The present invention relates to a light source device comprising a bulb, a discharge medium mainly composed of a rare gas sealed inside the bulb, and an electrode for exciting the discharge medium. The present invention also relates to a lighting device, such as a back light device, comprising this light source device, and a liquid crystal device comprising this back light device.
Recently, research on a light source device that does not use mercury (hereafter referred to as mercury-less type) as a lamp or light source device used for a back light device of a liquid crystal display device is actively progressing, in addition to research on a light source device using mercury for such usage. The mercury-less type light source device is preferable due to low fluctuation of light emission intensity along with time variation of temperature and in view of consideration of environments.
A known mercury-less light source device has a tubular bulb in which a rare gas is sealed, an internal electrode disposed inside the bulb, and an external electrode disposed outside the bulb. Application of a voltage between the internal electrode and external electrode causes a dielectric barrier discharge, resulting in that the rare gas is converted into plasma to emit light.
Various types of external electrodes are known. For example, a conventional light source device shown in
An external electrode, in which a conductive element is mechanically pressed to an outer surface of a bulb, is also known. For example, one of conventional light source devices has an external electrode made of a conductive wire member and wound spirally around a bulb so as to closely contact an outer surface of the bulb (for example, see Japanese Patent Application Laid-Open Publication No. 10-112290). Further, another one of conventional light source devices has an external electrode made of a conductive wire member and wound in a coil manner around an outer surface of a bulb, and a shrink tube that secures the external electrode so as to be closely in contact with the outer surface of the bulb (for example, see Japanese Patent Application Laid-Open Publication No. 2001-325919).
Even if the external electrode 2 is formed by coating with metal paste, the external electrode 2 cannot be completely contacted with the outer surface of the bulb 3. In other words, as shown in
Even if mechanically pressed onto the outer surface of the bulb, this conductive element is detached from the outer surface of the bulb by deflection of the conductive element. Even if such a measure as a shrink tube is used, it is impossible to completely contact the conductive member with the outer surface of the bulb. Therefore, the above-mentioned gap exists between the external electrode and the outer surface of the bulb without exception, thereby causing unstable light emission and dielectric breakdown of the atmospheric gas.
As discussed above, even in a case of an external electrode formed by a chemical method employing metal paste, deposition, sputtering and adhesive, rather than such a physical method as mechanical pressing and use of a shrink tube, a gap between the external electrode and the outer surface of the bulb inevitably exists. The gap causes unstable emission and dielectric breakdown of the atmospheric gas.
It is an object of the present invention to solve the problems caused by the gap inevitably generated between the external electrode and the outer surface of the bulb, and provide a highly reliable light source device that has a stable light emission characteristic and can reliably prevent dielectric breakdown of atmospheric gas.
A first aspect of the present invention provides a light source device comprising at least one bulb, a discharge medium containing a rare gas and sealed inside the bulb, a first electrode disposed inside the bulb (internal electrode), a second electrode disposed outside the bulb (external electrode), and a holder for holding the second electrode so that the second electrode is opposed to the bulb via a predetermined distance of a space. Specifically, the light source device further comprises a lighting circuit to which the first electrode is electrically connected, and the second electrode is grounded.
The second electrode disposed outside the bulb is opposed to the bulb via the predetermined distance of the space by the holder. In other words, the space is intentionally created between the bulb and the second electrode. Presence of the space achieves stable light emission of the light source device and prevents dielectric breakdown of atmospheric gas, resulting in that a highly reliable light source device can be implemented. Gas molecules of the atmospheric gas ionized by the dielectric breakdown cause damage to peripheral members. For example, if the atmospheric gas is air, dielectric breakdown generates ozone that causes damage to the peripheral members. According to the present invention, by preventing dielectric breakdown of the atmospheric gas, such ionization of the gas molecules of the atmospheric gas can be prevented.
A void is created between the bulb and the second electrode by the holder, so that any shape of bulb can be used. The space between the bulb and the second electrode held by the holder allows any shape of the bulb. Further, since the second electrode does not closely contact the bulb, shape and structure of the second electrode can be simplified. These features achieve a light source device that is inexpensive and easy to manufacture.
To prevent dielectric breakdown of the atmospheric gas with reliability, it is preferable that a distance between the second electrode and the bulb is longer than a shortest distance defined by the following equation.
X1L: shortest distance
E0: dielectric breakdown field of atmospheric gas
V: input voltage
∈1: dielectric constant of space
∈2: dielectric constant of a wall of the bulb
X2: thickness of the wall of the bulb.
