JP2005285789A - High-pressure discharge lamp - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a high-pressure discharge lamp having an extremely uniform temperature distribution and applicable any attitude of the discharge lamp. <P>SOLUTION: An outline of an inner wall of a ceramic made discharge lamp has an almost straight single tubular center part of a length of L (cm) and an inside radius of R (cm) and two terminated ends shaped in an almost hemisphere with the same radius R as that of the center part. The length L of the center part is smaller than or equal to the inside radius R (L≤R), an inside length (2R+L) of the discharge tube is at least 10% larger than an electrode interval EA (cm) [(2R+L)≥1.1 EA], and the diameter 2R of the discharge tube is equivalent to at least 80% of the electrode interval EA and is the length of 150% of the electrode interval EA at a maximum (1.5 EA≥2R≥0.8EA). A tube wall load of the discharge tube P/(4πR<SP>2</SP>+2πRL)(W/cm<SP>2</SP>) is selected to be 25≤P/(4πR<SP>2</SP>+2πRL)≤45 in association with the rated power P (W) of the discharge tube. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

  In the present invention, the contour of the inner wall of the ceramic discharge tube defines an inner chamber containing the luminescent enclosure, and the inner chamber has one long axis and two ends with openings, and the openings are electrically conductive. The present invention relates to a high pressure discharge lamp in which the bushings are fitted in an airtight manner, the bushings are electrically connected to electrodes, and both the electrodes are disposed facing each other with an electrode interval in the inner chamber.

  This ceramic discharge tube is a ceramic discharge tube especially for metal halide lamps or high-pressure sodium lamps. This discharge tube is generally made of aluminum oxide which can contain a dopant. However, other known materials such as sapphire and aluminum nitride can also be used.

  An elongated cylindrical discharge tube for a high-pressure sodium discharge lamp or a discharge tube having an expanded center is known, and the inner diameter of the inner chamber of the discharge tube is made larger than the inner diameters at both ends (see, for example, Patent Document 1). In particular, it is recommended that the inner diameter at the height of the electrode tip is at least 60% of the inner diameter at the center.

  There is known a discharge tube formed of a straight cylindrical tube having both ends reduced in diameter (for example, see Patent Document 2). The cylindrical tube has an elliptical cross section. Alternatively, a very elongated elliptical discharge tube is described in which the length ratio of the short axis to the long axis is 1: 4 to 1: 8.

  In this type of elongated discharge tube, when the enclosure contains a metal halide, the lamp posture cannot be universally used. That is, in the vertical lamp posture, the cold spot (cold spot location) temperature existing in the range of the lower electrode is considerably lower than that in the case of the lamp in the horizontal posture. As a result, a noticeable color shift occurs between the horizontal lamp posture and the vertical lamp posture. Furthermore, in the case of such an elongated discharge tube geometry, the temperature distribution is very non-uniform and a large temperature gradient is produced. At the pre-selected cold spot temperature required to obtain the desired optical value, a very high hot spot temperature occurs in the case of elongated geometries, which overloads the discharge tube ceramics.

  A cylindrical discharge tube is known in which the end surfaces are applied at right angles and electrodes are deeply inserted into these end surfaces (see, for example, Patent Document 3). Although this type of cylindrical discharge tube can have a universal lamp orientation, its temperature distribution is similarly non-uniform, which again results in a very high hot spot temperature.

  High temperature gradients such as occur in elongated elliptical discharge tubes as well as cylindrical discharge tubes promote the occurrence of corrosion in the ceramics during the life of the lamp.

  Furthermore, methods that use ceramics in these geometries to increase the cold spot temperature and thus improve the optical data relative to quartz glass are limited due to the very high hot spot temperatures that occur there. When a life of 6000 to 10,000 hours is desired, the hot spot temperature of the ceramic is limited to a maximum of about 1250 ° C.

