Patent Application
20090262278
The present invention relates to an external electrode lamp, a backlight unit, and a liquid crystal display device, and in particular to technology for improving an in-dark starting characteristic of the external electrode lamp.
One example of an external electrode lamp is an external electrode fluorescent lamp (EEFL: External Electrode Fluorescent Lamp). Similarly to cold cathode fluorescent lamps, EEFLs are more suited for reductions in diameter than hot cathode fluorescent lamps. EEFLs are therefore favorably used as light sources in backlight units for which a reduction in thickness (reduction in size) is demanded.
There are two main types of backlight units, namely an edge-light type in which a light guide plate is provided on a back face of an LCD panel and a fluorescent lamp is disposed on an edge surface of the light guide plate, and a direct type in which a plurality of fluorescent lamps are arranged parallel to the back face of the LCD panel. When the two types are compared, generally edge-light type backlight units can be said to be superior in terms of brightness uniformity of the light emitting face and reductions in thickness and disadvantageous in terms of increases in brightness, whereas direct type backlight units can be said to be superior in terms of increases in brightness and somewhat disadvantageous in terms of reductions in thickness.
For this reason, direct type backlight units are often employed in LCD apparatuses that are used in liquid crystal TVs in which an increase in brightness is emphasized.
When cold cathode fluorescent lamps are employed as a light source in a direct type backlight unit, a different high frequency lighting circuit (inverter) is required for each cold cathode fluorescent lamp, which leads to a rise in cost. In view of this, in recent years there has been active development of EEFLs in which an external electrode is provided on an outer circumference of each end of a tube-shaped glass container, the glass tube wall is used as a capacitance, and light is emitted by a dielectric barrier discharge (patent document 1). Given that the EEFL itself has a capacitance, a plurality of lamps can be lit by one inverter, thereby enabling a significant reduction in cost.
Patent document 1: Japanese Patent Application Publication No. S61-126559
However, EEFLs, which do not have an electron-generating electrode in the discharge space, have a poor in-dark starting characteristic. Specifically, the number of electrons required for starting is not sufficient in the dark, thereby incurring the risk of a starting failure. Due to the structure of general backlight units, EEFLs used therein are in an environment of scarce external light. This problem is therefore significant in EEFLs used in backlight units.
The voltage applied to the external electrodes may be increased in order to prevent starting failures. However, doing so incurs the risk that the difference in potential between the external electrodes and the glass container will exceed the dielectric breakdown voltage of air. As a result, a discharge would occur between the external electrodes and the glass container, thereby producing ozone which has a strong oxidizing property.
Note that the aforementioned in-dark starting characteristic problem is not limited to EEFLs. This problem is also shared by, for example, external electrode ultraviolet lamps that directly use only ultraviolet light and that are used for sterilization etc.
The present invention has been achieved in light of the above problem, and an aim thereof is to provide an external electrode lamp that can, compared to conventional technology, further suppress the voltage applied to an external electrode for discharge inception, a backlight unit including such external electrode lamp, and a liquid crystal display device including such backlight unit.
In order to achieve the above aim, the present invention is an external electrode lamp including: a discharge container having a discharge medium enclosed therein; and a first external electrode and a second external electrode that have been provided external to the discharge container, wherein a capacitance of a first capacitor is greater than a capacitance of a second capacitor, the first capacitor being constituted from the first external electrode and a first dielectric part that includes a portion of the discharge container between the first external electrode and the discharge medium, and the second capacitor being constituted from the second external electrode and a second dielectric part that includes a portion of the discharge container between the second external electrode and the discharge medium.
In order to achieve the above aim, the present invention is also a backlight unit including: the above external electrode lamp; and a lighting circuit unit operable to apply an alternating voltage to the first external electrode and the second external electrode such that in at least a half cycle of the alternative voltage, a potential of the first external electrode is higher than a potential of the second external electrode.
In order to achieve the above aim, the present invention is also a liquid crystal display apparatus including: a liquid crystal display panel; and the backlight unit of claim 19, the backlight unit including an envelope that houses a plurality of the external electrode lamps, and the envelope having been provided on a back face of the liquid crystal display panel.
According to the external electrode lamp of the present invention, since the capacitance of the first capacitor that includes the first external electrode is greater than the capacitance of the second capacitor that includes the second external electrode, if for example the high voltage output of a lighting circuit is connected to the first external electrodes and the other end of the lighting circuit is grounded and connected to the second external electrode, the voltage-to-ground at a portion of the inner wall of the discharge container that opposes the first external electrode is higher than a conventional external electrode lamp in which the capacitances of both capacitors are substantially equal. As a result, if the magnitude of the voltage applied to both external electrodes is the same, a discharge can be started more easily than in conventional technology, and the in-dark starting characteristic is improved. In other words, the voltage applied to the first and second external electrodes to start a discharge can be lower than in conventional technology.
Embodiments of the present invention are described below with reference to the drawings.
