Patent Grant
7719173
The present invention relates to an electrodeless discharge lamp having no electrode in a bulb into which discharge gas is filled, and generates discharge in the discharge gas by liberating high frequency electromagnetic field generated by supplying high frequency current to an induction coil to the discharge gas, and relates to a lighting apparatus using the same.
The electrodeless discharge lamp is configured that the discharge gas filled in the bulb is activated by high frequency electromagnetic field generated by supplying high frequency current to the induction coil, and ultraviolet light emitted at that time is converted into visible light through fluorescent material. Since the electrodeless discharge lamp apparatus has a configuration that no electrode inside, non-lighting due to deterioration of the electrode may not occur, and thus, it is relatively longevity life in comparison with generic fluorescent lamp.
In a conventional electrodeless discharge lamp shown in Japanese Laid-Open Patent Publication No. 7-272688 or Japanese Laid-Open Utility Model Publication No. 6-5006, for example, uses a bismuth-indium amalgam as a luminescent material. According to this amalgam, it is possible to obtain a higher optical output in a wide range than the optical output at ambient air temperature 25 degrees Celsius, even when ambient air temperature changes. On the other hand, although a high mercury vapor pressure is necessary to realize a high optical output, there, however, is a disadvantage that start-up of the lamp is slower because a time until reaching a temperature value that it is necessary for evaporation of mercury. When the bismuth-indium amalgam was used, a consequence that it is necessary for approximately 1 minute to secure optical output of 60% with respect to optical output at the time of stable lighting was provided.
In contrast, a pure mercury drop is used for the discharge gas to shorten the start-up time in an electrodeless discharge lamp shown in Japanese Laid-Open Patent Publication No. 2001-325920. According to this document, it is mentioned that the optical output was reached 50% of maximum output within two or three seconds after the lamp was activated. This is because the mercury drop needs a shorter time until reaching the temperature value necessary for evaporation than amalgam. When an input power is much larger with respect to a volume of the bulb, or when the ambient air temperature is higher, temperature value of the bulb rises, and mercury vapor pressure falls down adversely, and thus, the optical output falls.
When an amalgam was used as above, variation of optical output is small regardless of variation of ambient air temperature. In contrast, when mercury drop is used, mercury vapor pressure is largely varied corresponding to variation of ambient air temperature, and thus, optical output fall. Accordingly, when mercury drop is used, it is necessary to secure a coldest spot (a portion of a surface of a bulb where temperature value becomes the lowest) so as to control mercury vapor pressure. The temperature is around 35-45 degrees Celsius.
By the way, in an electrodeless discharge lamp shown in Japanese Laid-Open Patent Publication No. 2001-325920, when installation posture thereof is changed, the coldest spot of the bulb is changed. For example, when the lamp is lit in a posture that a ferrule or a cap thereof is disposed upward (hereinafter, it is called “base-up lighting”), a protrusion formed at an apex of the bulb becomes the coldest spot. Alternatively, when the lamp is lit in a posture that a ferrule thereof is disposed downward (hereinafter, it is called “base-down lighting”), a portion of the bulb just above the ferrule becomes the coldest spot. When the volume of the bulb is small, a volume of a portion where discharge occurs becomes relatively larger with respect to the volume of the bulb, so that it is difficult to maintain temperature at the coldest point constant regardless of the posture of installation of the electrodeless discharge lamp. Although temperature at the protrusion of the bulb in the base-up lighting can be controlled by changing a diameter and a height of the protrusion, it is a problem to control temperature at a bulb neck portion in the base-down lighting.
The present invention is conceived to solve the above mentioned problems, and a purpose of the present invention is to provide an electrodeless discharge lamp a lighting apparatus using the same, which can maintain a high optical output even when the posture of installation is changed by providing the coldest spot in the bulb and controlling the temperature of the coldest spot.
