CA1298344C - High efficacy electrodeless high intensity discharge lamp - Google Patents
High efficacy electrodeless high intensity discharge lampInfo
- Publication number
- CA1298344C CA1298344C CA000578095A CA578095A CA1298344C CA 1298344 C CA1298344 C CA 1298344C CA 000578095 A CA000578095 A CA 000578095A CA 578095 A CA578095 A CA 578095A CA 1298344 C CA1298344 C CA 1298344C
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- CA
- Canada
- Prior art keywords
- lamp
- halide
- arc tube
- fill
- cerium
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J65/00—Lamps without any electrode inside the vessel; Lamps with at least one main electrode outside the vessel
- H01J65/04—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05B—ELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
- H05B41/00—Circuit arrangements or apparatus for igniting or operating discharge lamps
- H05B41/14—Circuit arrangements
- H05B41/24—Circuit arrangements in which the lamp is fed by high frequency ac, or with separate oscillator frequency
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/12—Selection of substances for gas fillings; Specified operating pressure or temperature
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J65/00—Lamps without any electrode inside the vessel; Lamps with at least one main electrode outside the vessel
- H01J65/04—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels
- H01J65/042—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels by an external electromagnetic field
Abstract
RD-17,640 HIGH EFFICACY ELECTRODELESS
HIGH INTENSITY DISCHARGE LAMP
Abstract of the Disclosure Improved efficacy and color rendition at white color temperatures is achieved in an electrodeless metal halide arc discharge lamp with a novel combination of arc tube fill materials, including sodium halide, cerium halide, and xenon. A preferred lamp structural configuration imparts further efficacy improvement at higher lamp operating temperatures and isothermal lamp operation.
HIGH INTENSITY DISCHARGE LAMP
Abstract of the Disclosure Improved efficacy and color rendition at white color temperatures is achieved in an electrodeless metal halide arc discharge lamp with a novel combination of arc tube fill materials, including sodium halide, cerium halide, and xenon. A preferred lamp structural configuration imparts further efficacy improvement at higher lamp operating temperatures and isothermal lamp operation.
Description
1298~44 RD-17,640 HIGH EFFICACY ELECTRODELESS
HIGH_INTENSITY DISCHARGE LAMP
Background of the Invention This invention relates generally to high intensity discharge lamps wherein the arc discharge is generated by a solenoidal electric field and more particularly to use of a novel combination of fill materials in the arc tube compo-nent of such lamp to generate white color lamp emission at improved efficacy and color rendering indices.
The lamps described in the present invention are part of the class referred to as high intensity discharge lamps (HID) because in their basic operation a medium to high pressure gas is caused to emit visible wavelength radiation upon excitation typically caused by passage of current through an ionizable gas such as mercury or sodium vapor.
The original class of such HID lamps was that in which the discharge current was caused to flow between a pair of electrodes. Since the electrode members in such electroded HID lamps were prone to vigorous attack by the arc tube fill materials, causing early lamp failure, the more recently developed solenoidal electric field lamps of this type have been proposed to broaden the choice of arc tube materials through elimination of the electrode component. Such more recently developed solenoidal electric field lamps are described in U.S. Patent Nos. 4,017,764; 4,180,763; and 4,591,759, all assigned to the assignee of the present invention, and generate a plasma arc in the arc tube compo-nent during lamp operation, all in a previously known manner.
Such electrodeless HID lamps suffer from a number of problems, however, which primarily cause these lamps to operate less efficiently than other type lamp designs. Lamp efficiency or "efficacy", as used in the present applica-tion, means luminous efficacy as measured in conventional terms of lumens per watt. A different type problem experi-enced with electrodeless lamps is that they exhibit lower ~298344 RD-17,640 than acceptable color rendering capability in order to be employed for general purpose illumination. More particu-larly, general purpose illumination requires that objects illuminated by a particular light source display much the same color as when illuminated by natural sunlight. Such requirement is measured by known standards such as the C.I.E. color rendering index values (CRI), and CRI values of 50 or greater are deemed essential for commercial accept-ability of lamps in most general lighting applications. A
still further requirement for commercially acceptable general purpose illumination is the white color temperature provided with such lamp, which is fixed at about 3000K for the warm white lamp, about 3500~K for the standard white lamp and about 4200K for the cool white lamp, as measured by the C.I.E. chromaticity x and y values. It is a further generally recognized principle that increasing efficacy for such type discharge lamps impairs the lamp color rendering capabilities. Thus, while the prior art electrodeless lamps partially meet the foregoing merit criteria as a result of utilizing some of the same arc tube fill materials that are employed in the present invention, it has not yet been recognized that a particular combination of all such arc tube materials is needed to achieve color improvement without adverse impact on efficacy in such lamps.
Accordingly, it is a principal object of the present invention to provide solenoidal electric field lamps demon-strating improvement in both efficacy and color rendition at white color temperatures.
Another object of the present invention is to provide a particular design for solenoidal electric field lamps which optimizes performance achieved with present arc tube fill materials.
Still another important object of the present invention is to operatively associate the arc tube fill materials for a solenoidal electric field lamp with the lamp structural 1298344 RD-17,640 configuration in a manner which optimizes the lamp perfor-mance.
The foregoing and other aspects of the present inven-tion together with the features and advantages thereof, will become apparent from the following detailed description, when read in connection with the accompanying drawings.