The fluorescent lamp 2 has a glass container 4, which is an example of a discharge container. The glass container 4 is a long and thin cylindrical glass tube whose ends have been hermitically sealed. The material of the glass container 4 is, for example, borosilicate glass, quartz glass, soda glass, or lead glass. Also, in a case of being used as a backlight light source in a liquid crystal display device, the glass container 4 has an outer diameter of approximately 1 to 20 mm, and the value of half the difference between the outer and internal diameters of the glass container 4, that is to say, the thickness of the glass container 4 is set to approximately 0.1 to 2 mm. Note that if one of the above-listed glass materials is selected, the glass container 4 (the selected glass material) has a relative permittivity in the range of 3 to 10.
A first external electrode 6 and a second external electrode 8 have been formed on the outer circumference of respective ends of the glass container 4. The first external electrode 6 has been formed so as to, over the width W1 thereof (the length W1 of the electrode in the tube axis X1 direction of the glass container 4), encompass the entire circumference of the glass container 4. Note that although not depicted in
A protective film 10 has been formed on substantially an entirety of the inner circumferential surface of the glass container 4, including portions thereof that oppose the first and second external electrodes 6 and 8. The protective film 10 is made of an aggregation of metal oxide particles. Yttrium oxide (Y2O3), alumina (Al2O3), etc. can be used as the metal oxide.
A phosphor film 12 has been laminated on the inner side of the protective film 10. With respect to the longitudinal direction of the glass container 4 (tube axis X1 direction), the phosphor film 12 has been formed in a range from the first external electrode 6 to the second external electrode 8. Note that as shown in
Also, a predetermined amount of mercury and a mixture of rare gases at a predetermined pressure have been enclosed in the glass container 4 as a discharge medium. The mixture of rare gases can be, for example, a neon-argon gas mixture.
In the fluorescent lamp 2 having the above structure, when a high-frequency voltage is applied to the first and second external electrodes 6 and 8 by a high frequency lighting circuit 14, a discharge phenomenon occurs in the hermitically sealed space (discharge space) in the glass container 4, thereby causing ultraviolet radiation to be emitted. The ultraviolet radiation is converted into visible light by the phosphor film 12 and emitted out of the glass container 4. In other words, when a high-frequency, high-voltage alternating voltage is applied to the first and second external electrodes 6 and 8, dielectric polarization occurs at portions of the glass container 4, which is a dielectric, that are directly below the first and second external electrodes 6 and 8, and the inner walls of these portions act as electrodes. Accordingly, a high voltage is introduced into the glass container 4, and a dielectric barrier discharge occurs therein. As such, in the dielectric barrier discharge, the electrodes are not directly exposed to plasma since the discharge space is surrounded by a dielectric (the glass container 4).
However, as mentioned above, EEFLs, which do not have an electron-generating electrode in the discharge space, have a poor in-dark starting characteristic. The following describes, with reference to
Generally, the status of an external electrode lamp before discharge inception can be shown by an equivalent circuit such as shown in
For the sake of clarity in the description, as shown in
Ct=(Ce×CD)/(Ce+Cd) (1)
Also, in the following relationship, Vt is the overall voltage applied to the external electrode lamp, Ve is the voltage applied to the capacitor Ce, and Vd is the voltage applied to the capacitor Cd (the discharge medium).
Vt=Ve+VD (2)
Vd=Vt×{Ce/(Ce+Cd)} (3)
Expression (3) shows that in order to increase Vd to improve the in-dark starting characteristic without raising the voltage Vt, Cd can be reduced or Ce can be increased.
However, since Cd is in inverse proportion to the distance between the electrodes, reducing Cd requires increasing the distance between the electrodes, which brings about an increase in the discharge starting voltage.
In the following expression for obtaining Ce, De is the thickness of the glass container, Ee is the relative permittivity of the glass container, and Se is the effective area of the external electrodes (the surface area of the portions of the external electrodes that face the discharge medium).
Ce=(∈e×Se)/2De (4)
Therefore, although Ce can be increased if ∈e and Se are increased and De is decreased, increasing Ce more than necessary causes the discharge current during lighting of the lamp to rise, which invites an excessive rise in temperature and reduction in luminance efficiency.
In view of this, as a result of dedicated research, the inventors of the present invention found that, letting the first capacitor be the capacitor constituted from one of the external electrodes (the first external electrode) and the portion of the glass container between the first external electrode and the discharge medium, letting the second capacitor be the capacitor constituted from the other external electrode (the second external electrode) and the portion of the glass container between the second external electrode and the discharge medium, letting C1 be the capacitance of the first capacitor, and letting C2 be the capacitance of the second capacitor, whereas C1 and C2 are conventionally substantially equal (C1≈C2), the in-dark starting characteristic can be improved without increasing the overall voltage applied to the lamp, by setting C1 to be greater than C2 (C1>C2), connecting the first external electrode to the high tension side of the lighting circuit, and connecting the second external electrode to the ground (GND) side of the lighting circuit.
The following describes the above with reference to
When an external electrode lamp is mounted and used in the housing of a backlight unit, a capacitance forms between the glass container and the ground (GND) line, and between the glass container and an adjacent conductor such as the metal frame inside the backlight unit. Focusing now on one external electrode from the external electrode pair (here, the first external electrode), a higher potential-to-ground at a portion of the inner wall of the glass container opposing the first electrode is more advantageous to starting.
