The present invention relates to a cold-cathode tube lamp, and more particularly, to a cold-cathode tube lamp that includes a cup-shape cold-cathode tube electrode.
Conventionally, a cold-cathode tube lamp is used as a light source for various devices. For example, because a cold-cathode tube lamp has low power consumption and a long life as a light source, it is used as a light source (backlight) for a liquid crystal display device and the like.
When an electric voltage is applied across the electrode 402 and the electrode 403 of the above cold-cathode tube lamp via the lead terminal 404 and the lead terminal 405, electrons that are present slightly in the glass tube 401 are attracted to and collide with the electrode. Here, secondary electrons are emitted from the electrode with which the electrons collide and electric discharge begins; and the emitted electrons collide with atoms of the mercury in the glass tube 401, so that ultraviolet rays are radiated. And, this ultraviolet ray excites the fluorescent material coated on the inner surface of the glass tube 401 to allow visible light to be emitted, so that the cold-cathode tube lamp emits light.
Incidentally, if the above cold-cathode tube lamp continues to be used for a long time, ions and the like collide with the electrode, so that a phenomenon (sputtering phenomenon) in which atoms are emitted from a metal material that constitutes the electrode occurs. If a sputtering phenomenon occurs, atoms (sputtered matter) of the electrode metal emitted by the sputtering combine with mercury filled in the glass tube; accordingly, a disadvantage that mercury used for the discharge is consumed occurs. As described above, if mercury is consumed, the radiation of ultraviolet rays becomes less, the light emission becomes weak, and the brightness of the lamp becomes low. According to this, there is a problem that the life of the cold-cathode tube lamp becomes short. Besides, in a case of a cup-shape electrode, the collision of ions and the like easily occurs on a bottom-portion inner surface of the electrode in a concentrated fashion; accordingly, through-holes appear through the bottom portion of the electrode, and in some cases, the electrode comes off, so that the electrode is likely to be broken.
To resolve the electrode breakdown caused by the above sputtering, for example, there is a method for mounting a reinforcement member on the electrode (e.g., a patent document 1). The patent document 1 describes a structure of a cold-cathode type electrode that is composed of: a cylindrical metal body; a reinforcement member mounted on an inner-side bottom-surface portion of the cylindrical metal body; and a space portion. Accordingly, because it is possible to increase a thickness of the cylindrical metal body by forming the reinforcement member on the inner-side bottom-surface portion of the cylindrical metal body, it is possible to alleviate the inner-side bottom-surface portion of the cylindrical metal body being damaged by the sputtering. According to this, it is possible to alleviate occurrence of a disadvantage and the like that the electrode comes off the sealed metal body.
[patent document 1]: JP-A-2002-289135
However, in the electrode described in the above patent document 1, because the reinforcement member is formed in the inner-side bottom-surface portion of the electrode, sputtered matter that is generated by collision of the ions and the like with the reinforcement member easily scatters from the electrode into the glass tube. Because the sputtered matter that scatters into the glass tube easily combines with mercury in the glass tube, a disadvantage that mercury is consumed occurs. According to this, there are problems that the brightness of the cold-cathode tube lamp becomes low, and the life of the cold-cathode tube lamp becomes short.
Incidentally, in recent years, less power consumption, a longer life, higher efficiency and the like of a backlight are required. For example, to raise light emission efficiency, it is known that a gas pressure in a glass tube is lowered and a large current is flown. However, if the gas pressure in the glass tube is lowered, a moving speed of the ions and the like becomes fast; accordingly, there are problems that sputtering easily occurs and the life of the cold-cathode tube lamp becomes short because of the sputtering. To resolve such problems, for example, a method for enlarging a tube diameter of the glass tube is thought of.
However, in a case where the tube diameter of the glass tube is enlarged, if an electrode that has the same size as the conventional one, a distance between an inner wall of the glass tube and the electrode becomes large, so that ions and the like collide with not only the bottom-portion inner surface and inside surface of the electrode but also the outside surface of the electrode. Accordingly, there are problems that sputtering easily occurs and breakdown of the electrode caused by the sputtering easily occurs. Besides, if the tube diameter of the glass tube is enlarged and the size of the electrode is enlarged, the inner diameter of the electrode also becomes large, so that ions and the like easily collide with the bottom-portion inner surface and the inside surface of the electrode. Accordingly, there are problems that sputtering occurs in a concentrative fashion on the bottom-portion inner surface and an inside surface near the bottom portion of the electrode; and breakdown of the electrode caused by the sputtering easily occurs. Further, if the inner diameter of the electrode becomes large, sputtered matter generated by the sputtering can easily scatter from the electrode into the glass tube; accordingly, there are problems that the sputtered matter combines with mercury in the glass tube and the mercury is consumed.
