EP3022763A1 - Gas discharge lamp and use thereof - Google Patents
Gas discharge lamp and use thereofInfo
- Publication number
- EP3022763A1 EP3022763A1 EP14734840.3A EP14734840A EP3022763A1 EP 3022763 A1 EP3022763 A1 EP 3022763A1 EP 14734840 A EP14734840 A EP 14734840A EP 3022763 A1 EP3022763 A1 EP 3022763A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- gas discharge
- housing part
- discharge lamp
- window
- aperture
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
- 230000003287 optical effect Effects 0.000 claims abstract description 14
- YZCKVEUIGOORGS-OUBTZVSYSA-N Deuterium Chemical compound [2H] YZCKVEUIGOORGS-OUBTZVSYSA-N 0.000 claims abstract description 11
- 229910052805 deuterium Inorganic materials 0.000 claims abstract description 11
- 239000000463 material Substances 0.000 claims abstract description 6
- 239000004020 conductor Substances 0.000 claims abstract description 5
- 238000005192 partition Methods 0.000 claims abstract 2
- 229910052751 metal Inorganic materials 0.000 claims description 13
- 239000002184 metal Substances 0.000 claims description 13
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 claims description 12
- 229910052759 nickel Inorganic materials 0.000 claims description 6
- 239000000956 alloy Substances 0.000 claims description 3
- 229910045601 alloy Inorganic materials 0.000 claims description 3
- 239000005388 borosilicate glass Substances 0.000 claims description 3
- 238000010183 spectrum analysis Methods 0.000 claims description 3
- 239000002245 particle Substances 0.000 description 11
- 239000000919 ceramic Substances 0.000 description 6
- 239000011521 glass Substances 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
- 230000015572 biosynthetic process Effects 0.000 description 3
- 230000005684 electric field Effects 0.000 description 3
- 230000031700 light absorption Effects 0.000 description 3
- 238000000465 moulding Methods 0.000 description 3
- 230000005855 radiation Effects 0.000 description 3
- 238000013459 approach Methods 0.000 description 2
- 238000000149 argon plasma sintering Methods 0.000 description 2
- 239000002800 charge carrier Substances 0.000 description 2
- 150000002500 ions Chemical class 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 229910010293 ceramic material Inorganic materials 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000005520 cutting process Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 239000012777 electrically insulating material Substances 0.000 description 1
- 230000003628 erosive effect Effects 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000012811 non-conductive material Substances 0.000 description 1
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 1
- 230000008092 positive effect Effects 0.000 description 1
- 238000004080 punching Methods 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 230000001960 triggered effect Effects 0.000 description 1
- 238000002211 ultraviolet spectrum Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/04—Electrodes; Screens; Shields
- H01J61/10—Shields, screens, or guides for influencing the discharge
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/68—Lamps in which the main discharge is between parts of a current-carrying guide, e.g. halo lamp
Definitions
- the invention relates to a gas discharge lamp, in particular a
- a deuterium lamp comprising a lamp bulb filled with gas and an arrangement inside the lamp bulb, comprising: an electrode housing having a front housing part of non-electrically conductive material, a rear housing part and a housing intermediate wall separating the front housing part from the rear housing part, wherein the front housing part
- Cathode arranged in front of the cathode cathode and a light emission window, which emits light caused by discharge to the outside, and wherein the rear housing part accommodates an anode, which lies with the light exit window in the front housing part on an optical axis A.
- the invention relates to a use of the gas discharge lamp for analytical purposes
- Gas discharge lamps consist of a filled with a filling gas
- Lamp bulb in which two electrodes (cathode and anode) are arranged. When a voltage is applied between the electrodes, a gas discharge takes place, which is associated with the emission of optical radiation. The gas discharge causes a plasma state within the filling gas.
- Plasma consists partly or wholly of free positively and negatively charged particles (ions, electrons) whose motion is influenced by the strength of the field between the two electrodes and by special designs of the cathode and anode spaces within the lamp envelope.
