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US4004180A
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Traveling wave tube with rectangular coupling waveguides
Assignee: Siemens AG
•
Filing: 1975-06-09
•
Granted: 1977-01-18
•
Expires: 1995-06-09
Abstract
Abstract A broad-band, low-reflection energy coupling or decoupling with a coupled cavity line in a traveling wave tube, particularly high-efficiency traveling field tubes, in which a rectangular hollow conductor is not loaded, and has the opposed walls thereof, of minimum spacing and greatest width, tapering in a direction toward the delay line, with the spacing between such walls at the delay line being approximately that between adjacent transverse walls defining respective cells of the delay line, an inductive shield being provided within the hollow conductor and spaced from the line axis, the coupling opening at the hollow conductor having an open angle larger than the corresponding angle of the coupling openings in the transverse walls of adjacent line cells.
Inventors
- 👤 Franz Gross
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-11-04 16:01
CPC Classifications
H; H01; H01J; H01J23/00; H01J23/36
Claims Analysis
Total Claims: 10
Claim 1
Independent Claim
412 words
In a traveling wave, particularly high-efficiency traveling field tubes having a magnetic system for the bundled guidance of an electron beam, which system surrounds a delay line comprising line cells arranged one behind the other, separated from one another by transverse walls, each of which is provided with an opening therein for the passage of the electron beam, and a coupling opening therein extending substantially in circumferential direction, with the delay line coupled, at least at one of its frontal sides with a rectangular hollow conductor whose broad side, adjacent the longitudinal axis of the delay line (line axis), extends perpendicular thereto, and which conducts at a right angle with respect to the line axis, the combination of the hollow rectangular conductor, preferably employed in connection with a spatial periodic permanent magnet system (PPM System), without loading, which has the opposite transverse walls of minimum spacing and greatest width tapering in a direction toward the delay line, with the spacing between such walls at the delay line being approximately that between adjacent transverse walls defining the respective cells, the opposite longitudinal side walls of maximum spacing and least width having opposed, inwardly directed projections forming a shield, the transverse wall of said conductor adjacent said delay line having a coupling opening therein whose open angle, with respect to the line axis is larger than the corresponding angle of the coupling openings in the transverse walls of adjacent line cells, and having the following dimensions: ______________________________________
0.1 λ.sub.o
< a < 0.15 λ.sub.o
0.07 λ.sub.o
< b < 0.12 λ.sub.o
0.22 λ.sub.o
< c < 0.3 λ.sub.o
0.04 λ.sub.o
< d < 0.07 λ.sub.o
0.22 λ.sub.o
< e < 0.3 λ.sub.o
α
< α.sub.1
< 1.2 α
______________________________________ in which a = thickness of the shield projections b = width of the shield projections c = the distance between the end wall of the hollow conductor and the remote wall of the shield projections d = the distance between the shield projections and the coupling opening, the corner points of the arcuate shaped coupling opening remote from the line axis e = the distance between the line axis and the remote edge of the coupling opening α 1 = the open angle of the coupling opening at the hollow conductor α = the open angle of the remaining coupling openings in the cell walls λ o = the wavelength and free space corresponding to the mean operational frequency of the traveling field tube.
Claim 2
Dependent Claim
412 words
In a traveling wave, particularly high-efficiency traveling field tubes having a magnetic system for the bundled guidance of an electron beam, which system surrounds a delay line comprising line cells arranged one behind the other, separated from one another by transverse walls, each of which is provided with an opening therein for the passage of the electron beam, and a coupling opening therein extending substantially in circumferential direction, with the delay line coupled, at least at one of its frontal sides with a rectangular hollow conductor whose broad side, adjacent the longitudinal axis of the delay line (line axis), extends perpendicular thereto, and which conducts at a right angle with respect to the line axis, the combination of the hollow rectangular conductor, preferably employed in connection with a spatial periodic permanent magnet system (PPM System), without loading, which has the opposite transverse walls of minimum spacing and greatest width tapering in a direction toward the delay line, with the spacing between such walls at the delay line being approximately that between adjacent transverse walls defining the respective cells, the opposite longitudinal side walls of maximum spacing and least width having opposed, inwardly directed projections forming a shield, the transverse wall of said conductor adjacent said delay line having a coupling opening therein whose open angle, with respect to the line axis is larger than the corresponding angle of the coupling openings in the transverse walls of adjacent line cells, and having the following dimensions: ______________________________________
0.1 λ.sub.o
< a < 0.15 λ.sub.o
0.07 λ.sub.o
< b < 0.12 λ.sub.o
0.22 λ.sub.o
< c < 0.3 λ.sub.o
0.04 λ.sub.o
< d < 0.07 λ.sub.o
0.22 λ.sub.o
< e < 0.3 λ.sub.o
α
< α.sub.1
< 1.2 α
______________________________________ in which a = thickness of the shield projections b = width of the shield projections c = the distance between the end wall of the hollow conductor and the remote wall of the shield projections d = the distance between the shield projections and the coupling opening, the corner points of the arcuate shaped coupling opening remote from the line axis e = the distance between the line axis and the remote edge of the coupling opening α 1 = the open angle of the coupling opening at the hollow conductor α = the open angle of the remaining coupling openings in the cell walls λ o = the wavelength and free space corresponding to the mean operational frequency of the traveling field tube.