An electrodeless discharge lamp in accordance with an aspect of the present invention comprises a bulb into which discharge gas and mercury which is controlled at a temperature of a coldest spot are filled, a power coupler generating high frequency electromagnetic field, and a ferrule for coupling the bulb and the power coupler, wherein
the bulb is configured of a barrel formed of a transparent material and having an opening, and a sealing member welded to the opening of the barrel and having a cylindrical cavity;
a protrusion, which becomes a coldest spot when the lamp is lit in a state that the ferrule is disposed upward, is formed at an apex of the bulb; and
a protruding portion is formed in a vicinity of a portion of the bulb just above the ferrule so that the vicinity of the portion of the bulb just above the ferrule serves as a coldest spot when the lamp is lit in a state that the ferrule is disposed downward.
According to such a configuration, when the lamp is lit in the state that the ferrule is disposed upward (base-up lighting), the protrusion formed at the apex of the bulb becomes as the coldest spot, so that temperature of the protrusion can be controlled by changing a diameter and a height of the protrusion, similar to the conventional case. On the other hand, when the lamp is lit in the state that the ferrule is disposed downward (base-down lighting), doctrine is different according to the orientation where the protruding portion is formed. When the protruding portion is formed to protrude inward of the bulb, a volume of a discharge space near to the protruding portion is partially shrunk, so that luminescence in the vicinity of the protruding portion is restrained when the electrodeless discharge lamp is lit in base-down lighting, and a part of heat generated corresponding to the luminescence is shielded by the protruding portion. Consequently, a temperature rise of the portion just above the ferrule, that is, the bulb neck portion is restrained, and thus, the bulb neck portion becomes the coldest spot. When the protruding portion is formed to protrude outward of the bulb, inside concavity of the protruding portion is positioned away from a portion where the discharge actually occurs, so that heat generated corresponding to the luminescence is hard to transmit to the protruding portion. Consequently, a temperature rise in the protruding portion is restrained, and thus the protruding portion becomes the coldest spot. In this way, although a location of the coldest spot is changed corresponding to the posture of installation of the electrodeless discharge lamp, the temperature value of the coldest spot can be maintained substantially constant in each case, so that a constant optical output is provided regardless of the posture of installation of the electrodeless discharge lamp.
At first, an electrodeless discharge lamp in accordance with a first embodiment of the present invention is described.
A protective coating 2 and a phosphor coating 3 are applied to an inner peripheral face of the spherical barrel 14. Similarly, the protective coating 2 and the phosphor coating 3 are applied to an outer peripheral face of the cavity 5 of the sealing member 11 (It is partially illustrated in the figure). Therefore, the protective coating 2 and the phosphor coating 3 are applied to substantially whole area of an inner peripheral face of the bulb 10. In addition, metal oxide such as Al2O3 is used as a binding agent of the fluorescent material, and the phosphor coating 3 is protected by increasing quantity of addition of the agent so as to prevent deterioration of the fluorescent material. As for the binding agent, Y2O3 or MgO can be used other than Al2O3.
A ferrule 15, which is formed of a resin material, is attached to a bulb neck portion 19 near to the bottom of the bulb 10 by an adhesive, for example. A mounting structure such as a bayonet not show in the figure is provided on the ferrule 15 and a pedestal of the power coupler 20, respectively, so that the bulb 10 which is integrated with the ferrule 15 is detachably attached to the power coupler 20.
A protrusion 4 is formed at an apex of the bulb 10 so that it becomes the coldest shot when the lamp is lit in a state that the ferrule 15 is disposed upward (base-up lighting). In addition, an annular protruding portion 17, which protrude inward of the bulb 10 along an outer peripheral face of the cavity 5, is formed in the vicinity of the welded portion of the barrel 14 and the sealing member 11 of the bulb 10, that is, the sealed portion of the bulb 10, more precisely, a portion just above the ferrule 15 in a state that the ferrule 15 is disposed below. When the lamp is lit in the state that the ferrule 15 is disposed below (base-down lighting), the protruding portion 17 functions as a discharge shielding means so that the vicinity of the protruding portion 17 becomes the coldest spot. Details are described later.
