US3599032A - Crossed-fields traveling wave tubes - Google Patents

Crossed-fields traveling wave tubes Download PDF

Info

Publication number
US3599032A
US3599032A US838595A US3599032DA US3599032A US 3599032 A US3599032 A US 3599032A US 838595 A US838595 A US 838595A US 3599032D A US3599032D A US 3599032DA US 3599032 A US3599032 A US 3599032A
Authority
US
United States
Prior art keywords
pole pieces
tube
magnetic
crossed
delay line
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
Application number
US838595A
Inventor
Pierre Nicodeme
Walter Sobotka
Roland Valat
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Thales SA
Original Assignee
Thomson CSF SA
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Thomson CSF SA filed Critical Thomson CSF SA
Application granted granted Critical
Publication of US3599032A publication Critical patent/US3599032A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/02Electrodes; Magnetic control means; Screens
    • H01J23/10Magnet systems for directing or deflecting the discharge along a desired path, e.g. a spiral path

Definitions

  • the present invention relates to crossed field travelling wave tubes.
  • the beam is propagated between a delay line and an electrode generally called sole, respectively placed at positive and negative potentials in relation to the cathode and a uniform magnetic field is provided in the space where the beam propagates, perpendicularly to the direction of propagation thereof and perpendicularly to the electric field.
  • a travelling wave tube with crossed electric and magnetic fields comprising an envelope and within said envelope, a delay line and a sole electrode bounding the space wherein the electron beam is propagated, and pole pieces positioned along said space for providing a magnetic field therein, said envelope comprising along each of said pole pieces a magnetic window for allowing the association of said pole pieces with a magnetic circuit.
  • FIG. I is a perspective exploded view of a crossed-field tube in accordance with the invention.
  • FIGS. 2 and 3 are schematic sectional views of details of a tube in accordance with the invention.
  • the tube shown in FIG. 1 is built up from three portions (1 (2) and (3). These three portions are assembled one upon the other, in a manner which will be indicated hereinafter.
  • the portion (1) comprises a base I which can be cut in a piece of metal and has a stepped profile with a central part 1a and two shoulders lb and 1c, resting on a flange 1d.
  • the base 1 carries the delay line 2 of any suitable design.
  • the base 1 and the delay line 2, both being made of metal, are insulated from one another by a layer of glucine, for example, which is not visible in the figure because of the scale on which it is drawn.
  • the two pole pieces 3 and 4 are assembled by means of respective screws v and v.
  • pole pieces 3 and 4 there are fixed distance pieces of insulating material, such as alumina for example, two for each pole piece in the example of FIG. 1, namely the distance pieces 5, 6, 7 and 8.
  • the screws 9, 10, 11 and 12 secure these distance pieces to the pole pieces.
  • the electron beam passes through the tube from the left to the right, above the delay line 2 and between the pole pieces 3 and 4.
  • the end 14 of the central portion 1a, where the electron beam emerges, has a curved profile.
  • the base is connected to a circulatory fluid cooling system, through connections which have not been shown.
  • the tube has a coupling for collecting the input signal; the power is picked up at the output by an antenna 13.
  • the portion (2) of FIG. 1 shows the sole of the tube. It is essentially formed by a rectangular-section body 21 to which two T-shaped clamps 22 and 23 are fixed by the respective screws 24 and 25.
  • the bars of the Tees are perpendicular to the body 21.
  • Each contains two holes I, and 1 or 1 and t disposed symmetrically with respect to the leg of the T t, is not visible.