For example, if gas filled in the space is air (which has a dielectric constant of 1), then it is preferable that the distance between the second electrode and the bulb is set to a range between 0.1 mm and 2.0 mm.
A lower limit of the distance, i.e. 0.1 mm, is obtained based on the above equation. An upper limit of the distance, i.e. 2.0 mm, on the other hand, is determined according to a condition where the light source device can be lit by a reasonable input power. In other words, if the distance is excessively long, the input power for lighting the light source device should also be set excessively high, which is not practical.
An example of the rare gas to be contained in the discharge medium is xenon. Other gases, such as krypton, argon and helium, may be applied. The discharge medium may contain a plurality of types of these rare gases.
The discharge medium may contain mercury in addition to the rare gas.
If the bulb has an elongated shape which extends along an axis line thereof, it is preferable that a cross-section of the second electrode perpendicular to the axis line has a shape surrounding the bulb except for an open section.
It is also preferable that a reflection layer is formed on a surface of the second electrode so as to be opposed to the bulb.
Since the second electrode is disposed via space from the bulb, the electrode is not provided on an outer surface of the bulb. Therefore, the reflection layer formed on the second electrode significantly reduces a ratio of light reflected by the second electrode to return to inside the bulb with respect to light radiated from the bulb. As a result, a total luminous flux of the light radiated from the light source device, i.e. an efficiency of the light source device, can be improved.
Further, it is unnecessary to dispose a separate reflection member to direct light radiated from the bulb to a predetermined direction. In other words, the second electrode also functions as a reflection element. Therefore, structure of the light source device can be simplified.
The reflection layer may be a layer of material with high reflectance formed on a surface of the second electrode, or may be the surface of the second electrode itself with high reflectance.
If the cross-section of the bulb perpendicular to the axis line has a circular shape, it is preferable that a cross-section of the second electrode perpendicular to the axis line of the bulb has a shape except for a concentric circle with respect to the cross-section of the bulb.
For example, the cross-section of the second electrode perpendicular to the axis line of the bulb comprises a pair of first flat walls opposed to each other with the bulb therebetween, and a second flat wall which links the pair of first flat walls and is opposed to an open section with the bulb therebetween. The cross-section of the second electrode may have other shapes, such as an arc, pentagon and triangle.
Alternatively, the bulb has a shape extending along the axis line thereof, and the second electrode has a strip-like shape extending along the axis line of the bulb.
Alternatively, the bulb has a shape extending along the axis line thereof, and plural second electrodes are disposed at intervals along the axis line.
A double tube structure may be applied. In other words, the light source device may further comprise a vessel in which the bulb is enclosed, and the second electrode is formed on an inner face of the vessel. This arrangement allows for gas other than air, such as rare gas, to be filled in the space between the bulb and second electrode.
The light source device may comprise a plurality of bulbs.
In this arrangement, at least one unit of the first electrode is provided for each of the bulbs, and one unit of the second electrode is provided in common for the plurality of bulbs.
A second aspect of the present invention provides a light source device, comprising at least one bulb, a discharge medium containing rare gas and sealed inside the bulb, a first electrode disposed outside the bulb, a second electrode disposed outside the bulb, and a holder for holding the first and second electrodes so that the first and second electrodes are opposed to the bulb via a predetermined distance of space. Specifically, the light source device further comprises a lighting circuit to which the first electrode is electrically connected, with the second electrode being grounded.
A third aspect of the present invention provides a lighting device, comprising the above-mentioned light source device, and a light guide plate for guiding light emitted by the light source device from a light incident surface to a light emitting surface, and emitting the light from the light emitting surface.
A fourth aspect of the present invention provides a liquid crystal display device comprising the above mentioned lighting device, and a liquid crystal panel disposed so as to be opposed to the light emitting surface of the light guide plate.
According to the light source device of the present invention, since the second electrode disposed outside the bulb is opposed to the bulb via a predetermined distance of a space by a holder, light emission is stabilized, and dielectric breakdown of an atmospheric gas can be prevented. Further, the light source device is inexpensive, and can be easily manufactured.
Other objects and characteristics of the present invention shall be clarified by the following description of preferred embodiments with reference to the accompanying drawings.
Embodiments of the present invention will now be described in detail with reference to the accompanying drawings.
As described with reference to
According to the definition of a capacitor, capacitances C1 and C2 of capacitors 11 and 12 are respectively given by following equation (1).
