Traditionally, dimming of hot cathode fluorescent lamps is accomplished by controlling the operating frequency of a series resonant inverter that drives all the lamps in series. A closed loop control circuit regulates the lamp current or power to adjust the lumen output of the lamp to provide dimming.
In order to provide a satisfactory life of the lamp, a cathode voltage is provided to the lamp cathodes with increasing value as the lamp is dimmed. This applied cathode voltage has the effect of heating the cathode in such a way as to reduce the sputtering effect of the lamp at lower operating currents when operated in a dimmed mode. The cathode voltage continuously supplies the cathode heating, although at an increased voltage, as the lamp is dimmed.
The dimming system and method described heretofore has some disadvantages. First, a series lamp configuration results in an increase in maintenance costs relative to a parallel lamp configuration. All lamps in a series configuration will fail if one lamp fails. This failure mode necessitates service calls every time one lamp fails. Secondly, a continuously supplied voltage to the cathodes, even when the lamp is providing 100% lumen output, is an inefficient technique for dimming. The cathodes dissipate up to 3 watts or 10% of the system power for each lamp without producing any visible light.
This disclosure provides a ballast circuit and method of dimming lamps that overcomes some of the disadvantages associated with a continuously supplied cathode voltage lighting system. In addition, this disclosure also demonstrates a method for parallel lamp dimming.
A ballast lamp circuit comprising an inverter circuit configured to convert a dc waveform to a first ac current waveform for driving a first lamp; and a cathode heating circuit operatively connected to the inverter circuit and configured to generate a second ac waveform for heating the electrodes of the first lamp, the RMS value of the second ac waveform decreasing as the RMS value of the first ac current waveform increases, and the RMS value of the second ac waveform increasing as the RMS value of the first ac current waveform decreases, wherein the RMS value of the first and second ac waveform are controlled with pulse width modulation.
A method of operating a hot cathode lamp, comprising driving one or more lamps with a lamp current to produce a lamp lumen output, the lamp lumen output decreasing as the lamp current RMS value is decreased and increasing as the lamp current is increased by the control of the lamp current via pulse width modulation; and supplying a pulse width modulated cathode heating voltage that is synchronized with the lamp's current to the electrodes of the one or more lamps, the cathode heating voltage decreasing as the lamp current is increased and increasing as the lamp current is increased, the cathode heating voltage limited to a minimum voltage when the lamp current is less than a predetermined value and the cathode heating voltage is at a minimum or zero when the lamp current is more than a predetermined value.
With reference to
A voltage supply 12 provides an AC line voltage to the ballast lamp circuit 10. The voltage supply 12 can include a wide range of voltages depending on the line voltages available. For example, 120V and 277V are typically available in the U.S., however, other line voltages can be utilized to supply the ballast circuit.
The ballast circuit 10 includes an EMI filter 14, an AC to DC PFC circuit 16, and a High Frequency Inverter circuit 18. The High Frequency Inverter circuit 18 includes a Cathode Heating power source 24, a Cathode Heating switching transistor Q126, switching capacitor C128 and transformer T130. This ballast circuit 10 is utilized to drive Lamp 120 and Lamp 222, however, additional lamps can be added to this circuit. Moreover, the ballast circuit 10 illustrated in
The operation of the ballast circuit is now described. As previously discussed, an AC line voltage 12 provides power to the ballast circuit. The AC line voltage 12 is initially filtered by an EMI filter 14, and subsequently fed to an AC to DC PFC circuit 16. The AC to DC PFC circuit 16 converts the filtered AC line voltage to a DC voltage. This DC voltage is fed to a High Frequency Inverter circuit 18 to be inverted to a high frequency ac waveform for driving lamps 20 and 22, and an ac waveform to heat cathodes 21, 23, 25 and 27 of the lamps when dimming.