  • the body 21 is terminated at its right-hand end in a raised portion 26 shaped to match the portion 14 of FIG. (1) and, at its left-hand end, where the beam enters, is terminated in a wedge 27.
  • a member 28, inclined in relation to the body 21 and attached both to said body and to the T 22 is designed to carry the electron-gun.
  • FIG. 1 perspectively illustrates, the cover 30 of the tube, a portion of the cover having been cut away.
  • the cover 30 has a flange 31.
  • the cover 30 has a vacuum connection 36 and a cooling connection 37 and 38. 1
  • the sole section 20 is offered -up-above the base 1, with the face opposite that carrying the T members 22 and 23, facing the base, the holes t and z being opposite the screws 11 and 9 and holes t and t opposite the screws 12 and 10, respectively. Then, the sole section 20 is lowered until the bar of the T 22 rests on the distance pieces 5 and 7 and the bar of the T 23 rests on the distance pieces 6 and 8. After adjustment of the position of the sole section (the holes 1,, t t t have slightly larger diameters than those of the screws 9, 10, ll, 12) it is locked on the distance pieces by nuts.
  • the cover 30 is fitted on the flange 1d, the windows 34 being applied against the pole pieces 3 and 4 respectively.
  • the cover is welded to the base by a weld extending around the periphery of the flange 1d of the base 1, for example by electron bombardment or any other suitable technique.
  • the crossed-field tube of the invention offers numerous advantages over the prior art, namely:
  • the structure is very compact, as may be seen from the foregoing description;
  • the various elements of the tube can be assembled together and their positions adjusted in relation to one another with great ease in particular in so far as the mutual position of the sole and the delay line is concerned, due in particular to the insulating distance pieces mounted on the pole pieces;
  • the cover is a one-piece component which does not have to satisfy any particular accuracy conditions, except that the magnetic windows must be located exactly in front of the pole pieces located inside the tube.
  • FIG. 2 schematically illustrates, in section, the arrangement of the magnetic circuit in relation to the cover and the base, in a tube in accordance with the invention.
  • e represents the clearance in question
  • A the magnets.
  • the electron collector is in the leakage field of the magnetic circuit in order to be able to exploit this effect to lessen the impact of the electron beam the collector.
  • the collector 39 which is an integral part of the cover but, being inside it, is not visible in the FIG. ll (3), receives the beam after the latter has passed between the two profiled members 14 FIG. I (1) and 26 FIG. ll (2). It has the form shown schematically in FIG. 3.
  • a uniform magnetic field B is produced by the magnets A, and is directed towards the rear in FIG. 3, normally to the electric field E.
  • the induction B which exists over the full length of the pole pieces, such as 3, also extends towards the profiled end 14 of the base 1 and 26 of the sole 20, and towards the collector 39.
  • the invention is not limited to the embodiments described and shown which has been given solely by way of example.
  • the example described is concerned with a linear tube in which the beam is propagated along a linear trajectory between a sole and a delay line which are planar and parallel to each other.
  • the invention is equally applicable to circular tubes of the kind produced by turning this structure into a cylinder the axis of which is perpendicular to the direction of propagation of the beam.
  • a travelling wave tube with crossed electric and magnetic fields comprising:
  • a tube as claimed in claim 1 comprising a base member carrying said delay line and said pole pieces, a sole supported by said pole pieces and a cover member welded to said base member and wherein said magnetic windows are formed.