- Deuterium lamps deuterium filling gas
- Deuterium filling gas are generally constructed in such a way that particles from the cathode space and from the area of the Plasma arc between the cathode and anode can pass through the light exit window on the lamp envelope made of glass. It happens there
- Lamp bulb made of quartz glass or other UV-transparent glass and has a housing whose rear part and the housing intermediate wall made of ceramic.
- the anode is located in the rear of the housing, just behind an opening in the housing intermediate wall, in which a
- the housing front part is made of metal and has a light exit window.
- the housing front part is used as a front electrode (front electrode 23)
- the cathode region In the front part of the housing is the cathode region, wherein the cathode of a so-called cathode box (cathode box) is surrounded by a wing of the front electrode (front housing part) and a
- Cathode slot electrode (cathode slit electrode 27) is formed.
- Kathodenbox causes a reliable ignition and a stable potential in the cathode compartment, whereby the operating state with respect to the maintenance and direction of the charge carrier path from the cathode over the molding body (focusing electrode 26) to the anode gains in stability.
- the electric circuit for adjusting the desired luminosity of the gas discharge lamp is set so that the potential of the molded article is negative or zero, thereby optimizing the discharge guidance from the cathode to the anode and the shape of the plasma can be.
- DE 10 2008 062 410 A1 relates to a deuterium lamp in which
- the housing front part and the intermediate wall are made of ceramic, the rear wall of the housing is made of metal.
- the cathode in the front housing part is partially surrounded by the ceramic housing front, in addition, is a metallic
- the ceramic housing front part has an opening for the jet outlet, through which, in the unfavorable case, charged particles can also pass from the plasma to the lamp bulb surface.
- the cathode compartment or the cathode shielding window made of electrically insulating material, the entire housing, the intermediate wall, and the molded body, however, are made of metal. Also in this construction of the deuterium lamp, the formation of side streams is avoided.
- the metallic housing front part has an opening for the jet exit in the direction of the lamp bulb, which in this case is provided with a dazzle-type attachment. Since the attachment forms a unit with the metallic housing, it can not be attributed any independent electrical potential. The attachment has here only the function of a holder for a possible filter plate.
- the discharge lamps described here have the disadvantage that during operation particles which are released in the electrode housing, whether from the cathode space or from the area of the plasma arc between cathode and anode, can pass through the light exit window onto the lamp envelope made of glass and cause damage there.
- Lifespan of the gas discharge lamp decreases significantly.
- the particles can change the glass of the lamp bulb so that it comes to light absorption and / or light scattering.
- Gas discharge lamp should also be easy and inexpensive to manufacture.
- the gas discharge lamp according to the invention comprises one with gas,
- an electrode housing which has a front housing part made of non-electrically conductive material, a rear housing part and the front separating from the rear housing part housing intermediate wall.
- the anode compartment with an anode is located in the rear housing part.
- the anode faces an opening in the housing intermediate wall and a light exit window in the front housing part, so that the anode, the opening in the housing intermediate wall and the light exit window lie on an optical axis A.
- the light caused by the discharge is emitted to the outside via the light emission window.
- an outlet panel having an adjustable electrical potential is arranged with an aperture outside the front housing part and in front of the light exit window.
- Aperture is in projection of the light exit window and has a distance from this. The center of the aperture and that of the
- Light exit window thus lie on the optical axis A of the gas discharge lamp.
- the electrical potential of the exit aperture affects the electrical
- the electrical potential of the exit aperture can be of similar magnitude as the potential of the cathode screen window, but it is adjustable independently of this.
- the geometry of the exit aperture plays a role, so that a minimum distance between the light exit window and aperture is necessary to bring the shielding effect sufficiently advantage. The interaction of the geometrical relationships of the exit aperture and the electrical potential of the exit aperture affects the electric field in the region of
- Light emission window which in turn affects the movement of particles (ions, electrons) from the plasma or particles that arise in the electrode housing during operation of the lamp.
- Exit orifice is designed as a U-profile, whose legs are the front
- U-profile as exit aperture is a solution that is easy to implement in terms of assembly.