Summarv of the Invention In accordance with the invention, it has now been discovered that a particular combination of fill materials in the arc tube of an electrodeless metal halide arc lamp provides white color lamp emission at improved efficacy and color rendition. More particularly, this improved lamp construction features a light transmissive arc tube con-taining a fill which is mercury-free and comprises a combi-nation of sodium halide and cerium halide along with xenon gas in the proper weight proportions to generate white color lamp emission at an efficacy of 200 lumens per watt (LPW) or greater and accompanied by color rendering indices (CRI) of at least 50. The white color temperature for the improved lamps extends from about 3000~ up to about 5000~K so that such lamps are suitable for general illumination purposes.
Useful sodium and cerium halides in the present lamp fill can be selected from the group consisting of bromides, chlorides and iodides, including mixtures thereof such as sodium iodide (NaI) and cerium chloride (CeC13). The weightproportion of cerium halide is maintained no greater than the weight proportion of sodium halide in the present lamp fill in order to provide the aforementioned characteristics, with a reservoir of these fill materials in the arc tube being desirable to compensate for any loss of the individual constituents during lamp operation. With respect to the relative weight proportions of the aforementioned sodium and cerium halides, it has been found that too much sodium halide lowers CRI values whereas too much cerium halide RD-17,640 lowers lamp efficacy. The composite white color lamp emission provided with the aforementioned fill materials consists mainly of otherwise conventional high pressure sodium discharge emission to which has been added visible radiation provided by cerium halide which extends in a continuous manner over the 400 - 700 nanometer visible wavelength region.
The present improvement is further attributable to maintaining controlled proportions of xenon gas in the lamp fill. Specifically, the replacement of mercury with xenon at high pressures to serve as a barrier or buffer against undesirable transport of thermal energy from the arc dis-charge to the arc tube walls further enhances efficacious radiation output in the present lamp. First of all, the use of high pressure mercury vapor assymetrically broadens the sodium D-line emission in the red spectral region, which is undesirable, while xenon broadens the sodium D-line emission more symmetrically to contribute greater desirable emission in the yellow and green spectral region. Secondly, the relatively high excitation energy of xenon as compared with mercury precludes xenon radiation in the present lamp as distinct from the energy loss experienced in undesirable spectral regions when a radiating mercury discharge is employed. Moreover, arc voltages are lower with xenon than mercury in the present lamps, thereby making the present lamps easier to start and operate. A still further perfor-mance advantage experienced in the present lamps by replacing mercury with xenon in the arc tube fill is attrib-utable to the relatively lower thermal conductivity of xenon. Such lower thermal conductivity more effectively avoids undesirable dissocation of the halide materials in the arc discharge with subsequent recombination of the halide materials at or near the arc tube walls. A higher observed efficacy in electrodeless metal halide lamps having the above described sodium and cerium halide arc tube fills when xenon replaces the conventional mercury is also ~298344 RD-17,640 presumed attributable to avoiding a tie-up of said halides by the mercury constituent.
The amount of xenon employed in the present arc tube fill to achieve the above noted lamp performance gains is a sufficient quantity, dependent upc7n the arc tube internal volume, to limit the transport of thermal energy by conduc-tion from the arc discharge to the walls of the arc tube.
As above noted, the xenon buffer gas participates actively in achieving the performance gains primarily due to elimi-nating drawbacks which the conventional use of high pressure mercury buffering gas has now been found to cause in these lamps. Specifically, xenon may be present in a sufficient quantity, providing a partial pressure in the range of about 60 Torr and higher at room temperature or about 600 Torr and higher at the operating temperature of the lamp of the present invention in order to produce these performance gains. Increasing the xenon partial pressure to 500 Torr at room temperature can further improve the lamp performance.
For example, one tested lamp having a structural configura-tion of the "pillbox" type, hereinafter further described, wherein the arc tube measured 20 millimeters outside diame-ter, or O.D., x 17 millimeters in height, and was filled with 5 milligrams,~a~d 2.3 milligrams CeC13 along with xenon at 500 Torr partial pressure at room temperature, achieved 203 LPW efficacy and a 54 CRI value at a color temperature of 3699K. Similarly, a large size arc tube having the same structural configuration and filled with 101 milligrams NaI, 9.8 milligrams CeC13, 5 milligrams TlI, and xenon at a partial pressure of 200 Torr at room temperature, exhibited 193 LPW and 50.1 CRI at a color temperature of 3610K.
As above indicated, the present arc tube fill may include additional vaporizable metal atoms other than mercury to furnish still other radiating species in the arc discharge. The color of lamp emission can be altered, without adversely affecting performance, by employing minor amounts of indium halide and lithium halide to impart ~2983~4 RD- 17,640 monochromatic blue and red emission, respectively, as well as by employing a thallium halide addition to provide more green color emission to the lamp discharge. Other supple-mental lamp color temperature modifying atoms can be S employed in the arc discharge, including other alkali metals such as cesium, as well as alkaline earth metals, such as barium, and still further including other rare earth metals, to provide continuous radiation across the visible spectral region. To further illustrate a useful source in the lamp fill for the latter category of lamp color temperature modifying atoms, halides of dysprosium, holmium, ytterbium and thulium are contemplated as being chemically compatible in the present type lamp design. Accordingly, it follows that color temperature in the present lamps can be desirably lS modified, without deleterious effect upon either efficacy or color rendition, when the arc tube fill includes metal ions providing supplemental monochromatic radiation or continuous radiation in the visible spectral region, and further including both types of supplemental radiative species.