In equation (1), “S” denotes an area of the external electrode 2 covering bulb 3, “∈1” denotes a dielectric constant of the gap 7, “∈2” denotes a dielectric constant of the solid dielectric layer 8, “X1” denotes a distance of the gap 7, and “X2” denotes a thickness of the solid dielectric layer 8.
Since the capacitors 11 and 12 are connected in series, a combined capacitance C0 is given by following equation (2).
By applying equation (1) to equation (2), following equation (3) is acquired.
If air is filled in the gap 7, “∈1” equals 1, and following expression (3)′ is established.
Generally, a relationship indicated by following equation (4) is established among an electric charge Q, a capacitance C and a voltage V.
Q=CV (4)
If the distance X1 of the gap 7 (layer of air) increases, the combined capacitance C0 decreases, as understood by equation (3)′. If the combined capacitance C0 decreases, the electric charge Q decreases, as understood by equation (4). Decreasing of the electric charge Q means a decrease of the electric charge of the dielectric layer, i.e. the solid dielectric layer 8 and the gap 7. This means that energy to contribute to light emission decreases; in other words, a luminous efficiency is reduced.
As discussed above, the increase of the distance X1 of the gap 7 results in reduction of luminous efficiency. Therefore, for those skilled in the art, the idea of increasing the distance X1 of the gap 7, that is intentionally creating the gap 7 between the external electrode 2 and the bulb 3, is entirely beyond their assumption. In other words, according to a general idea of those who skilled in the art, the external electrode 2 should closely contact the bulb 3 as much as possible so that generation of the gap 7 is prevented.
The bulb 23 has an elongated straight tubular shape extending along an axis line L thereof. As shown in
The bulb 23 is essentially made of material with transparency, such as borosilicate glass. The bulb 23 may be made of such glass as quartz glass, soda glass and lead glass, or organic matter such as acrylic. An outer diameter of the glass tube used for the bulb 23 is normally about 1.0 mm to 10 mm, but is not limited to this size. For example, the bulb 23 may be approximately 30 mm, which is common as a size of a fluorescent lamp for general-purpose illumination. A distance between an outer surface and an inner face of the glass tube, i.e. a thickness of the glass tube, is approximately 0.1 mm to 1.0 mm.
The bulb 23 is sealed, in which the discharge medium (not illustrated) is sealed. The discharge medium is one or more types of gas, mainly rare gas, but may contain mercury. The gas includes xenon, for example. Other rare gases, such as krypton, argon and helium, can be adopted. The discharge medium may contain a plurality of types of these rare gases. A pressure of the discharge medium sealed inside the bulb 23, i.e. an internal pressure of the bulb 23, is approximately 0.1 kPa to 76 kPa.
As shown in
The internal electrode 24 is disposed at one end inside the bulb 23. The internal electrode 24 is comprised of such metal as tungsten or nickel. A surface of the internal electrode 24 may be partially or entirely covered by such a metal oxide layer as cesium oxide, barium oxide or strontium oxide. By using such a metal oxide layer, a lighting start voltage can be decreased, and deterioration of the internal electrode by ion impact can be prevented. A surface of the internal electrode 24 may be covered by a dielectric layer (e.g. glass layer). A conductive member 29 has a distal end to which the internal electrode 24 is provided and a proximal end disposed outside the bulb 23. The conductive member 29 is electrically connected to the lighting circuit 31 via lead wires 30.
The external electrode 25 is comprised of conductive material such as metal including copper, aluminum and stainless steel. Further, the external electrode 25 is grounded. As described later in detail, the external electrode 25 may be a transparent conductor of which a main component is tin oxide and indium oxide. In the present embodiment, the external electrode 25 has an elongated shape extending along a direction of the axis line L of the bulb 23. As most clearly shown in
As shown in
In the light source device 21, a dielectric barrier discharge is generated between the internal electrode 24 and the external electrode 25 by applying an internal voltage using the lighting circuit 31, resulting in that the discharge medium is excited. This excited discharge medium emits ultraviolet light when moving back to a ground state. The ultraviolet light is transformed to visible light by the fluorescent layer 13, and then the visible light is emitted from the bulb 23.