A rare gas such as argon or krypton is enclosed in the inside of the bulb 10. In addition, a metal container 13 made of iron-nickel alloy is established in an inside of the exhaust tube 8, and Zn—Hg of total quantity about 17 mg and 50:50 of a weight ration is filled in the metal container 13 so as to emit mercury for controlling mercury vapor pressure. Moreover, a recess 9 is formed on an inner peripheral face of the exhaust tube 8 to fix a location of the metal container 13, and a glass rod 12 is provided in the exhaust tube 8.
Subsequently, a lighting apparatus in accordance with the first embodiment is described.
The power coupler 20 constituting the electrodeless discharge lamp 1 is fixed on a heatsink 21, and the heatsink 21 is installed on a ceiling, a side wall, or a floor of a building. The power coupler 20 is configured of an induction coil for generating high frequency electromagnetic field and a ferrite core, and terminals of the induction coil are connected to a lightning circuit 23 through an electric cable 22. Then, the lighting apparatus comprising the electrodeless discharge lamp 1 is configured when the bulb 10 which is integrated with the ferrule 15 is attached to the power coupler 20. Since a high frequency current supplied to the induction coil of the power coupler 20 has a lower frequency of several hundred kHz, the ferrite core (magnetic core) inside the induction coil.
When a high-frequency current is flown into the induction coil of the power coupler 20, a high frequency electromagnetic field occurs around the induction coil. Electrons in the bulb 10 are accelerated by such high frequency electromagnetic field, so that electrolytic dissociation occurs due to collision of electrons, and thus, discharge occurs. While discharge occurs, the discharge gas filled in the bulb 10 is activated, and ultra-violet light occurs when activated atoms come back to ground state. This ultra-violet light is converted to visible light with the phosphor coating 3 applied to the inner peripheral face of the bulb 10. The visible light passes through the barrel 14 of the bulb 10 so that it is emitted outward.
In the electrodeless discharge lamp 1 according to the first embodiment, since the protruding portion 17 is formed just above the ferrule 15 of the bulb 10, that is, in the bulb neck portion 19, a volume of a discharge space in the vicinity of the protruding portion 17 is partially shrunk. When the electrodeless discharge lamp 1 is lit in the base-down lighting, luminescence in the vicinity of the protruding portion 17 is restrained, and a part of heat which occurs following to the luminescence is shielded by the protruding portion 17. Consequently, a temperature rise of the bulb neck portion 19 is restrained, and thus, the bulb neck portion 19 becomes the coldest spot. On the other hand, when the lamp is lit in the base-up lighting, the protrusion 4 formed at the apex of the bulb 10 becomes the coldest spot similar to the conventional case. In this way, although a location of the coldest spot is changed corresponding to the posture of installation of the electrodeless discharge lamp 1, it was confirmed that the temperature value of the coldest spot could be maintained substantially constant in each case, when the temperature of the coldest spot was measured. Consequently, a constant optical output can be provided regardless of the posture of installation of the electrodeless discharge lamp 1.
In the above mentioned first embodiment, although the protruding portion 17 is formed annularly along a circumferential direction of the cavity 5, it, however, is not limited to this. It is sufficient that the protruding portion 17 should be formed at least a portion of the outer peripheral face of the cavity 5. Alternatively, the protruding portion 17 may be formed at a plurality of portions along the circumferential direction of the cavity 5.
Subsequently, an electrodeless discharge lamp in accordance with a second embodiment of the present invention is described.
In the second embodiment shown in
In the above mentioned second embodiment, although the protruding portion 16 is formed annularly along a circumferential direction of the barrel 14, it, however, is not limited to this. It is sufficient that the protruding portion 16 should be formed at least a portion of the outer peripheral face of the barrel 14. Alternatively, the protruding portion 16 may be formed at a plurality of portions along the circumferential direction of the barrel 14.
Subsequently, an electrodeless discharge lamp in accordance with a third embodiment of the present invention is described.