Since all radiating species in the present arc tube fill limit radiation output primarily to the visible spectral region, it can also be appreciated that energy losses in such lamps which decrease lamp efficacy, such as infrared losses, are thereby minimal.
A preferred lamp structural configuration utilizing the above disclosed arc tube materials of the present invention to optimize lamp performance features a cylindrically-shaped arc tube of a height less than its outside diameter, a light transmissive outer envelope disposed around the arc tube and defining a space therebetween, and excitation means for coupling radio-frequency energy to the arc tube fill. As such, these improved lamps can be operated as relatively isothermal devices not experiencing various thermal losses found in electroded lamps, particularly at the walls and ends, as well as found in prior art electrodeless lamps of the type having a relatively long and narrow arc tube.
RD-17,640 ~29834~
Since efficacy of high intensity discharge lamps is limited by such thermal losses, it becomes desirable to avoid such impairment to a greater extent than heretofore found possi-ble in prior art high intensity discharge lamps which generally are operated at cold spot wall temperatures of below 750C. By combining the above preferred lamp design configuration with the present arc tube materials it is now possible to achieve more nearly isothermal lamp operation, with cold spots around 900C, for an efficacy gain attribut-able to increased vapor pressure of the lamp fill. In thepreferred lamp design configuration, the arc tube can be formed of a high temperature glass, such as fused quartz, or an optically transparent ceramic, such as polycrystalline alumina. The filled arc tube generates a plasma arc during lamp operation by excitation from a solenoidal electric field employed in the lamp, all in known manner. The excitation is created by a magnetic field, changing with time, to establish within the tube an electric field which closes completely upon itself, resulting in the light-producing high intensity discharge. The excitation sourcein the preferred lamp design comprises an excitation coil disposed outside the outer lamp envelope and connected to a power supply through an impedance matching network. The spacing between the arc tube and outer envelope members in the preferred lamp device can be occupied by thermal energy barrier means, such as metal ba~fles or quartz wool, or even a vacuum. Such thermal barrier means desirably reduces heat loss from the lamp, which would otherwise be considerable due to the more elevated lamp operating temperatures and isothermal manner of lamp operation now being achieved.
Brief Description of the Drawings FIG. 1 is a cross-sectional side view depicting one electrodeless lamp configuration of the present invention employing the present arc tube material composition; and RD-17,640 FIG. 2 is a spectral emission diagram for a typical lamp construction utilizing the arc tube fill material composition of the present invention.
Detailed Description of the Preferred Embodiment FIG. 1 depicts an electrodeless arc discharge lamp which includes an arc tube 10 for containing a fill 11. Arc tube 10 comprises a light-transmissive material, such as fused quartz or a refractory ceramic material such as sintered polycrystalline alumina. An optimum shape for arc tube lO, as depicted, is a flattened spherical shape or a short cylindrical (e.g. hockey puck or pillbox) shape with rounded edges. The major diameter of arc tube 10 is also shown to be greater than its height dimension. An outer envelope 12 is disposed around arc tube 10. Outer enve-lope 12 is light-transmissive and may also be comprised of quartz or a refractory ceramic. Convective cooling of arc tube 10 is limited by outer envelope 12. A blanket of ~uartz wool 15 may also be provided between arc tube 10 and outer envelope 12 to further limit cooling. A primary coil 13 and a radio-frequency (RF) power supply 14 are employed to excite a plasma arc discharge in fill 11. As previously indicated, this configuration including pri-mary 13 and RF power supply 14 is commonly referred to as a high intensity discharge solenoidal electric field (HID-SEF) lamp. The SEF configuration is essentially a transformer which couples radio-frequency energy to a plasma, the plasma acting as a single-turn secondary for the transformer. An alternating magnetic field which results from the RF current in primary coil 13 creates an electric field in arc tube 10 which closes upon itself completely. Current flows as a result of the electric field and an arc discharge results in arc tube 10. A more detailed description for such HID-SEF lamp structures is found in previously cited U.S.
Patents 4,017,764 and 4,180,763 RD-17,640 An exemplary frequency of operation for RF power supply 14 is 13.56 megahertz. Typical power input to the lamp can be in the range of 100 - 2000 watts.
Lamps having the above described structural configura-5 tion were built and found to exhibit the spectral emissionc:urve depicted in FIG. 2. More particularly, the depicted emission curve represents such HID-SEF lamp emission, with the lamp further exhibiting a color temperature of around 3985K, a 182 LPW efficacy, and a 54.8 CRI value. The 10 depicted emission is provided in composite fashion formed by the line spectrum from a high pressure sodium discharge which further includes the visible spectral continuum, with cerium emission also being present in the lamp discharge.
The arc tube fill in this particular lamp consisted of 15 approximately 100 milligrams NaI, approximately S.l milli-grams TlI, approximately 19.8 milligrams CeC13 and xenon gas at a partial pressure of approximately 200 Torr at room temperature. The following examples are provided to demon-strate still other successfully tested arc tube fills for 20 the present metal halide arc lamp construction.
EXAMPLE I
An arc tube having 20 millimeter O.D. x 17 millimeter height dimensions was filled with approximately 6 milligrams NaI, 2.3 milligrams CeC13, and approximately 500 Torr 25 partial pressure of xenon gas at room temperature. The lamp operated at approximately 265 watts input power to produce 203 LPW and 54 CRI values at a color temperature of approxi-mately 3699K which approaches the cool white oval.
