US2541195A

US2541195A - Resonator with multiple electrodes

Info

Publication number: US2541195A
Application number: US695025A
Authority: US
Inventors: Arnold E Bowen
Original assignee: Bell Telephone Laboratories Inc
Current assignee: AT&T Corp
Priority date: 1946-09-05
Filing date: 1946-09-05
Publication date: 1951-02-13
Anticipated expiration: 1968-02-13
Also published as: BE473975A; FR947740A

Description

3, 1951 A. E. BOWEN 2,541,195

RESONATOR WITH MULTIPLE ELECTRODES Filed Sept. 5, 1946 INVENTOR By 14.5. BUWf/V ATTORNEY Patented Feb. 13, 1951 RESONATOR WITH MULTIPLE ELECTRODES Arnold E. Bowen, Fair Haven, N. J assignor to Bell Telephone Laboratories, Incorporated, New

York, N. Y., a corporation of New York Continuation of application Serial No. 408,303,

August 26, 1941.

This invention relates to vacuum tubes and more particularly to an anode structure integral with and enclosed by a resonating chamber or substantially non-radiating resonator for electromagnetic waves. The structure of the invention is particularly adapted for, but not limited to, use in a multiple anode magnetron oscillator for generating waves a few centimeters or less in length. n This application is a continuation of my copending application, Serial No. 408,303, filed August 26, 1941, and assigned to the same assignee as the present application, and which is now 'abandoned. In'accordance with the invention, the anode elements are formed in two subassemblles attached respectively to a pair of end members, the latter being fitted into the ends of a tubular casing and arranged so that the respective sets "of anode elements are interleaved. Access to the interior of the structure for purposes of coupling may be had through a slot in the casing or in any other suitable manner. The assembled anode structure may be mounted within an evacuated envelope.

Among the objects of the invention are improvement in frequency stability and increase in .efliciency of oscillation generators as well as greater facility in their construction. The reduction of radiation losses due to the form of structure employed results in an increased ratio of reactanoe to resistance, commonly referred to as the Q of the system. A high value of Q promotes both frequency stability and efficiency.

The type of construction lends itself readily to-tlie use of a large number of anode segments, which is in itself an advantage. It has been found that for a given wave-length and a given ..diameter of anode structure, the larger the num ber of anode segments, the lower are the anode voltage and magnetic field intensity required to maintain oscillations. The reason for this result becomes evident from the following qualitative considerations. Electrons in first passing along *a'path in the vicinity of the gap between two adjacent anode segments are subjected to a sorting action according to the particular phase'of the oscillations during which the individual elec- '1 tron passes the gap. Those electrons which make the passage in unfavorable phase so that they take energy from the high frequency field during the passage are likely to be drawn to and intercepted by th next anode segment, while those making the passage in favorable phase give energy to the field, are repelled by the next adja- I segments.

This application September 5, 1946, Serial No. 695,025

3 Claims. (Cl. 315-40) cent segment and continue their travel in a path which takes them near the following gap between In order to deliver energy to the field during its transit of the region near this next gap, and thus help to sustain the high frequency oscillations, one half period of the oscillation must have elapsed between transits. With 'a.

iven anode diameter, the distance between adjacent gaps is inversely proportional to the nuniber of segments 50 that a smaller electron velocity and hence a smaller anode voltage is required to get the electrons from one gap to the next in one half period. Instead of using this advantage to secure a smaller anode diameter and a correspondingly lower anode voltage, in many cases it may be preferable to employ a reasonably high anode voltage and increase the diameter of the anode structure accordingly. In this way greater ease in fabricating the parts andin their assembly can be had as well as larger output'jof oscillations.

Other objects and features of this invention will be evident from the following detailed description while the scope of the invention is indicated by the appended claims.

In the drawings:

Fig. 1 is a view in perspective and partially in section or broken away, showing a vacuum tube assembly embodying the invention, and Fig. 2 is an exploded view of the anode structure of th tube shown in Fig. 1.

structure indicated generally at I4 and shown in exploded view in Fig. 2. v The rod I3 is conductively and mechanically attached to a tubular casing l5. The casing is countersunk at each end to receive members it and ll,-respectively. The member is has attached to or integrally formed therewith a plurality of spaced cylindrical segments l8 and I9.

Similar segments

20 and 25 are associated with the member I! and when assembled in the casing Hi, the segments 20 and ii are slightly separated from and interleaved with the segments i8 and It. A slot 22 is provided in the casing I 5 to accommodate a coupling conductor 23 which may be formed to make a loop inside'the casing 15. The ends of the conductor 23 may be led out through the envelope l0 rication standpoint.

