The invention is based on a UV radiator having an essentially tubular discharge vessel, which is designed to produce dielectric barrier discharges at one end and is sealed in a gas-tight manner at both ends.
Here, the term UV (ultraviolet) radiator is understood to mean radiators which, during operation, emit electromagnetic radiation having shorter wavelengths than in the visible range of the spectrum (approximately 380 to 770 nm), i.e. radiation having wavelengths below approximately 380 nm. In particular, it also includes radiation having shorter wavelengths than approximately 200 nm, which is also referred to as VUV (vacuum ultraviolet) radiation. UV radiators are thus unsuitable for illumination purposes, such as general-purpose illumination, for example. Instead, they are used in process engineering, in particular for surface purification and activation, photolysis, ozone generation, drinking water purification, metalization, and UV curing.
In particular, the invention also relates to high-power UV radiators, i.e. long radiators, for example having lengths of typically a few 10 cm to approximately 2 m, or even more.
Particularly efficient UV radiators have proved to be those based on dielectric barrier discharge, in particular when they are operated using the pulsed operating method described in U.S. Pat. No. 5,604,410.
The term “dielectric barrier discharge” requires by definition at least one so-called dielectrically impeded electrode. A dielectrically impeded electrode is separated from the interior of the discharge vessel or from the discharge medium by means of a dielectric, for example in which the electrode is arranged on the outside of the wall of the discharge vessel which is typically made of glass or another dielectric. This type of electrode is referred to below as the “outer electrode” for short.
The present invention relates to a UV radiator which has at least one outer electrode of the abovedescribed type. In addition, the UV radiator comprises a tubular discharge vessel which is sealed at both ends and surrounds a discharge medium. The discharge medium used is an ionizable filling which is usually made of a noble gas, for example xenon or a gas mixture with an added buffer gas such as neon or halogen additives, for example chlorine, fluorine etc. At least one electrode, referred to below as the “inner electrode” for short, is arranged within the discharge vessel. This inner electrode is unimpeded, i.e. is in direct contact with the discharge medium. The UV radiator is therefore one which is based on a discharge which is dielectrically impeded at one end.
During operation, a high voltage is applied between the inner and outer electrodes, and, as a result, a gas discharge is produced in the interior of the discharge vessel. Owing to the high radiation efficiency, use is preferably made of the pulsed operating method described in the abovementioned U.S. Pat. No. 5,604,410, in particular unipolar voltage pulses. For the purposes of shock protection, the outer electrode is preferably connected to zero potential with respect to ground (“grounded”). The inner electrode is supplied with negative voltage pulses, i.e. acts as a cathode during each voltage pulse. For further details in this regard, reference is again made to U.S. Pat. No. 5,604,410. During the gas discharge, so-called excimers are formed in the discharge medium. Excimers are excited molecules, for example Xe2*, XeCl*, which emit electromagnetic radiation when they return to the initial state, which is generally unbound or is in any case weakly bound. In the case of Xe2* or XeCl*, the maximum of the molecular band radiation is approximately 172 nm and 308 nm, respectively.
The specification WO 01/35442 shows a UV radiator having a tubular discharge vessel. Arranged centrally and axially within the discharge vessel is a coiled electrode. Provided on the outside of the discharge vessel are a number of strip-shaped electrodes extending parallel to the tube axis and distributed evenly over the circumference. As a result, the radiator essentially radiates evenly over the entire circumference, i.e. rotationally symmetrically, in a non-directional manner. In order for it to be possible for planar surfaces to be irradiated efficiently, it is necessary to use additional reflectors which deflect as much radiation as possible evenly onto the surface to be irradiated. In order also to be able to produce radiators having lengths of more than 20 cm, a holder, for example an axial supporting tube, is provided for the central inner electrode. However, in the case of very long radiators, in particular longer than approximately 1 m, production is increasingly difficult owing to the increasing risk of the supporting tube breaking. On the other hand, it is necessary to prevent the inner electrode from sagging, since this would have a negative effect on the uniformity of the production of radiation along the entire radiator.
The object of the present invention is to specify a UV radiator having a tubular discharge vessel and having radiation characteristics which are not rotationally symmetrical. Further aspects are the possibility of being able to produce high-power radiators, i.e. long radiators, and of achieving a high radiation efficiency.
This object is achieved by a UV radiator having an essentially tubular discharge vessel, which is designed to produce dielectric barrier discharges at one end and is sealed in a gas-tight manner at both ends, and having in each case at least one elongate inner and outer electrode which is oriented parallel to the longitudinal axis of the discharge vessel, whereby the at least one inner electrode is arranged on the inside of an imaginary first tube half of the tubular part of the discharge vessel, and the at least one outer electrode is arranged on the outside of an imaginary second tube half, which is opposite said first tube half, the two opposing tube halves being defined by an imaginary section, which contains the longitudinal axis of the tubular discharge vessel, through the discharge vessel.
Particularly advantageous refinements are described in the dependent claims.
In other words, it is possible to imagine the tubular part of the discharge vessel being split into two equal halves by an imaginary longitudinal section. The at least one inner electrode is arranged on the inside of the first imaginary tube half. The at least one outer electrode is arranged on the outside of the second imaginary tube half, and, specifically, at least in the case of one inner and one outer electrode, essentially diametrically. Even when it is not always expressly mentioned in the considerations below, it should always be remembered that the splitting of the discharge vessel into two tube halves is not real but is purely imaginary in nature and merely serves the purpose of facilitating a more precise description of the arrangement of the inner and outer electrodes.