1298344 RD-17,640 EXAMPLE II
The same size arc tube as in Example I above was filled with approximately 6.1 milligrams NaI, 3 milligrams CeI3, and 500 Torr xenon partial pressure buffering gas at room temperature. The subsequent operation of the lamp at approximately 206 watts input power provided 195 LPW effi-cacy, 49 CRI, and a lamp color temperature of approximately 3290K which approaches the warm white color oval.
EXAMPLE III
In this example, an arc tube having dimensions of 15 millimeters O.D. x 13 millimeters in height was employed.
The arc tube fill consisted of approximately 1 milligram NaI
and 1 milligram CeC13 along with xenon gas at a partial pressure of approximately 500 Torr at room temperature.
When supplied with 202 watts input power, the lamp exhibited 185 LPW and 57 CRI at a color temperature of approximately 4856K which approaches other recognized white color ovals.
EXAMPLE IV
An arc tube having the same physical dimensions as in Example I above was filled with 6.1 milligrams NaI, 1.4 milligrams CeC13, 0.5 milligrams TlI, and 500 Torr partial pressure of xenon at room temperature. At 204 watts input power the lamp yielded 204 LPW and 49 CRI at a color temper-ature of 3381K which approaches the stand~ white color oval.
EXAMPLE V
An arc tube with an O.D. of 54 millimeters and 25 millimeters in height was filled with approximately 100 milligrams NaI, 5.1 milligrams TlI, 19.8 grams CeCl3, and 200 Torr partial pressure of xenon at room temperature.
When operated at 1087 watts input power the lamp demon-strated 182 LpW, 54.8 CRI and a color temperature of 3985K
which again approaches the cool white oval.
The above lamp embodiments exhibit optimum performance for a HID-SEF type lamp containing the present combination of arc tube fill materials including sodium halide, cerium halide and xenon gas. As has been shown, efficacy of over 200 LPW is gained, accompanied by CRI values of 50 or greater, and lamp color temperatures in the white color spectral region are varied by addition of still other vaporizable metal atoms which radiate in the lamp discharge.
As evident in the above examples, such supplemental radi-ating species are incorporated in the arc tube fill ashalide compounds so as to be vaporizible at the lamp oper-ating temperatures without requiring intermediate conver-sion.
The foregoing describes a broadly useful, improved HID
electrodeless lamp exhibiting superior performance. It will be apparent from the foregoing description, however, that various modifications in the specific embodiments above described can be made without departing from the spirit and scope of the present invention. For example, color cor-recting radiators other than those specifically illustratedcan be included in the present lamp fill in minor amounts to meet specific lamp requirements, so long as these radiators are compatible during lamp operation. Additionally, phys-ical configurations for the lamp other than those above disclosed are possible to make still better use of the lamp fill medium. It is intended to limit the present invention, therefore, only by the scope of the following claims.
HIGH_INTENSITY DISCHARGE LAMP
Background of the Invention This invention relates generally to high intensity discharge lamps wherein the arc discharge is generated by a solenoidal electric field and more particularly to use of a novel combination of fill materials in the arc tube compo-nent of such lamp to generate white color lamp emission at improved efficacy and color rendering indices.
The lamps described in the present invention are part of the class referred to as high intensity discharge lamps (HID) because in their basic operation a medium to high pressure gas is caused to emit visible wavelength radiation upon excitation typically caused by passage of current through an ionizable gas such as mercury or sodium vapor.
The original class of such HID lamps was that in which the discharge current was caused to flow between a pair of electrodes. Since the electrode members in such electroded HID lamps were prone to vigorous attack by the arc tube fill materials, causing early lamp failure, the more recently developed solenoidal electric field lamps of this type have been proposed to broaden the choice of arc tube materials through elimination of the electrode component. Such more recently developed solenoidal electric field lamps are described in U.S. Patent Nos. 4,017,764; 4,180,763; and 4,591,759, all assigned to the assignee of the present invention, and generate a plasma arc in the arc tube compo-nent during lamp operation, all in a previously known manner.
Such electrodeless HID lamps suffer from a number of problems, however, which primarily cause these lamps to operate less efficiently than other type lamp designs. Lamp efficiency or "efficacy", as used in the present applica-tion, means luminous efficacy as measured in conventional terms of lumens per watt. A different type problem experi-enced with electrodeless lamps is that they exhibit lower ~298344 RD-17,640 than acceptable color rendering capability in order to be employed for general purpose illumination. More particu-larly, general purpose illumination requires that objects illuminated by a particular light source display much the same color as when illuminated by natural sunlight. Such requirement is measured by known standards such as the C.I.E. color rendering index values (CRI), and CRI values of 50 or greater are deemed essential for commercial accept-ability of lamps in most general lighting applications. A
still further requirement for commercially acceptable general purpose illumination is the white color temperature provided with such lamp, which is fixed at about 3000K for the warm white lamp, about 3500~K for the standard white lamp and about 4200K for the cool white lamp, as measured by the C.I.E. chromaticity x and y values. It is a further generally recognized principle that increasing efficacy for such type discharge lamps impairs the lamp color rendering capabilities. Thus, while the prior art electrodeless lamps partially meet the foregoing merit criteria as a result of utilizing some of the same arc tube fill materials that are employed in the present invention, it has not yet been recognized that a particular combination of all such arc tube materials is needed to achieve color improvement without adverse impact on efficacy in such lamps.
