Wedding ring shaped excitation coil

Details Wedding ring shaped excitation coil Wedding ring shaped excitation coil

2000-07-14

2001-12-04

Philogene, Haissa (Department: 2821)

Electric lamp and discharge devices: systems

Pulsating or a.c. supply

Induction-type discharge device load

C315S039000, C315S344000, C313S231410, C313S153000, C313S634000

Reexamination Certificate

active

06326739

ABSTRACT:

BACKGROUND
1. Field of the Invention
The invention relates generally to discharge lamps. The presently claimed invention relates more specifically to novel excitation coils for inductively coupled electrodeless lamps.
2. Related Art
In general, the present invention relates to the type of lamps disclosed in U.S. Pat. Nos. 5,404,076 and 5,903,091, each of which is herein incorporated by reference in its entirety.
Electrodeless lamps are known in the art. Such lamps may be characterized according to the type of discharge they produce. Electrodeless discharges may be classified as either E discharges, microwave discharges, travelling wave discharges, or H discharges. The invention relates to those discharges preponderantly characterized as H discharges.
FIG. 1
is a schematic diagram of a conventional electrodeless lamp which produces an H discharge. Electrodeless lamps which produce an H discharge are also referred to as inductively coupled lamps. Inductively coupled lamps were described more than 100 years ago by J. J. Thomson in the article “On the discharge of Electricity through Exhausted Tubes without Electrodes,” printed in the London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science, Fifth Series, Vol. 32, No. 197, October 1891. More recently, D. O. Wharmby, PhD surveyed the state of the electrodeless lamp art in the article entitled “Electrodeless lamps for lighting: a review,” IEEE PROCEEDINGS-A, Vol. 140, No. 6, November 1993, pages 465 to 473.
Certain aspects of the operation of inductively coupled lamps are well understood and have been characterized analytically, for example, in articles by R. B. Piejack, V. A. Godyak and B. M. Alexandrovich entitled “A simple analysis of an inductive RF discharge,” Plasma Sources Sci. Technol. 1, 1992, pages 179-186, and “Electrical and Light Characteristics of RF-Inductive Fluorescent Lamps,” Journal of the Illuminating Engineering Society, Winter 1994, pages 40-44.
Inductively coupled lamps having various bulb and coil configurations are described in U.S. Pat. No. 843,534, entitled “Method of Producing Electric Light.” More recently, inductively coupled lamps having novel excitation coils are described in U.S. Pat. Nos. 4,812,702, 4,894,591, and 5,039,903 (hereinafter, “the '903 patent”).
As shown in
FIG. 1
, one example for a conventional inductively coupled lamp includes a low frequency power source
31
providing power to a coil
32
which is wound around a gas-filled vessel
33
. The alternating current around the coil
32
causes a changing magnetic field, which induces an electric field which drives a current in the plasma. In effect, the plasma can be analyzed as a single turn secondary to the coil
32
. See Piejack et al., referenced above. An H discharge is characterized by a closed electrical field, which in many examples forms a visible donut-shaped plasma discharge.
Other geometries have been disclosed for inductively coupled lamps. For example,
FIG. 1
of the Wharmby article set forth examples (a)-(e), including a high inductance coil wound on a ferrite toroid, internal (or optionally external) to the bulb. See Wharmby at p. 471.
As used herein, “low frequency” with respect to an inductively coupled lamp is defined as a frequency less than or equal to about 100 MHz. For example, a typical operating frequency for conventional inductively coupled lamps is 13.56 MHz. For example, the '903 patent discusses an operating frequency range of 1 to 30 MHz, with an exemplary operating frequency being 13.56 MHz. Most, if not all, of the developments relating to known inductively coupled lamps provide lamps operating at low frequency (i.e. less than or equal to about 100 MHz).
Referring again to
FIG. 1
, during the starting operation of an inductively coupled lamp, an E field ionizes the fill in the gas-filled vessel
33
and the discharge is initially characteristic of an E discharge. Once breakdown occurs, however, an abrupt and visible transition to the H discharge occurs. During operation of an inductively coupled lamp, both E and H discharge components are present, but the applied H discharge component provides greater (usually much greater) power to the plasma than the applied E discharge component.
As used herein, “high frequency” with respect to an electrodeless lamp is defined as a frequency substantially greater than about 100 MHz. The prior art describes electrodeless lamps operating at high frequency, including lamps exhibiting coil structures. However, none of the “high frequency” electrodeless lamps in the prior art are, in fact, inductively coupled lamps.
For example, U.S. Pat. No. 4,206,387 describes a “termination fixture” electrodeless lamp which includes a helical coil around the bulb. The “termination fixture” lamp is described as operating the range from 100 MHz to 300 GHz, and preferably at 915 MHz. As noted by Wharmby, “termination fixture” lamps have a size-wavelength relationship such that they produce a microwave discharge, not an inductively coupled discharge.
U.S. Pat. No. 4,908,492 (hereinafter “the '492 patent”) describes a microwave plasma production apparatus which includes a helical coil component. The apparatus is described as operating at 1 GHz or higher, and preferably at 2.45 GHz. As disclosed, however, the coil need not be terminated and a large diameter, multi-turn coil is preferred to produce a large diameter plasma. In such a configuration, the dimension of the exciting structure is comparable to the wavelength of the microwave frequency power and the discharge appears to be a travelling wave discharge, a microwave discharge, or some combination thereof. In any event, the resulting structure apparently does not operate by inductive coupling.
U.S. Pat. No. 5,070,277 describes an electrodeless lamp which includes helical couplers. The lamp is described as operating in the range of 10 MHz to 300 GHz, with a preferred operating frequency of 915 MHz. The helical couplers transfer energy through an evanescent wave which produces an arc discharge in the lamp. The arc discharge is described as very straight and narrow, comparable to an incandescent filament. Hence, this lamp apparently does not operate by inductive coupling.
U.S. Pat. No. 5,072,157 describes an electrodeless lamp which includes a helical coil extending along a discharge tube. The operating range for the lamp is described as 1 MHz to 1 GHz. The discharge produced by the lamp is a travelling wave discharge. The effect of the helical coil is discussed as enhancing the light output and providing some RF screening.
Japanese publication No. 8-148127 describes a microwave discharge light source device which includes a resonator inside the microwave cavity which has the shape of a cylindrical ring with a gap. The resonator is described as a starting aid and microwave field concentrator.
A number of parameters characterize highly useful sources of light. These include spectrum, efficiency, brightness, economy, durability (working life), and others. For example, a highly efficient, low wattage light source with a long working life, particularly a light source with high brightness, represents a highly desirable combination of operating features. Electrodeless lamps have the potential to provide a much longer working life than electroded lamps. However, low wattage electrodeless lamps have found only limited commercial applications.
SUMMARY
Various aspects, features, advantages, and applications of electrodeless lamps utilizing the novel excitation coils of the present invention may be understood with reference to the parent '230 application.
According to one aspect of the invention, an excitation coil is configured as a non-helical, semi-cylindrical conductive surface having less than one turn, in the general shape of a wedding ring. At high frequencies, the current in the coil forms two loops which are spaced apart and parallel to each other. Configured appropriately, the coil approximates a Helmholtz configuration.
According to another aspect of the present invention, an excitation coil for an ind

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