Landscapes

  • Microwave Tubes (AREA)
  • Particle Accelerators (AREA)

Abstract

A crossed fields traveling wave tube wherein the pole pieces providing the magnetic field are mounted along the delay line, inside the tube, and magnetic windows are formed in the tube envelope for associating the pole pieces with the magnetic circuit of the tube.

Description

United States Patent 72] Inventors Pierre Nicodeme;
Walter Sobotka; Roland Valat, all of Paris, France [211 Appl. No 838,595
[22] Filed July 2, 1969 [45] Patented Aug. 10, I971 [73 I Assignee Thomson-CS! [32] Priority July 16, 1968 [33] France [541 C ROSSED-F [ELDS TRAVELING WAVE TUBES 3 Claims, 3 Drawing Figs.
52 11.5.0! sis/3.5, 31515.35.315/39.71,313/l60 s1 lnt.Cl ..l-l0lj25/34 [501 Field oiSearch 315/35, 3.6, 39.3,5.35,39.71
[56] References Cited UNITED STATES PATENTS 7 3,027,487 3/1962 Dench 1. 315/393 3,346,766 10/1967 Feinstein 315/3971 3,376,466 4/1968 Gerard 315/3971 Primary Examiner--Herman Karl Saalbach Assistant Examiner-Saxfield Chatmon, .lr. AnorneyCushman, Darby & Cushman ABSTRACT: A crossed fields traveling wave tube wherein the pole pieces providing the magnetic field are mounted along the delay line, inside the tube, and magnetic windows are formed in the tube envelope for associating the pole pieces with the magnetic circuit of the tube.
PATENTEU AUBIOIQ?! 3,599,032
' sum 1 BF 2 CROSSED-FIELDS TRAVELING WAVE TUBES The present invention relates to crossed field travelling wave tubes.
In such tubes the beam is propagated between a delay line and an electrode generally called sole, respectively placed at positive and negative potentials in relation to the cathode and a uniform magnetic field is provided in the space where the beam propagates, perpendicularly to the direction of propagation thereof and perpendicularly to the electric field.
Certain difficulties have been so far experienced in assembling the various components of such tubes with the requisite degree of precision.
It is an object of this invention to overcome such difficulties.
According to the invention there is provided a travelling wave tube with crossed electric and magnetic fields, comprising an envelope and within said envelope, a delay line and a sole electrode bounding the space wherein the electron beam is propagated, and pole pieces positioned along said space for providing a magnetic field therein, said envelope comprising along each of said pole pieces a magnetic window for allowing the association of said pole pieces with a magnetic circuit.
For a better understanding of the invention and to show how the same may be carried into effect, reference will be made to the drawing accompanying the ensuing description and in which:
FIG. I is a perspective exploded view of a crossed-field tube in accordance with the invention; and
FIGS. 2 and 3 are schematic sectional views of details of a tube in accordance with the invention.
In all the figures similar reference numbers designate similar elements.
The tube shown in FIG. 1 is built up from three portions (1 (2) and (3). These three portions are assembled one upon the other, in a manner which will be indicated hereinafter.
The portion (1) comprises a base I which can be cut in a piece of metal and has a stepped profile with a central part 1a and two shoulders lb and 1c, resting on a flange 1d. The base 1 carries the delay line 2 of any suitable design. The base 1 and the delay line 2, both being made of metal, are insulated from one another by a layer of glucine, for example, which is not visible in the figure because of the scale on which it is drawn. On the shoulders lb and 1c, the two pole pieces 3 and 4 are assembled by means of respective screws v and v.
Upon the pole pieces 3 and 4, there are fixed distance pieces of insulating material, such as alumina for example, two for each pole piece in the example of FIG. 1, namely the distance pieces 5, 6, 7 and 8. The screws 9, 10, 11 and 12 secure these distance pieces to the pole pieces.
In operation, the electron beam passes through the tube from the left to the right, above the delay line 2 and between the pole pieces 3 and 4. The end 14 of the central portion 1a, where the electron beam emerges, has a curved profile.
In operation, the base is connected to a circulatory fluid cooling system, through connections which have not been shown.
The tube has a coupling for collecting the input signal; the power is picked up at the output by an antenna 13.
The portion (2) of FIG. 1 shows the sole of the tube. It is essentially formed by a rectangular-section body 21 to which two T- shaped clamps 22 and 23 are fixed by the respective screws 24 and 25. The bars of the Tees are perpendicular to the body 21. Each contains two holes I, and 1 or 1 and t disposed symmetrically with respect to the leg of the T t, is not visible.