If the magnitude of the voltage applied to the first and second external electrodes is the same, setting the capacitance C1 to be greater than the capacitance C2 raises the potential-to-ground Vb at the inner wall of the glass container opposing the first external electrode of the external electrode lamp pertaining to the present embodiment over the potential-to-ground Va at the inner wall of the glass container opposing the first external electrode of the conventional external electrode lamp. The present invention therefore enables improving the in-dark starting characteristic without increasing the voltage applied to the external electrodes. In other words, the present invention enables obtaining the same in-dark starting characteristic as in conventional technology while using a lower discharge starting voltage (voltage applied to both external electrodes).
Here, the capacitance C1 is obtained in the following expression.
C1=(∈1×S1)/d1 (5)
C2=(∈2×S2)/d2 (6)
Since generally ∈1=∈2, in order to realize C1>C2, based on expressions (5) and (6), S1 may be set to be greater than S2 (S1>S2), or d1 may be set to be less than d2 (d1<d2). Alternatively, these two may be combined (i.e., S1>S2 in addition to d1<d2).
In the fluorescent lamp 2 pertaining to the present embodiment shown in
Note that in the fluorescent lamp 2 (see
The inventors of the present invention examined variations in the difference between the values of C1 and C2 in conventional external electrode lamps that occur due to manufacturing reasons. Main causes of such variations are thought to be variations in the thickness of the glass container, and variations in the lengths of the external electrodes in the tube axis direction (in the present examination, simply called “electrode length”).
First, ten test external electrode lamps each having an overall length of 880 mm were provided to examine variations in the thickness of the glass container at sites corresponding to the external electrodes. Note that the design value of the inner diameter a and outer diameter b of the glass container in the test lamps was 2.90 mm and 4.00 mm respectively.
The capacitance C of the capacitor constituted at one external electrode portion is expressed as follows.
C=2π∈0L/{ln(b/a)} (7)
Based on expression (7), the ratio of the capacitances at the external electrode portions is ln(b/a) if the electrode lengths L are the same.
For each test lamp, the inner and outer diameters a and b of the glass container were measured at both ends, and ln(b/a) was calculated for each end using the measured values. The smaller of the two resulting calculated values was divided by the larger calculated value to obtain the capacitance ratio (percentage). The average value AVG of the ten obtained capacitance ratios was 98.9%, where 3σ=2.75%. Therefore, the variation in the capacitance ratio attributable to the thickness of the glass container is between 100% and 96.1% (=AVG−3σ).
Also, when the external electrodes are formed by screen printing, the tolerance for the electrode length L is approximately ±0.1 m. Therefore, when the design value of the electrode length L is 20 mm, the variation in the capacitance ratio attributable to variations in electrode length is at most 99.0% (=20.1/19.9).
When both the thickness of the glass container and electrode length are taken into consideration, the variation in the capacitance ratio is between 100% and 95.1% (=96.1×99.0).
In other words, even in conventional external electrode lamps, there are cases in which C1 is greater than C2 within the range of 100>C2/C1≧95.1%.
In view of this, the value of C2/C1 of the external electrode lamp pertaining to the present embodiment is preferably less than or equal to 95.0%. Setting such a range enables reducing the discharge starting voltage lower than in conventional external electrode lamps. In other words, in the present embodiment, setting C1 to be greater than C2 means creating a larger difference between C1 and C2 than in the case of an external electrode lamp obtained by normal manufacturing in which C1 and C2 are to be equal.
The lower the value of C2/C1 is set, that is to say, the greater C1 is over C2, the lower the discharge starting voltage is, thereby enabling an improvement in the in-dark starting characteristic. However, as the value of C2/C1 is reduced, that is to say, as the difference between C1 and C2 increases, the brightness gradually changes in the tube axis direction of the EEFL, that is to say, there is the phenomenon in which the degree of luminance imbalance increases. In other words, in the case of the present example, the brightness decreases from the first capacitor side which has the larger capacitance C1 to the second capacitor side which has the smaller capacitance C2.
In view of this, the inventors of the present invention performed a test to examine the degree of luminance imbalance when changing the value of C2/C1, as well as the starting voltage reduction effect.
The EEFLs provided for the test (hereinafter, called “test lamps”) had basically the same structure as the fluorescent lamp 2 pertaining to embodiment 1 shown in
The specifications of the test lamps were specifically as follows.
The glass container 4 was made of borosilicate glass. The glass container 4 had an overall length of 880 mm, an outer diameter of 3.0 mm, and an inner diameter of 2.0 mm.
YOX, LAP, and BAM were used as the red, green, and blue phosphors constituting the phosphor film 12, and the phosphors emitted white light overall.
Mercury and a mixture of rare gases were enclosed in the glass container 4. The rare gas mixture was made of 95% neon and 5% argon, and enclosed at a pressure of 8 kPa.
The first and second external electrodes 6 and 8 were both formed by wrapping copper tape (CU-35C made by 3M, Inc.) around the entire circumference of the glass container 4. Here, in order to obtain test lamps having different values for C2/C1, four test lamps A, B, C, and D were manufactured, each having a different combination of sizes for the width W1 of the first external electrode 6 and the width W2 of the second external electrode 8.