Besides, in a case where the size of the electrode is enlarged as described above, a load on a lead terminal that supports the electrode becomes large, so that there is a possibility that deformation and breakdown of the lead terminal occur at a connection portion of the lead terminal and the electrode. Besides, because a heat generation amount of the electrode also increases by enlarging the electrode, there are possibilities that a disadvantage that light emission efficiency becomes low because of the heat generation; and the heat generated at the electrode concentrates on the lead terminal, so that there is a possibility that a lamp base connected to the lead terminal and a nearby connector are subjected to thermal damage.
The present invention has been made to solve the above problems, and it is an object of the present invention is to provide a cold-cathode tube lamp that is able to increase stability of an electrode, a lighting device for a display device, a display device and a television receiving device.
To achieve the above object, the present invention includes: a glass tube in which at least a rare gas is filled; a pair of first electrodes that are disposed to face each other at both inner end portions of the glass tube and composed of a first cylinder-shape cylindrical portion that has an opening portion at one end and a first bottom portion that closes the other end of the first cylindrical portion; and a second electrode that is disposed in each of the first electrodes; wherein the second electrode has a second cylinder-shape cylindrical portion that has an opening portion at least one end; and the second electrode is disposed in such a way that the second cylindrical portion is away from the first cylindrical portion of the first electrode by a predetermined distance.
According to the above structure, because the cold-cathode tube lamp according to the present invention includes the second electrode disposed in the first electrode, a discharge area becomes large and current densities in the first electrode and the second electrode become low. According to this, it becomes possible to alleviate occurrence of sputtering. Besides, because ions and the like in the glass tube collide with not only the first electrode but also the second electrode, it is possible to alleviate concentrative occurrence of sputtering on one electrode. According to this, because it is possible to alleviate the electrode being broken by sputtering, it is possible to alleviate the life of the cold-cathode tube lamp becoming short.
Besides, the first electrode includes the first cylinder-shape cylindrical portion that has the opening portion at one end and the first bottom portion that closes the other end of the first cylindrical portion, while the second electrode has the second cylinder-shape cylindrical portion that has the opening portion at least one end; the second electrode is disposed in such a way that the second cylindrical portion is away from the first cylindrical portion of the first electrode by the predetermined distance; accordingly, it is possible to alleviate occurrence of sputtering in a concentrative fashion on the first bottom-portion inner surface and a nearby inside surface. According to this, because it is possible to alleviate the first electrode being broken by the sputtering, it is possible to alleviate the life of the cold-cathode tube lamp becoming short. Besides, because sputtered matter generated by the sputtering collides with the second cylindrical portion of the second electrode, it becomes possible to alleviate the sputtered matter scattering into the glass tube. According to this, it is possible to alleviate mercury being consumed because of combination of the sputtered matter with the mercury, so that it is possible to alleviate the life of the cold-cathode tube lamp becoming short because of consumption of the mercury.
Besides, in the cold-cathode tube lamp having the above structure, the second electrode may further have a second bottom portion that closes the other end of the second cylindrical portion.
In this case, it is preferable that the second electrode is disposed in such a way that the second bottom portion butts against the first bottom portion of the first electrode. According to such structure, it becomes possible to unitarily form the first electrode and the second electrode in the same process; accordingly, even if the second electrode is formed in the first electrode to alleviate the electrode being broken by sputtering, it is possible to alleviate increase of production manpower. According to this, it is possible to alleviate the production process becoming onerous.
Besides, in the cold-cathode tube lamp having the above structure, it is preferable that the second electrode is formed concentrically with the first electrode. According to such structure, so that the predetermined distance between the first cylindrical portion of the first electrode and the second cylindrical portion of the second electrode becomes equal, the second electrode is disposed in the first electrode; accordingly, it is possible to easily alleviate concentrative occurrence of sputtering on the first bottom portion of the first electrode. According to this, because it is possible to alleviate breakdown of the electrode, it is possible to alleviate the life of the cold-cathode tube lamp becoming short.
Besides, in the cold-cathode tube lamp having the above structure, it is preferable that an outer diameter of the second cylindrical portion of the second electrode is 0.1 to 0.8 times of an outer diameter of the first cylindrical portion of the first electrode. According to such structure, because it is possible to easily alleviate concentrative occurrence of sputtering on the bottom portion of either of the first electrode and the second electrode, it is possible to alleviate the first electrode or the second electrode being broken by the sputtering. According to this, it is possible to alleviate the life of the cold-cathode tube lamp becoming short.
