US2306860A - Electron discharge device for very high frequencies - Google Patents
Electron discharge device for very high frequencies Download PDFInfo
- Publication number
- US2306860A US2306860A US354657A US35465740A US2306860A US 2306860 A US2306860 A US 2306860A US 354657 A US354657 A US 354657A US 35465740 A US35465740 A US 35465740A US 2306860 A US2306860 A US 2306860A
- Authority
- US
- United States
- Prior art keywords
- electrons
- cylinders
- electron discharge
- resonator
- discharge device
- 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.)
- Expired - Lifetime
Links
- 230000010355 oscillation Effects 0.000 description 5
- 239000002184 metal Substances 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- MJBPUQUGJNAPAZ-AWEZNQCLSA-N butin Chemical compound C1([C@@H]2CC(=O)C3=CC=C(C=C3O2)O)=CC=C(O)C(O)=C1 MJBPUQUGJNAPAZ-AWEZNQCLSA-N 0.000 description 2
- MJBPUQUGJNAPAZ-UHFFFAOYSA-N Butine Natural products O1C2=CC(O)=CC=C2C(=O)CC1C1=CC=C(O)C(O)=C1 MJBPUQUGJNAPAZ-UHFFFAOYSA-N 0.000 description 1
- 241000555745 Sciuridae Species 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/02—Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators
- H01J25/10—Klystrons, i.e. tubes having two or more resonators, without reflection of the electron stream, and in which the stream is modulated mainly by velocity in the zone of the input resonator
- H01J25/18—Klystrons, i.e. tubes having two or more resonators, without reflection of the electron stream, and in which the stream is modulated mainly by velocity in the zone of the input resonator with radial or disc-like electron stream perpendicular to the axis of the resonators
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/02—Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators
Definitions
- This invention relates to electron discharge de-v vices Aof the so-called velocity modulated type.
- a beam of .electrons of uniform velocity is passed through a gap in a resonator to which is applied the resonant frequency, across the gap, the electrons are accelerated or decelerated according to the phase of the oscillations at the time at which they pass.r After In passing leaving this resonant system, ⁇ or modulator, the
- the invention resides in an electron discharge device of the velocity modulated type comprising two co-axial cavity resonators of annular cross-section lying one within the other and an electrode system for projecting electrons radially through grids or apertures in the resonator walls.
- the invention resides in an y electron discharge device of the velocity modulated type wherein two resonant cavities of annular cross-section are deiined by co-axial cylindrical surfaces, an electron source being provided along the axis of the structure for projecting electrons radially through grids or apertures in the cylindrical surfaces.
- FIG. 1 is a cross-sectional elevation of an electron discharge' device Aincorr'noiating features of the invention
- Fig. z is a cross-sectional view taken substantially in the kplane of 2-2 in Fig. l;
- Figs. 3 and 4 are further cross-sectional views taken transversely to the plane of Fig. 1,
- Fig. 1 is a section through the structure a cathode I is surrounded by av series of concentric grids 2, 3, 5, 1 ⁇ 9, the axis of revolution being X- ⁇ X.
- the grids are represented by dottedlines butin practice would probably be of squirrel cage formation, up from a series of rods.
- Fig.'2 shows a sectional view across the line 2-2 of Fig. 1. It will be noticed that the rods forming the respective grids lie on radial lines extending from the cathode. This is a preferred arrangement in order to reduce the number lof electrons collected by the grids.
- Grid 2 is normally operated at a negative potential with respect to the cathode and its purposeis to control the magnitude of the space current.
- the spaces between the ends of the cylinders are closed by the annular discs I6 and I9.
- the two cylinders with their end discs thus form a resonator of the concentric line type.
- grids 1 and 9 form portions of the cylinders 8 and I which with the end discs I1 and I8 form a second concentric line resonator.
- Cylinders 6 and 8 are Joined by two discs placed at the ends of the grid portions as shown.
- the cylinder I I collects the electrons which pass through the system.