In the case of this type of elongated cylindrical discharge tube or elliptical discharge tube, it has been found that the optical and electrical lamp data greatly depends on the lamp posture due to its non-uniform temperature distribution. Therefore, this type of discharge tube can be used only when the independence between the lamp data and the lamp attitude is not required. This is only possible with a double-ended lamp, and in such a lamp, generally only a horizontal lamp position is allowed.
West German Patent Application No. 3137676 European Patent Application No. 34056 European Patent Application No. 587238

  The object of the present invention is to make a high-pressure discharge lamp as described in the opening part of the specification which has a very uniform temperature distribution and is therefore applicable to any lamp position. In particular, it is intended to be able to be applied to a single-piece lamp.

According to the present invention, this object is achieved by the fact that the inner wall of the discharge tube has the following geometric shape: one cylindrical central part whose profile is substantially straight with a length L (cm) and an inner radius R (cm). In addition, it has two substantially hemispherical end portions having the same radius R (cm), and the length L (cm) of the cylindrical central portion is smaller than or equal to the inner radius R (cm) {L (cm) ≦ R (cm)}, the inner length of the discharge tube (2R + L) (cm) is at least 10% larger than the electrode interval EA (cm) {(2R + L) (cm) ≧ 1.1 EA (cm)}, the diameter of the discharge tube 2R (Cm) corresponds to at least 80% of the electrode interval EA (cm) and the length of the electrode interval EA (cm) is at most 150% {1.5 EA (cm) ≧ 2R (cm) ≧ 0.8 EA (cm) }, And the tube wall load P / (4πR ² + 2πRL) of the discharge tube (W / c m ² ) so that 25 (W / cm ² ) ≦ P / (4πR ² + 2πRL) (W / cm ² ) ≦ 45 (W / cm ² ) in relation to the rated power P (W) of the discharge tube. It is solved by being selected.

  The present invention provides a special “bulging” geometry of the discharge tube that produces photometric lamp data that is approximately equivalent to a known discharge tube having an elongated cylindrical or elliptical geometry in any lamp position. It is characterized by its shape. This geometry particularly lowers the hot spot temperature and makes the temperature distribution very uniform.

  In particular, the present invention is directed to a ceramic discharge tube for a high-pressure discharge lamp containing a luminescent enclosure. The contour of the inner wall of the discharge tube defines the internal volume. The discharge tube has a long axis as well as both ends with openings, and conductive bushings are hermetically fitted at the ends, and these bushings are electrically connected to electrodes, respectively. They are arranged to face each other with a predetermined electrode interval.

  The contour of the inner wall has the following geometric shape. That is, the inner contour of the discharge tube can be considered to be composed of three parts, ie, a single straight cylindrical central part having a length L (cm) and an inner radius R (cm) and on both sides thereof. It is composed of two substantially hemispherical end portions having the same radius R (cm) as that.

  It has been found that the independence of the lamp attitude can be reliably obtained by simultaneously complying with a plurality of geometric peripheral conditions.

  The basic condition is that the length L (cm) of the cylindrical central portion is smaller than or equal to the inner radius R (cm), that is, L (cm) ≦ R (cm).

  In other words, the inner diameter of the discharge tube must be at least 2/3 of the total length of the discharge tube. Particularly preferably, L (cm) ≦ 0.8 R (cm).

  The length L (cm) and the inner diameter R (cm) must be selected so that predetermined peripheral conditions for the electrode spacing EA (cm) are observed. These conditions define an upper limit and a lower limit for the fitting length of the electrode in the inner chamber.

  Otherwise, the electrode will be too close to the termination range and will overheat the bushing site, so the total internal length of the discharge tube must be at least 10% longer than the electrode spacing EA (cm), ie (2R + L ) (Cm) ≧ 1.1 EA (cm).