Besides, in the cold-cathode tube lamp having the above structure, it is preferable that a length of the second cylindrical portion of the second electrode is 0.5 to 1.0 times of a length of the first cylindrical portion of the first electrode. According to such structure, it is possible to alleviate ions and the like colliding with a tip end portion of the second cylindrical portion of the second electrode in a concentrative fashion. Besides, because a step is formed between the second cylindrical portion of the second electrode and the first cylindrical portion of the first electrode, it becomes hard for sputtered matter generated in the first electrode and the second electrode to scatter into the glass tube. According to this, it is possible to alleviate the life of the cold-cathode tube lamp becoming short because of combination of the sputtered matter with the mercury.
Besides, in the cold-cathode tube lamp having the above structure, it is preferable that an inner diameter of the glass tube is 3 mm or longer. According to such structure, because it is possible to enlarge the tube diameter of the cold-cathode tube lamp, it is possible to secure a sufficient amount of light and raise light emission efficiency by flowing a large current into the cold-cathode tube lamp.
Besides, in the cold-cathode tube lamp having the above structure, it is preferable that total gas pressure of the rare gas filled in the glass tube is 50 Torr or lower. According to such structure, it is possible to raise the light emission efficiency.
Besides, in the cold-cathode tube lamp having the above structure, it is preferable that a plurality of lead terminals one end of which is connected to the first electrode and the other end of which is led out to outside of the glass tube are disposed on each first electrode. According to such structure, even in a case where the size of the first electrode is large, because it is possible to surely support the first electrode with a good balance and reduce a load on one lead terminal, it is possible to alleviate deformation and breakdown of the lead terminal occurring at a connection portion of the first electrode and the lead terminal. According to this, it is possible to alleviate the life of the cold-cathode tube lamp becoming short because of breakdown of the electrode.
Besides, even in a case where the heat generation amount increases by enlarging the size of the first electrode, the generated heat is radiated from each of the plurality of lead terminals, so that it is possible to alleviate a disadvantage and the like that the heat generated at the first electrode propagates to the glass tube and the tube-wall temperature of the glass tube rises; and because of this, the mercury reabsorbs ultraviolet rays emitted. According to this, it becomes possible to alleviate the light emission efficiency becoming low. Besides, because the heat generated at the first electrode is radiated from each of the plurality of lead terminals, it is possible to alleviate a disadvantage that the heat concentrates on any of the lead terminals; and because of this, a lamp base connected to the lead terminal and a nearby connector are damaged.
Besides, to achieve the above object, a lighting device for a display device according to the present invention includes the above cold-cathode tube lamp.
According to the above structure, by including the above cold-cathode tube lamp, the lighting device for a display device is able to alleviate the life of the cold-cathode tube lamp becoming short because of sputtering; accordingly, it is possible to alleviate a disadvantage and the like that the life of the cold-cathode tube lamp becomes short; and because of this, brightness of the lighting device for a display device becomes low.
Besides, to achieve the above object, a display device according to the present invention includes the above lighting device for a display device.
According to the above structure, because the display device includes the above lighting device for a display device, it is possible to alleviate a disadvantage and the like that the life of the cold-cathode tube lamp becomes low; and because of this, brightness of the display device becomes low; accordingly, it is possible to raise reliability of the display device.
Besides, to achieve the above object, a television receiving device according to the present invention includes the above display device.
According to the above structure, because the television receiving device includes the above display device, it is possible to alleviate a disadvantage and the like that the life of the cold-cathode tube lamp becomes low; and because of this, the brightness of the display device becomes low; accordingly, it is possible to raise reliability of the television receiving device.
As described above, according to the present invention, it is possible to provide a cold-cathode tube lamp, a lighting device for a display device, a display device and a television receiving device that use the cold-cathode tube lamp.
The cold-cathode tube lamp 100 according to the first embodiment, as shown in
In the first embodiment, outer diameters (a) of the electrode 21 and the electrode 22 are each 2 mm to 10 mm, preferably, 2 mm to 3.5 mm; and total lengths (b) of the electrode 21 and the electrode 22 are each 4 mm to 20 mm, preferably, 4 mm to 10 mm. Besides, a ratio value of the outer diameter (a) of the electrode to the total length (b) of the electrode, that is, a/b=0.5 to 1. Here, in the first embodiment, the electrode 21 and the electrode 22 are made of nickel (Ni) and formed by pressing or the like. Besides, the electrode 21 and the electrode 22 are examples of a “first electrode” of the present invention; and the cylindrical portion 21a and the cylindrical portion 22a are examples of a “first cylindrical portion” of the present invention. Besides, the bottom portion 21b and the bottom portion 22b are examples of a “first bottom portion” of the present invention.
