The disclosure of Japanese Patent Application No. 2005-026854, filed Feb. 2, 2005, including the specification, claims and drawings thereof, is incorporated herein by reference in its entirety.
The present invention relates to a rare gas fluorescent lamp and, in particular, to a rare gas fluorescent lamp that includes a light-emitting tube whose inner surface is coated by a fluorescent material and which is filled with a rare gas, a plurality of external electrodes which is provided on an outer surface of the light-emitting tube, and a conductive material, which is provided on an inner surface of an end portion of the light-emitting tube that corresponds to a portion on which the external electrodes are arranged.
Conventionally, as a fluorescent lamp used for a light source of a business machine or a backlight of a liquid crystal display panel, a rare gas fluorescent lamp has been widely used, in which a plurality of strip-shaped external electrodes is provided on an outer surface of a light-emitting tube, and a high frequency voltage is applied to the external electrodes to turn on the rare gas fluorescent lamp.
Even though the external electrode 102 is made from, for example, an aluminum tape, it is not limited to the strip-shaped tape. The external electrodes 102 may be formed in a line shape or a mesh shape. In addition, the external electrodes 102 may be made from a metal tape such as a copper tape, or a conductive pigment such as a silver paste, instead of the aluminum tape.
A conductive material 104 is provided in a peripheral direction of an inner surface at an end portion of the light-emitting tube 101 to form a short circuit over a region on an inner surface of the light-emitting tube 101 on which both the external electrodes 102 are arranged. Examples of the conductive material 104 include a carbon paste and a silver paste.
Functions of the conductive material 104 will be described. The conductive materials 104 provided in the glass tube 101 are provided over inner sides of both of the external electrodes 102. Since the areas occupied by the conductive materials are almost equal to each other, it has the same effect that capacitors having a substantially same capacitance are shorted by the same conductive materials 104. Thus, the conductive material 104 has an electric potential that is almost half of the potential of both of the external electrodes 102. On the other hand, since a discharge space has very large impedance before the discharge is initiated in the space, an inner wall of the light-emitting tube 101 provided on an inner side of the external electrode 102 has almost the same potential as that of the external electrode 102. As a result, since very high electric field is applied between the conductive material 104 and the vicinity of the conductive material 104 on the inner wall of the light-emitting tube 101 provided on the inner side of the external electrode 102, a desired preliminary discharge is generated. Thus, it becomes easy to generate main discharge. Since the preliminary discharge causes a lamp to be started, it is possible to generate the main discharge without failure of starting even when a low voltage is applied. Refer to, for example, Japanese Patent No. 3149780 Japanese Unexamined Patent Application Publication No. 10-188910.
In general, a rare gas fluorescent lamp includes a region (hereinafter referred to as ‘effective light-emitting region’) for ensuring a predetermined output, and the remaining region (hereinafter referred to as ‘dead space’). The rare gas fluorescent lamp is preferably configured such that the effective light-emitting region is wide and the dead space is narrow in terms of space-saving design.
However, there is a problem in the conventional rare gas fluorescent lamp in that an undesired creeping discharge is extensively formed on an inner surface of the light-emitting tube due to the conductive material provided on the light-emitting tube for improving starting performance, thereby increasing a dead space and reducing an effective light-emitting region. That is, in the case the conductive material is provided, the starting performance is improved due to generation of preliminary discharge, but extensive creeping discharge is generated on end portions of the light-emitting tube, thereby reducing the effective light-emitting region.
A cause of the above-mentioned problem will be described with reference to
When high voltage is applied to the external electrode 102, high voltage is generated in a discharge space within the light-emitting tube 101 to cause discharge. As shown in
The present rare gas fluorescent lamp can prevent reduction of an effective light-emitting by securely suppressing extensive spread of creeping discharge on an inner surface of a light-emitting tube even when a conductive material is provided so as to improve the starting performance.
In order to solve the above-mentioned problems, the rare gas fluorescent lamp having a light-emitting tube whose inner surface is coated by a fluorescent material and which is filled with a rare gas, a plurality of external electrodes which are provided on an outer surface of the light-emitting tube, and a conductive material, which is provided at an end portion of the light-emitting tube that corresponds to a portion on which the external electrodes are arranged, the rare gas fluorescent lamp comprises a creeping discharge prevention unit that is provided inward of the conductive material in an axial direction to prevent diffusion of creeping discharge occurring between the conductive material and electrical charges stored on the inner surface of the light-emitting tube.