Note that in order to ensure reliability, external electrodes are normally constituted from a silver (Ag) paste film and a lead (Pb)-free solder film as previously described. However, using copper tape was not a problem in the present examination of initial characterization where C2/C1 is the parameter, and therefore copper tape was used in order to simplify the experiment. What was important was for the same external electrode material to be used for the first and second external electrodes 6 and 8.
As described above, since the glass containers 4 of the above test lamps are long, the two lighting circuits 16 and 18 shown by dashed-dotted lines in
When measuring the starting voltage, the four test lamps A, B, C, and D were covered by a blackout curtain to obtain a lighting intensity of 0.1 lux or less under the cloth.
To measure the starting voltage, an oscilloscope (WavePro 7200, made by LeCroy Corp.) was used, and a 1,000:1 high-voltage probe (P6015A, made by Tektronix, Inc.) was connected to the oscilloscope.
Also, the degree of luminance imbalance was measured with the use of a luminance meter (BM8, made by Topcon Technohouse Corp.) by measuring the brightness at the five sites of, in the tube axis direction, 147 mm, 293 mm, 440 mm, 587 mm, and 733 mm from the end of the glass container 4 corresponding to the first external electrode 6. For each of the test lamps, the smallest of the measured brightness values was divided by the largest of the measured brightness values (smallest value/largest value), and the calculated value was used as an indicator of the degree of luminance imbalance (luminance uniformity). The smaller the value of the luminance uniformity (%), the greater the degree of luminance imbalance, whereas the greater the value of the luminance uniformity, the smaller the degree of luminance imbalance.
In
Using the values of
Based on the above results, it is preferable for C2/C1 to be no more than 95% and no less than 43%.
The upper limit is 95% since, as previously described, setting the ratio of C1 and C2 in this way enables reducing the discharge starting voltage at least lower than in conventional external electrode lamps.
The lower limit is set to 43% for the following reason. Specifically, a luminance uniformity of 50% or higher is normally required when using the fluorescent lamp of the present embodiment as the light source in the backlight unit of a liquid crystal display device. Here, the luminance uniformity is 50% when C2/C1=43%, and therefore a luminance uniformity of 50% or greater can be maintained as long as C2/C1 is 43% or greater.
Furthermore, it is preferable for C2/C1 to be no more than 77%. Although the discharge starting voltage can be reduced lower than conventionally possible when C2/C1 is 95% or less, it is preferable for at least the starting voltage relative value to be 85% or less when actual use in a liquid crystal display device or the like is taken into consideration.
In embodiment 1, the width W1 of the first external electrode 6 is set to be greater the width W2 of the second external electrode 8, thereby giving the first external electrode 6 a larger effective area than the second external electrode 8 and making C1 greater than C2 (see
In contrast, in an external electrode fluorescent lamp 20 (hereinafter, called the “fluorescent lamp 20”) pertaining to embodiment 2 and shown in
Accordingly, provided that the light-emitting lengths in the tube axis direction of the fluorescent lamps are equal, the overall length of the fluorescent lamp of the present embodiment can be made shorter than the fluorescent lamp of embodiment 1. In other words, provided that the overall lengths of the fluorescent lamps are equal, the light-emitting length of the fluorescent lamp of the present embodiment can be made longer than (the light-emitting area can be increased more than) the fluorescent lamp of embodiment 1.
Note that in the fluorescent lamp 20 shown in
In embodiments 1 and 2, C1 is set to be greater than C2 by giving the first external electrode a greater effective area than the second external electrode.
In contrast, in the EEFLs of this and subsequent embodiments, C1 is set to be relatively greater than C2 by setting the average thickness d1 of the first dielectric part in the first capacitor that includes the first external electrode to be relatively smaller than the average thickness d2 of the second dielectric part in the second capacitor that includes the second external electrode.
In an external electrode fluorescent lamp 28 (hereinafter, called the “fluorescent lamp 28”) pertaining to embodiment 3 and shown in
The above structure enables a reduction in cost without making large changes to the manufacturing process.
The inventors of the present invention made a working example of the fluorescent lamp 28 pertaining to embodiment 3 and measured the starting voltage. Here, the working example lamp had the same structure as the aforementioned test lamp A, with the exception of a different external diameter of the glass container portion 34A on which the first external electrode 30 is provided. In the working example lamp, the external diameter of the glass container portion 34 on which the first external electrode 30 is provided is 2.4 mm.
The measuring tools, environment for measuring the starting voltage, and the like were the same as in the previously described test. The measurement results showed that the starting voltage of the working example lamp pertaining to embodiment 3 was 2140 [V]. In other words, the starting voltage of the working example lamp was verified to be lower than the 2850 [V] starting voltage of the test lamp A (see
In an external electrode fluorescent lamp 36 (hereinafter, called the “fluorescent lamp 36”) pertaining to embodiment 4 and shown in
According to this structure, the outward form of the lamp is symmetrical, which enables use thereof in the housing of a conventional backlight unit.