- the leg length is easy to dimension in standard components.
- the aperture can be mounted in advance in such U-profiles by punching, so that only a cutting to length of the required for each lamp U-profile is required as an exit panel.
- the U-profile is arranged approximately over the entire height of the front housing part, which is in view of the shielding effect of this
- the U-profile may have at one or more points approaches that as attachment and / or
- An alternative and also preferred embodiment of the exit aperture is that of the ring shape.
- the exit aperture encloses the light exit window, whereby the shielding space created by this embodiment of the exit aperture can be further developed in front of the light exit window by the choice of the ring diameter and a ring profile with respect to optimum protection of the lamp envelope from damage by any particles from the plasma , It has proved to be advantageous if the annular exit aperture has an angle profile, one leg determines the distance to the light exit window, or if the annular
- Exit aperture has a semi-circular profile whose diameter determines the distance to the light exit window.
- the exit aperture is preferably made of a metal.
- Metal as a good electrically conductive material is available in a variety of geometric shapes, so that metal is particularly suitable as a material for the exit aperture.
- a preferred metal for this application is nickel or a nickel-base alloy. Other metals are in principle also suitable, as far as the electric
- Lamp bulbs do not limit their use or exclude.
- Light emission window is at least one millimeter. Limiting the distance between the light exit window and the aperture is the distance of the exit aperture to the lamp envelope. However, direct contact of the exit aperture with the lamp envelope must be avoided as this is too
- the minimum distance of 1 mm to the light exit window is necessary to create a space in front of the light exit window, which forms a kind of shield for emerging from the electrode housing or the plasma particles relative to the lamp envelope.
- This shielding space has its effect also with regard to limiting the temperature of the lamp bulb, at least in the
- the electrical potential of the exit aperture is adjustable by a connection to a lying outside the electrode housing voltage source.
- a voltage source for example, a laboratory power supply is suitable, which ensures a precise adjustment of low voltage values up to voltage values in the range of up to 100 volts.
- An alternative and equally preferred way of adjusting the electrical potential of the exit aperture is that the electrical potential is adjustable by connection to the cathode shield window.
- a contact between the exit panel and cathode shield is necessary.
- the connection has the lowest possible contact resistance. The location of the electrical connection is of minor importance.
- connection between the exit aperture and the cathode shielding window is effected through the front housing part by means of at least one metallic rivet which at the same time mechanically fastens the exit aperture to the front housing part.
- the riveted joint ensures a good conductive connection between the exit aperture and the cathode shield window, which is also clean and precise in design.
- the rivet is set through the front housing part and also serves to attach the
- Rivet also a connection by means of a screw possible, which is optionally set by a hole through the front housing part.
- the front housing part itself is made of electrically non-conductive material, that is usually made of a ceramic material such as
- Design of the aperture is taken into account the fact that the light cone emanating from the plasma in the interior of the front housing part is not or only slightly limited by the aperture in the exit aperture. This measure is particularly important in terms of the highest possible light output of the gas discharge lamp of importance.
- a borosilicate glass is preferably used as the material for the lamp envelope.
- the borosilicate glass is chemical and
- Gas discharge lamp sufficiently transparent. Such a lamp bulb is therefore well suited for gas discharge lamps, which are used for example in spectrophotometers.
- Gas discharge lamp with the aforementioned features are used for analytical purposes, in particular as a light source in spectral analysis.
- the invention is based on a patent drawing and a
- Figure 2 is a front perspective view of the housing a
- 3a, 3b are each a perspective view from above of the housing of
- FIG. 2 a deuterium lamp 1 is shown schematically in cross section along the optical axis A.
- the lamp 1 has a lamp bulb 2 and a two-part housing, consisting of a front housing part 3 with a housing intermediate wall 4 made of ceramic, in this case aluminum oxide, as well as a rear housing part 5 made of metal.
- the lamp bulb 2 is filled with gas, here deuterium.
