Reduction of vertical segregation in a discharge lamp

• US 6,184,633 B1
• Filed: 06/17/1999
• Issued: 02/06/2001
• Est. Priority Date: 06/17/1999
• Status: Expired due to Fees

• Current Assignee: Philips Electronics North America Corporation (Koninklijke Philips N.V.)
• Original Assignee: Philips Electronics North America Corporation (Koninklijke Philips N.V.)
• Inventors: Kramer, Jerry M.
• Primary Examiner(s): Wong, Don
• Assistant Examiner(s): Dinh, Trinh Vo
• Application Number:
  US09/335,020
• Time in Patent Office: 600 Days
• Field of Search: 315/246, 315/174, 315/291, 315/307, 315/326, 332/120, 332/149, 332/117, 332/179
• US Class Current: 315/246
• CPC Class Codes: H05B 41/2928 for protecting the lamp against abnormal operating conditions
• CPC Class Codes: Y02B 20/00 Energy efficient lighting technologies, e.g. halogen lamps or gas discharge lamps

Abstract

An apparatus for reducing vertical segregation of a discharge lamp. A current/voltage input sweeps through a frequency range between the first azimuthal acoustic resonance mode and a first radial acoustic resonance mode of the discharge lamp. The current/voltage input is subsequently amplitude modulated. Alternatively, without amplitude modulation, the current/voltage input sweeps through the frequency range for a first portion of the period, and then for a second portion of the period drops to a relatively constant frequency.

Claims

1. An apparatus for operating a high-intensity discharge lamp, which comprises:

an amplitude modulator with a first input, a second input and an output coupled to the lamp,

means for providing a current to said first input, said current periodically sweeping from a first frequency to a second frequency in a sweep time; and

means for providing to said second input a modulating frequency which excites a longitudinal mode of the lamp wherein metal halides within the lamp are moved along the lamp axially in response to the level of longitudinal mode excitation.

2. The apparatus of claim 1, wherein said first frequency and said second frequency define a frequency range which is between a first azimuthal acoustic resonance mode and a first radial acoustic resonance mode of said lamp.

3. The apparatus of claim 2, wherein said first frequency is substantially equal to 45 kHz and said second frequency is substantially equal to 55 kHz.

4. The apparatus of claim 1, wherein said sweep time is substantially equal to ten milliseconds.

5. The apparatus of claim 4, wherein said modulating frequency is substantially equal to 24.5 kHz.

6. The apparatus of claim 5, wherein said modulator has an amplitude modulation index of substantially 0.24.

7. An apparatus for operating a high-intensity discharge lamp, which comprises:

means for providing an input power signal to the high-intensity discharge lamp, and

means for varying said input power signal over a period, said period having a first portion and a second portion,

wherein the input power signal sweeps from a first frequency to a second frequency during said first portion of said period and wherein said input power signal maintains a substantially constant third frequency during said second portion of said period, and wherein the third frequency excites a longitudinal mode of the lamp and wherein metal halides within the lamp are moved along the lamp axially and vertical segregation of light output from said lamp is reduced in response to the longitudinal mode excitation.

8. The apparatus of claim 7, wherein said substantially constant third frequency is substantially equal to one half of a power frequency of a longitudinal acoustic mode of the lamp.

9. The apparatus of claim 8, wherein said substantially constant third frequency is substantially equal to 12.3 kHz.

10. The apparatus of claim 9, wherein said first frequency is substantially equal to 45 kHz and said second frequency is substantially equal to 55 kHz.

11. The apparatus of claim 7, wherein said first portion of said period is substantially equal to 7.5 milliseconds and said second portion of said period is substantially equal to 2.5 milliseconds.

12. The apparatus of claim 7, wherein the apparatus is without an amplitude modulator.

13. An apparatus for operating a high intensity discharge lamp comprising:

an amplitude modulator having a first input, a second input and an output coupled to the lamp,

means for providing a current to said first input, said current periodically sweeping from a first frequency to a second frequency in a sweep time, and

means for providing to said second input an amplitude modulating signal at a modulating frequency which excites a longitudinal acoustic mode of the lamp whereby vertical color segregation in the lamp is reduced in response to said longitudinal acoustic mode excitation.

14. The apparatus as claimed in claim 13 wherein said first frequency and said second frequency define a frequency range which is between a first azimuthal acoustic resonance mode and a first radial acoustic resonance mode of said lamp.

15. The apparatus as claimed in claim 13 wherein the modulating signal is a non-pulsatory constant frequency signal which amplitude modulates the frequency swept current.

16. The apparatus as claimed in claim 13 wherein the amplitude modulation frequency is lower than the current frequency.

17. The apparatus as claimed in claim 13 wherein the amplitude modulating frequency corresponds to a second longitudinal acoustic mode of the lamp.

18. The apparatus as claimed in claim 13 which further comprises means for sweeping the amplitude modulating frequency over a small frequency range relative to a frequency range defined by said first frequency and said second frequency.

19. An apparatus for operating a high intensity discharge lamp comprising:

means for supplying over a time period a varying input power signal to the high intensity discharge lamp without amplitude modulation thereof, said input power signal having a first portion and a second portion of said time period such that the input power signals sweeps from a first frequency to a second frequency during said first portion of said time period and wherein said input power signal maintains a substantially constant third frequency during the second portion of said time period, and wherein the third frequency excites a longitudinal acoustic mode of the lamp whereby vertical segregation of light output from said lamp is reduced in response to the longitudinal acoustic mode excitation.

20. The apparatus as claimed in claim 19 wherein said substantially constant third frequency is substantially equal to one half of a power frequency of a longitudinal acoustic mode of the lamp.

21. The apparatus as claimed in claim 19 further comprising means for sweeping the input power signal during said second portion of said period over a small frequency range relative to a frequency range defined by said first frequency and said second frequency.

22. The apparatus as claimed in claim 19 further comprising means for alternating the frequency of the input power signal during said second portion of said period between a fourth fixed frequency and a fifth fixed frequency.

23. A method of operating a high intensity discharge lamp, comprising:

supplying the high intensity discharge lamp with an input power waveform,

stabilizing an arc discharge of the lamp by periodically sweeping the frequency of said input power waveform from a first frequency to a second frequency in a sweep time period, and

exciting a longitudinal acoustic mode in said lamp.

24. The method as claimed in claim 23 wherein said longitudinal acoustic mode is excited in the lamp by amplitude modulating the input power waveform with a modulating frequency.

25. The method as claimed in claim 24 wherein said modulating frequency is lower than any frequency in a frequency range defined by said first frequency and said second frequency.

26. The method as claimed in claim 23 wherein the amplitude modulating frequency corresponds to a second longitudinal acoustic mode of the lamp.

27. The method as claimed in claim 23 wherein the arc discharge is stabilized by periodically sweeping the frequency of said input power waveform from the first frequency to the second frequency in a first portion of the sweep time period, and

said longitudinal acoustic mode is excited in the lamp by maintaining the frequency of said input power waveform at a substantially constant third frequency during a second portion of the sweep time period.

28. The method as claimed in claim 27 wherein said substantially constant third frequency is substantially equal to one half of a power frequency of a longitudinal acoustic mode of the lamp.