Next, a supporting structure of the external electrode 25 relative to the bulb 23 will be described. As described above, the external electrode 25 is secured to the bulb 23 by two holder members 27. Each holder member 27 is made of a material with insulation and elasticity, such as silicon rubber. As shown in
As most clearly shown in
In the present embodiment, the distances X′1, X′2 and X′3 between the wall sections 32 to 34 of the external electrode 25 and the outer surface of the bulb 23 are respectively constant in the direction of the axis line L. Further, the distances X′1, X′2 and X′3 are the same as one another. However, the distance between the external electrode 25 and the bulb 23 need not be constant in the direction of the axis line L as long as the distance is within a range between a later mentioned shortest distance and longest distance. Further, the distance between the external electrode 25 and the bulb 23 in a circumferential direction of the bulb 23 as well need not be constant.
As described above, the gap between the external electrode and the bulb is inevitably generated even if it is tried to contact the external electrode with the bulb by a physical method or a chemical method. Further, the gap destabilizes light emission intensity and causes a dielectric breakdown of atmospheric gas. Contrary to this, the present invention completely departs from the conventional technical common knowledge owned by those skilled in the art, which is that the external electrode must contact the bulb as closely as possible. That is, according to the present invention, the space 26 is intentionally provided between the external electrode 25 and the outer surface of the bulb 23 in order to intentionally separate the external electrode 25 and the bulb 23 from each other. Therefore even if a spatial relationship between the external electrode 25 and the bulb 23 is slightly changed, this shift has only small influence on the distances, X′1, X′2 and X′3 of the space 26 between the external electrode 25 and the bulb 23. In other words, even if the spatial relationship between the external electrode 25 and the bulb 23 is slightly changed, the external electrode 25 can maintain a status of being separated from the bulb 23. This results in stable power supply to the bulb 23, which achieves remarkably stable emission intensity. Further, as described later, by appropriately setting the distances X′1 to X′3 of the space 26, prevented can be that an excessive voltage is applied to the space 26 and that a dielectric breakdown of the atmospheric gas (air in the present embodiment) filled in the space 26 occurs.
Then, quantitative settings of the distances X′1, X′2 and X′3 of the space 26 between the external electrode 25 and the bulb 23 will be described in detail. In the following description, the distances X′1, X′2 and X′3 between the outer surface of the bulb 32 and each of wall sections 32 to 34 of the external electrode 25 are collectively referred to as a “distance X1 of the space 26”.
Referring again to
Regarding the electric charge Q stored in the capacitors 41 and 42, following equation (5) is established.
Q=C0·V=C1·V1=C2·V2 (5)
In this equation, “C1” and “C2” denote capacitances of the capacitors 41 and 42, “C0” denotes combined capacitance of the capacitors 41 and 42, “V1” denotes a voltage applied to the space 26, “V2” denotes a voltage applied to the solid dielectric layer 40, and “V” denotes a voltage applied between the discharge space 22 and the external electrode 25.
The voltage V1 applied to the space 26, the voltage V2 applied to the solid dielectric layer 40, the voltage V applied between the discharge space 22 and the external electrode 25, electric field E of the space 26, and electric field E′ of the solid dielectric layer 40 have relationships defined by following equations (6) to (8).
V=V1+V2 (6)
From equations (5) to (7), following equation (9) is obtained.
By applying afore-mentioned equation (1) to equation (9), following equation (10) regarding the electric field E of the space 26 is obtained.
In the present embodiment, since air that has a dielectric constant of 1 is filled in the space 26, following equation (10)′ is established.
If a dielectric breakdown electric field of the space 26 is “E0”, following equation (11) needs to be established in order to prevent an occurrence of dielectric breakdown in the space 26.
E0>E (11)
By applying equation (10) to equation (11), following inequality (12) is obtained.
If the space 26 is filled with air (∈1=1), following inequality (12)′ is established.
Therefore, in order to prevent dielectric breakdown in the space 26, the distance X1 of the space 26 needs to be set to be longer than a shortest distance X1L defined by following equation (13).
Especially, when air is filled in the space 26, the shortest distance X1L is defined by following equation (13)′.
The distance X1 of the space 26 set to be longer than the shortest distance X1L prevents dielectric breakdown of the atmospheric gas filled in the space 26 and damage to peripheral members due to gas molecules ionized by the dielectric breakdown. In the present embodiment, since the atmospheric gas is air, prevented is ozone being generated by the dielectric breakdown which causes damage to the peripheral members.
A longest distance of the distance X1 of the space 26 can be determined according to a condition where the light source device can be lit by reasonable input power. In other words, if the distance is excessively long, the input power in order to activate the light source device should be set excessively high, which is impractical.