Note that in the fluorescent lamp 36, constituent elements that are substantially the same as any of the fluorescent lamps of the above embodiments have been given the same reference notations, and descriptions thereof have been omitted.
In an external electrode fluorescent lamp 40 (hereinafter, called the “fluorescent lamp 40”) pertaining to embodiment 5 and shown in
This structure enables a greater cost reduction than embodiment 4 since the protective film material is normally more inexpensive than the phosphor material.
Note that in the fluorescent lamp 40, constituent elements that are substantially the same as any of the fluorescent lamps of the above embodiments have been given the same reference notations, and descriptions thereof have been omitted.
In an external electrode fluorescent lamp 44 (hereinafter, called the “fluorescent lamp 44”) pertaining to embodiment 6 and shown in
The dielectric material forming the dielectric film 46 can be, for example, titanium oxide microparticles (relative permittivity: 100). Using such a material gives the dielectric film 46 the characteristics of transmitting visible light and absorbing ultraviolet light. This prevents, as much as possible, ultraviolet light from being emitted out of the glass container 4, thereby preventing the degradation of members in the vicinity of the fluorescent lamp 44 in the device in which it is mounted.
In the fluorescent lamp 44, d2 is set to be greater than d1 by extending the dielectric film 46 toward the second external electrode 32. As described above, since the relative permittivity of the dielectric film 46 is the same as or less than that of the glass container, increasing d2 enables setting C2 to be less than C1.
Also, the dielectric material forming the dielectric film 46 may be, for example, aluminum oxide microparticles (relative permittivity: 8.5). Using such a material gives the dielectric film 46 the characteristics of transmitting visible light and reflecting ultraviolet light. As a result, rather than being absorbed by the glass container, the ultraviolet light is efficiently converted into visible light by the phosphor film 12, thereby improving the brightness of the emitted visible light.
Note that in the fluorescent lamp 44, constituent elements that are substantially the same as any of the fluorescent lamps of the above embodiments have been given the same reference notations, and descriptions thereof have been omitted.
In an external electrode fluorescent lamp 48 (hereinafter, called the “fluorescent lamp 48”) pertaining to embodiment 7 and shown in
The dielectric material forming the dielectric film 50 can be, for example, silica glass (relative permittivity: 3). Using such a material gives the dielectric film 50 the characteristics of transmitting visible light and ultraviolet light, and protecting the phosphor film 12 from plasma. This prevents, as much as possible, the degradation of the phosphor film 12 due to exposure to discharge plasma.
In the fluorescent lamp 48, d2 is set to be greater than d1 by extending the dielectric film 50 toward the second external electrode 32. As described above, since the relative permittivity of the dielectric film 50 is the same as or less than that of the glass container, increasing d2 enables setting C2 to be less than C1.
Note that in the fluorescent lamp 48, constituent elements that are substantially the same as any of the fluorescent lamps of the above embodiments have been given the same reference notations, and descriptions thereof have been omitted.
In an external electrode fluorescent lamp 52 (hereinafter, called the “fluorescent lamp 52”) pertaining to embodiment 8 and shown in
This enables freely changing the value of C2/C1 since the thickness and material of the dielectric paste can be changed easily.
Note that in the fluorescent lamp 52, constituent elements that are substantially the same as any of the fluorescent lamps of the above embodiments have been given the same reference notations, and descriptions thereof have been omitted.
The following describes an example of using any of the fluorescent lamps pertaining to the above embodiments as a light source in a backlight unit. Although any fluorescent lamp from embodiments 1 to 8 or the later-described embodiments 10 to 14 may be used, the following describes a case of using the fluorescent lamp 2 (see
The backlight unit 56 has an envelope 62 that is made of a rectangular reflecting plate 58, side plates 60 encompassing the reflecting plate 58, and the light-focusing plate 46 that is provided parallel to the reflecting plate 58. The reflecting plate 58 and the side walls 60 are each formed from a plate material made of PET (polyethylene terephthalate) resin, and a reflecting film (not depicted) has been formed on one of the main surfaces of each plate (the surface facing inward when assembled as the envelope 62) by vapor depositing silver or the like. Note that the reflecting plate 58 and the side walls 60 can be constituted from, for example, a metal material such as aluminum or cold rolling material (e.g., SPCC). The reflecting film may be formed by adding calcium carbonate, titanium dioxide, or the like to PET resin. Doing so further raises the rate of reflectivity.
The light-focusing plate 64 is formed by laminating a diffusion plate 66, a diffusion sheet 68, and a lens sheet 70 in the stated order, beginning from the reflecting plate 58 side. The diffusion plate 66 is a plate-shaped material made of polymethyl methacrylate (PMMA) resin, and is disposed so as to block the opening of the housing. The diffusion sheet 68 is made of, for example, polyester resin. The lens sheet 70 is made by, for example, laminating an acrylic resin and a polyester resin.
The envelope 62 internally stores a plurality (in the present example, 16) of the fluorescent lamps 2 that have been disposed parallel with the long edge of the reflecting plate 58, with equal intervals therebetween in the short edge direction. Also, the fluorescent lamps 2 are electrically connected in parallel by wiring members not depicted in
The inverter 72 converts a 50/60 Hz alternating current from a commercial power supply 74 into a high-frequency current (e.g., 60 kHz as previously mentioned), and supplies the converted current to the fluorescent lamps 2. Note that it goes without saying that the first external electrodes 6 are connected to the high-tension side of the inverter 72, and the second external electrodes 8 are connected to the ground side.