Magnetizing coils

35 and 36 may be provided to supply an axial magnetomotive force. coaxial with the filament 32 and the anode structure I4.

The casing 15 together with the members It and I! and the

end plates

28 and 29 comprise a. substantially non-radiating resonance chamber which in itself tends to give a high value. of Q. Ohmic losses, further, are reduced by virtue of the large surfaces presented for the flow of high frequency currents; the inner surfaces of the parts being preferably of high electrical conductivity. The casing l5 and the members l6 and; H are also preferably made to have a large thermal capacity and are placed in good thermal contact with each other to assist in cooling the anode. during operation. vohmic losses contributes further to a high value of Q and the improved cooling facilities perthe handling of large amounts of. power. The parts may conveniently be made of metal of, good conductivity, such as copper, which is .readily machined in a lathe and the conductivity ,of the inner surfaces may be increased if desired, by gold or silver plating-or in any other "suitable manner.

The reduction of While four anode segments are represented in the figures, any desired number of segments may be used. It is not necessary that the anode segments be cylindricahand in the case of a large number of segments, it may be particularly desirazble that the segments take the form of wires or rods in which case the anode assembly would be of a squirrel cage type with alternate wires connected to opposite end walls of the cylindrieal resonant cavity. The structure of this sort has. considerable advantages from the fab- In a series of anode structures which have been constructed and successfully operated in .rnagnetron generators, an anode diameter of 0.419 centimeter, an anode length of 0.952 centimeter and an inner diameter of resonants chamber of 1.93 centimeters were employed in each of. four resonators having 2, 4, 8 and 1B anode segments, respectively. The following op- ,erating data were, obtained with the resonators:

in the capacitance due to increase in the numher of gaps is partially compensated by a decrease in the inductance due to parallelling segments. On the other hand the optimum anode voltage and magnetic field decrease rather rapidly with the increase in the number of segments. The advantage of increasing the number of segments is brought out. by a comparison of the values of the product of wave-length and magnetic field intensity, this product falling from a value of 10,300 for a Z-segment anode to a value of 4,300 for a l6-segment anode. With these resonators. efficiencies of power conversion as high as 20 per cent have been found as contrasted with values of 10 to 12 per cent for conventional magnetrons operated in the same wavelength range.

What is claimed is:

I. An oscillatory system comprising a hollow continuous length of conductive cylinder hav ing countersunk ends, first and second annular disc end members, each fitted. into one of said countersunk. ends of said hollow cylinder, a. first plurality of spaced cylindrical segments each ,having one free endand the other end conductively attached to said first annular end memher, the, free end of each segment of said first plurality extending in the direction toward said second annular end member, a second plurality ofcylindrical segments spaced from and interleaved with said first plurality of cylindrical segments, said second plurality of cylindrical segments each having one end free and the other end being conductively attached to said second annular end member, the free end of each. of

said second plurality of cylindrical segments extending in the. direction toward said first annular end, member, said first and second. pluralities' of anode segment all being coaxial with. said hollow conductive cylinder and defining there.- withandwith said first and second annular end members a substantially closed cavity resonator coupled to a central reaction space through the spaces between said interleaved cylindrical segments.

2. An oscillatory system in accordance with claim 1 and; having a cathode mounted within the central reaction space.

3. An oscillatory system in accordance with claim 2 together with a pair of centrally apertured shielding discs mounted coaxially with said hollow cylinder and in opposed relation to the said annular end members and substantially closing the central opening of the respective annular end member, and'cathode leads extending through, the apertures in said shielding discs.

ARNOLD E. BOWEN.

file of this patent:

I Products! 4 No. of Anode ifigfi Wave-length Wave-length Segments Voltage G centimeters and Magnetic H auss Field In'the above series of resonators the wavelength. rises only slowly as the number of segments, is increased. This isbecause the increase UNITED STATES PATENTS Number Name Date 2 ,115,521 Fritz et al. Apr. 26', 1938 2,144,222. Hollmann Jan. 17', 1939 2,145,361 Linder Jan. 31, 1939 i 2,147,143 Braden Feb. 14, 1939 r 2,147,159 Gutton et al. Feb. '14, 1939 2,167,201 Dallenbach July 25, 1939 2,278,210 Morton Mar. 31, 1942 2,409,222 Morton Oct. 15, 1946