As shown in
In this way, since the annular protruding portion 17 is formed along the outer peripheral face of the cavity 5, when the electrodeless discharge lamp 1 is lit in the base-down lighting, a temperature rise of the bulb neck portion 19 between the protruding portion 16 and the protruding portion 17 and the sealing portion of the bulb 10 is restrained, and the protruding portion 16 and the bulb neck portion 19 become the coldest spots. On the other hand, when the electrodeless discharge lamp 1 is lit in the base-up lighting, the protrusion 4 formed at the apex of the bulb 10 becomes the coldest spot similar to the first and second embodiments. In this way, although a location of the coldest spot is changed corresponding to the posture of installation of the electrodeless discharge lamp 1, it was confirmed that the temperature value of the coldest spot could be maintained substantially constant in each case, when the temperature of the coldest spot was measured. Consequently, a constant optical output can be provided regardless of the posture of installation of the electrodeless discharge lamp 1.
Furthermore, since the spring members 18 provided on the power coupler 20 are fit to utilizing the inside concavity the protruding portion 17, it is possible to fix the bulb 10 and the power coupler 20 stably. In addition, since the lighting apparatus according to the third embodiment is substantially the same as that in the second embodiment shown in
Subsequently, an electrodeless discharge lamp in accordance with a fourth embodiment of the present invention is described.
The exhaust tube 8 is used to exhaust an internal air and to full a discharge gas such as argon or krypton after welding the barrel 14 and the sealing member 11 in the manufacturing processes of the bulb 10. Therefore, it is not necessarily disposed at the center of the cavity 5. As for the reason why the exhaust tube 8 is conventionally provided at the center of the cavity 5, it is recited to ease the manufacturing of the spherical barrel 14 and to enhance a good appearance of the electrodeless discharge lamp 1. However, it is not need to consider the above reason in the electrodeless discharge lamp 1 in accordance with the present invention, since the protrusion 4 is formed at the apex of the bulb 10. Therefore, in the electrodeless discharge lamp according to the fourth embodiment, a single protruding portion 16, which protrudes outward along the circumferential direction of the barrel 14 constituting the bulb 10, is formed in the vicinity of the sealing portion of the bulb 10, that is, just above the ferrule 15 in a state that the ferrule 15 is disposed downward. In addition, the metal container 13 into which Zn—Hg is filled is provided in the protruding portion 16. Then, both of the protrusion 4 and the protruding portion 16 are used as the exhaust tubes or a part of the same to exhaust impurity gas such as air in the bulb 10 and to fill a discharge gas therein.
As shown in
In this way, it is possible to shorten a time necessary to exhaust the impurity gas and to fill the discharge gas by providing the exhaust tubes 8A and 8B at two places. In particular, by using one to exhaust the impurity gas and the other to fill the discharge gas, it is possible to shorten a time necessary for manufacturing the bulb 10, largely. In addition, the protruding portions 16 each serving as the exhaust tube 8B may be formed at a plurality places so that the same effect can be obtained.
Since the present invention is not limited to the configurations of the above mentioned embodiments, various kinds of modification can be applied in a scope where the purpose of the invention is not changed. For example, as shown in
The present application is based on Japan patent application No. 2005-84862, the contents of which are hereby incorporated with the present invention by referring to the description and drawings of the above patent application, consequently.
Although the present invention has been fully described by way of example with reference to the accompanying drawings, it is to be understood that various changes and modifications will be apparent to those skilled in the art. Therefore, unless otherwise such changes and modifications depart from the scope of the present invention, they should be construed as being included therein.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2005-084862 | Mar 2005 | JP | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/JP2006/305778 | 3/23/2006 | WO | 00 | 9/21/2007 |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2006/101153 | 9/28/2006 | WO | A |
| Number | Name | Date | Kind |
|---|---|---|---|
| 5789855 | Forsdyke et al. | Aug 1998 | A |
| 5834890 | Girach | Nov 1998 | A |
| Number | Date | Country |
|---|---|---|
| 6-005006 | Jan 1994 | JP |
| 7-272688 | Oct 1995 | JP |
| 8-153489 | Jun 1996 | JP |
| 09063543 | Mar 1997 | JP |
| 9-320522 | Dec 1997 | JP |
| 10-092390 | Apr 1998 | JP |
| 2001-325920 | Nov 2001 | JP |
| Number | Date | Country | |
|---|---|---|---|
| 20090051291 A1 | Feb 2009 | US |
