US2620458A - Microwave amplifier - Google Patents
Microwave amplifier Download PDFInfo
- Publication number
- US2620458A US2620458A US84699A US8469949A US2620458A US 2620458 A US2620458 A US 2620458A US 84699 A US84699 A US 84699A US 8469949 A US8469949 A US 8469949A US 2620458 A US2620458 A US 2620458A
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- waveguide
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/50—Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field
- H01J25/52—Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field with an electron space having a shape that does not prevent any electron from moving completely around the cathode or guide electrode
- H01J25/58—Magnetrons, i.e. tubes with a magnet system producing an H-field crossing the E-field with an electron space having a shape that does not prevent any electron from moving completely around the cathode or guide electrode having a number of resonators; having a composite resonator, e.g. a helix
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- This invention relates to amplifying devices, and more particularly to amplifying devices for electrical energy in the microwave region of the electromagnetic spectrum.
- an amplifying device constructed as aforesaid has certain disadvantages. It is complicated and therefore difficult and expensive to manufacture, and its linear construction requires excessively high accelerating potentials.
- the present invention contemplates the provision of an evacuated envelope in which is; mounted a source of electrons and a helical waveguide, preferably, in the form of a toroid, spaced from and surrounding said source of electrons.
- a magnetic field is established tranverse to the path between said source of electrons and said waveguide, and said waveguide is maintained at a positive potential with respect to said source of electrons.
- the electrons emitted from said source are, by proper relative adjustment of the above-mentioned magnetic and electric fields, caused to travel in paths similar to the electron paths in a conventional multiple cavity magnetron.
- Microwave energy applied to the helical waveguide is thereby-caused to extract energy from these electrons and become amplified.
- Fig. 1 is a longitudinal sectional view taken alon line II of Fig. 2, substantially through the center of a microwave amplifier made in accordance with the principles of the present invention; and 1 Fig. 2 is a transverse sectional view taken along line 2-2 of Fig. 1.
- the numeral H] designates an envelope made of a dielectric material such as glass.
- the envelope is provided with a reentrant press I! in which there is embedded a pair of wire supports l2 which carry at their inner ends a centrally disposed cathode sleeve I3 provided with .a conventional electron emissive coating.
- a cathode heater M has one end thereof electrically connected to the sleeve l3 and the other end thereof passed through the press -I I and electrically connected to one terminal of a source it of heating current. The other terminal of the source It is connected to one of the cathode supports I 2.
- a waveguide structure Spaced from and surrounding the cathode i3 is a waveguide structure it, this structure, preferably, takin the form of a helical wire, the successive turns of which are uniformly spaced from each other, the entire helix being formed into a toroid having a gap l'l between the adjacent ends thereof.
- the spaced ends of the toroid are closed by conducting plates i8 and [9 in order to isolate the input end of the waveguide from the output end thereof, thus eliminating unwanted feedback which might otherwise cause oscillation.
- the waveguide i6 is maintained at a positive potential with respect to the cathode l3 by appropriate connection to a source of voltage 20.
- Another coaxial transmission line 25, coupled to any preferred utilization circuit 26, has its outer conductor 21 electrically connected to the last turn of the helical waveguide l6 adjacent the end plate l9, and its central conductor formed into a coupling loop 28 which, like the coupling loop 24, extends into said waveguide.
- a control electrode consisting of a disk 29 from which depends a plurality of spaced pins 30, the control electrode being maintained at a suitable negative potential with respect to the cathode I3 by connecting the same to the adjustable arm of a potentiometer 3
- is returned to the cathode l3.
- the magnitude of the bias will control the width of the beams projected from between adjacent pins 30, thereby enabling greater control over the relative phase between the electron beam and the travelling microwave energy to be amplified.
- the device is completed by providing a coil 34 about the envelope In to establish a magnetic field in the space between the cathode l3 and waveguide IS, in a direction transverse to the electron path therebetween.
