EP2073242A2 - Tube, notamment tube électronique - Google Patents
Tube, notamment tube électronique Download PDFInfo
- Publication number
- EP2073242A2 EP2073242A2 EP08169844A EP08169844A EP2073242A2 EP 2073242 A2 EP2073242 A2 EP 2073242A2 EP 08169844 A EP08169844 A EP 08169844A EP 08169844 A EP08169844 A EP 08169844A EP 2073242 A2 EP2073242 A2 EP 2073242A2
- Authority
- EP
- European Patent Office
- Prior art keywords
- tube
- temperature
- sensor
- electrodes
- electrode
- 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- Withdrawn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 9
- 238000010438 heat treatment Methods 0.000 claims description 13
- 230000004913 activation Effects 0.000 claims description 2
- 239000011521 glass Substances 0.000 abstract description 3
- 238000011144 upstream manufacturing Methods 0.000 abstract description 2
- 239000003779 heat-resistant material Substances 0.000 abstract 1
- 238000005259 measurement Methods 0.000 description 11
- 238000001704 evaporation Methods 0.000 description 10
- 230000008020 evaporation Effects 0.000 description 8
- 238000009529 body temperature measurement Methods 0.000 description 6
- 229910052788 barium Inorganic materials 0.000 description 4
- DSAJWYNOEDNPEQ-UHFFFAOYSA-N barium atom Chemical compound [Ba] DSAJWYNOEDNPEQ-UHFFFAOYSA-N 0.000 description 4
- 239000000463 material Substances 0.000 description 4
- 238000011156 evaluation Methods 0.000 description 3
- 239000000919 ceramic Substances 0.000 description 2
- 238000013461 design Methods 0.000 description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- 206010053648 Vascular occlusion Diseases 0.000 description 1
- 230000032683 aging Effects 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 239000000969 carrier Substances 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 239000010406 cathode material Substances 0.000 description 1
- 238000004140 cleaning Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000018109 developmental process Effects 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005672 electromagnetic field Effects 0.000 description 1
- 230000005670 electromagnetic radiation Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
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- 150000002500 ions Chemical class 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000012544 monitoring process Methods 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 230000009291 secondary effect Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 230000035882 stress Effects 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 238000002207 thermal evaporation Methods 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J1/00—Details of electrodes, of magnetic control means, of screens, or of the mounting or spacing thereof, common to two or more basic types of discharge tubes or lamps
- H01J1/02—Main electrodes
- H01J1/13—Solid thermionic cathodes
- H01J1/135—Circuit arrangements therefor, e.g. for temperature control
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/34—Circuit arrangements not adapted to a particular application of the tube and not otherwise provided for
Definitions
- the invention relates to an improved tube, in particular an electron tube, and an improved system for controlling the electrodes and / or the heating of a tube and for determining the life of a tube.
- Electronic tubes particularly vacuum electron tubes, have a limited life, as is well known.
- An important factor influencing the service life is the emissivity of the cathode.
- the emissivity of the cathode deteriorates steadily in the operation of a tube with directly or indirectly heated cathode by evaporation of the electron-emitting material. This degradation can be expressed, for example, by the filament evaporation rate or Barium Evaporation Rate (Barium Evaporation Rate).
- EP 0 339 714 A1 called: tensile stress of the cathode wire, length of the cathode wire, spectrum and intensity of the emitted electromagnetic radiation, number of emitted electrons per unit time and their velocity distribution and the electrical resistance of the cathode wire.
- JP 09245712 A suggests to avoid blown cathode wires to monitor the voltage drop across the cathode and to regulate the drive voltage accordingly.
- the problem with these solutions is that the determination of the temperature of the cathode wire is only indirectly via the detour of a measurement of a different physical size. As with every measurement, specific inaccuracies of the respective measurement occur. In addition still occur modeling inaccuracies, for example, can be closed only error-prone to the temperature of a determined with low relative error electrical resistance of a cathode wire. This follows from the mere fact that tubes have manufacturing tolerances, for example, the diameter or the length of the cathode wire. In the case of indirectly heated cathodes, the temperature of the heating wire is first determined from the resistance measurement and then the (erroneous) assumption is made that the cathode temperature is identical or deviates by an empirically determined value. Furthermore, environmental influences and aging phenomena have a negative effect on the precision of the indirect temperature determination.