  The discharge tube diameter 2R (cm) must have a length of at least 80% of the electrode spacing EA (cm). Otherwise, the discharge tube will be unnecessarily significantly heated by the curvature of the arc at its center. At the same time, this diameter must be at most 150% of the electrode spacing EA (cm), otherwise the central part will be too cold, ie 1.5 EA (cm) ≧ 2R (cm) It is necessary to make ≧ 0.8 EA (cm).

  Overall, from these dimensions for the discharge tube, the ratio of total length to maximum inner diameter is at most 1.5, in particular 1.3 or less.

With this geometry, the wall load (rated power on the inner surface) of the discharge tube is adjusted to 25-45 W / cm ² , preferably 25-35 W / cm ^2, and in the case of low power lamps It is adjusted to 35 W / cm ² or less (up to 45 W / cm ² in the value of 20 W rated power), and to 25 W / cm ² or less in the case of a high power lamp. This is especially true in the range of about 20W to about 250W lamp power. As a result, the tube wall load is reduced by about 10% from the conventional lamp in the prior art.

In a particularly advantageous embodiment, the discharge tube wall load P / (4πR ² + 2πRL) (W / cm ² ) for a lamp with a rated power of 35 to 250 W is given by the rated power P (W) and the inner diameter R ( cm) and length L (cm) are selected such that 25 (W / cm ² ) ≦ P / (4πR ² + 2πRL) (W / cm ² ) ≦ 35 (W / cm ² ).

  The inner volume of the discharge tube is about 100 to 150 μl (microliter) for a 35 W lamp, and increases by about 7 to 10 μl per 1 W of additional rated power. This is correspondingly reduced for low power. The 20W lamp has an interior volume of about 35 μl.

In a particularly advantageous embodiment, the inner volume V (μl) of the discharge tube is 0.16 × P ^5/3 (μl) ≦ V (μl) ≦ 0.32 × P ^{5 / with} respect to the rated power P (W). ³ (μl), particularly 0.22 × P ^5/3 (μl) ≦ V (μl) ≦ 0.32 × P ^5/3 (μl).

  In order to obtain as uniform a temperature distribution as possible, it has been found that L (cm) ≦ 0.6 R (cm) is advantageous. This is especially important for low power lamps where the heat loss at both ends is relatively high. In this case, the inner contour is drawn very close to a spheroid with a semi-minor axis a (cm) and a semi-minor axis b (cm), and R (cm) ≦ a (cm) ≦ 1.1 R (cm) and b = R + L / 2.

  Advantageously, the wall thickness of the discharge tube is 5-15% of the inner radius R (cm) at least in the central part of the discharge tube. Particularly suitable is a discharge tube in which the wall thickness of the discharge tube increases toward both ends of the discharge tube, and the wall thickness at both ends is twice the wall thickness at the central portion.

  Typically, the discharge tube is made of aluminum oxide, optionally doped with magnesium oxide and other oxides, or made of other materials such as aluminum nitride or sapphire.

  The present invention relates to a high-pressure discharge lamp having a ceramic discharge tube as described above.

  Advantageously, separate ceramic plugs (possibly made as cermets in some cases) are provided at both ends of the discharge tube to accommodate the bushings. However, the tip can also be an integral part of the discharge tube.

  The bushing can be selected from molded articles known per se (niobium or molybdenum tubes or pins or conductive cermets), in particular made as capillaries to which a suitable electrode system is brazed.

  Here, the inner contour of the discharge tube has been mainly described. The outer contour which is not very important for the present invention is predetermined approximately by the wall thickness.

  The outer contour is predefined in the simplest case by a uniform wall thickness. The wall thickness is 5-15% of the inner diameter of the discharge tube. However, it is advantageous for the wall thickness to increase slightly from the center towards the ends. This primarily acts as a heat dam, which partially compensates for heat losses due to the electrode system and bushing sites. Accordingly, a more uniform temperature distribution is achieved. In this case, the wall thickness increases from a typical value of 10% of the inner diameter at the center of the discharge tube to twice this value in the termination range. This further prevents the rapid corrosion of the ceramic that occurs earliest at the termination site during the lifetime.