- the electrons in passing from the cathode I to the collector II pass through two resonators. If the inner resonator has oscillations applied to it, the electrons will be velocity modulated as described above. While moving between the field free space between the inner and the outer cylinders, bunching or the electrons will take place and energy will be imparted to the outer resonator. Oscillations set up in the second resonator may be taken ol by means of lead I2 which contacts with the cylinder 8 through a concentric tube I3. Other methods for withdrawing energy from the second resonator are possible.
- Fig. 1 and Fig. 3 which is a section across the line being made Y 3-3 Fig. 1.
- An elongated loop of wire Il has 'one limb, in fthe centre of a connecting tube I 5 and theother'limb just outside@ in the wall o! Il.
- the rounded ends of the '99p project into the inner and outer resonators.v v ⁇ '*Ihe coupling between the two resonators displacement of the loop which exposes a greater area of loop in one resonator than in the other.
- Fig. 4 shows how this may Abe imf byannular discs, said inner and said outer pairs" being coaxial with each spaced annular discs between said inner and outer pairs of cylinders providing a substantially ileldother, a pair of axially :I vfree ,drift/space., generally longitudinally extendproved by replacing the rods with stripsl ofmetal set radially. The could then be placed on the inner cumferences of 1 and 9 respectively.
- nator may have a xed frequency vand the other may beA tuned by sliding the end -disclsof the inner resonator up and down.
- the structure may be wholly enclosedor'parts of the resonators may'form parts of envelope.
- An electron ldischarge device including an inner pair of coaxialvsheet-metal cylinders joined at their ends by annular discs, an outer pair ⁇ of coaxial sheet-metal cylinders joined at their ends by annular discs. said inner and said outer pairs said cylinders, through said tube into the two cylinders. a' 3.
- An- .e1ectrcn discharge device including a/ han outer pair of Vcoaxial ing vgrid members provided between said axially spaced annular discs in apertures in each of the wallsofsaid cylinders, a connecting tube between "and a loop ot wire projecting cathode, a grid surrounding/said cathode; inner pairof coaxial sheet-metal cylinders surrounding said grid and joined at their ends yby lanniiva'rdiscs.
Landscapes
- Microwave Tubes (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB266982X | 1939-09-13 |
Publications (1)
Publication Number | Publication Date |
---|---|
US2306860A true US2306860A (en) | 1942-12-29 |
Family
ID=10247792
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US354657A Expired - Lifetime US2306860A (en) | 1939-09-13 | 1940-08-29 | Electron discharge device for very high frequencies |
Country Status (4)
Country | Link |
---|---|
US (1) | US2306860A (en, 2012) |
BE (1) | BE441498A (en, 2012) |
CH (1) | CH266982A (en, 2012) |
GB (1) | GB534696A (en, 2012) |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2424805A (en) * | 1942-11-13 | 1947-07-29 | Gen Electric | High-frequency magnetron |
US2432571A (en) * | 1943-02-24 | 1947-12-16 | Rca Corp | Electron discharge device employing resonators |
US2434962A (en) * | 1940-05-17 | 1948-01-27 | Int Standard Electric Corp | Electron discharge device of the cavity resonator type |
US2438832A (en) * | 1943-09-16 | 1948-03-30 | Rca Corp | Oscillator for centimeter waves |
US2445810A (en) * | 1942-12-04 | 1948-07-27 | Standard Telephones Cables Ltd | Ultra high frequency electric oscillator |
US2458556A (en) * | 1941-04-08 | 1949-01-11 | Bell Telephone Labor Inc | Coupled cavity resonator and wave guide apparatus |
US2459806A (en) * | 1942-01-09 | 1949-01-25 | Int Standard Electric Corp | Velocity-modulated electron discharge device |
US2466063A (en) * | 1943-02-03 | 1949-04-05 | Sperry Corp | High-power high-frequency electron discharge apparatus |