If the atmospheric gas filled in the space 26 is air (which has the dielectric constant of 1) as in the present embodiment, it is preferable that the distance X1 of the space 26 is set to be not less than 0.1 mm and not more than 2.0 mm. A lower limit (0.1 mm) of the distance X1 is determined by equations (13) and (13)′. For an upper limit of the distance X1, a maximum voltage between the internal electrode 24 and the external electrode 25 is approximately 5 kV, and the distance X1 of the space 26 should be set to approximately 2.0 mm at maximum in order that a voltage of approximately 5 kV generates discharge in the bulb 23.
Next, luminous efficiency will be described. As described with reference to equations (1) to (4), the distance X1 of the space 26 set to be long, that is disposing the external electrode 25 away from the bulb 23, causes a decrease in luminous efficiency. In the present embodiment, however, an area S of the external electrode 25 that covers the bulb 23 is set to be large so as to compensate for the decrease in the luminous efficiency due to existence of the space 26, and to achieve high luminous efficiency. Specifically, as understood by equations (3) and (3)′, increasing the area S of the external electrode 25 increases the combined capacitance C0, thereby the luminous efficiency improves as understood by equation (4).
It should be noted that the space 26 arranged between the external electrode 25 and the bulb 23 makes it possible to enhance the luminous efficiency by increasing the area S of the external electrode 25. In case the external electrode 2 contacts the bulb 3 as the light source device shown in
In order to increase the luminous efficiency it is preferable that an elevation angle θ (see
If a shape of the cross-section of the bulb 23 perpendicular to the axis line L has a circular shape, as in this embodiment, it is preferable for improvement of the luminous efficiency that a cross-section of the external electrode 25 perpendicular to the axis line L has a shape except for a concentric circle with respect to the cross-sectional shape of the bulb 23. A cross-sectional shape that is not a concentric circle reduces a ratio of light which is reflected back to the bulb 23 by the external electrode 25 with respect to total light emitted from the bulb 23, thereby improving luminous efficiency. In the present embodiment, by having a U-like shape as described with reference to
The external electrode 25 is separated from the bulb 23 not by a solid layer such as a solid dielectric layer, but by the space 26 in which gas (air in the present embodiment) is filled. A first reason for this arrangement is that if the external electrode is separated from the bulb by a solid layer such as a solid dielectric layer, micro-air portions such as air bubbles exist in a boundary between the solid layer and the external electrode. Similar micro-air portions also exist in a boundary between the solid layer and the bulb. These micro-air portions cause dielectric breakdown that generates ozone, thereby causing damage to peripheral members.
A second reason for the arrangement is that a low-profile or small light source device with lighter weight can be achieved. As is clear by above-mentioned equation (11), it is necessary to decrease the electric field E of the space 26 for prevention of dielectric breakdown. A spatial separation of the external electrode and the bulb by the solid layer corresponds to an increase in the thickness X2 of the solid dielectric layer in the denominator on the right-hand side of equation (10)′ indicating the electric field E of the space 26. A coefficient by which the thickness X2 is multiplied in the denominator on the right-hand side of equation (10)′ is 1 (∈1=1). On the other hand, a coefficient by which the distance X1 of the space 26 is multiplied in the denominator on the right-hand side of equation (10)′ is dielectric constant ∈2 of the solid dielectric layer, which is greater than 1. Therefore, in order to effectively decrease the electric field E of the space 26, it is more efficient to increase the distance X1 of the space 26 rather than to increase the thickness X2 of the solid dielectric layer. Therefore, separating the external electrode 25 from the bulb 23 by the space 26 can achieve a light source device with a low-profile or small and lighter weight more effectively than providing a solid layer such as a solid dielectric layer.
Although, in the present embodiment, the reflection layer 37 is formed on the external electrode 25, the reflection layer 37 is not an essential feature. However, if mirror-finishing for visible light has been applied to the external electrode 25, luminous efficiency may become 15% higher compared to a case in which diffused reflection finishing has been applied.
Owing to the space 26 provided between the bulb 23 and the external electrode 25 by the holder member 27, the light source device 21 of the present embodiment can adopt an arbitrary shape of the bulb 23. Owing to that the external electrode 25 does not contact the bulb 23, a shape and the structure of the external electrode 25 can be simplified. Owing to the reflection layer 37 formed on the external electrode 25, a function as a reflection element can be provided to the external electrode 25. In other words, since a dedicated reflection element other than the external electrode 25 is unnecessary, a number of composing elements can be decreased. Therefore, the light source device 21 is simple, inexpensive, and easy to manufacture.