The essentially diametrical arrangement of inner and outer electrode firstly has the advantage of high radiation efficiency owing to the large arcing distance, relative to the discharge vessel diameter, for the discharge, as is the teaching of U.S. Pat. No. 5,604,410 which has already been mentioned at the beginning. Secondly, it is now possible to move away from a radiation characteristic which is essentially rotationally symmetrical and move towards a more directional radiation characteristic.
For this purpose, in the simplest case, an either strip-shaped or flat outer electrode is arranged diametrically with respect to the inner electrode on the outside of the second tube half of the discharge vessel. In the latter case, the physical extent of the outer electrode, when viewed in the direction of the circumference of the tubular discharge vessel, extends over approximately the entire corresponding physical extent of the second imaginary tube half of the discharge vessel. In this case, the flat outer electrode may be realized by a coating, for example, or else by a suitably shaped metal part, in which the outside of the second tube half of the discharge vessel is embedded, as it were. The flat design of the outer electrode has the advantage that it can also act at the same time as a reflector for the UV radiation, as a result of which targeted radiation is improved further still. For this purpose, a material having sufficient reflection properties for UV radiation, for example aluminum, must be selected for the outer electrode.
As an alternative to the flat outer electrode, more than one, for example two, three or more strip-shaped outer electrodes may also be used. This makes it possible to come close to the radiation characteristics of a flat outer electrode without having the undesirably high capacitive load owing to the large electrode surface. In this case, although the electrodes are arranged unsymmetrically with respect to the entire circumference of the discharge vessel, they can preferably be arranged symmetrically with respect to a plane, which intersects the imaginary tube half and (when viewed in cross section) represents the vertical central line of the semicircle corresponding to the imaginary tube half. It has also been shown that the radiation efficiency is higher with, for example, two strip-shaped outer electrodes than with one flat outer electrode, for example in the form of an arrangement, in which one half is mirror-coated. In addition, it is also possible to achieve a correspondingly higher radiated power than with only one strip-shaped outer electrode.
For this last-mentioned reason, it may also be advantageous to use more than one inner electrode which are then likewise arranged symmetrically with respect to the plane, which intersects the imaginary tube half and (when viewed in cross section) represents the vertical central line of the semicircle corresponding to the imaginary tube half. If the tube half belonging to the inner electrodes is intended to be used as a radiating surface, i.e. in particular when the other tube half is largely or even completely covered by one or more outer electrodes, the inner electrodes are preferably positioned relatively close to the imaginary sectional plane, but only to an extent such that sufficient clearance remains between them and the next outer electrode. It is thus possible to achieve an electrode-free radiating surface which is as large as possible. However, it is also possible to use the other tube half belonging to the outer electrodes as the preferred radiating surface. To which side preference is given in each individual case depends in the end on the specific arrangement of all of the electrodes.
In contrast to the outer electrodes, no strip-shaped electrodes can be used for the inner electrodes, since said strip-shaped electrodes are typically made of conductive silver tracks or the like. Since, for efficiency reasons, the inner electrode is not covered by an additional dielectric layer and is thus not separated from the discharge medium (discharge which is dielectrically impeded at one end), few solvent residues and similar, volatile constituents of such an electrode track would be blown out during lamp operation and, as a result, enter the discharge medium and impair the production of radiation in an unacceptable manner. Instead, a metal wire or the like which is as pure as possible is used for the inner electrode.
In the case of long radiators, it is generally necessary to fix at least one inner electrode to the inside of the first tube half of the discharge vessel. For this purpose, a holder is preferably used which is fixed to the inside of the first tube half. The holder comprises, for example, depending on the length of the radiator, one or more narrow tube pieces, half-tube pieces or rings, through which the elongate inner electrode is threaded. As a result, the inner electrode is held sufficiently well on the mentioned inside of the discharge vessel even in the case of very long radiators, for example having a length of more than approximately 1 m, without sagging to a significant extent. The inner electrode is, for example, in the form of a rod which can be threaded through the “ear-like” holder particularly easily. As an alternative, the inner electrode is in the form of a coil. This can be slightly more complex to thread through the holder. However, it has the advantage that the numerous partial discharges produced in the pulsed operating method form at exactly defined preferred points between the coil and the usually strip-shaped outer electrodes, and are thus very uniformly distributed. For further details in this regard, reference is made to U.S. Pat. No. 6,060,828, in particular to the description associated with
The holder is made of a temperature-resistant, dielectric material, preferably glass, quartz glass or ceramic. The holder is preferably made of the same material as the discharge vessel wall. It is then possible for the holder to be fixed to the inside by simply fusing it with the discharge vessel. Alternatively, the holder may also be fixed using glass solder, but this may be problematic with regard to impurities in the discharge medium owing to the solvent of the glass solder paste which is to be removed before the discharge vessel is sealed.
The invention will be explained in more detail below with reference to exemplary embodiments. In the figures:
a shows a side view of a UV radiator according to the invention having a rod-shaped inner and two strip-shaped outer electrodes,
b shows a cross section of the UV radiator from
c shows an enlarged detail of the region C of the cross section shown in
Reference is made below to the side view of a UV radiator 1, the cross-sectional illustration along line AB and the enlarged detail of the region C, illustrated schematically in
Of course, the invention also makes it possible to build longer radiators than those illustrated in
In one variant (not shown), the inner electrode does not comprise a rod-shaped wire but rather a wire coil. For this purpose, the holding parts, for example short tube pieces or rings, are first connected to the vessel wall, and then the wire coil is threaded through the holding parts.
FIGS. 2 to 5 show variants of the UV radiator according to the invention, which differ only in their respective electrode configuration. In this case, identical features are provided with identical reference numerals.
Number | Date | Country | Kind |
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103 36 088.3 | Aug 2003 | DE | national |