The following describes a structure in which the fluorescent lamps 2 have been mounted in the envelope 62 in the backlight unit with reference to
Connectors 84, which are formed from springy metal plates that have been curved, have been set upright on the surface of the reflecting plate 58. The fluorescent lamps 2 are mounted to the envelope 62 by fitting the first and second external electrodes 6 and 8 at the ends of the lamps into the corresponding connectors 84. The provision of such connectors 84 enables the fluorescent lamps 2 to be freely removed from the envelope 62 (from the connectors 84).
In conventional backlight units, light emitted from the light-focusing plate is generally brightest at the central portion in the longitudinal direction of the fluorescent lamp, and gradually decreases in brightness toward the ends. In other words, the brightness of the light-focusing plate surface is uneven.
In the fluorescent lamp 2 of the above embodiment, there is the previously-described luminance imbalance in which the brightness gradually decreases from the first external electrode 6 toward the second external electrode 8 (or to put it the other way around, the brightness gradually increases from the second external electrode 8 toward the first external electrode 6). In view of this, the unevenness in the brightness of the light-focusing plate surface can be mitigated with use of the luminance imbalance of the fluorescent lamp 2.
Specifically, arranging the fluorescent lamps 2 (of embodiment 1) in the envelope 86 as shown in
When arranging the fluorescent lamps 2 such as in
As previously mentioned, setting 95% as the upper limit enables reducing the discharge starting voltage more than in a conventional external electrode lamp.
The lower limit is set to 70% for the following reason. Regardless of whether the above lamp arrangement is used, if C2/C1 falls below 70%, the ends of the light-focusing plate in the longitudinal direction (horizontal direction) of the fluorescent lamps will be brighter than the central portion of the light-focusing plate. In other words, the brightness distribution of the backlight unit would revert to being imbalanced as in conventional technology, which causes users a sense of discomfort.
The following describes an example in which the backlight unit 56 is used in a liquid crystal TV, which is one example of a liquid crystal display apparatus.
The liquid crystal display panel 78 is made of a color filter substrate, liquid crystals, a TFT substrate, etc., and is driven by a driving module (not depicted) to form color images based on an image signal received from an external device.
The envelope 62 of the backlight unit 56 is provided on the back face of the liquid crystal display panel 78, and illuminates the liquid crystal display panel 78 from the back face.
The inverter 72 is disposed, for example, inside a housing 80 of the liquid crystal TV 76, but outside of the envelope 62.
Based on embodiments 10 to 14, the following describes EEFLs that, due to innovations in the configuration of members in a vicinity of the ends of the external electrodes, even more effectively suppress discharges between the external electrodes and the glass container.
The fluorescent lamp 100 has basically the same structure as the fluorescent lamp 2 (
Also, similarly to the first external electrode 6 of the fluorescent lamp 2 (
As shown in
Similarly to the first external electrode 102, the thickness of the second external electrode 104 in a vicinity of the ends thereof in the tube axis X1 direction smoothly and gradually decreases toward the ends 102A and 102B.
Note that in the fluorescent lamp shown in
In the fluorescent lamp 110, the portion of the outer circumferential surface of a glass container 118 where the first and second external electrodes have been formed has been roughened (the portion corresponding to the second external electrode is not depicted). With the exception of the roughening, the fluorescent lamp 110 has the same structure as the fluorescent lamp 100 (
The roughening is performed to increase the adhesion of the external electrodes (particularly the first electrode layer 114) to the surface of the glass container 118. Note that the roughening is performed by sandblasting before the formation of the first electrode layer 114. Also, the surface roughness after the roughening processing is approximately 1 to 3 μm. Although portions of the outer circumferential surface of the glass container 118 are worn away by the sandblasting, the degree of the surface roughness is very small as mentioned above, and the change in the outer diameter is extremely small. The change in the capacitance of the external electrode portions due to the roughening processing is therefore considered to be negligible. As such, the reduction in thickness due to the roughening processing is not taken into account with the average thickness of the dielectric (the thickness of the glass container 118).
Similarly to the fluorescent lamp 100 of embodiment 10 (
When calculating the capacitance (expression (5)) of the first external electrode 122 portion having the aforementioned shape, the effective area of the first external electrode 122 is the surface area in the range shown by W3 in the tube axis X1 direction. Out of the area where the first external electrode 122 is formed in the tube axis X1 direction, W3 is the range where the thickness of the glass container 4 (half of the difference between the outer and inner diameters) is substantially uniform. This is because discharges only occur in portions of the inner wall (inner circumferential surface) of the glass container 122 corresponding to this range. Note that in expression (7), the length of W3 in the tube axis X direction corresponds to the electrode length L when calculating the capacitance C of the capacitor constituted by the external electrode portions.