(Experiment)
Concerning the light source device 21 of the first embodiment, an experiment for confirming an ozone generation suppression effect (first experiment) and an experiment for confirming luminous efficiency (second experiment) were conducted.
With reference to
Dimensions of bulb 23: outer diameter OD: 2.6 mm, inner diameter ID: 2.0 mm, length: 165 mm;
Material of bulb 23: borosilicate glass (dielectric constant is 5);
Discharge medium: mixed gas of 60% Xe and 40% Ar (160 Torr);
Material of internal electrode 24: tungsten;
Dimensions of internal electrode 24: diameter: 0.3 mm, length: 3 mm;
Material of external electrode 25: aluminum;
Dimensions of external electrode 25: thickness of wall sections 32 to 34: 0.3 mm, width W of wall sections 32 and 33: 14.0 mm, width W of wall section 34: 23.6 mm, length: 165 mm;
Distance between external electrode 25 and internal electrode 24: distances X′1 and X′2 are 0.5 mm (constant), distance X′3 (variable);
Dielectric breakdown field of air: about 10 kV/mm (measured value);
Drive waveform: rectangular wave created by inverter
Drive frequency: 28 kHz; and
Drive voltage: +2 kV, −2 kV (4 kV amplitude).
Experimental conditions of the second experiment example are the same as the experimental conditions of the first experiment example, except that the outer diameter OD of the bulb 23 is 3.0 mm, the inner diameter ID is 2.0 mm, the length of the bulb 23 and the external electrode 25 is 210 mm, and the distances X′1, X′2 and X′3 are 0.3 mm.
For both the first and second experiments, it was confirmed that ozone is hardly generated when the distance X′3 increases to approximately 0.1 mm (100 μm).
By substituting numeric values corresponding to the first and second experiment examples into equation (13)′, shortest distance X1L was calculated. As a result, shortest distance X1L of the first experiment example was 0.14 mm, and the shortest distance X1L of the second experiment example was 0.10 mm. These calculation results approximately match experiment results of the first and second experiment examples shown in
In the second experiment, a total luminous flux of the light source device was measured for the above-mentioned first experiment example (elevation angle θ is approximately 280 degrees) with changing input voltage. As a first comparison example, a light source device shown in
Compared with the measurement result of the first comparison example, total luminous flux in the second comparison example hardly increases, and rather tends to decrease. Therefore, it is confirmed that the external electrode formed so as to contact the outer face of the bulb 23 does not increase the luminous efficiency, even if the elevation angle θ is increased, that is even if the area of the external electrode is increased.
Compared with the measurement result of the first comparison example, the total luminous flux in the first experiment example remarkably increases. Particularly, when an input voltage is approximately 7 W, the total luminous flux of the first experiment example increases approximately 1.7 times the total luminous flux in the first comparison example. Therefore, it is confirmed that when the space 26 is provided between the external electrode 25 and the bulb 23, the luminous efficiency is increased by increasing the elevation angle θ, that is by increasing the area of the external electrode.
By the experiment result of the second experiment, it is confirmed that merely increasing the area of the external electrode does not increase the luminous efficiency, and that increasing the area of the external electrode with a precondition that the space 26 is provided between the external electrode 25 and the bulb 23 can achieve an increase of the luminous efficiency.
The arrangement where the space 26 is provided between the bulb 23 and the external electrode 25 is particularly effective when the internal electrode 24 is disposed at one end inside the external electrode 25 which is elongated along the axis line L of the bulb 23. A reason for this effectiveness will be described hereinbelow.
When the internal electrode 24 is at the end inside the bulb 23, high voltage needs to be supplied to the bulb 23 in order to allow light to emit from discharge medium between the internal electrode 24 and a part of the external electrode 25 positioned mostly away from the internal electrode 24. For example, in a case of the light source device of this embodiment, 2 kV of voltage needs to be supplied for this reason. By supplying such a high voltage, dielectric breakdown tends to occur between the bulb 23 and the external electrode 25 by the high voltage (maximum voltage) applied between the internal electrode 24 and a part of the external electrode 25 positioned most closely to the internal electrode 24. Contrary to this, when a distance between the internal electrode and the external electrode is approximately constant (e.g. in a case where both the internal electrode and the external electrode extend parallel to the axis line direction of the bulb), a necessary voltage for activating the light source device is approximately ⅙ of necessary voltage for activating the light source device of the present embodiment, i.e., approximately 300 V of a relatively low voltage. Therefore, for the arrangement where the internal electrode 24 is disposed at the end inside the bulb 23 and the external electrode 25 is elongated along the axis line L of the bulb 23, as the present embodiment, a voltage for activation needs to be equal to at least six-times the voltage for activating the arrangement where the distance between the internal electrode and the external electrode is constant. For such high supplied voltage, prevention of dielectric breakdown by the space 26 provided between the bulb 23 and the external electrode 25 works more effectively than the arrangement of the present embodiment.
