in claim 1, further comprising current feedback circuitry coupled to the said second lamp and generating a current feedback signal indicative of current delivered to said second load.
  • 12. A system as claimed in claim 1, wherein said first and second loads each having a high side and a low side, said low sides coupled together and said high sides coupled to the power source.
  • 13. A lamp driving system, comprising:a transformer; a first impedance network coupled in series to a second impedance network, said first impedance network having a larger impedance value than said second impedance network, said first and second impedance networks coupled in parallel to a secondary side of said transformer; and a first lamp coupled in series to a second lamp, said first and second lamps coupled in parallel to said first and second impedance networks, respectively; wherein the said larger impedance value of said first compared to second impedance networks causing said first lamp to strike before said second lamp.
  • 14. A system as claimed in claim 13, said first impedance comprising a resistor and second impedance comprising a capacitor.
  • 15. A system as claimed in claim 13, said first impedance comprising a resistor and second impedance comprising an inductor.
  • 16. A system as claimed in claim 13, wherein said second impedance providing a return path for said first lamp between the top and bottom of said transformer.
  • 17. A system as claimed in claim 13, wherein said first lamp providing a return path for said second lamp between the top and bottom of said transformer once said first lamp is struck.
  • 18. A system as claimed in claim 13, wherein the total voltage delivered by said transformer, Vt, satisfies the equation Vt=(x2+y2); where x is the voltage developed across said first impedance network and y is the voltage developed across the phased impedance network.
  • 19. A system as claimed in claim 13, wherein said first lamp receiving a majority of initial voltage provided by said transformer so that said first lamp is struck first with a lamp striking voltage, thereafter said first lamp receiving an operational voltage less than said striking voltage; said second lamp receiving a striking voltage after said first lamp is struck.
  • 20. A system as claimed in claim 13, wherein said second impedance being approximately 90 degrees out of phase from said first impedance.
  • 21. A system as claimed in claim 13, further comprising voltage feedback circuitry coupled to said first and second impedances and generating a voltage feedback signal indicative of the voltage across said first and second impedances.
  • 22. A system as claimed in claim 13, further comprising current feedback circuitry coupled to the said second lamp and generating a current feedback signal indicative of current delivered to said second lamp.
  • 23. A system as claimed in claim 13, wherein said first and second lamps each having a high side and a low side, said low sides coupled together and said high sides coupled to the top and bottom of said transformer.
  • 24. A circuit, comprising a first impedance network coupled in series to a second impedance network, said second impedance network having a different impedance value and phase-shifted with respect to said first impedance network, said first and second impedance networks coupled in parallel to a power source; and a first load coupled in series to a second load, said first and second loads coupled in parallel to said first and second impedance networks; wherein said impedance difference between said first and second impedance networks generating a selected sequence of initial voltage for said first and second loads.
  • 25. A circuit, comprising a first impedance network coupled in series to a second impedance network, said second impedance network having a different impedance value and phase-shifted with respect to said first impedance network, said first impedance network having a larger impedance value than said second impedance network, said first and second impedance networks coupled in parallel to a power source; and a first lamp coupled in series to a second lamp, said first and second lamps coupled in parallel to said first and second impedance networks, respectively; wherein said impedance difference between said first and second impedance networks causing said first lamp to strike before said second lamp.
  • 26. A system as claimed in claim 1, wherein said loads selected from the group consisting of cold cathode fluorescent lamps, metal halide lamps, sodium vapor lamps and x-ray tubes.
  • 27. A system as claimed in claim 10, said voltage feedback circuitry comprising a first impedance coupled in series with said first impedance network generating a first component voltage feedback signal indicative of voltage appearing across said first impedance network, and a second impedance coupled in series with said second impedance network generating a second component voltage feedback signal indicative of voltage appearing across said second impedance network; said first and second component voltage feedback signals being tied together at a common node and wherein the larger of said first or second component voltage feedback signals representing said voltage feedback signal.
  • 28. A system as claimed in claim 10, wherein said voltage feedback signal being utilized to control voltage developed by said power source.
  • 29. A system as claimed in claim 27, wherein said first impedance having a resistance value less than the resistance value of said first impedance network; said second impedance having an impedance value larger than the resistance of said second impedance network.
  • 30. A system as claimed in claim 13, wherein said lamps selected from the group consisting of cold cathode fluorescent lamps, metal halide lamps, sodium vapor lamps, and x-ray tubes.
  • 31. A system as claimed in claim 21, said voltage feedback circuitry comprising a first impedance coupled in series with said first impedance network generating a first component voltage feedback signal indicative of voltage appearing across said first impedance network, and a second impedance coupled in series with said second impedance network generating a second component voltage feedback signal indicative of voltage appearing across said second impedance network; said first and second component voltage feedback signals being tied together at a common node and wherein the larger of said first or second component voltage feedback signals representing said voltage feedback signal.
  • 32. A system as claimed in claim 21, wherein said voltage feedback signal being utilized to control voltage developed by said transformer.
  • 33. A system as claimed in claim 31, wherein said first impedance having a resistance value less than the resistance value of said first impedance network; said second impedance having a resistance value larger than the resistance of said second impedance network.
  • 34. A system as claimed in claim 1, wherein said power source comprises a transformer.
US Referenced Citations (2)
Number Name Date Kind
3878431 Petrina Apr 1975 A
6222327 Shoji et al. Apr 2001 B1