Needless to say, in the fluorescent lamp 120 pertaining to embodiment 12, the effective area of the second external electrode (not depicted) is set to be smaller than the effective area of the first external electrode 122.
Similarly to the fluorescent lamp 110 (
The fluorescent lamp 140 has a glass container 142. The glass container 142 is formed from a cylindrical glass tube whose ends have been hermitically sealed. The glass material of the glass container 142 is the same as in embodiment 1. Longitudinal cross sections of ends portions of the glass container 142 are round in shape, as shown in
A phosphor film 144 has been formed on the inner circumferential surface of the flattened portion of the glass container 142. The phosphor film 144 can be constituted from the same phosphors as in embodiment 1.
A first external electrode 146 has been formed on the outer circumference of one of the round portions of the glass container 142, and a second external electrode 148 has been formed on the outer circumference of the other round portion. The first external electrode 146 has a two-layered structure including a first electrode layer 150 and a second electrode layer 152, and the second external electrode 148 has a two-layered structure including a first electrode layer 154 and a second electrode layer 156. The first electrode layers 150 and 154, and the second electrode layers 152 and 156 can be formed from the same material as in embodiment 1.
Note that although the portions of the glass container on which the external electrodes are provided are round in shape, such portions may be elliptical or substantially flattened. In other words, the glass container may have a longitudinal cross section that is elliptical or substantially flattened.
Although described above based on the embodiments, the present invention is of course not limited to the above embodiments. For example, the following modifications are also included in the present invention.
(1) Although an example of the present invention being applied to an EEFL is described in the above embodiments, the present invention is not limited to a fluorescent lamp. The present invention can also be applied to an external electrode ultraviolet lamp. Specifically, the phosphor film may be removed from the structure of the EEFL pertaining to the above embodiment (the phosphor film is not formed) in order to construct an external electrode ultraviolet lamp. An ultraviolet lamp can be used for irradiating an object in order to, for example, sterilize the object.
(2) Although the glass container has a straight tube shape in the embodiments, the shape of the glass container is not limited to this. The glass container can have an L-shape, a U-shape, or other known shape.
(3) Although constituted from a metallic tape that has a two-layered structure including a silver (Ag) paste film and a lead (Pb)-free solder film in the embodiments, the structure of the external electrodes is not limited to this. For example, as shown in
Also, the external electrodes may be constituted from only one layer. In this case, the solder material forming the external electrodes can be a material that includes tin, a tin-indium alloy, or a tin-bismuth alloy as a main component. Also, at least one of antimony, zinc and aluminum is preferably included in the solder material as an additive from the standpoint of fixability to the glass container. Furthermore, antimony or zinc is preferably included in the solder material as an additive from the standpoint of wettability with respect to the surface of the glass container.
(4) In the above embodiments, C1 is set to be greater than C2 by giving the external electrodes different effective areas or giving the first and second dielectric parts different average thicknesses (d1 and d1). However, the present invention is not limited to this. The first and second dielectric parts may be given different relative permittivities. In other words, C1 may be set to be greater than C2 by setting the relative permittivity of the first dielectric part higher than the relative permittivity of the second dielectric part.
Specifically, for example, a first dielectric film made of a dielectric paste (whose relative permittivity is 8 to 12) may be provided between the first external electrode and the outer circumference of the glass container, and a second dielectric film made of silica glass (whose relative permittivity is 3) may be provided between the second external electrode and the outer circumference of the glass container. Instead of the above positions, the first and second dielectric films may be formed on the inner circumference of the glass container.
(5) Similarly to the EEFLs of embodiments 10 to 14, the EEFLs of embodiments 1 to 8 may have a structure in which the thickness of the external electrodes in a vicinity of the ends thereof smoothly and gradually decreases toward the ends.
Similarly to the EEFLs of embodiments 11 and 13 (
Similarly to the EEFLs of embodiments 12, 13 and 14 (
(6) Although various materials can be used for the glass container as described above, the in-dark starting characteristics can be improved if the material of the glass container is soda glass, lead glass or lead-free glass. Specifically, such types of glass include a large amount of alkali metal oxides such as most notably sodium oxide (Na2o), and in the exemplary case of sodium oxide, the sodium (Na) component elutes into the surface of the glass container as time passes. Since sodium has a low electronegativity, the sodium that elutes into the inner ends of the glass container (not provided with a protective film) is though to contribute to the improvement in in-dark starting characteristics.
In particular, in embodiments 12, 13 and 14 (
For example, in a case in which the alkali metal oxide is sodium oxide, it is preferable for 5 [mol %] to 20 [mol %] of sodium oxide to be included in the material of the glass container. If the alkali metal oxide content is lower than 5 [mol %], there is an increased probability that the in-dark starting time will exceed 1 [sec] (in other words, if the alkali metal oxide content is 5 [mol %] or greater, there is an increased probability that the in-dark starting time will be within 1 [sec]). Also, an alkali metal oxide content of over 20 [mol %] leads to whitening or darkening (browning) of the glass container over prolonged use, thereby causing a reduction in brightness, and also reduces the strength of the glass container.