Accordingly, it is a principal object of the present invention to provide solenoidal electric field lamps demon-strating improvement in both efficacy and color rendition at white color temperatures.
Another object of the present invention is to provide a particular design for solenoidal electric field lamps which optimizes performance achieved with present arc tube fill materials.
Still another important object of the present invention is to operatively associate the arc tube fill materials for a solenoidal electric field lamp with the lamp structural 1298344 RD-17,640 configuration in a manner which optimizes the lamp perfor-mance.
The foregoing and other aspects of the present inven-tion together with the features and advantages thereof, will become apparent from the following detailed description, when read in connection with the accompanying drawings.
Summarv of the Invention In accordance with the invention, it has now been discovered that a particular combination of fill materials in the arc tube of an electrodeless metal halide arc lamp provides white color lamp emission at improved efficacy and color rendition. More particularly, this improved lamp construction features a light transmissive arc tube con-taining a fill which is mercury-free and comprises a combi-nation of sodium halide and cerium halide along with xenon gas in the proper weight proportions to generate white color lamp emission at an efficacy of 200 lumens per watt (LPW) or greater and accompanied by color rendering indices (CRI) of at least 50. The white color temperature for the improved lamps extends from about 3000~ up to about 5000~K so that such lamps are suitable for general illumination purposes.
Useful sodium and cerium halides in the present lamp fill can be selected from the group consisting of bromides, chlorides and iodides, including mixtures thereof such as sodium iodide (NaI) and cerium chloride (CeC13). The weightproportion of cerium halide is maintained no greater than the weight proportion of sodium halide in the present lamp fill in order to provide the aforementioned characteristics, with a reservoir of these fill materials in the arc tube being desirable to compensate for any loss of the individual constituents during lamp operation. With respect to the relative weight proportions of the aforementioned sodium and cerium halides, it has been found that too much sodium halide lowers CRI values whereas too much cerium halide RD-17,640 lowers lamp efficacy. The composite white color lamp emission provided with the aforementioned fill materials consists mainly of otherwise conventional high pressure sodium discharge emission to which has been added visible radiation provided by cerium halide which extends in a continuous manner over the 400 - 700 nanometer visible wavelength region.
The present improvement is further attributable to maintaining controlled proportions of xenon gas in the lamp fill. Specifically, the replacement of mercury with xenon at high pressures to serve as a barrier or buffer against undesirable transport of thermal energy from the arc dis-charge to the arc tube walls further enhances efficacious radiation output in the present lamp. First of all, the use of high pressure mercury vapor assymetrically broadens the sodium D-line emission in the red spectral region, which is undesirable, while xenon broadens the sodium D-line emission more symmetrically to contribute greater desirable emission in the yellow and green spectral region. Secondly, the relatively high excitation energy of xenon as compared with mercury precludes xenon radiation in the present lamp as distinct from the energy loss experienced in undesirable spectral regions when a radiating mercury discharge is employed. Moreover, arc voltages are lower with xenon than mercury in the present lamps, thereby making the present lamps easier to start and operate. A still further perfor-mance advantage experienced in the present lamps by replacing mercury with xenon in the arc tube fill is attrib-utable to the relatively lower thermal conductivity of xenon. Such lower thermal conductivity more effectively avoids undesirable dissocation of the halide materials in the arc discharge with subsequent recombination of the halide materials at or near the arc tube walls. A higher observed efficacy in electrodeless metal halide lamps having the above described sodium and cerium halide arc tube fills when xenon replaces the conventional mercury is also ~298344 RD-17,640 presumed attributable to avoiding a tie-up of said halides by the mercury constituent.
The amount of xenon employed in the present arc tube fill to achieve the above noted lamp performance gains is a sufficient quantity, dependent upc7n the arc tube internal volume, to limit the transport of thermal energy by conduc-tion from the arc discharge to the walls of the arc tube.
As above noted, the xenon buffer gas participates actively in achieving the performance gains primarily due to elimi-nating drawbacks which the conventional use of high pressure mercury buffering gas has now been found to cause in these lamps. Specifically, xenon may be present in a sufficient quantity, providing a partial pressure in the range of about 60 Torr and higher at room temperature or about 600 Torr and higher at the operating temperature of the lamp of the present invention in order to produce these performance gains. Increasing the xenon partial pressure to 500 Torr at room temperature can further improve the lamp performance.
For example, one tested lamp having a structural configura-tion of the "pillbox" type, hereinafter further described, wherein the arc tube measured 20 millimeters outside diame-ter, or O.D., x 17 millimeters in height, and was filled with 5 milligrams,~a~d 2.3 milligrams CeC13 along with xenon at 500 Torr partial pressure at room temperature, achieved 203 LPW efficacy and a 54 CRI value at a color temperature of 3699K. Similarly, a large size arc tube having the same structural configuration and filled with 101 milligrams NaI, 9.8 milligrams CeC13, 5 milligrams TlI, and xenon at a partial pressure of 200 Torr at room temperature, exhibited 193 LPW and 50.1 CRI at a color temperature of 3610K.
