EP2839499A1 - Funkenstrecke - Google Patents
FunkenstreckeInfo
- Publication number
- EP2839499A1 EP2839499A1 EP12729934.5A EP12729934A EP2839499A1 EP 2839499 A1 EP2839499 A1 EP 2839499A1 EP 12729934 A EP12729934 A EP 12729934A EP 2839499 A1 EP2839499 A1 EP 2839499A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- spark gap
- anode
- cathode
- useful
- pressure
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J35/00—X-ray tubes
- H01J35/22—X-ray tubes specially designed for passing a very high current for a very short time, e.g. for flash operation
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J35/00—X-ray tubes
- H01J35/02—Details
- H01J35/025—X-ray tubes with structurally associated circuit elements
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05G—X-RAY TECHNIQUE
- H05G1/00—X-ray apparatus involving X-ray tubes; Circuits therefor
- H05G1/08—Electrical details
Definitions
- Spark gap The invention relates to a spark gap with an anode and a cathode.
- a spark gap of the type described above is described in ⁇ example in DE 2 259 382.
- This is an X-ray source which uses a spark gap to generate X-radiation.
- the Fun ⁇ ken zone consists of an anode and a cathode, wherein the anode is used as a target for the generation of the X-ray radiation.
- the X-radiation is produced when an arc is ignited in the spark gap, which excites the target to emit X-ray radiation.
- the object of the invention is therefore to provide a spark gap with which a possible defined ignition point can be realized.
- High-pressure spark gap and a useful spark gap which are interconnected by a center piece.
- the spark gap between the cathode and the with ⁇ telst Culture is formed.
- the middle piece is connected to the anode via a line in which an electrical resistance is provided.
- the useful spark gap is formed between the middle piece and the anode.
- the arrangement of the high-pressure spark gap and the useful spark gap is a series connection. However, the middle piece is over the resistance with the anode connected. To ignite the useful spark gap an increasing voltage is applied to the ge ⁇ entire arrangement. Since the high-pressure spark gap is filled with a gas which is under high pressure, a comparatively high flashover potential is ensured here. While the tension ⁇ voltage increases, is up to the useful radio link at no switching relevant differential potential because it is connected to the center piece, which is equivalent to at this time an on-circuit to ground. Once the comparatively defined switching point of the high-pressure spark gap it is ⁇ enough ignites them.
- the resistance is 100 to 1000 ⁇ . In this case, it is ensured that switching of the useful spark gap takes place because the adjacent
- the useful spark gap is provided for generating X-radiation.
- the anode is used as the target for generating the X-ray radiation.
- the X-ray radiation can be made available at a defined time switching point. This is an important advance ⁇ requisite for various applications.
- the X-ray radiation can be used for imaging methods - for example in a flash X-ray source.
- monochromatic X-ray radiation can be generated with the anode.
- Monochromatic X-ray radiation can be generated, for example, if the target used is a very thin metal foil, for example made of aluminum or another light metal.
- the lanthanides can also be used as the target material.
- the metals and their alloys LE will be referred to aschtme ⁇ metals in the sense of the application, the density of which is less than 5 g / cm 3.
- this definition applies to the following light metals: all alkali metals, alkaline earth metal all ⁇ le except radium, also scandium, yttrium, titanium and aluminum.
- Other advantageous material groups for forming the target are tungsten, molybdenum and the group of Lanthanoi ⁇ de. Specifically, this is the element lanthanum, the 14 elements following the lanthanum in the periodic table.
- the useful spark gap is housed in an evaku ⁇ ible housing, in which a gene for Rönt ⁇ ray radiation transparent window is provided and from which the X-ray radiation can be coupled out.
- the purpose of the collector is to electrostatically decelerate the electron flow accelerated by the anode, thus depriving it of kinetic energy so far that when the electrons hit the collector, the kinetic energy below the level required for the generation of bremsstrahlung is reached , In this way, the parasitic Erzeu- is avoided by broadband bremsstrahlung supply that would otherwise superimpose the monochromatic, charac ⁇ cal radiation generated by the anode.
- the anode, the middle piece and the cathode are arranged coaxially. Moreover, it is advantageous if the anode, the center piece and the cathode are formed centrally symmetrical to the common axis. As a result, the formation of inductances is minimized, which would adversely affect the temporal pulse behavior of the spark gaps (rise time of the pulse current).
- Figure 1 shows schematically the structure of an embodiment of the spark gap according to the invention with a representation of the switching operation without the inclusion of the function of the collector and
- Figure 2 schematically shows a geometric configuration
- spark gap according to Figure 1 in section with depicting ⁇ development of the collector. From Figure 1, the structure of the spark gap according to the invention is clear. This has an anode 11 and a cathode 12. Between the anode 11 and the cathode 12, a middle ⁇ piece 13 is connected, so that two spark gaps, namely a high-pressure spark gap 14 and a useful spark gap 15, arise.
- the center piece 13, which acts as an anode for the useful spark gap 15, via a line 16 and the resistor 17 high impedance to the anode potential is ⁇ connected.
- the center piece 13 forms the Ka ⁇ method.
- the high pressure Spark gap shows the defined switching behavior 18, wherein at a defined voltage increase U with known steep ⁇ unit the switching point is reached after a defined time t. With the switching point (t s / U s ), the switching timing of the useful spark gap can be predicted comparatively accurately.
- the center piece 13 Due to the low-impedance characteristic of the useful spark gap 14, the center piece 13 has cathode potential in the switching instant of the spark plug 14. The resistor 17 is now the full voltage between the cathode and anode.