- the microwave energy to be amplified is applied to the input end of the waveguide I6 by means of the coupling loop 24.
- the energy is propagated around the waveguide and extracted by the loop 28, the helical form of the waveguide reducing the phase velocity of the energy to a value below the speed of light.
- the electrons emitted by the cathode l3 are caused, under the influence of the electric field between the cathode and the waveguide, and the magnetic field in the space between said cathode and waveguide, to follow paths similar to those taken in a conventional magnetron. In following such paths, the electrons give up their energy to the microwave energy traveling along the waveguide whereby said microwave energy, when extracted at the output end of the waveguide, is amplified.
- An amplifier for microwave energy comprising: an evacuated envelope; a helical waveguide, the turns of which are spaced with respect to each other, mounted in said envelope; a source of electrons mounted in said envelope exteriorly of and in spaced relationship to said waveguide; a control electrode interposed between said electronsource and said waveguide; means for establishing a magnetic field transverse to the path between said electron-source and said waveguide; and microwave input and output means coupled to said waveguide at predetermined points along the length thereof.
- An amplifier for microwave energy comprising: an evacuated envelope; a helical waveguide, the turns of which are spaced with respect to each other, mounted in said envelope and formed into a toroid; a source of electrons mounted in said envelope coaxially with said toroid; a control electrode interposed between said electronsource and said waveguide; means for establishing a magnetic field transverse to the path between said electron-source and said waveguide; and microwave input and output means coupled to said waveguide at predetermined points along the length thereof.
- An amplifier for microwave energy comprising: an evacuated envelope; a source of electrons mounted in said envelope; a helical waveguide, theturns of which are spaced with respect to each other, mounted in said envelope, in spaced relationship to said electron-source; the turns of said helical waveguide having non-arcuate portions facing said electron-source and lying in planes parallel to planes including the longitudinal axis of said electron-source; a control electrode interposed between said electronsource and said waveguide; means for establishing a magnetic field transverse to the path between said electron-source and said waveguide; and microwave input and output means coupled to said waveguide at predetermined points along the length thereof.
- An amplifier for microwave energy comprising: an evacuated envelope; a cylindrical source of electrons mounted in said envelope; a helical waveguide, the turns of which are spaced with respect to each other, mounted in said envelope and formed into a toroid to substantially surround said electron-source, in spaced relationship thereto; the turns of said helical waveguide having non-arcuate portions facing said electron-source and lying in planes parallel to planes including the longitudinal aXis of said electron-source; a cylindrical control electrode interposed between said electronsource and said waveguide, means for establishing a magnetic field transverse to the path between said electron-source and said waveguide; and microwave input and output means coupled to said waveguide at predetermined points along the length thereof,
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- Microwave Amplifiers (AREA)
Description
1366- 1952 P. L. SPENCER MICROWAVE AMPLIFIER Filed March 51, 1949 MICIIPOWAVE ENE/2G V soulzce R m EQW w. A .Y% Y B lNl/ENTOI? w N R m Patented Dec. 2, 1952 UNITED STATES PATENT OFFICE MICROWAVE AMPLIFIER Percy L. Spencer, West Newton, Mass vassigncr Lto Raytheon .Manufacturing Company, Newton, Mass, a corporation of Delaware Application March 31, 1949, Serial No. 84,699
4Claims. 1
This invention relates to amplifying devices, and more particularly to amplifying devices for electrical energy in the microwave region of the electromagnetic spectrum.
It has heretofore been proposed to produce amplification of such energy by propagating the same down an elongated waveguide, and projecting an electron beam along the axis of said waveguide, extracting amplified energy from the end of the waveguide remot from the input. The waveguide in such an arrangement took the form of a helix in order to reduce the linear phase velocity of the energy to be amplified to a point below th speed of light, this condition obviously being necessary in order to enable the electron beam to be accelerated to velocities in excess of said phase velocity, whereby said electron beam could interact with the microwave energy and transfer its own energy thereto. Such an arrangement further included an anode disposed adjacent the output end of the waveguide to collect the spent electron beam, and a magnetic field along the axis of the waveguide to focus the electron beam.