Operation of the High Frequency Inverter circuit 18 to drive Lamps 120 and 222 will now be described with reference to a bi-level lumen output. However, the ballast circuit illustrated in
With reference to
With further reference to
Transistor Q126 provides the control to produce the V cathode waveforms of
During a dimmed lamp mode of operation, the switching of Q126 is controlled to provide a voltage at cathodes 21, 23, 25 and 27 of Lamp 1 and Lamp 2 to maintain proper heating of the cathodes while I lamp is at the minimum of the lamp rated current. The proper heating of the cathodes is the amount of heating, i.e. V cathode RMS, necessary to maintain an acceptable cathode temperature to minimize sputtering.
The technique described heretofore to control the RMS value of the voltage applied to the cathodes of Lamp 120 and Lamp 222 is synchronized with the pulse width modulation (PWM) dimming of the lamp's current. In general, the lower the Lamp lumen output, the higher the duty ratio of pulse width modulated voltage generated and applied to the Lamp cathodes. In contrast, the higher the lamp current, the lower the duty ratio of the pulse width modulated voltage generated and applied to the lamp cathodes.
Stated another way, as the pulse width of the positive cathode voltage increases, the RMS voltage across the cathode increases, thereby providing a relative increase in energy to heat the cathode. Conversely, as the pulse width of the positive cathode voltage decreases, the RMS voltage across the cathode decreases, thereby providing a relative decrease in energy to heat the cathode. As the lamp(s) reach their maximum rated power, the cathode heating voltage approaches a minimum or zero RMS volts depending on the type of lamp and inverter circuit used.
It should be noted the vertical bars illustrated in
As substantially described above, this disclosure describes a ballast lamp circuit comprising an inverter circuit and a cathode heating circuit operatively connected to the inverter circuit. The inverter circuit and cathode heating circuit are operatively connected to one or more lamps to provide multiple lumen output levels, i.e. dimming, while maintaining a minimum cathode temperature for reducing sputtering of the one or more lamps.
Variations of the ballast lamp circuit 10 illustrated in
Other variations include the High Frequency Inverter circuit comprising two or more inverter and cathode heating circuits as described, wherein multiple lamps are driven and dimmed to produce a multitude of dimming modes.
With regard to controlling the substantially inverse relationship between the lamp(s) current and cathode voltage, multiple configurations of the ballast lamp circuit described heretofore are available. In general, these configurations control the lamp current circuit and cathode heating voltage circuit to generate a cathode heating ac voltage with an RMS value which decreases as the RMS value of the ac lamp current increases. In addition to this inverse relationship between the lamp current and cathode heating voltage, predetermined limits can be implemented via programming of the controller or hardware implementation to provide a minimum cathode heating voltage and/or a maximum cathode heating voltage.
As previously discussed, the cathode voltage RMS value is controlled via PWM. For example, a relatively low frequency oscillator voltage, i.e. 100 Hz to 1 kH, is generated by the cathode heating circuit and this oscillator voltage is pulse width modulated to provide the appropriate RMS voltage to the cathodes of the lamps. As the lamp current is increased, the cathode voltage is decreased by reducing the pulse width of the cathode heating circuit oscillator voltage. The opposite scenario takes place for a decrease in lamp current. Specifically, the lamps are dimmed, the RMS value of the cathode voltage is increased by increasing the width of the pulse width modulated cathode voltage waveform.
Embodiments of this disclosure comprise a synchronous or nonsynchronous operation with regard to the control of the cathode voltage as related to the lamp current. For synchronous operation, one embodiment, as illustrated in
A nonsynchronous relationship between the lamp current and cathode voltage, as described above, is also within the scope of this disclosure. For example, where the lamp current and cathode voltage are independently controlled.
Examples of other variations for PWM control comprise a PWM voltage RMS related to a frequency modulated lamp current and a PWM voltage RMS related to an amplitude modulated lamp current.
With reference to
In one embodiment of this disclosure,
With reference to
In one embodiment,
With reference to
In one embodiment,
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.
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Number | Date | Country | |
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