As shown in
In the first embodiment, as described above, the discharge tube that is composed of: the glass tube 11 that has the inner diameter (f) of 3 mm or longer; and the pair of electrodes 21 and 22 that have the outer diameter (a) of 2 mm to 10 mm and the total length (b) of 4 mm to 20 mm is included; and the mixed gas of argon and neon is filled in such a way that the total gas pressure of the rare gases become 50 Torr or lower, so that it becomes possible to raise brightness and improve light emission efficiency of the cold-cathode tube lamp 100 by flowing a large current into the cold-cathode tube lamp 100.
Besides, in the first embodiment, as shown in
Besides, in the first embodiment, as shown in
In the first embodiment, as shown in
In the first embodiment, as described above, because the electrode 41 and the electrode 42 are formed in the electrode 21 and the electrode 22, respectively, a discharge area becomes large and current densities become low. According to this, it is possible to easily alleviate occurrence of sputtering. Besides, because ions and the like generated in the glass tube 11 collide with not only the electrode 21 and the electrode 22 but also the electrode 41 and the electrode 42, it is possible to alleviate concentrative occurrence of sputtering on one electrode. Besides, because the electrode 21 and the electrode 41, and the electrode 22 and the electrode 42, as shown in
Further, because part of the sputtered matter generated in the electrode 21 and the electrode 22 collides with the cylindrical portion 41a and the cylindrical portion 42a of the electrode 41 and the electrode 42, it becomes possible to alleviate the sputtered matter scattering into the glass tube 11. Besides, because each of the cylindrical portion 41a and the cylindrical portion 42a of the electrode 41 and the electrode 42 are formed not to protrude beyond each of the cylindrical portion 21a and the cylindrical portion 22a of the electrode 21 and the electrode 22, it becomes hard for the sputtered matter to scatter into the glass tube; accordingly, it is possible to alleviate a disadvantage that the sputtered matter combines with mercury; and because of this, the mercury is consumed. According to this, it is possible to alleviate a disadvantage that the mercury decreases; and because of this, the brightness and life of the cold-cathode tube lamp decrease.
In the second embodiment, as shown in
In the second embodiment, as shown in
Besides, by connecting the three lead terminals 33 (34) to the electrode 21 (22), heat generated at the electrode 21 (22) is radiated from each of the three lead terminals 33 (34), so that even in a case where the heat generation amount increases by enlarging the outer diameter of the electrode 21 (22), it is possible to efficiently radiate the generated heat from each of the three lead terminals 33 (34). According to this, it is possible to alleviate a disadvantage and the like that the heat generated at the electrode 21 (22) propagates to the glass tube and the tube-wall temperature of the glass tube rises; and because of this, the mercury reabsorbs ultraviolet rays emitted; accordingly, it becomes possible to alleviate the light emission efficiency becoming low. Besides, the heat generated at the electrode 21 (22) is radiated from each of the three lead terminals 33 (34), so that it is possible to alleviate a disadvantage that the heat concentrates on any one of the lead terminals 33 (34); and because of this, a lamp base connected to the lead terminals 33 (34) and a nearby connector are damaged.
Here, the other structures of the second embodiment are the same as the first embodiment.
The lighting device 200 for a display device, as shown in
The plurality of cold-cathode tube lamps 100, as shown in
Because the lighting device 200 for a display device according to the third embodiment, as described above, includes the cold-cathode tube lamp 100 according to the first embodiment of the present invention, decrease in the life of the cold-cathode tube lamp caused by sputtering is alleviated. According to this, it becomes possible to alleviate a disadvantage and the like that brightness of the lighting device for a display device becomes low because of decrease in the life of the cold-cathode tube lamp.
The liquid crystal display device 300, as shown in
In the fourth embodiment, as described above, the lighting device 200 for a display device that includes the cold-cathode tube lamp 100 is disposed on a rear surface of the liquid crystal panel 62; and each of the other constituent members is disposed, so that light emitted from the cold-cathode tube lamp 100 is output to the liquid crystal panel 62 side. According to this, it becomes possible to display an image and the like on the liquid crystal panel 62.