- Figure 2 can be inferred that the arrangement of the anodes de 12, the middle piece 13, the cathode 11 and a collector ⁇ gate 21 is coaxially constructed. In addition, all of these construction ⁇ parts are also centrally symmetrical to the common axis 22 of the coaxial structure.
- the high-pressure spark gap is housed in a first housing 23, wherein the first housing can be filled with a suitable working gas with the required pressure (filling device not shown in detail).
- the useful spark gap 15 is located together with the collector ⁇ tor 21 in a second housing 24, which is evacuated.
- This second housing also has a window 25, can be coupled out of the housing by the X-ray radiation 26 and ei ⁇ ner application can be supplied.
Landscapes
- X-Ray Techniques (AREA)
Abstract
Description
Claims
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
PCT/EP2012/061298 WO2013185824A1 (de) | 2012-06-14 | 2012-06-14 | Funkenstrecke |
Publications (2)
Publication Number | Publication Date |
---|---|
EP2839499A1 true EP2839499A1 (de) | 2015-02-25 |
EP2839499B1 EP2839499B1 (de) | 2017-03-22 |
Family
ID=46384350
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP12729934.5A Not-in-force EP2839499B1 (de) | 2012-06-14 | 2012-06-14 | Funkenstrecke |
Country Status (7)
Country | Link |
---|---|
US (1) | US9679737B2 (de) |
EP (1) | EP2839499B1 (de) |
JP (1) | JP2015526838A (de) |
KR (1) | KR101689486B1 (de) |
CN (1) | CN104364875B (de) |
RU (1) | RU2608364C2 (de) |
WO (1) | WO2013185824A1 (de) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU2654493C1 (ru) * | 2017-03-06 | 2018-05-21 | Российская Федерация, от имени которой выступает Государственная корпорация по атомной энергии "Росатом" | Вакуумный разрядник |
RU2654494C1 (ru) * | 2017-03-10 | 2018-05-21 | Российская Федерация, от имени которой выступает Государственная корпорация по атомной энергии "Росатом" | Вакуумный искровой разрядник |
RU200561U1 (ru) * | 2019-12-09 | 2020-10-29 | Российская Федерация, от имени которой выступает Государственная корпорация по атомной энергии "Росатом" | Управляемый вакуумный разрядник |
RU196930U1 (ru) * | 2019-12-09 | 2020-03-23 | Российская Федерация, от имени которой выступает Государственная корпорация по атомной энергии "Росатом" | Малогабаритный двухсекционный управляемый вакуумный разрядник |
US20230293394A1 (en) | 2021-09-07 | 2023-09-21 | Nihon Kolmar Co., Ltd. | Topical composition for nanobubble cosmetic |
Family Cites Families (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US656667A (en) * | 1899-11-27 | 1900-08-28 | Wolfgang Schmid | Flexible metal pipe-coupling. |
US1283318A (en) | 1918-09-03 | 1918-10-29 | Henry Ruschmeyer | Spring-bed support. |
US3475646A (en) * | 1967-04-10 | 1969-10-28 | Everett Chapman | Spark gap light source for impact photoelasticity |
FR2075303A5 (de) * | 1970-01-08 | 1971-10-08 | Tsukerman Veniamin | |
GB1443048A (en) | 1972-12-05 | 1976-07-21 | Strahlen Umweltforsch Gmbh | X-ray source |
JPH01225218A (ja) * | 1988-03-04 | 1989-09-08 | Hitachi Ltd | 真空トリガギヤツプ |
US5199054A (en) * | 1990-08-30 | 1993-03-30 | Four Pi Systems Corporation | Method and apparatus for high resolution inspection of electronic items |
JP3500079B2 (ja) * | 1998-11-10 | 2004-02-23 | 日新電機株式会社 | 方形波電源装置 |
EP1353422B1 (de) * | 2002-04-11 | 2004-08-11 | OBO Bettermann GmbH & Co. KG. | Funkenstrecke |
JP5468911B2 (ja) * | 2010-01-05 | 2014-04-09 | 株式会社日立メディコ | X線管装置及びそれを用いたx線ct装置 |
CN104412470B (zh) * | 2012-05-30 | 2016-11-09 | 西门子公司 | 带有电容式储能器的火花间隙 |
-
2012
- 2012-06-14 US US14/407,163 patent/US9679737B2/en not_active Expired - Fee Related
- 2012-06-14 CN CN201280073946.XA patent/CN104364875B/zh not_active Expired - Fee Related
- 2012-06-14 KR KR1020157000984A patent/KR101689486B1/ko active IP Right Grant
- 2012-06-14 JP JP2015516483A patent/JP2015526838A/ja active Pending
- 2012-06-14 RU RU2015100885A patent/RU2608364C2/ru not_active IP Right Cessation
- 2012-06-14 WO PCT/EP2012/061298 patent/WO2013185824A1/de active Application Filing
- 2012-06-14 EP EP12729934.5A patent/EP2839499B1/de not_active Not-in-force
Also Published As
Publication number | Publication date |
---|---|
CN104364875A (zh) | 2015-02-18 |
CN104364875B (zh) | 2017-05-03 |
KR20150023015A (ko) | 2015-03-04 |
JP2015526838A (ja) | 2015-09-10 |
US20150187539A1 (en) | 2015-07-02 |
RU2608364C2 (ru) | 2017-01-18 |
EP2839499B1 (de) | 2017-03-22 |
US9679737B2 (en) | 2017-06-13 |
RU2015100885A (ru) | 2016-08-10 |
KR101689486B1 (ko) | 2016-12-23 |
WO2013185824A1 (de) | 2013-12-19 |
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