- a tube in particular an electron tube, with an evacuated or gas-filled region in which one or more electrodes and means for measuring the temperature of one of the electrodes are arranged.
- the means, which are arranged in the evacuated or gas-filled region of the tube, for measuring the electrode temperature comprise a pyrometric sensor.
- the sensor or an optical element upstream of the sensor is protected by a shutter which is opened and / or closed electronically or electromechanically can.
- the invention further relates to a system comprising such a tube having a controller with means for detecting an electrode temperature measurement.
- a controller may be provided which detects an impending end of life of the tube by continuous evaluation of the electrode temperature and the tube supplied heating power and signals to an operator and / or a maintenance center.
- a controller may be provided, which additionally or alternatively continuously evaluates the electrode temperature and has means for driving the electrodes and / or an electrode heater, wherein the control of the electrodes and / or the electrode heating takes place so that the electrode temperature corresponds to a desired value ,
- the advantage of the present invention is the fact that with relatively little effort, a precise determination of the electrode temperature of an electronic tube can be done. As a result, on the one hand the life of the tube can be predicted more accurately. On the other hand, by monitoring the electrode temperature and corresponding activation of the electrodes and / or the electrode heating, it is possible to keep the electrode temperature exactly at a desired value (nominal value). This is advantageous because, for example, in a klystron, exceeding the nominal surface temperature of 890 ° C by only 50K results in an undesirable doubling of the barium evaporation rate.
- Fig. 1 shows the gun area of a klystron 100.
- a klystron is an electron tube that exploits the transit time of the electrons to generate or amplify high-frequency signals.
- a housing 120 made of non-conductive, temperature-resistant material, for example ceramic or glass, encloses an evacuated area 110, in which a cathode with a cathode surface 140 is arranged, which is heated by a heater 130.
- a means 150 for temperature measurement here comprising a sensor body 160 with closure 170 and electrical connections 180.
- an anode 190 of the electron tube 100 is shown.
- Fig. 2 shows with further details the means 150 for temperature measurement.
- This is comprised of the tube housing 120 and consists of the sensor body 160, which may optionally be associated with an optical element 162, for example a lens, in order to achieve a better focus on the area to be detected.
- an optical element 162 for example a lens
- a so-called central shutter 170 is used to protect the surface of the optical sensor 160 and the lens 162, respectively.
- the central closure consists of several curved steel plates, which are pivoted about fixed pivot points out of the beam path. Such central closures are known from the photo camera technology and available in high quantities at low prices.
- the shutter also called shutter
- a shutter 170 is also a disc with an opening which rotates when actuated and the beam path to the sensor 160 releases.
- the control of the closure 170 is electromechanical, wherein the necessary electrical energy is supplied via electrical connections 184.
- the signal generated by the sensor 160 is provided at further terminals 182.
- the integrated optical measuring arrangement 150 is used to determine the evaporation rate in the tube 100, by means of which periodically a surface temperature measurement of cathode or anode (for example, in X-ray tubes is the anode temperature of great interest) performed becomes.
- the direct measurement of the actual surface temperature can effectively realize a heating control.
- the senor 160 is a photosemiconductor. Temperatures above about 700 ° C can be measured pyrometrically with photodiodes in the visible spectral range. Pyrometers are units that include the sensor 160 and an evaluation unit - not shown. Pyrometers are used for non-contact temperature measurement of temperatures between -50 ° C and + 4000 ° C. In most cases, the reception wavelength range of high-temperature pyrometers is determined by the photoreceiver used: the lowest reception wavelength of silicon photodiodes is z. B. about 1.1 microns. A body with a temperature of 3000 K has its radiation maximum here, but temperatures can be measured as low as about 700 ° C.