In the modification of
A light source device 21 according to a second embodiment of the present invention shown in
Since other arrangements and functions of the second embodiment are the same as those of the first embodiment, same elements are denoted by the same reference symbols, and descriptions thereof are omitted.
In a third embodiment shown in
Since other arrangements and functions of the third embodiment are the same as those of the first embodiment, same elements are denoted by the same reference symbols, and descriptions thereof are omitted.
In a fourth embodiment shown in
The external electrode 25 is formed on the inner surface of the external vessel 48. As clearly shown in
Since other arrangements and functions of the fourth embodiment are the same as those of the first embodiment, same elements are denoted by same reference symbols, and descriptions thereof are omitted.
In the light source device 21 according to a modification of the fourth embodiment shown in
A light source device 21 according to a fifth embodiment of the present invention shown in
The light source device 21 may be provided with at least three bulbs 23. The bulbs 23 need not be in parallel with each other, and the bulbs 23 can be freely arranged as long as each of the bulbs 23 is opposed to common external electrode 25 with the space 26 therebetween.
If the external electrode 2 is formed so as to closely contact the outer surface of the bulb 3 as shown in
Since other arrangements and functions of the fifth embodiment are the same as those of the first embodiment, same elements are denoted by same reference symbols, and descriptions thereof are omitted.
A light source device 21 according to a sixth embodiment of the present invention shown in
Since other arrangements and functions of the sixth embodiment are the same as those of the first embodiment, same elements are denoted by same reference symbols, and descriptions thereof are omitted.
A light source device 21 according to a seventh embodiment of the present invention shown in
An arrangement where plural internal electrodes 24 are disposed inside the single bulb 23 as the present embodiment stabilize discharge occurring inside the bulb 23, even if the bulb 23 has a long elongated shape.
Since other arrangements and functions of the seventh embodiment are the same as those of the first embodiment, same elements are denoted by same reference symbols, and descriptions thereof are omitted.
An eighth embodiment of the present invention shown in
As shown in
As shown in
The external electrode 25 has a U-like cross-sectional shape perpendicular to axis line L of the bulb 23, which comprises a back wall section 64 at a back cover side, a front wall section 65 at a top cover side, and a side section 66 which links the back wall section 64 and the front wall section 65. An extended section 64a is formed at an edge of the back wall section 64, and a fold back section 65a is formed at an edge of the front wall section 65. As most clearly shown in
Structure and material of the holder member 27 are the same as those of the first embodiment (see
The external electrode 25 is electrically connected to one end of a lead wire 71 via the back cover 56, and another end of the lead wire 71 is grounded. A proximal end side of rod-like conductive member 29 having the internal electrode 24 at a proximal end is electrically connected to a lead wire 73 inside the connector 72. The connector 72 is attached to the external electrode 25 at an opposite end from the holder member 27, and is made of insulation material. The lead wire 73 is electrically connected to a lighting circuit not illustrated. At one edge of the back cover 56, a fixation member 74 made of insulation material is secured by screws 75. Between the fixation member 74 and the back cover 56, a terminal at a tip end of the lead wire 71 for the external electrode 25 is fixed The fixation member 74 also has a function to guide the lead wire 73 at an internal electrode side out of the case 57. The fixation member 74 also has a function to position edges of each light source device 21A and 21B with respect to the case 57 by engaging the connector 72.
By disposing the external electrode 25 away from the bulb 23 with the space 26, the external electrode 25 of the back light device 53 has two functions in addition to primary functions. First, the external electrode 25 functions as a reflection member for directing light radiated from the bulb 23 to the end faces 59a to 59c of the light guide plate 59. In other words, it is unnecessary to dispose a dedicated reflection member in addition to the external electrode 25, resulting in that a number of elements is decreased. Secondly, the external electrode 25 has a function to position the light source devices 21A and 21B with respect to the light guide plate 59 as mentioned above.
