This application claims the priority benefit of Taiwan application serial no. 101141027, filed on Nov. 5, 2012. The entirety of the above-mentioned patent application is hereby incorporated by reference herein and made a part of this specification.
The technical field generally relates to a lamp and a fabrication method thereof, and more particularly, to a dielectric barrier discharge lamp and a fabrication method thereof.
In a dielectric barrier discharge lamp, a discharge gas is excited based on the gas discharge theory to convert electric energy into light energy. Aforementioned discharge gas may be an inert gas, such as Xe, Ar, or Kr, or a halogen gas, such as F2 or Cl2. In a dielectric barrier discharge lamp, an AC voltage can be applied to different discharge gases through a plurality of electrodes, and the different excited discharge gases can generate light beams of different wavelengths. Accordingly, the dielectric barrier discharge lamp can be used for many different purposes. For example, a dielectric barrier discharge lamp filled with Xe can generate a light beam having a wavelength of 172 nm. Because this light beam can dissolve organic compounds on electronic parts, the dielectric barrier discharge lamp can be used for cleaning electronic parts. In other words, besides being used as illuminating light source, dielectric barrier discharge lamps are also broadly used in the industrial, agricultural, medical, and scientific fields.
In a dielectric barrier discharge lamp, because an AC voltage is applied to the discharge gas, so as to generate the illuminating light beam, by using electrodes, it is very important to provide a uniform light source through the design of the electrodes. Conventionally, the electrodes are usually disposed on inner and outer surfaces of a double-layered lamp tube, and an AC voltage is applied to the electrodes for stimulating the discharge gas between the electrodes to generate the illuminating light beam. However, this technique offers a high cost. In addition, as for a single-layered lamp tube, while placing an inner electrode in a lamp tube, if both ends of the electrode are fixed to the lamp tube, the metal electrode may be deformed or twisted when it is heated and expands. As a result, unsatisfactory illumination uniformity may occur or the dielectric barrier discharge lamp may be damaged. Thereby, there is still a lot of space for improvement in the present design of dielectric barrier discharge lamp.
Accordingly, the disclosure is directed to a dielectric barrier discharge lamp. The dielectric barrier discharge lamp has a simple structure and is easy to assemble, and a lamp tube is prevented from being damaged by thermal expansion of electrodes in the dielectric barrier discharge lamp. Thereby, a uniform illuminating light beam can be generated and an optimal illumination effect can be achieved.
The disclosure is directed to a fabrication method of a dielectric barrier discharge lamp. The dielectric barrier discharge lamp offers a stable illumination quality, in which electrodes are precisely positioned in a lamp tube, and the lamp tube is prevented from being damaged by thermal expansion of the electrodes.
The disclosure is directed to another fabrication method of a dielectric barrier discharge lamp, in which the fabrication of the dielectric barrier discharge lamp is simplified through an assembly technique, and a lamp tube is prevented from being damaged by thermal expansion of electrodes in the dielectric barrier discharge lamp.
An embodiment of the disclosure provides a dielectric barrier discharge lamp. The dielectric barrier discharge lamp includes a lamp tube, a discharge gas, a support member, a first electrode, and a second electrode. The lamp tube has a first sealed end and a second sealed end. The discharge gas is filled in the lamp tube. The support member is disposed at the first sealed end of the lamp tube and extended from the first sealed end toward the inside of the lamp tube. Besides, the support member has an accommodating space, and an opening of the accommodating space faces the inside of the lamp tube. The first electrode is disposed from inside to outside of the lamp tube. A first terminal of the first electrode passes through the opening of the accommodating space so that a part of the first electrode is in the accommodating space. A gap exists between the end of the first terminal of the first electrode and the closed end of the accommodating space. A second terminal of the first electrode penetrates through the second sealed end of the lamp tube and is closely fitted with the second sealed end. The second electrode is disposed outside the lamp tube.