Accordingly, it is possible to prevent an effective light-emitting region from being reduced by securely suppressing the creeping discharge from being extensively diffused on an inner surface of the light-emitting tube even when the conductive material is provided to improve starting performance.
The creeping discharge prevention unit may be formed such that at least one of the external electrodes protrudes toward the outside of the light-emitting tube in a vicinity of an end of the at least one of the external electrodes.
Accordingly, dielectric polarization is suppressed in dielectric under the light-emitting tube in which the external electrode is protruded, such that only weak barrier discharge is formed. As a result, since the amount of negative and positive charges, which are respectively accumulated on an inner surface of dielectric on high voltage side and on an inner surface of dielectric on low voltage side under the light-emitting tube, is very small, it is possible to suppress the creeping discharge from being diffused between the charges and the conductive material.
The creeping discharge prevention unit may be formed such that a thickness of a wall of the light-emitting tube, which corresponds to at least one of the external electrodes is larger than that of the other portion, in a vicinity of an end of the at least one of the external electrodes.
Accordingly, it is possible to make electrostatic capacitance small under the thick portion of the light-emitting tube. As a result, since it is possible to make charges stored on an inner surface of a dielectric very small, thereby suppressing the creeping discharge from being diffused between the charges and the conductive material.
The creeping discharge prevention unit may be formed such that an additional member is interposed between the light-emitting tube and at least one of the external electrodes, in a vicinity of an end of the external electrode.
Accordingly, since electrostatic capacitance is reduced under part of the light-emitting tube in which the additional member is provided, it is possible to make charges stored on an inner surface of a dielectric very small, thereby suppressing the creeping discharge from being diffused between the charges and the conductive material.
The creeping discharge prevention unit may be formed such that a surface area per unit length of at least one of the external electrodes in an axial direction is less than a surface area per unit length of the other portion in the axial direction, in a vicinity of an end of the external electrode.
Accordingly, since electrostatic capacitance is reduced under the part of the light-emitting tube which corresponds to the portion having a small surface area, it is possible to make charges stored on an inner surface of a dielectric very small, thereby suppressing the creeping discharge from being diffused between the charges and the conductive material.
The creeping discharge prevention unit is formed such that a wall of the light-emitting tube which corresponds to at least one of the external electrodes protrudes toward inside or outside of the light-emitting tube, in a vicinity of an end of the at least one of the external electrode.
Accordingly, since a creeping distance from the conductive material to charges stored on an inner surface of the light-emitting tube is increased by a distance protruded along the inner surface, the creeping distance is longer compared to the conventional lamp. As a result, barrier discharge is formed under the protruded part of the light-emitting tube, such that charges are accumulated. However, since the distance from the charges stored on the inner surface of the light-emitting tube to the conductive material is elongated compared to the conventional structure, it is possible to prevent the effective light-emitting region from being reduced.
These and other features and advantages of the present rare gas fluorescent lamp will be apparent from the following description taken in conjunction with the accompanying drawings, in which:
A rare gas fluorescent lamp according to the present invention is divided into two types as set forth below.
A first-type rare gas fluorescent lamp includes a creeping discharge prevention unit 4 for preventing electrical charges from being accumulated on an inner surface of a light-emitting tube 1 (under external electrodes) corresponding to portions at which external electrodes 21 and 22 are arranged, as shown in the following first embodiment (
The creeping discharge prevention unit 4 shown in the sixth embodiment (
A first embodiment of the present invention will be described with reference to
As shown in
In the creeping discharge prevention unit 4 according to the present embodiment, when the external electrode 21 on a side on which the protrusion 42 is provided is at a high voltage, since the external electrode 21 is not in contact with the light-emitting tube 1 at the protrusion 42, dielectric polarization is suppressed in a dielectric on the high voltage side under the protrusion 42, such that only weak barrier discharge is formed. As a result, since the amount of negative and positive charges, which are respectively accumulated on an inner surface of the dielectric on high voltage side and on an inner surface of a dielectric on low voltage side, is very small on the inner surface of the light-emitting tube 1 under the protrusion 42, it is possible to suppress the creeping discharge from being spread between the charges and the conductive material 3.
A second embodiment of the present invention will be described with reference to
As shown in the above drawing, each of the external electrodes 21 and 22 includes the protrusion 44, which has approximately a ‘U’-shaped portion in a cross-section view including a tube axis and is formed to cover the thickness portion 43 in the light-emitting tube 1, and is provided to cover the thickness portion 43 and other portion of the light-emitting tube 1.
