Patent Application
20090322225
The present invention is directed to high-intensity discharge (HID) lamps and more particularly to an HID lamp with a starting aid.
HID lamps are started with a voltage that is higher than the operating voltage of the lamp and that provides an electric field sufficient to cause a breakdown, in the presence of an avalanche-initiating electron. Some starting aids use ultraviolet (UV) enhancers to assure the presence of the avalanche-initiating electron.
For example, U.S. Pat. No. 5,323,091 to Morris describes a UV starting aid for a metal halide arc discharge lamp that includes a cavity in a press seal of the arc tube, where the cavity includes part of the foil of the electrode seal. A ground plane is provided on the exterior of the press seal. The lamp is energized by charging the foil negative with respect to the ground. An electron leaks from a sharp edge of the foil and initiates a dielectric barrier discharge (DBD) in the cavity. The DBD produces UV and vacuum-UV (VUV) photons, depending on the fill gas and its pressure, which in order to facilitate ignition of the lamp have to reach the cathode in the main vessel. As the photons must travel through the press seal material their utility as a starting aid is diminished due to transmission losses
U.S. Pat. No. 6,201,348 to Nortrup et al. describes a starting aid for a metal halide discharge lamp in which an arc discharge tube is positioned inside a hermetically sealed jacket. The jacket contains a gas that aids in starting the discharge in the tube. An outer conductor extends on the outside of the jacket and is connected to one of the leads of the tube. When voltage is applied to the electrodes the presence of the external electrode concentrates the electric field near the adjacent internal electrode. This effect in itself helps the breakdown in the tube, but may also lead to formation of a DBD in the jacket. If the latter is the case then these photons must travel through the wall of the arc discharge tube and reach the cathode in the arc tube. Their effectiveness is greatly reduced because of lack of control over the location where the DBD may occur and its position with respect to the cathode. Additionally, the spectrum of the DBD photons depends strongly on the jacket fill gas and may be strongly absorbed by the gas before it reaches the cathode (typically N2, the DBD spectrum of which is shifted more toward visible light compared to Xe or Ar which contain strong UV and VUV components).
Butler et al. (U.S. Pat. No. 7,083,383) disclose a starting aid comprised of conducting strips embedded in the walls of the discharge space. Its primary purpose is to concentrate the electric field at the cathode to promote electron emission. Additionally, the aid can be viewed as a capacitively coupled external electrode and as such it may produce a DBD. This reference does not disclose formation of the photons or recognize the importance of the insulation and geometry in the production of the photons. U.S. Pat. No. 7,187,131 to Budinger discloses a starting aid with two loops of wire round the neck of each of the electrodes, where the loops are connected and fed with an ignition pulse. The starting aid extends over the light-emitting part of the lamp, affecting the optical properties of the lamp.
Hon (U.S. Pat. No. 4,010,397) discloses an arrangement for triggering a flash lamp in which a conductive patch is bonded to a portion of the outer surface of the lamp and extended over a part of the high voltage electrode. This patent also does not recognize the importance of the insulation and geometry in formation of the photons.
An object of the present invention is to provide a novel HID lamp and method for starting the lamp in which a UV starting aid for the lamp avoids the problems of the prior art.
A further object of the present invention is to provide a novel high-intensity discharge lamp and method in which the lamp includes a discharge vessel made of an insulator, and a cathode and anode. A V-shaped gap filled with gas is provided between the anode and a first region of the vessel directly adjacent to where the anode separates from an interior surface of the vessel. A secondary cathode is provided on an exterior surface of the vessel at the first region, where the secondary cathode is positioned so that the V-shaped gap and the first region are between the secondary cathode and the anode. An electric field in the first region sufficient to ionize the gas or eject free electrons from the insulating wall creates a DBD. The UV and VUV photons generated by the DBD impinge on the cathode and initiate a breakdown between the cathode and anode and start the lamp.
These and other objects and advantages of the invention will be apparent to those of skill in the art of the present invention after consideration of the following drawings and description of preferred embodiments.
With reference now to
The lamp 10 further includes a secondary cathode 30 on an exterior surface of the vessel at the first region 18 so that the V-shaped gap 22 with the gas 26 and the first region 18 of the solid insulator are between the secondary cathode 30 and the anode 16.
The secondary cathode 30 is connected to the cathode 14 via electrical conductor 41 with circuitry (not shown) suitable for the ignition specifications. Anode 16 is connected to the circuitry via a separate electrical conductor 43. An electric field in the V-shaped gap 22 forms at the first region 18 between the secondary cathode and anode and creates a DBD. The gas 26 is xenon or argon; the DBD in both produces UV and VUV photons via an excimer-molecule decay mechanism. The UV and VUV photons impinge on the cathode 14 to initiate a breakdown between the cathode and the anode, and thereby facilitate ignition of the lamp 10. It is to be noted that the polarities of the electrodes cannot be reversed: a ‘secondary anode’ will not create the desired DBD as the near-cathode electric field is insufficient to extract an electron in reasonable time.
The duration of the DBD is limited by the motion of ions—once they reach the insulating wall they extinguish the DBD. It has been found that the pulse of photons starts 50-100 ns after applying a voltage to the cathode and may last as long as a few (e.g., 1-5) microseconds. The VUV and UV photons provide the necessary energy needed to eject electrons from the cathode and to help them to ionize the gas.
In a preferred embodiment, the secondary cathode 30 is a ring around the first region of the vessel. The secondary cathode may also be a rod (shown as 30′ in dashed lines in
While embodiments of the present invention have been described in the foregoing specification and drawings, it is to be understood that the present invention is defined by the following claims when read in light of the specification and drawings.