An embodiment of the disclosure provides a fabrication method of a dielectric barrier discharge lamp. The fabrication method includes following steps. A lamp tube, a first electrode, a first side tube, and a second side tube are provided. A first sealed end and a second sealed end are formed at both ends of the lamp tube. The first side tube is inserted into the first sealed end of the lamp tube and advanced toward the inside of the lamp tube for a predetermined distance, and an outer surface of the first side tube is connected to the first sealed end to form a tube-shaped support member inside the lamp tube. An opening of the second side tube is fixed to the second sealed end of the lamp tube, and the second side tube and the lamp tube are internally connected with each other. The first electrode is placed and fixed at the second sealed end through the inside of the second side tube, so that a part of the first electrode is outside the lamp tube while another part of the first electrode is inside the support member. A gap exists between the end of the first terminal of the first electrode and a closed end of an accommodating space of the support member located at the first sealed end. The second side tube is sealed so that the second side tube and the first electrode are closely fitted with each other. The inside of the lamp tube is vacuum degassed and then filled with a discharge gas through the first side tube. The first side tube is sealed to form a protruding portion at the first sealed end.
An embodiment of the disclosure provides a fabrication method of a dielectric barrier discharge lamp. The fabrication method includes following steps. A lamp tube, a first electrode, a first side cover, and a second side cover are provided. The lamp tube has a side discharging vent. Herein the first side cover has a support member with an accommodating space, and the first electrode is closely fixed to and penetrates the second side cover. A first sealed end is formed at one end of the lamp tube, and the first side cover is fixed at the first sealed end. The support member of the first side cover is extended from the first sealed end toward the inside of the lamp tube, where an opening of the accommodating space faces the inside of the lamp tube. A second sealed end is formed at the end of the lamp tube opposite to the first sealed end, and the second side cover is fixed to the second sealed end, and the first electrode penetrates the second sealed end. A first terminal of the first electrode passes through the opening of the accommodating space, so that a part of the first electrode is in the support member, and a gap exists between an end of the first terminal of the first electrode and a closed end of the support member. A second terminal of the first electrode is toward outside of the lamp tube. The inside of the lamp tube is vacuum degassed and then filled with a discharge gas through the side discharge of the lamp tube. The side discharging vent is sealed to form a protruding portion.
As described above, embodiments of the disclosure provide a dielectric barrier discharge lamp and a fabrication method thereof. In the dielectric barrier discharge lamp, a part of a first electrode in a lamp tube is in an accommodating space of a support member, and a gap is kept between an end of the first electrode and a closed end of the accommodating space. Besides the purpose of supporting the first electrode, a space is reserved for the support member so that the lamp tube is prevented from being twisted or compressed when the first electrode is heated and expands. Thus, the dielectric barrier discharge lamp offers optimal illumination uniformity even when first electrode is heated and expands.
Several exemplary embodiments accompanied with figures are described in detail below to further describe the disclosure in details.
The accompanying drawings are included to provide further understanding, and are incorporated in and constitute a part of this specification. The drawings illustrate exemplary embodiments and, together with the description, serve to explain the principles of the disclosure.
As described above, in the present embodiment, the first electrode 140 is disposed from inside to outside of the lamp tube 110, and the first terminal 140a of the first electrode 140 is placed into the accommodating space 132 of the support member 130 so that a part of the first electrode 140 is in the accommodating space 132 and is loosely fitted with the support member 130. To be specific, the cross-sectional area of the accommodating space 132 is slightly greater than that of the first electrode 140, so that the first electrode 140 can still move around in the accommodating space 132 of the support member 130. In addition, the second terminal 140b of the first electrode 140 directly passes through the second sealed end S2 and is closely fitted and fixed to the second sealed end S2, so that the first electrode 140 is disposed in the dielectric barrier discharge lamp 100.