- the surface temperatures of Klystron, Magnetron, Thyratron and Accelerator are 890 ° C to 1050 ° C, depending on the cathode type used (oxide or impregnated).
- the surface temperature of the tungsten heating wire in X-ray tubes is about 2000 ° C.
- the present invention makes possible a more reliable lifetime prediction with at the same time minimally higher costs for the integrated optical measuring arrangement. Slowly approaching failures can be detected as the temperature reached decreases while the heating power supplied remains the same. Integration of the evaluation into the higher-level control of the overall system allows service messages to be issued before the system fails and produces expensive downtime (so-called predictive maintenance). about the rate of evaporation so determined and the amount of barium available in the cathode from the beginning can be used to calculate an arcing probability.
- the present invention allows a targeted lifetime extension of the electron tube 100.
- the exact measurement of the surface temperature of the state (electron emission at currently supplied heating power) of the cathode can be determined and from an accurate heating control can be derived.
- the consequence of accurate heater control is the significant increase in tube life.
- the period duration ie the frequency with which the shutter 170 is opened and a temperature measurement is carried out, can be set.
- the period duration will be in the range of seconds or less, however, for the life-time prediction a period in the minute or even hour range may be sufficient.
- the present invention is not limited to the described embodiments. Rather, it is applicable to all types of tubes, preferably those tubes whose failure - as in the medical field - cause high costs by stoppage of an expensive overall system, such as X-ray tubes or tubes of the type Thyratron, Klystron, Magnetron, or Accelerator.
- the present invention is applicable to both evacuated and gas-filled tubes, as well as to tubes that are not strictly referred to as electron tubes, such as because, as in a thyratron, ions act as carriers.
Landscapes
- Physical Vapour Deposition (AREA)
- Discharge Heating (AREA)
- X-Ray Techniques (AREA)
- Measurement Of Radiation (AREA)
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE102007062054A DE102007062054B4 (de) | 2007-12-21 | 2007-12-21 | Röhre, insbesondere Elektronenröhre, mit Mitteln zur Messung der Elektrodentemperatur und Schutz hierfür |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| EP2073242A2 true EP2073242A2 (fr) | 2009-06-24 |
| EP2073242A3 EP2073242A3 (fr) | 2010-01-13 |
Family
ID=40328647
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP08169844A Withdrawn EP2073242A3 (fr) | 2007-12-21 | 2008-11-25 | Tube, notamment tube électronique |
Country Status (4)
| Country | Link |
|---|---|
| US (1) | US20090167133A1 (fr) |
| EP (1) | EP2073242A3 (fr) |
| CN (1) | CN101504900A (fr) |
| DE (1) | DE102007062054B4 (fr) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2022229005A1 (fr) * | 2021-04-28 | 2022-11-03 | Koninklijke Philips N.V. | Systèmes et procédés pour améliorer une prédiction de défaillance de filament de tube à rayons x |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE102009034646A1 (de) * | 2009-07-24 | 2010-09-16 | Siemens Aktiengesellschaft | Strahlkopf |
| CN109769310A (zh) * | 2017-11-10 | 2019-05-17 | 庄品洋 | 一种真空管音色微控装置和真空管音响功放系统 |
| US20230154720A1 (en) * | 2021-11-16 | 2023-05-18 | Nuflare Technology, Inc. | Method for estimating cathode lifetime of electron gun, and electron beam writing apparatus |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4708677A (en) | 1985-12-27 | 1987-11-24 | Itt Electro Optical Products, A Division Of Itt Corporation | Method of measuring the temperature of a photocathode |