Also, it is preferable to use lead-free glass in consideration of the protection of the environment. However, even with lead-free glass, there are cases in which lead is included as an impurity in the manufacturing process. Lead-free glass is therefore defined as glass that contains lead at an impurity level, which is 0.1 [wt %] or less.
Also, the glass container can be caused to absorb 254 [nm] or 313 [nm] ultraviolet radiation by doping the glass with a predetermined amount of a transition metal oxide, where the predetermined amount depends on the transition metal oxide used. Specifically, in the case of titanium oxide (TiO2), doping at a composition rate of 0.05 [mol %] or less causes the glass container to absorb 254 [nm] ultraviolet radiation, and doping at a composition rate of 2 [mol %] or more causes the glass container to absorb 313 [nm] ultraviolet radiation. However, since the glass devitrifies if the composition rate of the titanium oxide is 5.0 [mol %] or more, doping is preferably performed at a composition rate of 0.05 [mol %] to 5.0 [mol %].
Also, in the case of cerium oxide (CeO2), doping at a composition rate of 0.05 [mol %] or more causes the glass container to absorb 254 [nm] ultraviolet radiation. However, since the glass becomes colored if more than 0.5 [mol %] of cerium oxide is doped, cerium oxide is preferably doped at a composition rate of 0.05 [mol %] to 0.5 [mol %]. Note that since doping tin oxide (SnO) in addition to cerium oxide suppresses the coloration of the glass, cerium oxide can be doped at a composition rate of up to 5.0 [mol %]. In this case, the glass can be caused to absorb 313 [nm] ultraviolet radiation by doping cerium oxide at a composition rate of 0.5 [mol %] or more. However, even in this case, the glass devitrifies if cerium oxide is doped at a composition rate of more than 5.0 [mol %].
Also, in the case of zinc oxide (ZnO), doping at a composition rate of 2.0 [mol %] or more causes the glass container to absorb 254 [nm] ultraviolet radiation. However, since there is a risk of the glass devitrifying if more than [mol %] of zinc oxide is doped, zinc oxide is preferably doped at a composition rate of 2.0 [mol %] to 20 [mol %].
Also, in the case of iron oxide (Fe2O3), doping at a composition rate of 0.01 [mol %] or more causes the glass container to absorb 254 [nm] ultraviolet radiation. However, since the glass becomes colored if more than 2.0 [mol %] of iron oxide is doped, iron oxide is preferably doped at a composition rate of 0.01 [mol %] to 2.0 [mol %].
It is preferable for the infrared transmissivity coefficient indicating the amount of water contained in the glass to be adjusted so as to fall in the range of 0.3 to 1.2, or particularly 0.4 to 0.8. An infrared transmissivity coefficient of 1.2 or less makes it easier to obtain a low dielectric tangent that is applicable to high voltage lamps in external electrode fluorescent lamps (EEFLs) and long cold cathode fluorescent lamps. An infrared transmissivity coefficient of 0.8 or less further reduces the dielectric tangent, which is further advantageous in high voltage lamps.
Note that the infrared transmissivity coefficient (X) can be expressed in the following expression.
X=(log(a/b))/t
(7) The phosphors constituting the phosphor film are not limited to the ones previously described. For example, the phosphor film may be constituted from phosphors that absorb 313 [nm] ultraviolet radiation, such as the red phosphor (YVO4:Eu3+), the green phosphor (BaMg2Al16O27:Eu2+, Mn2+), and the blue phosphor (BaMg2Al16O27:Eu2+). If 50 [wt %] or more of the total weight of phosphors is made of the above phosphors that absorb 313 [nm] ultraviolet radiation, the leakage of 313 [nm] ultraviolet radiation out of the lamp can be almost entirely prevented, and the use of such a lamp in a backlight unit (
Also, a phosphor absorbing 313 [nm] ultraviolet radiation is defined as a phosphor in which an intensity of an excitation wavelength spectrum of 313 nm is 80% or more when an intensity of an excitation wavelength spectrum around 254 [nm] is 100% (the excitation wavelength spectrum is a type of spectrum that plots an excitation wavelength and a light intensity when a phosphor is excited over a range of wavelengths). In other words, a phosphor absorbing 313 [nm] ultraviolet radiation is a phosphor capable of absorbing 313 [nm] ultraviolet radiation and converting it to visible light.
The following are examples of phosphors that absorb 313 [nm] ultraviolet radiation
(i) Blue Phosphor
(ii) Green Phosphor
(iii) Red Phosphor
Note that a mixture of phosphors of different compounds may be used for one color. One example is to use only BAM for blue, LAP (does not absorb 313 [nm] ultraviolet radiation) and BAM:Mn2+ for green, and YOX (does not absorb 313 [nm] ultraviolet radiation) and YVO4:Eu3+ for red. In such a case, the leakage of ultraviolet radiation from the glass container can be reliably prevented by adjusting the phosphors such that 50% or more of the total weight proportion is made of the phosphors absorbing 313 [nm] ultraviolet radiation.
An external electrode lamp of the present invention can be favorably applied as a light source in a backlight unit etc. that is used in an environment having scarce external light.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2005-284304 | Sep 2005 | JP | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/JP2006/319064 | 9/26/2006 | WO | 00 | 2/20/2008 |