It has been found that an amplifying device constructed as aforesaid has certain disadvantages. It is complicated and therefore difficult and expensive to manufacture, and its linear construction requires excessively high accelerating potentials.
It is, therefore, an object of the present invention to provide a microwave amplifier which is simple in construction and easy and economical to manufacture.
It is a further object of the present invention to provide an amplifying device which is so designed as to require much lower operating voltages than has heretofore been the case.
These, and other objects of the present invention, which will become more apparent as the detailed description thereof progresses, areattained, broadly, in the following manner.
The present invention contemplates the provision of an evacuated envelope in which is; mounted a source of electrons and a helical waveguide, preferably, in the form of a toroid, spaced from and surrounding said source of electrons. A magnetic field is established tranverse to the path between said source of electrons and said waveguide, and said waveguide is maintained at a positive potential with respect to said source of electrons. The electrons emitted from said source are, by proper relative adjustment of the above-mentioned magnetic and electric fields, caused to travel in paths similar to the electron paths in a conventional multiple cavity magnetron. Microwave energy applied to the helical waveguide is thereby-caused to extract energy from these electrons and become amplified.
In the accompanying specification there shall be describechand in the annexed drawing shown, an illustrative embodiment of the amplifying device of the present invention. It is, however, to be clearly understood that the present invention is not to be limited to the exact details of construction herein shown and described for purposes of illustration only, inasmuch as changes therein may be made without the exercise of invention and within the true spirit and scope of the claims hereto appended.
In said drawing:
Fig. 1 is a longitudinal sectional view taken alon line II of Fig. 2, substantially through the center of a microwave amplifier made in accordance with the principles of the present invention; and 1 Fig. 2 is a transverse sectional view taken along line 2-2 of Fig. 1.
Referring now more in detail to the aforesaid illustrative embodiment of the present invention, with particular reference to the drawing illustrating the same, the numeral H] designates an envelope made of a dielectric material such as glass. The envelope is provided with a reentrant press I! in which there is embedded a pair of wire supports l2 which carry at their inner ends a centrally disposed cathode sleeve I3 provided with .a conventional electron emissive coating. A cathode heater M has one end thereof electrically connected to the sleeve l3 and the other end thereof passed through the press -I I and electrically connected to one terminal of a source it of heating current. The other terminal of the source It is connected to one of the cathode supports I 2.
Spaced from and surrounding the cathode i3 is a waveguide structure it, this structure, preferably, takin the form of a helical wire, the succesive turns of which are uniformly spaced from each other, the entire helix being formed into a toroid having a gap l'l between the adjacent ends thereof. The spaced ends of the toroid are closed by conducting plates i8 and [9 in order to isolate the input end of the waveguide from the output end thereof, thus eliminating unwanted feedback which might otherwise cause oscillation. The waveguide i6 is maintained at a positive potential with respect to the cathode l3 by appropriate connection to a source of voltage 20.
A coaxial transmission line 21, coupled to a source 22 of microwave energy to be amplified, has its outer conductor 23 electrically connected to the first turn of the helical waveguide I6 adjacent the end plate 18, and its central conductor formed into a coupling loop 24 which extends into said waveguide.
Another coaxial transmission line 25, coupled to any preferred utilization circuit 26, has its outer conductor 21 electrically connected to the last turn of the helical waveguide l6 adjacent the end plate l9, and its central conductor formed into a coupling loop 28 which, like the coupling loop 24, extends into said waveguide.
While not necessary, there may be disposed in the annular space between the cathode l3 and the waveguide IS a control electrode consisting of a disk 29 from which depends a plurality of spaced pins 30, the control electrode being maintained at a suitable negative potential with respect to the cathode I3 by connecting the same to the adjustable arm of a potentiometer 3|, in turn connected across a source of voltage 32. The positive end of the potentiometer 3| is returned to the cathode l3. The magnitude of the bias will control the width of the beams projected from between adjacent pins 30, thereby enabling greater control over the relative phase between the electron beam and the travelling microwave energy to be amplified.