Besides being used for the supporting and positioning effects, the support member 130 in the dielectric barrier discharge lamp 100 is further used for dealing with the thermal expansion of the first electrode 140. To be specific, a dielectric barrier discharge lamp in operation usually constantly generates heat due to the gas discharge effect. Accordingly, the temperature of the first electrode (also referred to as an inner electrode) in the lamp tube continuously increases. Because the thermal expansion coefficient of the first electrode (for example, metal) is usually much higher than that of the lamp tube (for example, quartz glass), when the lamp is in operation, the first electrode is heated and accordingly about to expand. In this case, however, if both ends of the first electrode are respectively coupled to the two sealed ends of the lamp tube, since this expanding is restricted by the two sealed ends of the lamp tube, it will result in bending of the first electrode and also produce an internal stress on the lamp tube and even may cause the lamp tube to break. Thus, the lifespan of the lamp tube is shortened. Additionally, if there is no space for the first electrode to expand when it is heated, the first electrode may be pressed by the two sealed ends and sag. As a result, uneven discharge may be produced in the lamp tube, and accordingly the illumination of the lamp tube may be non-uniform. For example, a lamp tube is usually made of quartz or glass, and the thermal expansion coefficient thereof is about 5˜80×10−7/° C. The first electrode is usually made of a metal, and the thermal expansion coefficient thereof is about 45˜200×10−7/° C. Thus, the expansion rate of the heated first electrode is greater than that of the heated lamp tube. As a result, the first electrode is deformed in the lamp tube, which affects the illumination of the lamp tube.
In the present embodiment, besides being loosely fitted with the support member 130, a gap 134 exists between the first terminal 140a of the first electrode 140 in the support member 130 and the closed end of the accommodating space 132 in the support member 130. The gap 134 is configured to accommodate the expansion of the first electrode 140 when the first electrode 140 is heated, such that deformation of the first electrode 140 in the lamp tube 110 is prevented. It should be noted that in the present embodiment, the length x of the gap 134 can be determined according to different standards and when the dielectric barrier discharge lamp 100 is not in use (i.e., no thermal expansion of the first electrode 140 is produced).
The major consideration in determining the length x of the gap 134 is the length variation of the first electrode 140 when it is heated and expands. In other words, within a predetermined temperature range (i.e., the possible temperature increment when the dielectric barrier discharge lamp 100 is in operation), the length x of the gap 134 when the dielectric barrier discharge lamp 100 is not in operation should be greater than the length variation of the first electrode 140 caused by thermal expansion. This will be explained below with an example.
Herein it is assumed that the first electrode 140 is made of tungsten and the lamp tube 110 and the support member 130 are made of quartz glass. The thermal expansion coefficient of tungsten is 4.5×10−6/° C., and the thermal expansion coefficient of quartz glass is 0.5×10−6/° C. Besides, the length of the first electrode 140 is 150 mm, and the temperature variation from that the dielectric barrier discharge lamp 100 is not in operation to that the dielectric barrier discharge lamp 100 is in operation is assumed to be 1000° C. Thus, when the dielectric barrier discharge lamp 100 is in operation, the expansion of the first electrode 140 in relation to the lamp tube 110 and the support member 130 can be calculated as:
ΔL=(4.5×10−6−0.5×10−6)×150 mm×1000° C. (1)
The expansion quantity ΔL is about 0.6 mm. Thus, when the dielectric barrier discharge lamp 100 is fabricated, the length x of the gap 134 can be set to at least 1 mm (for example, 1 mm). Accordingly, when the lamp tube 110 is in use, the thermal expansion (for example, 0.6 mm) of the first electrode 140 can be accommodated by the gap 134. However, the determination of the length x of the gap 134 is not limited to that described above, and those applying the present embodiment may also determine the length x of the gap 134 in different manners (for example, the length x of the gap 134 is determined to be greater than a half of the external diameter of the lamp tube 110). It should be noted that the length x of the gap 134 should be determined based on the thermal expansion quantity of the first electrode 140.