- the rear housing part 5 is the anode 6.
- a cathode 7 and an existing of a nickel sheet cathode shield 8 are arranged.
- the front housing part 3 has a light exit window 9 which faces the anode 6 and forms with it the optical axis A of the gas discharge lamp.
- the cathode shield window 8 has an opening 16 in the direction of the optical axis A.
- a discharge forms between the cathode 7 and the anode 6, which provides a continuous UV spectrum.
- a shaped body 10 is arranged in front of the opening 17 of the housing intermediate wall 4 and the anode 6, which constricts the plasma in the form of a sphere by means of charge carrier concentration.
- the light cone (not shown) resulting from the discharge and formation of the plasma passes along the optical axis A through the
- Light exit window 9 in the direction of the lamp bulb 2. Outside on the front housing part 3, in front of the light exit window 9, an exit aperture 1 1 is arranged from a nickel plate with a U-profile.
- the exit aperture 1 1 has an aperture 12 which is in projection to the light exit window 9, wherein the aperture 12 with a diameter of 8 mm is slightly larger than the light exit window 9 with a diameter of 6 mm.
- Exit aperture 1 1 has two legs 13, 13 'with a leg length of about
- the legs 13, 13 'of the U-profile of the exit aperture 1 1 determine the distance of the aperture 12 from the light exit window 9.
- this can also be used as an annular angle profile
- the exit aperture 1 1 is attached to the front housing part 3 and at the same time electrically conductively connected to the cathode shield 8.
- the rivet 14 consists of a nickel Base alloy and is positioned in a setting process through the ceramic housing front part 3 therethrough.
- Kathodenablesers 8 and the light exit window 9 and approximately adjusted to the level of the potential at the cathode screen. In this area is to be expected with a potential in the order of 10 to 20 volts, whereas between cathode 7 and anode 6 about 60 to 100 V are applied.
- the deuterium lamp 1 according to the invention is thus suitable as
- Light source to be used in a spectrophotometer Even with permanent operation of up to more than 2000 hours, there is no damage to the lamp bulb 2 due to increased light absorption or light scattering.
- Figure 2 shows only the light-emitting housing, which is located within a lamp envelope, not shown.
- the exit aperture 1 1 can be seen with a circular aperture 12.
- the aperture 12 is in the extension of the light exit window 9, which is not completely visible in Figure 2.
- the exit aperture 1 1 is formed as an elongated component with a U-profile, which is fastened with a rivet 14 on the front housing part 3 and via the contacting portion 15 with the
- Cathode shield 8 is electrically connected.
- Figures 3a and 3b show two variants of a view from above of the housing according to the figure 2.
- the cathode 7 with the
- Contacting section 15 which is connected via a rivet 14 with the exit panel 1 1 and attached and electrically contacted.
- the contacting section is formed by two webs 15 ', 15 ", which are spaced apart from the light exit window 9.
