This disclosure relates to a pulse starting method and circuit to pulse the primary winding of a high voltage transformer used to start a gas discharge (e.g. High Intensity Discharge (HID)) lamp. A gas discharge lamp typically uses a ballast circuit to convert an AC line voltage to a Low frequency bi-directional voltage. The ballast circuit includes a converter to convert the AC line voltage to a DC voltage and an inverter which converts the DC voltage to a Low frequency bi-directional voltage. The inverter can take the form of a series half-bridge or full bridge type connected to a DC voltage bus. In addition, a pulse starting circuit can be provided to cold start the gas discharge lamp.
One method and circuit to of igniting an HID lamp is a circuit as illustrated in
A drawback of the method and circuit described above is the inability of the circuit of
The inefficiencies of the circuit of
Accordingly, an improved efficient pulse starting method and circuit are needed to start a gas discharge lamp.
According to one embodiment of this disclosure, a ballast for a gas discharge lamp is provided. The ballast includes a DC voltage bus; a full-bridge inverter circuit including a DC voltage bus input and a bi-directional voltage output circuit, the bi-directional voltage output circuit generating a bi-directional voltage of alternating half cycles, and the DC voltage bus input of the full-bridge inverter circuit connected to the DC voltage bus outputs. In addition a starting circuit is provided, the starting circuit generating a pulse at the leading edge of each alternating half cycle and the polarity of the pulse being the same as the polarity of each alternating half cycle.
As briefly discussed in the background section, a pulse starting circuit can be utilized to provide a cold start for a gas discharge lamp.
The pulse position with respect to the low frequency square wave of voltage, prior to ignition, is important. This position determines how long the electrodes conduct before the polarity is reversed. Reversing polarity reverses the roles that each electrode plays, whether the electrode is a cathode or an anode. When it's a cathode, it emits electrons into the plasma and consequently loses temperature which is needed for thermionic emission. Without a high enough temperature, the electrode operating as a cathode can sputter tungsten onto the arc tube wall, reducing the luminous output of the lamp. When the electrode operates as an anode, it can absorb heat from the accelerating electrons. Therefore, after the gas breaks down, it is important to wait as long as possible before the electrode polarity changes. This provides the maximum time for the anode to heat before it takes on the role of a cathode. Thus, sputtering of tungsten can be minimized.
The pulse starting circuit illustrated by
Illustrated in
The full bridge inverter circuit includes transistors Q16, Q28, Q310, and Q412. The control circuit 13 operates to supply gate voltages to Q16 and Q412, simultaneously, for a ½ cycle of the desired bi-directional alternating voltage output. The gate voltages switch Q16 and Q412 to a conducting state which provides a DC bus voltage Vc to drive a lamp 14. During the subsequent ½ cycle of the desired bi-directional alternating voltage output, the control circuit operates to supply gate voltages to Q28 and Q310, simultaneously, for the ½ cycle. The gate voltages switch Q28 and Q310 to a conducting state which provides a negative DC bus voltage Vc to drive the lamp 14. The result of repeatedly switching Q16 and Q412, then Q28 and Q310, generates a bi-directional alternating voltage output with an amplitude approximately equal to the DC voltage bus.
The lamp starting circuit includes a transformer T116 including primary 26 and secondary 28 windings, a sidac S118, a diode D120, a resistor R121, a current limiting resistor R222 and a charging capacitor C124. The interconnections of these components are illustrated in
After the full-bridge inverter circuit cycles a few times, approximately 1-10, during the cold lamp 14 turn on phase of lamp operations, C124 is charged during the Q16 and Q412 conducting state through diode D120, resistor R121 and resistor R222. The sidac S118 does not conduct until its breakover voltage is exceeded. This breakover voltage is selected to be nearly twice the minimum DC bus voltage. For example, a breakover voltage of 720 Volts, three 240 Volt sidacs connected in series, was selected to operate from a 450 Volt bus. Although not quite twice the DC bus voltage, the combined breakover voltage of three sidacs is about 720 Volts.