The body 21 is terminated at its right-hand end in a raised portion 26 shaped to match the portion 14 of FIG. (1) and, at its left-hand end, where the beam enters, is terminated in a wedge 27. A member 28, inclined in relation to the body 21 and attached both to said body and to the T 22 is designed to carry the electron-gun.
The portion (3) of FIG. 1 perspectively illustrates, the cover 30 of the tube, a portion of the cover having been cut away. The cover 30 has a flange 31. On the side faces, 32 and 33 of the cover 30, two windows 34 and 34' ofsoft iron or another suitable ferromagnetic material, are provided.
The cover 30 has a vacuum connection 36 and a cooling connection 37 and 38. 1
The three portions are assembled one above the other in the following manner:
The sole section 20 is offered -up-above the base 1, with the face opposite that carrying the T members 22 and 23, facing the base, the holes t and z being opposite the screws 11 and 9 and holes t and t opposite the screws 12 and 10, respectively. Then, the sole section 20 is lowered until the bar of the T 22 rests on the distance pieces 5 and 7 and the bar of the T 23 rests on the distance pieces 6 and 8. After adjustment of the position of the sole section (the holes 1,, t t t have slightly larger diameters than those of the screws 9, 10, ll, 12) it is locked on the distance pieces by nuts.
After the fitting of the electron-gun, on the support 28, the cover 30 is fitted on the flange 1d, the windows 34 being applied against the pole pieces 3 and 4 respectively.
The cover is welded to the base by a weld extending around the periphery of the flange 1d of the base 1, for example by electron bombardment or any other suitable technique.
The crossed-field tube of the invention offers numerous advantages over the prior art, namely:
The structure is very compact, as may be seen from the foregoing description;
The various elements of the tube can be assembled together and their positions adjusted in relation to one another with great ease in particular in so far as the mutual position of the sole and the delay line is concerned, due in particular to the insulating distance pieces mounted on the pole pieces;
In so far as the manufacture of the cover is concerned, it is a one-piece component which does not have to satisfy any particular accuracy conditions, except that the magnetic windows must be located exactly in front of the pole pieces located inside the tube.
It should be pointed out that even if there is a small clearance between these components once they are assembled, this clearance will be taken up by deformation of the cover while evacuated. FIG. 2 schematically illustrates, in section, the arrangement of the magnetic circuit in relation to the cover and the base, in a tube in accordance with the invention. In this figure, e represents the clearance in question, and A the magnets.
In the tubes in accordance with the invention, it is arranged that the electron collector is in the leakage field of the magnetic circuit in order to be able to exploit this effect to lessen the impact of the electron beam the collector. The collector 39, which is an integral part of the cover but, being inside it, is not visible in the FIG. ll (3), receives the beam after the latter has passed between the two profiled members 14 FIG. I (1) and 26 FIG. ll (2). It has the form shown schematically in FIG. 3.
A uniform magnetic field B is produced by the magnets A, and is directed towards the rear in FIG. 3, normally to the electric field E.
The induction B, which exists over the full length of the pole pieces, such as 3, also extends towards the profiled end 14 of the base 1 and 26 of the sole 20, and towards the collector 39.
Of course the invention is not limited to the embodiments described and shown which has been given solely by way of example. Thus, the example described is concerned with a linear tube in which the beam is propagated along a linear trajectory between a sole and a delay line which are planar and parallel to each other. Obviousiy the invention is equally applicable to circular tubes of the kind produced by turning this structure into a cylinder the axis of which is perpendicular to the direction of propagation of the beam.
We claim:
1. A travelling wave tube with crossed electric and magnetic fields, comprising:
2. A tube as claimed in claim 1, wherein the electron collector is located within the field provided by said pole pieces.
3. A tube as claimed in claim 1 comprising a base member carrying said delay line and said pole pieces, a sole supported by said pole pieces and a cover member welded to said base member and wherein said magnetic windows are formed.