Claim 3
Dependent Claim
68 words
A traveling field tube according to claim 1, having the following dimensions: ______________________________________
0.115 λ.sub.o
< a < 0.135 λ.sub.o
0.085 λ.sub.o
< b < 0.105 λ.sub.o
0.24 λ.sub.o
< c < 0.28 λ.sub.o
0.05 λ.sub.o
< d < 0.06 λ.sub.o
0.24 λ.sub.o
< e < 0.28 λ.sub.o
1.05 α
< α.sub.1
< 1.5 α
______________________________________
-3. A traveling field tube according to claim 1, wherein the coupling
Claim 4
Dependent Claim
179 words
openings have an arcuate configuration. 4. A traveling field tube according to claim 3, having the following dimensions: ______________________________________
0.1 λ.sub.o
< a < 0.15 λ.sub.o
0.07 λ.sub.o
< b < 0.12 λ.sub.o
0.22 λ.sub.o
< c < 0.3 λ.sub.o
0.04 λ.sub.o
< d < 0.07 λ.sub.o
0.22 λ.sub.o
< e < 0.3 λ.sub.o
α
< α.sub.1
< 1.2 α
______________________________________ in which a = thickness of the shield projections b = width of the shield projections c = the distance between the end wall of the hollow conductor and the remote wall of the shield projections d = the distance between the shield projections and the coupling opening, the corner points of the arcuate shaped coupling opening remote from the line axis e = the distance between the line axis and the remote edge of the coupling opening α 1 = the open angle of the coupling opening at the hollow conductor α = the open angle of the remaining coupling openings in the cell walls λ o = the wavelength and free space corresponding to the mean
Claim 5
Dependent Claim
76 words
operational frequency of the traveling field tube. 5. A traveling field tube according to claim 4, having the following dimensions: ______________________________________
0.115 λ.sub.o
< a < 0.135 λ.sub.o
0.085 λ.sub.o
< b < 0.105 λ.sub.o
0.24 λ.sub.o
< c < 0.28 λ.sub.o
0.05 λ.sub.o
< d < 0.06 λ.sub.o
0.24 λ.sub.o
< e < 0.28 λ.sub.o
1.05 α
< α.sub.1
< 1.15 α
______________________________________
-6. A traveling field tube according to claim 5, wherein the coupling
Claim 6
Dependent Claim
21 words
openings have an arcuate configuration. 7. A traveling field tube according to claim 1, wherein the coupling openings have an arcuate
Claim 7
Dependent Claim
34 words
configuration. 8. A traveling field tube according to claim 1, wherein the rectangular hollow conductor is terminated by an end wall having a recess therein, which is generally aligned in line-axial direction with the
Claim 8
Dependent Claim
46 words
edges, of coupling openings, remote from the line axis. 9. A traveling field tube according to claim 3, wherein the rectangular hollow conductor is terminated by an end wall having a portion of arcuate configuration, which is aligned in line-axial direction with the edges, of coupling
Claim 9
Dependent Claim
180 words
openings, remote from the line axis. 10. A traveling field tube according to claim 9, having the following dimensions: ______________________________________
0.1 λ.sub.o
< a < 0.15 λ.sub.o
0.07 λ.sub.o
< b < 0.12 λ.sub.o
0.22 λ.sub.o
< c < 0.3 λ.sub.o
0.04 λ.sub.o
< d < 0.07 λ.sub.o
0.22 λ.sub.o
< e < 0.3 λ.sub.o
α
< α.sub.1
< 1.2 α
______________________________________ in which a = thickness of the shield projections b = width of the shield projections c = the distance between the end wall of the hollow conductor and the corresponding wall of the shield projections d = the distance between the shield projections and the coupling opening, the corner points of the arcuate shaped coupling opening remote from the line axis e = the distance between the line axis and the remote edge of the coupling opening α 1 = the open angle of the coupling opening at the hollow conductor α = the open angle of the remaining coupling openings in the cell walls λ o = the wavelength and free space corresponding to the mean
Claim 10
Dependent Claim
64 words
operational frequency of the traveling field tube. 11. A traveling field tube according to claim 10, having the following dimensions: ______________________________________
0.115 λ.sub.o
< a < 0.135 λ.sub.o
0.085 λ.sub.o
< b < 0.105 λ.sub.o
0.24 λ.sub.o
< c < 0.28 λ.sub.o
0.05 λ.sub.o
< d < 0.06 λ.sub.o
0.24 λ.sub.o
< e < 0.28 λ.sub.o
1.05 α
< α.sub.1
< 1.15 α
______________________________________
References Cited (Backward Citations)
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US2936395A
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US2966610A
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US3157814A
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US3532926A
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US3668460A
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USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1980-01-18 | 1980-07-19 | 1981-01-18 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1984-01-18 | 1984-07-19 | 1985-01-18 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1988-01-18 | 1988-07-19 | 1989-01-18 | $7700.00 | Window Closed / Lapsed |