Since other arrangements and functions of the eighth embodiment are the same as those of the first embodiment, same elements are denoted by same reference symbols, and descriptions thereof are omitted.
A back light device 53 of a liquid crystal display device 51 according to a ninth embodiment shown in
Since other arrangements and functions of the ninth embodiment are the same as those of the first embodiment, same elements are denoted by same reference symbols, and descriptions thereof are omitted.
A liquid crystal display device 51 according to a tenth embodiment of the present invention shown in
Since other arrangements and functions of the tenth embodiment are the same as those of the first embodiment, same elements are denoted by same reference symbols, and descriptions thereof are omitted.
In the first to tenth embodiments, the electrode connected to the lighting circuit is the internal electrode 24, with the external electrode 25 being grounded. Whereas in an eleventh embodiment shown in
Specifically light source device 21 according to the present embodiment comprises an external electrode 125 opposed to an external surface of bulb 23 at around one end of the bulb 23 via space 26, and electrically connected to lighting circuit 31, and an external electrode 25 opposed to the outer surface of the bulb 23 at around the other end of the bulb 23 with the space 26 and being grounded. These external electrodes 25 and 125 are opposed to each other in an axis line L direction of the bulb 23 via a space. Further, these external electrodes 25 and 125 are held respectively to the bulb 23 by a holder member 27. Distance X1 between each of the external electrodes 25 and 125 and the outer surface of the bulb 23 is set to be longer than shortest distance X1L defined by equation (13), resulting in that dielectric breakdown between the external electrodes 25, 125 and the bulb 23 is prevented.
In case that the electrodes for connection both to the lighting circuit 31 and ground are the external electrodes 25 and 125 as with the present embodiment, an arrangement where both of the external electrodes 25 and 125 are disposed relative to the outer surface of the bulb 23 via a space is particularly effective. A reason for this effectiveness will be described hereinbelow.
Because a starting voltage for dielectric barrier discharge between the external electrodes 25 and 125 is higher than that of a case when one is an internal electrode and the other is an external electrode, dielectric breakdown easily occurs when the dielectric barrier discharge is started by the external electrodes 25 and 125. Therefore, prevention of dielectric breakdown by providing the space 26 between the bulb 23 and the external electrodes 25 and 125 is particularly effective for the arrangement of the present embodiment.
Since the other arrangements and functions of the eleventh embodiment are the same as those of the first embodiment, same elements are denoted by same reference symbols, and descriptions thereof are omitted.
The light source device of the present invention can be used not only for the back light device of the liquid crystal display device as with the tenth embodiment, but also for various light sources such as a light source for general-purpose illuminations, an excimer lamp as a UV light source, and a bactericidal lamp.
Although the present invention has been fully described in conjunction with preferred embodiments thereof with reference to the accompanying drawings, various changes and modifications are possible for those skilled in the art. Therefore, such changes and modifications should be construed as included in the present invention unless they depart from the intention and scope of the invention as defined by the appended claims.
Number | Date | Country | Kind |
---|---|---|---|
2003-306619 | Aug 2003 | JP | national |
This is a continuation application of International Application No. PCT/JP2004/012283, filed Aug. 26, 2004.
Number | Name | Date | Kind |
---|---|---|---|
6194821 | Nakamura | Feb 2001 | B1 |
6331064 | Nishiyama et al. | Dec 2001 | B1 |
6806647 | Yamamoto et al. | Oct 2004 | B2 |
20010050735 | Yajima et al. | Dec 2001 | A1 |
20020027774 | Nishiyama et al. | Mar 2002 | A1 |
20030052611 | Yamamoto et al. | Mar 2003 | A1 |
Number | Date | Country |
---|---|---|
5-29085 | Feb 1993 | JP |
5-190150 | Jul 1993 | JP |
8-96768 | Apr 1996 | JP |
10-64478 | Mar 1998 | JP |
10-112290 | Apr 1998 | JP |
11-329365 | Nov 1999 | JP |
2000-162593 | Jun 2000 | JP |
2001-126664 | May 2001 | JP |
2001-325919 | Nov 2001 | JP |
2002-82327 | Mar 2002 | JP |
2003-178717 | Jun 2003 | JP |
2003-257377 | Sep 2003 | JP |
Number | Date | Country | |
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20060139934 A1 | Jun 2006 | US |
Number | Date | Country | |
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Parent | PCT/JP04/12283 | Aug 2004 | US |
Child | 11362033 | US |