Claims (3)

1. A travelling wave tube with crossed electric and magnetic fields, comprising: a nonmagnetic envelope and within said envelope, pole pieces, a delay line and a sole electrode bounding the space wherein an electron beam is propagated, said pole pieces being positioned along said space, said envelope comprising along each of said pole pieces a magnetic window of magnetically permeable material for magnetically coupling said pole pieces with an external magnetic circuit.
2. A tube as claimed in claim 1, wherein the electron collector is located within the field provided by said pole pieces.
3. A tube as claimed in claim 1 comprising a base member carrying said delay line and said pole pieces, a sole supported by said pole pieces and a cover member welded to said base member and wherein said magnetic windows are formed.
US838595A 1968-07-16 1969-07-02 Crossed-fields traveling wave tubes Expired - Lifetime US3599032A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
FR159315 1968-07-16

Publications (1)

Publication Number Publication Date
US3599032A true US3599032A (en) 1971-08-10

Family

ID=8652612

Family Applications (1)

Application Number Title Priority Date Filing Date
US838595A Expired - Lifetime US3599032A (en) 1968-07-16 1969-07-02 Crossed-fields traveling wave tubes

Country Status (4)

Country Link
US (1) US3599032A (en)
DE (1) DE1935790A1 (en)
FR (1) FR1603150A (en)
GB (1) GB1220649A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2000079650A1 (en) * 1999-06-22 2000-12-28 Thomson Tubes Electroniques Compact transmission module

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3027487A (en) * 1953-09-24 1962-03-27 Raytheon Co Electron discharge devices of the traveling wave type
US3346766A (en) * 1964-03-13 1967-10-10 Sfd Lab Inc Microwave cold cathode magnetron with internal magnet
US3376466A (en) * 1964-12-01 1968-04-02 Westinghouse Electric Corp Coaxial magnetron having magnetic return path through the cylindrical anode

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3027487A (en) * 1953-09-24 1962-03-27 Raytheon Co Electron discharge devices of the traveling wave type
US3346766A (en) * 1964-03-13 1967-10-10 Sfd Lab Inc Microwave cold cathode magnetron with internal magnet
US3376466A (en) * 1964-12-01 1968-04-02 Westinghouse Electric Corp Coaxial magnetron having magnetic return path through the cylindrical anode

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2000079650A1 (en) * 1999-06-22 2000-12-28 Thomson Tubes Electroniques Compact transmission module
FR2795559A1 (en) * 1999-06-22 2000-12-29 Thomson Tubes Electroniques Telecommunications high frequency transmitter module having frequency tube/amplifier structure having integrated radiation source/outer antenna reflector.

Also Published As

Publication number Publication date
GB1220649A (en) 1971-01-27
FR1603150A (en) 1971-03-22
DE1935790A1 (en) 1970-01-29

Similar Documents

Publication Publication Date Title
SE325965B (en)
US3781592A (en) Radial magnetized magnet
US3450930A (en) Permanent magnet focused linear beam tube employing a compensating magnet structure between the main magnet and the beam collector
US3394282A (en) Electron beam discharge with periodic permanent magnet focussing
JPH07118271B2 (en) Klystron output circuit and klystron including the output circuit
CA1099817A (en) Helix traveling wave tubes with resonant loss
US2701321A (en) Adjustable magnetic focusing system for beam tubes
JPS6256621B2 (en)
US3599032A (en) Crossed-fields traveling wave tubes
US3832596A (en) Magnetic structure for focusing of linear beams
US4399389A (en) Travelling wave tube with coupled cavities and focusing by alternating permanent magnets and amplifying system comprising such a tube
US5332948A (en) X-z geometry periodic permanent magnet focusing system
GB1512186A (en) Permanent magnet structure for crossedfield tubes
US3753031A (en) Output devices for microwave tubes such as klystrons, and klystrons incorporating such output devices
US3896329A (en) Permanent magnet beam focus structure for linear beam tubes
US3283200A (en) High frequency electron discharge device having improved permanent magnetic focusing
US3210593A (en) Method and apparatus for the broadbanding of power type velocity modulation electron discharge devices by interaction gap spacing
US3032677A (en) Traveling wave tubes
US3924152A (en) Electron beam amplifier tube with mismatched circuit sever
US3084277A (en) Traveling wave tubes
US3475644A (en) Linear beam tube employing a shielded beam focus solenoid having a reentrant cathode pole piece
US3417280A (en) Traveling wave time delay device having a magnetic field in the drift region different from that in the delay line regions
US3886384A (en) Collector electrode
US2787728A (en) Electron discharge device with toroidal permanent magnet
US3141992A (en) Focusing system for omicron-type travelling wave tubes