Because the display device 300 according to the fourth embodiment, as described above, includes the lighting device 200 for a display device that includes the cold-cathode tube lamp 100, it is possible to alleviate a disadvantage and the like that brightness of the display device 300 becomes low because of decrease in the life of the cold-cathode tube lamp 100. According to this, it is possible to raise reliability of the display device 300.
Here, in the fourth embodiment, the liquid crystal display device is described; however, this is not limitative, and the cold-cathode tube lamp may be applied to a display device other than the liquid crystal display device.
Besides, the liquid crystal display device according to the fourth embodiment is able to be used for a television receiving device, for example. A television receiving device according to the present invention includes, for example: a ground-wave antenna; a television receiving tuner; an output portion; a keyboard; a storage portion; a GPS receiving antenna: a television receiving portion; a GPS receiving portion; and a control portion. The liquid crystal display device according to the fourth embodiment is able to be used as a display that outputs an image signal and a sound signal that are converted by a MPEG 2 decoder or an image/sound decoder, and forms the output portion together with a speaker and the like.
Because the television receiving device includes the display device 300 according to the fourth embodiment, it is possible to alleviate a disadvantage and the like that brightness of the display device 300 becomes low because of decrease in the life of the cold-cathode tube lamp 100 that is used in the lighting device 200 for a display device of the display device 300. According to this, it is possible to raise reliability of the television receiving device.
Here, it should be thought that the embodiments disclosed this time are examples in all respects and not limitative. The scopes of the present invention are not represented by the description of the above embodiments but by the claims and further read on all modifications within the meaning equivalent to the claims.
For example, in the above first to fourth embodiments, the structure in which the mixed gas of argon and neon is filled in the glass tube is described as an example; however, this is not limitative, and a rare gas other than argon and neon may be filled. Specifically, there are xenon and krypton.
Besides, in the above first to fourth embodiments, the electrode that is made of nickel (Ni) is described as an example; however, this is not limitative, and a metal material other than nickel (Ni) may be used. Specifically, there are metal materials, for example, such as niobium (Nb), molybdenum (Mo), tungsten (W) and the like.
Besides, in the above first to fourth embodiments, the lead terminal that is made of nickel (Ni) is described as an example; however, this is not limitative, and a lead terminal that is made of a metal material other than nickel (Ni) may be used. As metal materials other than nickel (Ni), there are, for example, copper (Cu), tungsten (W) and the like. Here, the electrode and the lead terminal may be made of the same metal material or may be made of different metal materials.
Besides, in the above first and second embodiments, the second electrode that is composed of the second cylinder-shape cylindrical portion that has the opening portion at one end and the second bottom portion that closes the other end of the second cylindrical portion is described as an example; however, this is not limitative, and as shown in
Besides, in the above first and second embodiments, the structure in which the second electrode is disposed in such a way that the second bottom portion of the second electrode butts against the first bottom portion of the first electrode is described as an example; however, this is not limitative, and as shown in
Besides, in the above second embodiment, the structure in which the three lead terminals are used is described as an example; however, this is not limitative, and at least two or more lead terminals are sufficient as the plurality of lead terminals. Besides, the shape formed by the lead terminals may not be a regular-polygonal shape; and it is sufficient if the lead terminals are disposed in such a way that the center of gravity of a polygonal shape formed by the lead terminals substantially agrees with the center of the bottom portion of the electrode. Besides, the shape formed by the lead terminals may not be a polygonal shape; and it is sufficient if the lead terminals are disposed in such a way that at lest two lead terminals of the plurality of lead terminals are disposed at opposite positions with respect to the center of the bottom portion of the electrode when viewed in a planar fashion. Further, one lead terminal of the plurality of lead terminals may be disposed at the center of the bottom portion of the electrode.
Besides, in the above third and fourth embodiments, the structure in which the cold-cathode tube lamp according to the first embodiment is used is described as an example; however, this is not limitative, and it is possible to employ a structure which uses any cold-cathode tube lamps represented by the claims inclusive of the cold-cathode tube lamp according to the second embodiment and the cold-cathode tube lamps according to modifications of the present invention.
Besides, in the above fourth embodiment, a type in which the lighting device for a display device that includes the cold-cathode tube lamp is disposed on the rear-surface side of the liquid crystal panel, that is, a direct type is described as an example; however, this is not limitative, and an edge light type in which the lighting device for a display device that includes the cold-cathode tube lamp is disposed on an end portion side of the liquid crystal panel may be used.
Number | Date | Country | Kind |
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2007-245469 | Sep 2007 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2008/056980 | 4/9/2008 | WO | 00 | 3/19/2010 |