  In the following, the invention will be described in detail with reference to a plurality of embodiments shown in the drawings.

  The ceramic discharge tube 1 shown in FIG. 1 is assumed to be a 70 W lamp. This consists of a straight cylindrical central part 2 having a length L = 2 mm (= 0.2 cm) and two hemispherical end parts 3 having a radius R = 4 mm (= 0.4 cm) on both sides thereof. Yes. The total length of the inner chamber is 10 mm (= 1 cm). The wall thickness of the discharge tube is constant 0.9 mm (= 0.09 cm). The maximum outer diameter is 9.8 mm (= 0.98 cm). A cylindrical projection 4 having a length of about 1.5 mm (= 0.15 cm) is extended outwardly from both end portions 3. Extruded and elongated ceramic plugs 5 are fitted in both the protruding portions 4 respectively. The plugs 5 are fitted somewhat deeply in the protruding portions 4 so that they are even closer to the ideal shape of the semicircular inner contour. In the simplest case, these plugs 5 have an inner end face 6 which is straight (see left half of FIG. 1). Advantageously, the inner end face 6 ′ of the plug 5 is inclined or is itself curved concavely so that it is even more closely matched to the semicircular inner contour (see right half of FIG. 1). In this way, ideal isothermal properties are generated.

As described in Patent Document 3, the electrodes 7 are fitted in the plugs 5, respectively, and the electrode interval EA (cm) is 7.5 mm (= 0.75 cm). Fill contained in the discharge chamber is higher wall loading of the lamp for example such as are usually employed for DyI _3, TmI _3, rare earth such as HoI ₃ - metal halide NaI containing iodide, TlI Contains a mixture of As a result, an initial color temperature of 3030 ± 80K in the vertical lamp attitude and an initial color temperature of 2980 ± 80K in the horizontal lamp attitude are obtained. The temperature difference between the cold spot and the hot spot in this lamp is only 20 ° compared to 70 ° in the case of a general cylindrical lamp whose end face is applied at a right angle.

The tube wall load of this discharge tube is about 28 W / cm ² . The inner chamber volume of the discharge tube is 370 μl (microliter).

  FIG. 2 shows a discharge tube 1 for a 35 W lamp. Here, the length of the cylindrical central portion 2 is 1.9 mm (= 0.19 cm), and the radius R of the hemispherical terminal portion 3 is 2.55 mm (= 0.255 cm). The total length of the inner chamber is 7.0 mm (= 0.7 cm).

  The wall thickness of the discharge tube 1 increases from a wall thickness of 0.8 mm (= 0.08 cm) at the center to a maximum wall thickness of 0.95 mm (= 0.095 cm) outward. The maximum outer diameter is 6.8 mm (= 0.68 cm). Again, an integral projection 4 and a separate plug 5 are provided.

  In other similarly constructed embodiments, the lamp power is chosen higher. In the case of a 100 W lamp, the length L = 2.5 mm (= 0.25 cm) and the radius R = 4.5 mm (= 0.45 cm). In the case of a 150 W lamp, the length L = 2 mm (= 0.2 cm) and the radius R = 6 mm (= 0.6 cm). In the case of a 250 W lamp, the length L = 6 mm (= 0.6 cm) and the radius R = 7.0 mm (= 0.7 cm).

  In order to still fully meet the requirements for satisfying the above-mentioned contours, it is only necessary to approximately maintain the above dimensional criteria with a deviation of up to 15%.

  Therefore, when the central portion 2 has the shortest limit length {L (cm) ≈0.5 R (cm)}, the inner contour is drawn by an ellipse having a semi-minor axis a (cm) and a semi-major axis b (cm). Can do. This is because the approximation does not differ by 15%.