- Two rivets 14, 14' connect the exit screen 1 1 to the cathode shielding window 8 via the two webs 15 ', 15"
Landscapes
- Vessels And Coating Films For Discharge Lamps (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
Description
Claims
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP16184237.2A EP3118888B1 (en) | 2013-07-18 | 2014-07-04 | Gas discharge lamp, in particular deuterium lamp, with light exit diaphragm for blocking contaminants |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102013107694.7A DE102013107694A1 (en) | 2013-07-18 | 2013-07-18 | Gas discharge lamp and its use |
PCT/EP2014/064324 WO2015007548A1 (en) | 2013-07-18 | 2014-07-04 | Gas discharge lamp and use thereof |
Related Child Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP16184237.2A Division EP3118888B1 (en) | 2013-07-18 | 2014-07-04 | Gas discharge lamp, in particular deuterium lamp, with light exit diaphragm for blocking contaminants |
Publications (1)
Publication Number | Publication Date |
---|---|
EP3022763A1 true EP3022763A1 (en) | 2016-05-25 |
Family
ID=51062830
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP16184237.2A Active EP3118888B1 (en) | 2013-07-18 | 2014-07-04 | Gas discharge lamp, in particular deuterium lamp, with light exit diaphragm for blocking contaminants |
EP14734840.3A Withdrawn EP3022763A1 (en) | 2013-07-18 | 2014-07-04 | Gas discharge lamp and use thereof |
Family Applications Before (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP16184237.2A Active EP3118888B1 (en) | 2013-07-18 | 2014-07-04 | Gas discharge lamp, in particular deuterium lamp, with light exit diaphragm for blocking contaminants |
Country Status (4)
Country | Link |
---|---|
EP (2) | EP3118888B1 (en) |
CN (1) | CN105556639A (en) |
DE (1) | DE102013107694A1 (en) |
WO (1) | WO2015007548A1 (en) |
Family Cites Families (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59184451A (en) * | 1983-04-01 | 1984-10-19 | Hitachi Ltd | Hydrogen light emission tube |
US4910431A (en) * | 1987-04-24 | 1990-03-20 | W. C. Heraeus Gmbh | Hydrogen discharge ultraviolet light source or lamp, and method of its manufacture |
DE3902144A1 (en) * | 1989-01-25 | 1990-08-02 | Heraeus Gmbh W C | DEUTERIUM LAMP FOR SPECTRAL ANALYSIS DEVICES |
JPH0660852A (en) * | 1992-08-12 | 1994-03-04 | Hitachi Ltd | Heavy-hydrogen discharge tube |
JP2769436B2 (en) | 1994-08-31 | 1998-06-25 | 浜松ホトニクス株式会社 | Gas discharge tube and lighting device thereof |
JP4932185B2 (en) * | 2005-06-30 | 2012-05-16 | 浜松ホトニクス株式会社 | Gas discharge tube, light source device, and liquid chromatograph |
DE102006040613B3 (en) * | 2006-08-30 | 2007-11-29 | Heraeus Noblelight Gmbh | Translucent low pressure discharge hydrogen lamp for spectral analytical application, has metallic housing construction protecting discharge chamber in bulb filled with deuterium |
DE102008062410A1 (en) | 2008-12-17 | 2010-07-01 | Heraeus Noblelight Gmbh | Cathode shielding in deuterium lamps |
-
2013
- 2013-07-18 DE DE102013107694.7A patent/DE102013107694A1/en not_active Ceased
-
2014
- 2014-07-04 EP EP16184237.2A patent/EP3118888B1/en active Active
- 2014-07-04 WO PCT/EP2014/064324 patent/WO2015007548A1/en active Application Filing
- 2014-07-04 EP EP14734840.3A patent/EP3022763A1/en not_active Withdrawn
- 2014-07-04 CN CN201480039915.1A patent/CN105556639A/en active Pending
Also Published As
Publication number | Publication date |
---|---|
DE102013107694A1 (en) | 2015-01-22 |
CN105556639A (en) | 2016-05-04 |
WO2015007548A1 (en) | 2015-01-22 |
EP3118888A1 (en) | 2017-01-18 |
EP3118888B1 (en) | 2017-10-25 |
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Legal Events
Date | Code | Title | Description |
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PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
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17P | Request for examination filed |
Effective date: 20151210 |
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AK | Designated contracting states |
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AX | Request for extension of the european patent |
Extension state: BA ME |
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DAX | Request for extension of the european patent (deleted) | ||
RIN1 | Information on inventor provided before grant (corrected) |
Inventor name: FISCHER, NORBERT Inventor name: DESINGER, GUNTHER Inventor name: ARNOLD, ERICH Inventor name: RADOSEVIC, IGOR Inventor name: PERLET, GUENTER Inventor name: SOELLER, CHRISTOPH Inventor name: UEBBING, BRUNO Inventor name: SCHNABL, ANKE Inventor name: SCHNEIDER, THEO Inventor name: JENEK, TORSTEN Inventor name: DAMASCHKE, GERHARD |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
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18D | Application deemed to be withdrawn |
Effective date: 20160907 |