In the creeping discharge prevention unit 4 according to the present embodiment, it is possible to make electrostatic capacitance of a portion under the thickness portion 43 small, thereby making electrical charges stored on an inner surface of a dielectric small. Accordingly, it is possible to prevent diffusion of the creeping discharge between the charges and the conductive material 3.
In addition, the thick portion 43 of the light-emitting tube 1 may be formed toward the light-emitting space side instead of the opposite direction to the light-emitting space. In this case, it is possible to obtain the same effect as that obtained from the creeping discharge prevention unit shown in
A third embodiment of the present invention will be described with reference to
As shown in
In the creeping discharge prevention unit 4 according to the present embodiment, since electrostatic capacitance is reduced under the portion of the light-emitting tube 1 in which the additional member 45 is provided, it is possible to make charges stored on an inner surface of a dielectric very small, thereby suppressing the creeping discharge from being diffused between the charges and the conductive material 3.
A fourth embodiment of the present invention will be described with reference to
As shown in
In the creeping discharge prevention unit 4 according to the present embodiment, since electrostatic capacitance is reduced under the narrow portion 46, it is possible to make charges stored on an inner surface of a dielectric very small, thereby suppressing the creeping discharge from being diffused between the charges and the conductive material 3.
In addition, the same effect as that in the present embodiment can be obtained by making holes in a portion where a surface area needs to be reduced.
A fifth embodiment of the present invention will be described with reference to
As shown in
In the creeping discharge prevention unit 4 according to the present embodiment, since a creeping distance from the conductive material to charges stored on an inner surface of the light-emitting tube on the inner surface of the light-emitting tube 1 is increased by a distance protruded along the inner surface of the protrusion 47, the creeping distance is longer compared to the conventional lamp. As a result, barrier discharge is formed under the protrusion 47, such that charges are accumulated. However, since the distance from the charges stored on the inner surface of the light-emitting tube 1 to the conductive material 3 is elongated compared to the conventional structure, it is possible to prevent reduction of the effective light-emitting region.
In addition, as shown in
A sixth embodiment of the present invention will be described with reference to
As shown in
In the creeping discharge prevention unit 4 according to the present embodiment, when the external electrode 21 with the protrusion 47 provided is at a high voltage, the external electrode 21 is not in contact with the light-emitting tube 1 at the protrusion 47. Accordingly, dielectric polarization is suppressed in a dielectric on the high voltage side under the protrusion 47, such that only weak barrier discharge is formed. As a result, since the amount of negative and positive charges, which are respectively accumulated on an inner surface of a dielectric on high voltage side and on an inner surface of a dielectric on low voltage side, is very small on the inner surface of the light-emitting tube 1 under the protrusion 47, it is possible to suppress the creeping discharge from being diffused between the charges and the conductive material 3. In addition, since the light-emitting tube 1 includes the protrusion 47 and the distance from the charges stored on the inner surface of the light-emitting tube 1 to the conductive material 3 is elongated compared to the conventional structure, it is possible to prevent reduction of the effective light-emitting region.
Experimental results of the rare gas fluorescent lamp according to the present invention will be described.
According to the configuration shown in
The light-emitting tube 1 has a length of 500 mm, and a thickness of 0.4 mm. Each of the external electrodes 21 and 22 is made from an aluminum tape. Each of the external electrodes 21 and 22 has almost the same length as the light-emitting tube, and has a width of 1 mm.
The conductive material 3 corresponds to the external electrodes 21 and 22. The conductive material 3 is provided on an end portion of the external electrodes 21 and 22 and has a width of about 1 mm.
Finally, According to the configuration shown in
According to the configuration shown in
According to the configuration shown in
According to the configuration shown in
Comparing the above-mentioned examples 1 to 4 and the comparative example, when the rare gas fluorescent lamps according to Examples 1 to 4 were turned on with an input power of 5 W to 10 W, the starting performance was not deteriorated when the creeping discharge prevention unit 4 on the light-emitting tube has a length of 3 to 9 mm. In addition, the light intensity was not reduced in a region which is more than 15 mm distant from both ends of the light-emitting tube. On the other hand, in the rare gas fluorescent lamp according to the comparative example, the light intensity was decreased in a region which is 40 mm distant from both ends of the light-emitting tube.
Although only some exemplary embodiments have been described in detail above, those skilled in the art will readily appreciate that many modifications are possible in the exemplary embodiments without materially departing from the novel teachings and advantages. Accordingly, all such modifications are intended to be included within the scope.
Number | Date | Country | Kind |
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2005-026854 | Feb 2005 | JP | national |