Resistor R222 is much less than resistor R121 for reasons that will be explained below. Resistor R121 is typically a value approximately equal to 2M ohms. Resistor R121 limits the amount of charge accumulated by capacitor C124 during the initial Q16 and Q412 conducting state, but will not reach the full DC bus voltage. During the subsequent initial Q28 and Q310 conducting state, current will not conduct through C124 because diode D120 blocks current flow through resistor R121 and the voltage across the sidac S118 is not sufficient to breakover the sidac S118. Consequently, the voltage across capacitor C124 does not change significantly from the voltage provided during the previous initial Q16 and Q412 conducting state. During subsequent Q16 and Q412 conducting states, capacitor C124 continues to charge, eventually charging to a voltage which will enable the sidac S118 to breakover. Breakover of sidac S118 occurs during the Q28 and Q310 conducting state after capacitor C124 charges to approximately the DC bus voltage during the Q16 and Q412 conducting state. The voltage across sidac S118 is equal to the DC bus voltage in addition to the voltage across capacitor C124. The total voltage across the sidac S118 can be nearly twice the DC bus voltage. Therefore, if the bus voltage is 450 Volts and the sidac S118 breakover voltage is 720 Volts for example, the sidac will fire sometime during the transition of the square wave causing a high voltage pulse to be generated during a polarity reversal. This allows the high voltage negative pulse to be generated across the lamp at the transition and yield a maximum warm-up time for the electrode should the lamp ignite during the upcoming ½ cycle. Breakover of sidac S118 creates a voltage across the primary winding T1a 26 of the transformer which generates a high negative voltage Vp at the lamp input through the secondary winding 28 of the transformer.
During the Q28 and Q310 conducting state, after the sidac S118 has initially broken over, capacitor C124 discharges through sidac S118 and charges to the negative DC bus voltage within one cycle of the Q28 and Q310 conducting state. During the subsequent Q16 and Q412 conducting state, the voltage across the sidac S118 will be approximately twice the DC bus voltage, enabling the sidac S118 to breakover and generate a high voltage Vp at the lamp input. During this Q16 and Q412 conducting state, capacitor C124 will discharge through sidac S118 and charge to the negative DC bus voltage. This cycle continues to repeat, generating a bi-directional voltage of alternating half cycle including a superimposed pulse, with no delay, at the leading edge of each alternating half cycle, the polarity of the pulse being the same as the polarity of each alternating cycle. The energy transfer associated with this charging pattern is orders of magnitude faster than what occurs through diode D120. This is why resistor R222 is selected to be relatively small in comparison to resistor R121. Since resistor R222 is used primarily as a damping element, its particular value is chosen to adjust the shape of the ignition pulse across the secondary winding 28.
The starting circuit continues to operate until the lamp 14 breaks over and the current is regulated, thereby causing the DC bus voltage to drop significantly (ex. 25 volts). The starting circuit charging capacitor C124 charges to the decreased bus voltage through diode D120, resistor R121 and resistor R222. Because the voltage across the sidac S118 never reaches the breakover voltage, the starting circuit does not trigger a pulse and remains disabled until the lamp 14 is turned off and back on, thereby increasing the DC bus voltage and restarting the pulse starting circuit as described.
The pulse starting circuit of this disclosure provides nearly zero power dissipation during normal operation of the lamp 14 when the starting circuit is not triggering. Nearly zero power dissipation is achieved because diode D120 prevents capacitor C124 from discharging through resistor R222 and resistor R121.
This disclosure has been described with reference to the exemplary embodiments. Obviously, modifications and alterations will occur to others upon reading and understanding the preceding detailed description. It is intended that the disclosure be construed as including all such modifications and alterations.
This application claims priority to and the benefit of U.S. provisional application No. 60/666,967, filed Mar. 31, 2005, which application is incorporated herein by reference in its entirety.
Number | Date | Country | |
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60666967 | Mar 2005 | US |