US2480462A (en) * | 1944-01-07 | 1949-08-30 | Western Electric Co | Tunable magnetron |
US2516853A (en) * | 1942-02-16 | 1950-08-01 | Standard Telephones Cables Ltd | Electron discharge device for ultra high frequencies |
US2561727A (en) * | 1943-07-07 | 1951-07-24 | Harold G Cooper | Tuning of electrical resonators |
US2564385A (en) * | 1944-03-25 | 1951-08-14 | Csf | Electronic transmitting valve of great power for ultra short waves |
-
0
- BE BE441498D patent/BE441498A/xx unknown
-
1939
- 1939-09-13 GB GB25695/39A patent/GB534696A/en not_active Expired
-
1940
- 1940-08-29 US US354657A patent/US2306860A/en not_active Expired - Lifetime
-
1947
- 1947-09-06 CH CH266982D patent/CH266982A/de unknown
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2434962A (en) * | 1940-05-17 | 1948-01-27 | Int Standard Electric Corp | Electron discharge device of the cavity resonator type |
US2458556A (en) * | 1941-04-08 | 1949-01-11 | Bell Telephone Labor Inc | Coupled cavity resonator and wave guide apparatus |
US2459806A (en) * | 1942-01-09 | 1949-01-25 | Int Standard Electric Corp | Velocity-modulated electron discharge device |
US2516853A (en) * | 1942-02-16 | 1950-08-01 | Standard Telephones Cables Ltd | Electron discharge device for ultra high frequencies |
US2424805A (en) * | 1942-11-13 | 1947-07-29 | Gen Electric | High-frequency magnetron |
US2445810A (en) * | 1942-12-04 | 1948-07-27 | Standard Telephones Cables Ltd | Ultra high frequency electric oscillator |
US2466063A (en) * | 1943-02-03 | 1949-04-05 | Sperry Corp | High-power high-frequency electron discharge apparatus |
US2432571A (en) * | 1943-02-24 | 1947-12-16 | Rca Corp | Electron discharge device employing resonators |
US2561727A (en) * | 1943-07-07 | 1951-07-24 | Harold G Cooper | Tuning of electrical resonators |
US2438832A (en) * | 1943-09-16 | 1948-03-30 | Rca Corp | Oscillator for centimeter waves |
US2480462A (en) * | 1944-01-07 | 1949-08-30 | Western Electric Co | Tunable magnetron |
US2564385A (en) * | 1944-03-25 | 1951-08-14 | Csf | Electronic transmitting valve of great power for ultra short waves |
Also Published As
Publication number | Publication date |
---|---|
CH266982A (de) | 1950-02-28 |
BE441498A (en, 2012) | |
GB534696A (en) | 1941-03-14 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US2242275A (en) | Electrical translating system and method | |
US2566087A (en) | Tube of the magnetron type for ultra-short waves | |
US2306860A (en) | Electron discharge device for very high frequencies | |
US2419172A (en) | Electron discharge device having coupled coaxial line resonators | |
GB555162A (en) | Electron beam discharge apparatus incorporating resonant chamber circuits | |
GB578655A (en) | Improvements in or relating to high frequency electron discharge systems | |
US2445811A (en) | High-frequency tube structure | |
US2497831A (en) | Electron discharge device employing cavity resonators | |
US2445282A (en) | Tuning arrangement for cavity resonators | |
US2548808A (en) | Continuous-strip anode for magnetrons | |
US2617961A (en) | Electron tube for very high frequencies | |
US2496500A (en) | Electron discharge device | |
US2407708A (en) | Electron discharge device | |
US2411535A (en) | High-frequency electron discharge apparatus | |
US2404078A (en) | Electron discharge device | |
US2844756A (en) | Electron discharge device with resonator | |
US3248597A (en) | Multiple-beam klystron apparatus with periodic alternate capacitance loaded waveguide | |
US2462869A (en) | Electron discharge device | |
US2222898A (en) | High-frequency apparatus | |
US3046443A (en) | Traveling wave tubes | |
US2227376A (en) | Electrical converter | |
US2438954A (en) | Electronic oscillator of the cavity resonator type | |
US2428779A (en) | Ultra high frequency electronic device | |
US2415749A (en) | Electron discharge device with beam deflecting resonator | |
GB483839A (en) | Improvements in or relating to magnetron electron discharge devices and arrangementsincorporating the same |