While not necessary, it is preferred that portions 33 of the turns of the helical waveguide I6, facing the cathode l3 and lying in planes parallel to planes including the longitudinal axis of said cathode, be non-arcuate. V
The device is completed by providing a coil 34 about the envelope In to establish a magnetic field in the space between the cathode l3 and waveguide IS, in a direction transverse to the electron path therebetween.
In operation, the microwave energy to be amplified is applied to the input end of the waveguide I6 by means of the coupling loop 24. The energy is propagated around the waveguide and extracted by the loop 28, the helical form of the waveguide reducing the phase velocity of the energy to a value below the speed of light. The electrons emitted by the cathode l3 are caused, under the influence of the electric field between the cathode and the waveguide, and the magnetic field in the space between said cathode and waveguide, to follow paths similar to those taken in a conventional magnetron. In following such paths, the electrons give up their energy to the microwave energy traveling along the waveguide whereby said microwave energy, when extracted at the output end of the waveguide, is amplified.
This completes the description of the aforesaid illustrative embodiment of the invention. It will be noted from all of the foregoing that the construction herein proposed is such as to simplify manufacturing procedure and assembly and .is such as to require considerably lower accelerating potentials than has heretofore been necessary in operating so-called linear amplifiers.
Other objects and advantages of the device of the present invention will readily occur to those skilled in the art to which the present invention relates.
What is claimed is:
1. An amplifier for microwave energy comprising: an evacuated envelope; a helical waveguide, the turns of which are spaced with respect to each other, mounted in said envelope; a source of electrons mounted in said envelope exteriorly of and in spaced relationship to said waveguide; a control electrode interposed between said electronsource and said waveguide; means for establishing a magnetic field transverse to the path between said electron-source and said waveguide; and microwave input and output means coupled to said waveguide at predetermined points along the length thereof.
2. An amplifier for microwave energy comprising: an evacuated envelope; a helical waveguide, the turns of which are spaced with respect to each other, mounted in said envelope and formed into a toroid; a source of electrons mounted in said envelope coaxially with said toroid; a control electrode interposed between said electronsource and said waveguide; means for establishing a magnetic field transverse to the path between said electron-source and said waveguide; and microwave input and output means coupled to said waveguide at predetermined points along the length thereof.
3. An amplifier for microwave energy comprising: an evacuated envelope; a source of electrons mounted in said envelope; a helical waveguide, theturns of which are spaced with respect to each other, mounted in said envelope, in spaced relationship to said electron-source; the turns of said helical waveguide having non-arcuate portions facing said electron-source and lying in planes parallel to planes including the longitudinal axis of said electron-source; a control electrode interposed between said electronsource and said waveguide; means for establishing a magnetic field transverse to the path between said electron-source and said waveguide; and microwave input and output means coupled to said waveguide at predetermined points along the length thereof.
4. An amplifier for microwave energy comprising: an evacuated envelope; a cylindrical source of electrons mounted in said envelope; a helical waveguide, the turns of which are spaced with respect to each other, mounted in said envelope and formed into a toroid to substantially surround said electron-source, in spaced relationship thereto; the turns of said helical waveguide having non-arcuate portions facing said electron-source and lying in planes parallel to planes including the longitudinal aXis of said electron-source; a cylindrical control electrode interposed between said electronsource and said waveguide, means for establishing a magnetic field transverse to the path between said electron-source and said waveguide; and microwave input and output means coupled to said waveguide at predetermined points along the length thereof,
PERCY L. SPENCER.