As above indicated, the present arc tube fill may include additional vaporizable metal atoms other than mercury to furnish still other radiating species in the arc discharge. The color of lamp emission can be altered, without adversely affecting performance, by employing minor amounts of indium halide and lithium halide to impart ~2983~4 RD- 17,640 monochromatic blue and red emission, respectively, as well as by employing a thallium halide addition to provide more green color emission to the lamp discharge. Other supple-mental lamp color temperature modifying atoms can be S employed in the arc discharge, including other alkali metals such as cesium, as well as alkaline earth metals, such as barium, and still further including other rare earth metals, to provide continuous radiation across the visible spectral region. To further illustrate a useful source in the lamp fill for the latter category of lamp color temperature modifying atoms, halides of dysprosium, holmium, ytterbium and thulium are contemplated as being chemically compatible in the present type lamp design. Accordingly, it follows that color temperature in the present lamps can be desirably lS modified, without deleterious effect upon either efficacy or color rendition, when the arc tube fill includes metal ions providing supplemental monochromatic radiation or continuous radiation in the visible spectral region, and further including both types of supplemental radiative species.
Since all radiating species in the present arc tube fill limit radiation output primarily to the visible spectral region, it can also be appreciated that energy losses in such lamps which decrease lamp efficacy, such as infrared losses, are thereby minimal.
A preferred lamp structural configuration utilizing the above disclosed arc tube materials of the present invention to optimize lamp performance features a cylindrically-shaped arc tube of a height less than its outside diameter, a light transmissive outer envelope disposed around the arc tube and defining a space therebetween, and excitation means for coupling radio-frequency energy to the arc tube fill. As such, these improved lamps can be operated as relatively isothermal devices not experiencing various thermal losses found in electroded lamps, particularly at the walls and ends, as well as found in prior art electrodeless lamps of the type having a relatively long and narrow arc tube.
RD-17,640 ~29834~
Since efficacy of high intensity discharge lamps is limited by such thermal losses, it becomes desirable to avoid such impairment to a greater extent than heretofore found possi-ble in prior art high intensity discharge lamps which generally are operated at cold spot wall temperatures of below 750C. By combining the above preferred lamp design configuration with the present arc tube materials it is now possible to achieve more nearly isothermal lamp operation, with cold spots around 900C, for an efficacy gain attribut-able to increased vapor pressure of the lamp fill. In thepreferred lamp design configuration, the arc tube can be formed of a high temperature glass, such as fused quartz, or an optically transparent ceramic, such as polycrystalline alumina. The filled arc tube generates a plasma arc during lamp operation by excitation from a solenoidal electric field employed in the lamp, all in known manner. The excitation is created by a magnetic field, changing with time, to establish within the tube an electric field which closes completely upon itself, resulting in the light-producing high intensity discharge. The excitation sourcein the preferred lamp design comprises an excitation coil disposed outside the outer lamp envelope and connected to a power supply through an impedance matching network. The spacing between the arc tube and outer envelope members in the preferred lamp device can be occupied by thermal energy barrier means, such as metal ba~fles or quartz wool, or even a vacuum. Such thermal barrier means desirably reduces heat loss from the lamp, which would otherwise be considerable due to the more elevated lamp operating temperatures and isothermal manner of lamp operation now being achieved.
Brief Description of the Drawings FIG. 1 is a cross-sectional side view depicting one electrodeless lamp configuration of the present invention employing the present arc tube material composition; and RD-17,640 FIG. 2 is a spectral emission diagram for a typical lamp construction utilizing the arc tube fill material composition of the present invention.
Detailed Description of the Preferred Embodiment FIG. 1 depicts an electrodeless arc discharge lamp which includes an arc tube 10 for containing a fill 11. Arc tube 10 comprises a light-transmissive material, such as fused quartz or a refractory ceramic material such as sintered polycrystalline alumina. An optimum shape for arc tube lO, as depicted, is a flattened spherical shape or a short cylindrical (e.g. hockey puck or pillbox) shape with rounded edges. The major diameter of arc tube 10 is also shown to be greater than its height dimension. An outer envelope 12 is disposed around arc tube 10. Outer enve-lope 12 is light-transmissive and may also be comprised of quartz or a refractory ceramic. Convective cooling of arc tube 10 is limited by outer envelope 12. A blanket of ~uartz wool 15 may also be provided between arc tube 10 and outer envelope 12 to further limit cooling. A primary coil 13 and a radio-frequency (RF) power supply 14 are employed to excite a plasma arc discharge in fill 11. As previously indicated, this configuration including pri-mary 13 and RF power supply 14 is commonly referred to as a high intensity discharge solenoidal electric field (HID-SEF) lamp. The SEF configuration is essentially a transformer which couples radio-frequency energy to a plasma, the plasma acting as a single-turn secondary for the transformer. An alternating magnetic field which results from the RF current in primary coil 13 creates an electric field in arc tube 10 which closes upon itself completely. Current flows as a result of the electric field and an arc discharge results in arc tube 10. A more detailed description for such HID-SEF lamp structures is found in previously cited U.S.
Patents 4,017,764 and 4,180,763 RD-17,640 An exemplary frequency of operation for RF power supply 14 is 13.56 megahertz. Typical power input to the lamp can be in the range of 100 - 2000 watts.
Lamps having the above described structural configura-5 tion were built and found to exhibit the spectral emissionc:urve depicted in FIG. 2. More particularly, the depicted emission curve represents such HID-SEF lamp emission, with the lamp further exhibiting a color temperature of around 3985K, a 182 LPW efficacy, and a 54.8 CRI value. The 10 depicted emission is provided in composite fashion formed by the line spectrum from a high pressure sodium discharge which further includes the visible spectral continuum, with cerium emission also being present in the lamp discharge.