| EP0339714A1 (fr) | 1988-04-20 | 1989-11-02 | Koninklijke Philips Electronics N.V. | Dispositif de tube électronique et tube électronique |
| JPH09245712A (ja) | 1996-03-13 | 1997-09-19 | Mitsubishi Electric Corp | 陰極加熱監視装置およびその監視方法 |
| DE19956391A1 (de) | 1999-11-24 | 2001-05-31 | Nobile Ag | Verfahren und Vorschaltgerät zum Starten und Betreiben einer Leuchtstofflampe |
Family Cites Families (12)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB411891A (en) * | 1932-12-09 | 1934-06-11 | Victor Henry Gilbert | Improvements relating to pyrometers and like instruments |
| GB1157194A (en) * | 1967-04-05 | 1969-07-02 | Hirst Microwave Heating Ltd | Magnetron Temperature Control |
| GB1196103A (en) * | 1968-02-02 | 1970-06-24 | Ass Elect Ind | Improvements relating to Electron Guns |
| DE2312336A1 (de) * | 1973-03-13 | 1974-09-19 | Philips Patentverwaltung | Anordnung zur messung der anodentemperatur einer roentgenroehre |
| JPS5721100A (en) * | 1980-07-14 | 1982-02-03 | Toshiba Corp | X-ray generator |
| US5274305A (en) * | 1991-12-04 | 1993-12-28 | Gte Products Corporation | Low pressure mercury discharge lamp with thermostatic control of mercury vapor pressure |
| WO1999020988A1 (fr) * | 1997-10-20 | 1999-04-29 | Texaco Development Corporation | Appareil pour mesurer la temperature a l'interieur de reacteurs |
| US6512816B1 (en) * | 2001-10-09 | 2003-01-28 | Koninklijke Philips Electronics, N.V. | Temperature clock for x-ray tubes |
| US7161312B2 (en) * | 2003-08-14 | 2007-01-09 | Sluggo Lighting Ltd. | Distributed fluorescent light control system |
| FR2880510B1 (fr) * | 2005-01-03 | 2007-03-16 | Gen Electric | Procede et systeme de regulation de courant de tube a rayon x |
| JP2007073395A (ja) * | 2005-09-08 | 2007-03-22 | Tokyo Electron Ltd | マグネトロンの制御方法、マグネトロンの寿命判定方法、マイクロ波発生装置、マグネトロンの寿命判定装置、処理装置及び記憶媒体 |
| CN101410928B (zh) * | 2006-03-29 | 2010-11-03 | 皇家飞利浦电子股份有限公司 | X射线焦斑温度的双色高温测量 |
-
2007
- 2007-12-21 DE DE102007062054A patent/DE102007062054B4/de not_active Expired - Fee Related
-
2008
- 2008-11-25 EP EP08169844A patent/EP2073242A3/fr not_active Withdrawn
- 2008-12-15 US US12/335,120 patent/US20090167133A1/en not_active Abandoned
- 2008-12-22 CN CNA2008101910494A patent/CN101504900A/zh active Pending
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4708677A (en) | 1985-12-27 | 1987-11-24 | Itt Electro Optical Products, A Division Of Itt Corporation | Method of measuring the temperature of a photocathode |
| EP0339714A1 (fr) | 1988-04-20 | 1989-11-02 | Koninklijke Philips Electronics N.V. | Dispositif de tube électronique et tube électronique |
| JPH09245712A (ja) | 1996-03-13 | 1997-09-19 | Mitsubishi Electric Corp | 陰極加熱監視装置およびその監視方法 |
| DE19956391A1 (de) | 1999-11-24 | 2001-05-31 | Nobile Ag | Verfahren und Vorschaltgerät zum Starten und Betreiben einer Leuchtstofflampe |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2022229005A1 (fr) * | 2021-04-28 | 2022-11-03 | Koninklijke Philips N.V. | Systèmes et procédés pour améliorer une prédiction de défaillance de filament de tube à rayons x |
| US12507336B2 (en) | 2021-04-28 | 2025-12-23 | Koninklijke Philips N.V. | Systems and methods to improve X-ray tube filament failure prediction |
Also Published As
| Publication number | Publication date |
|---|---|
| EP2073242A3 (fr) | 2010-01-13 |
| US20090167133A1 (en) | 2009-07-02 |
| DE102007062054B4 (de) | 2010-04-08 |
| CN101504900A (zh) | 2009-08-12 |
| DE102007062054A1 (de) | 2009-07-02 |
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