REFERENCES CITED The following references are of record in the file of this patent:
UNITED STATES PATENTS Number Name Date 2,300,052 Lindenblad Oct. 27, 1942 2,446,826 McArthur Aug. 10, 1948 2,511,407 Kleen et al June 13, 1950 2,531,972 Doehler et a1. Nov. 28, 1950 2,566,087 Lerbs Aug. 28, 1951 OTHER REFERENCES Article by Kompfner, Proc. I. R. E. for Feb. 1947, pgs. 12 l-l27, inclusive.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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US84699A US2620458A (en) | 1949-03-31 | 1949-03-31 | Microwave amplifier |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
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US84699A US2620458A (en) | 1949-03-31 | 1949-03-31 | Microwave amplifier |
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US2620458A true US2620458A (en) | 1952-12-02 |
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US84699A Expired - Lifetime US2620458A (en) | 1949-03-31 | 1949-03-31 | Microwave amplifier |
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Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2768328A (en) * | 1946-11-05 | 1956-10-23 | Bell Telephone Labor Inc | High frequency electronic device |
US2807744A (en) * | 1951-07-27 | 1957-09-24 | Csf | Travelling wave magnetron tubes |
US2809328A (en) * | 1951-11-08 | 1957-10-08 | Raytheon Mfg Co | Magnetron amplifiers |
US2861212A (en) * | 1951-07-30 | 1958-11-18 | Cie Generale De Elegraphie San | Travelling wave magnetron tube |
US2971121A (en) * | 1951-11-08 | 1961-02-07 | Raytheon Co | Magnetron amplifiers |
US3376463A (en) * | 1964-10-26 | 1968-04-02 | Sfd Lab Inc | Crossed field microwave tube having toroidal helical slow wave structure formed by a plurality of spaced slots |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2300052A (en) * | 1940-05-04 | 1942-10-27 | Rca Corp | Electron discharge device system |
US2446826A (en) * | 1943-04-14 | 1948-08-10 | Gen Electric | Magnetron |
US2511407A (en) * | 1947-01-09 | 1950-06-13 | Csf | Amplifying valve of the progressive wave type |
US2531972A (en) * | 1949-02-12 | 1950-11-28 | Csf | Ultra short wave transmitting tube |
US2566087A (en) * | 1947-06-13 | 1951-08-28 | Csf | Tube of the magnetron type for ultra-short waves |
-
1949
- 1949-03-31 US US84699A patent/US2620458A/en not_active Expired - Lifetime
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2300052A (en) * | 1940-05-04 | 1942-10-27 | Rca Corp | Electron discharge device system |
US2446826A (en) * | 1943-04-14 | 1948-08-10 | Gen Electric | Magnetron |
US2511407A (en) * | 1947-01-09 | 1950-06-13 | Csf | Amplifying valve of the progressive wave type |
US2566087A (en) * | 1947-06-13 | 1951-08-28 | Csf | Tube of the magnetron type for ultra-short waves |
US2531972A (en) * | 1949-02-12 | 1950-11-28 | Csf | Ultra short wave transmitting tube |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2768328A (en) * | 1946-11-05 | 1956-10-23 | Bell Telephone Labor Inc | High frequency electronic device |
US2807744A (en) * | 1951-07-27 | 1957-09-24 | Csf | Travelling wave magnetron tubes |
US2861212A (en) * | 1951-07-30 | 1958-11-18 | Cie Generale De Elegraphie San | Travelling wave magnetron tube |
US2809328A (en) * | 1951-11-08 | 1957-10-08 | Raytheon Mfg Co | Magnetron amplifiers |
US2971121A (en) * | 1951-11-08 | 1961-02-07 | Raytheon Co | Magnetron amplifiers |
US3376463A (en) * | 1964-10-26 | 1968-04-02 | Sfd Lab Inc | Crossed field microwave tube having toroidal helical slow wave structure formed by a plurality of spaced slots |
DE1491469B1 (en) * | 1964-10-26 | 1970-07-30 | Sfd Lab Inc | Microwave tube of the traveling field type that works with crossed static, electric and magnetic fields |
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