The arc tube fill in this particular lamp consisted of 15 approximately 100 milligrams NaI, approximately S.l milli-grams TlI, approximately 19.8 milligrams CeC13 and xenon gas at a partial pressure of approximately 200 Torr at room temperature. The following examples are provided to demon-strate still other successfully tested arc tube fills for 20 the present metal halide arc lamp construction.
EXAMPLE I
An arc tube having 20 millimeter O.D. x 17 millimeter height dimensions was filled with approximately 6 milligrams NaI, 2.3 milligrams CeC13, and approximately 500 Torr 25 partial pressure of xenon gas at room temperature. The lamp operated at approximately 265 watts input power to produce 203 LPW and 54 CRI values at a color temperature of approxi-mately 3699K which approaches the cool white oval.
1298344 RD-17,640 EXAMPLE II
The same size arc tube as in Example I above was filled with approximately 6.1 milligrams NaI, 3 milligrams CeI3, and 500 Torr xenon partial pressure buffering gas at room temperature. The subsequent operation of the lamp at approximately 206 watts input power provided 195 LPW effi-cacy, 49 CRI, and a lamp color temperature of approximately 3290K which approaches the warm white color oval.
EXAMPLE III
In this example, an arc tube having dimensions of 15 millimeters O.D. x 13 millimeters in height was employed.
The arc tube fill consisted of approximately 1 milligram NaI
and 1 milligram CeC13 along with xenon gas at a partial pressure of approximately 500 Torr at room temperature.
When supplied with 202 watts input power, the lamp exhibited 185 LPW and 57 CRI at a color temperature of approximately 4856K which approaches other recognized white color ovals.
EXAMPLE IV
An arc tube having the same physical dimensions as in Example I above was filled with 6.1 milligrams NaI, 1.4 milligrams CeC13, 0.5 milligrams TlI, and 500 Torr partial pressure of xenon at room temperature. At 204 watts input power the lamp yielded 204 LPW and 49 CRI at a color temper-ature of 3381K which approaches the stand~ white color oval.
EXAMPLE V
An arc tube with an O.D. of 54 millimeters and 25 millimeters in height was filled with approximately 100 milligrams NaI, 5.1 milligrams TlI, 19.8 grams CeCl3, and 200 Torr partial pressure of xenon at room temperature.
When operated at 1087 watts input power the lamp demon-strated 182 LpW, 54.8 CRI and a color temperature of 3985K
which again approaches the cool white oval.
The above lamp embodiments exhibit optimum performance for a HID-SEF type lamp containing the present combination of arc tube fill materials including sodium halide, cerium halide and xenon gas. As has been shown, efficacy of over 200 LPW is gained, accompanied by CRI values of 50 or greater, and lamp color temperatures in the white color spectral region are varied by addition of still other vaporizable metal atoms which radiate in the lamp discharge.
As evident in the above examples, such supplemental radi-ating species are incorporated in the arc tube fill ashalide compounds so as to be vaporizible at the lamp oper-ating temperatures without requiring intermediate conver-sion.
The foregoing describes a broadly useful, improved HID
electrodeless lamp exhibiting superior performance. It will be apparent from the foregoing description, however, that various modifications in the specific embodiments above described can be made without departing from the spirit and scope of the present invention. For example, color cor-recting radiators other than those specifically illustratedcan be included in the present lamp fill in minor amounts to meet specific lamp requirements, so long as these radiators are compatible during lamp operation. Additionally, phys-ical configurations for the lamp other than those above disclosed are possible to make still better use of the lamp fill medium. It is intended to limit the present invention, therefore, only by the scope of the following claims.
Claims (18)
1. A mercury-free electrodeless metal halide arc lamp comprising:
(a) a light transmissive arc tube for containing an arc discharge;
(b) a fill disposed in said arc tube to generate said arc discharge, said fill including sodium halide and cerium halide, said halides selected from the group consisting of bromides, chlorides, and iodides, including mixtures thereof, said sodium halide and cerium halide being combined in weight proportions to generate white color lamp emission at improved efficacy and color rendition; and to provide a partial pressure in the range of about 60 Torr or higher at room temperature;
(c) said fill further including xenon in a sufficient quantity to limit the transport of thermal energy from said arc discharge to the walls of said arc tube; and (d) excitation means for coupling radio-frequency energy to said fill.
(a) a light transmissive arc tube for containing an arc discharge;
(b) a fill disposed in said arc tube to generate said arc discharge, said fill including sodium halide and cerium halide, said halides selected from the group consisting of bromides, chlorides, and iodides, including mixtures thereof, said sodium halide and cerium halide being combined in weight proportions to generate white color lamp emission at improved efficacy and color rendition; and to provide a partial pressure in the range of about 60 Torr or higher at room temperature;
(c) said fill further including xenon in a sufficient quantity to limit the transport of thermal energy from said arc discharge to the walls of said arc tube; and (d) excitation means for coupling radio-frequency energy to said fill.
2. The lamp of claim 1 wherein the weight proportion of cerium halide is no greater than the weight proportion of sodium halide.
3. The lamp of claim 1 wherein an amount of sodium halide is selected so that a reservoir of sodium halide condensate is present during lamp operation.