  The elliptical semi-minor axis a is deviated from the ideal contour {with respect to the radius R (cm) and length L (cm) of the central portion} up to 15%, ie R ≦ a ≦ 1. Assuming that it is chosen to be 1R, and taking into account that the semi-major axis b (cm) is expressed as b = R + L / 2, both contours are shown in contrast in FIG. Has been. In that case, a ratio of the elliptical semi-minor axis a (cm) and the semi-major axis b (cm) of b / a ≦ 1.25 occurs.

  The dimensional criteria for the remaining electrode spacing and tube wall loading then remain unchanged.

  FIG. 4 shows an example of a 70 W lamp, whose inner contour 10 of the discharge tube 9 starts from a design of R = 4 mm (= 0.4 cm), with a semi-minor axis a = 4.4 mm (= 0.44 cm) and a sealed ellipse with a semi-major axis b = 5 mm (= 0.5 cm). Therefore, b / a = 1.14. The end portion 11 is integrally formed with a plug 12 together with a single ceramic molded product made of aluminum oxide. The wall thickness of the discharge tube continuously increases from the wall thickness of 0.8 mm (= 0.08 cm) at the central portion to twice the size from the end of the discharge tube.

  In all lamps of this type, it has been found that the discharge tube is not corroded at all after 9000 hours. On the other hand, the most common lamp in the prior art mentioned at the beginning has a failure rate of 50% as early as 8000 hours.

Sectional drawing of the ceramic discharge tube of a metal halide lamp. Sectional drawing of the Example from which the discharge tube made from ceramics differs. The principle figure of the system approximated elliptically when the length L is short. Sectional drawing of the Example of the discharge tube made from ceramics based on the approximation system of FIG.

Explanation of symbols

1 Ceramic discharge tube 2 Central part 3 Terminal part 4 Attached part 5 Plug

Claims (3)

The contour of the inner wall of the ceramic discharge tube defines an inner chamber containing the luminescent enclosure, which has one major axis and two ends with openings, and conductive bushings are hermetically sealed in these openings. In the high-pressure discharge lamp, the bushings are fitted and electrically connected to the electrodes, respectively, and both the electrodes are arranged facing each other with an electrode interval EA (cm) in the inner chamber.
The contour of the inner wall of the discharge tube has the following geometric shape: one cylindrical central part (2) whose profile is almost straight with a length L (cm) and an inner radius R (cm) and the same radius R (cm ) Having two substantially hemispherical end portions (3),
The length L (cm) of the cylindrical central portion (2) is smaller than or equal to the inner radius R (cm) {L (cm) ≦ R (cm)},
The inner length (2R + L) (cm) of the discharge tube is at least 10% larger than the electrode interval EA (cm) {(2R + L) (cm) ≧ 1.1 EA (cm)},
The diameter of the discharge tube 2R (cm) corresponds to at least 80% of the electrode interval EA (cm), and the length of the electrode interval EA (cm) is at most 150% {1.5EA (cm) ≧ 2R (cm) ≧ 0 .8 EA (cm)},
The tube wall load P / (4πR ² + 2πRL) (W / cm ² ) of the discharge tube is related to the rated power P (W) of the discharge tube, 25 (W / cm ² ) ≦ P / (4πR ² + 2πRL) (W / Cm ² ) ≦ 45 (W / cm ² ). The tube wall load P / (4πR ² + 2πRL) (W / cm ² ) of the discharge tube is 25 (W / cm ² ) ≦ P / (4πR ² + 2πRL) (W / cm ² ) ≦ 35 (W / cm ² ) 2. The high-pressure discharge lamp according to claim 1, wherein the high-pressure discharge lamp is selected in such a manner. The inner volume V (μl) of the discharge tube is in accordance with the formula of 0.16 × P ^5/3 (μl) ≦ V (μl) ≦ 0.32 × P ^5/3 (μl) with respect to the rated power P (W). 2. The high pressure discharge lamp according to claim 1, wherein the high pressure discharge lamp is selected.

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