In the embodiment illustrated in
The second terminal 140b of the first electrode 140 penetrates the second sealed end S2 to outside of the lamp tube 110, and the first electrode 140 itself is closely fitted and fixed to the second sealed end S2. Several techniques can be designed to closely fit and fix the first electrode 140 to the second sealed end S2, and one of the techniques is illustrated in
Another technique for maintaining the closely fitted state between the first electrode 140 and the second sealed end S2 is illustrated in
In either the embodiments illustrated in
The first electrode 140 may be made of one or an alloy of Cu, Ni, Cr, Mo, Ag, Pt, Fe, Ti, W, and Co, and the second electrode 150 may be made of one or an alloy of Cu, Ni, Cr, Au, Mo, Ag, Pt, Fe, Ti, W, and Co. In addition, the discharge gas 120 may be gaseous Hg, He gas, Ne gas, Ar gas, Kr gas, Xe gas, Rn gas, N gas, hydrogen selenide gas, deuterium, F2 gas, Cl2 gas, Br gas, iodine gas, or a mixture of at least two of aforementioned gases.
If the protruding portion 212 of the lamp tube 210 is disposed on the axis of the lamp tube 210 and at the first sealed end S1 and protrudes toward the outside of the lamp tube 210, the metal cap 270a covering the first sealed end S1 also covers the protruding portion 212. In order to prevent the metal cap 270a from getting too close to the first terminal 240a of the first electrode 240 (which may cause gas discharge and accordingly damage the metal cap 270a), while determining the length x of the gap 234 (the area in
Additionally, an electric insulator 274 can be respectively filled between the metal caps 270a and 270b and the first sealed end S1 and the second sealed end S2 of the lamp tube 210. At the second sealed end S2, to prevent the second terminal 240b of the first electrode 240 from directly contacting the metal cap 270b (which may cause a short circuit between the first electrode 240 and the second electrode 250) when it protrudes out of the lamp tube 210 through the transition glass layer 214, the electric insulator 274 is filled between the lamp tube 210 and the metal cap 270b. Meanwhile, an electric insulation layer 272 covers the first electrode 240 at where the first electrode 240 is connected with the metal cap 270b, so that the metal cap 270b will not directly contacts the first electrode 240 due to the insulation of the electric insulation layer 272. The electric insulator 274 and the electric insulation layer 272 may be made of a ceramic insulating cement or a plastic material. Other aspects of the dielectric barrier discharge lamp 200 can be referred to descriptions related to the dielectric barrier discharge lamp 100 therefore will not be described herein.
Based on the embodiment described above, the main feature of the dielectric barrier discharge lamp 200 is that the first sealed end S1 is covered with the metal cap 270a. In addition, the second sealed end S2 may also be covered with the metal cap 270b. Thus, the dielectric barrier discharge lamp 200 can have the same design as that illustrated in
In
In
The disclosure provides several techniques for fixing the first electrode 440 to the second side cover C2. One of the techniques is to compress the first electrode 440 with the second side cover C2 to fix the first electrode 440, and another technique is to dispose a transition glass layer 414 on the second side cover C2 and/or on the first electrode 440. As described in the embodiment illustrated in
In
Additionally, in the dielectric barrier discharge lamp fabrication method, as shown in
As described above, in a dielectric barrier discharge lamp provided by an embodiment of the disclosure, a support member is disposed to position a first electrode, and a gap is maintained between the first electrode and the support member. When the first electrode is heated and expands, the gap can accommodate the expansion of the first electrode, so that the first electrode is prevented from being deformed or twisted. In addition, by disposing a side discharging vent, a side tube, or the support member, a discharge gas can be conveniently filled. Moreover, a dielectric barrier discharge lamp provided by the disclosure can be fabricated through simple fabrication and assembly processes. Thereby, the fabrication cost of the dielectric barrier discharge lamp is reduced.
It will be apparent to those skilled in the art that various modifications and variations can be made to the structure of the disclosed embodiments without departing from the scope or spirit of the disclosure. In view of the foregoing, it is intended that the disclosure cover modifications and variations of this disclosure provided they fall within the scope of the following claims and their equivalents.
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“Office Action of Taiwan Counterpart Application”, issued on Sep. 22, 2014, p. 1-p. 9. |
Number | Date | Country | |
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20140125217 A1 | May 2014 | US |