4. The lamp of claim 1 wherein an amount of cerium halide is selected so that a reservoir of cerium halide condensate is present during lamp operation.
5. The lamp of claim 1 wherein the selected amounts of both sodium halide and cerium halide provide a reservoir of mixed condensates during lamp operation.
RD-17,640
RD-17,640
6. The lamp of claim 1 wherein the quantity of xenon is sufficient to provide a partial pressure in the range of about 600 Torr and higher at the operating temperature of the lamp.
7. The lamp of claim 1 wherein the selected sodium halide is sodium iodide.
8. The lamp of claim 1 wherein the selected cerium halide is cerium chloride.
9. The lamp of claim 1 wherein the selected sodium halide is sodium iodide and the selected cerium halide is cerium chloride.
10. The lamp of claim 1 wherein the fill further includes metal lamp color temperature modifying atoms.
11. The lamp of claim 10 wherein a combination of said metal atoms imparts blue, green and red emission to the lamp emission spectrum.
12. The lamp of claim 10 wherein the selected metal atoms are thallium.
13. The lamp of claim 10 wherein the metal atoms are present in the fill as metal halide compounds.
14. The lamp of claim 11 wherein the fill includes rare earth halides, the rare earths being selected from the group consisting of dysprosium, holmium, ytterbium, and thulium to provide supplemental continuous radiation in the visible spectrum.
15. The lamp of claim 10 wherein the fill includes metal atoms providing supplemental monochromatic radiation in the visible spectrum.
16. A mercury-free electrodeless metal halide arc lamp comprising:
RD-17,640 (a) a light transmissive arc tube for containing an arc discharge, said arc tube being cylindrically shaped with the height of said arc tube being less than its outside diameter;
(b) a light transmissive outer envelope disposed around said arc tube and defining a space therebetween;
(c) a fill disposed in said arc tube to generate said arc discharge, said fill including sodium halide and cerium halide, said halides selected from the group consisting of bromides, chlorides and iodides, including mixtures thereof, said sodium halide and cerium halide being combined in weight proportions to generate white color lamp emission at improved efficacy and color renditions;
(d) said fill further including xenon in a sufficient quantity to limit the transport of thermal energy from said arc discharge to the walls of said arc tube as well as to increase lamp efficacy; to provide a partial pressure in the range of about 60 Torr or higher at room temperature and (e) excitation means for coupling radio-frequency energy to said fill.
RD-17,640 (a) a light transmissive arc tube for containing an arc discharge, said arc tube being cylindrically shaped with the height of said arc tube being less than its outside diameter;
(b) a light transmissive outer envelope disposed around said arc tube and defining a space therebetween;
(c) a fill disposed in said arc tube to generate said arc discharge, said fill including sodium halide and cerium halide, said halides selected from the group consisting of bromides, chlorides and iodides, including mixtures thereof, said sodium halide and cerium halide being combined in weight proportions to generate white color lamp emission at improved efficacy and color renditions;
(d) said fill further including xenon in a sufficient quantity to limit the transport of thermal energy from said arc discharge to the walls of said arc tube as well as to increase lamp efficacy; to provide a partial pressure in the range of about 60 Torr or higher at room temperature and (e) excitation means for coupling radio-frequency energy to said fill.
17. The lamp of claim 16 wherein the space between the light transmissive outer envelope and said arc tube is evacuated.
18. The lamp of claim 16 wherein the space between the light transmissive outer envelope and said arc tube is occupied with thermal energy barrier means.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US103,248 | 1987-10-01 | ||
| US07/103,248 US4810938A (en) | 1987-10-01 | 1987-10-01 | High efficacy electrodeless high intensity discharge lamp |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA1298344C true CA1298344C (en) | 1992-03-31 |
Family
ID=22294172
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA000578095A Expired - Fee Related CA1298344C (en) | 1987-10-01 | 1988-09-22 | High efficacy electrodeless high intensity discharge lamp |
Country Status (8)
| Country | Link |
|---|---|
| US (1) | US4810938A (en) |
| JP (1) | JPH01132039A (en) |
| KR (1) | KR910010109B1 (en) |
| BE (1) | BE1003235A3 (en) |
| CA (1) | CA1298344C (en) |
| DE (1) | DE3832717C2 (en) |
| GB (1) | GB2210498B (en) |
| NL (1) | NL8801855A (en) |
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- 1988-09-26 JP JP63239111A patent/JPH01132039A/en active Pending
- 1988-09-27 DE DE3832717A patent/DE3832717C2/en not_active Expired - Fee Related
- 1988-09-30 GB GB8822929A patent/GB2210498B/en not_active Expired - Fee Related
- 1988-09-30 BE BE8801121A patent/BE1003235A3/en not_active IP Right Cessation
Also Published As
| Publication number | Publication date |
|---|---|
| GB2210498B (en) | 1992-03-25 |
| DE3832717C2 (en) | 1994-03-10 |
| GB8822929D0 (en) | 1988-11-09 |
| GB2210498A (en) | 1989-06-07 |
| JPH01132039A (en) | 1989-05-24 |
| KR910010109B1 (en) | 1991-12-16 |
| NL8801855A (en) | 1989-05-01 |
| BE1003235A3 (en) | 1992-02-04 |
| DE3832717A1 (en) | 1989-04-20 |
| KR890007358A (en) | 1989-06-19 |
| US4810938A (en) | 1989-03-07 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| MKLA | Lapsed |