Patent Application
20140191657
This application claims priority to and the benefit of Japanese Application No. 2013-000512 filed on 7 Jan. 2013, the disclosure of which is incorporated by reference in its entirety.
The presently disclosed embodiment relates to magnetrons that oscillate microwaves, and particularly to a structure of coaxial magnetrons having an outer cavity outside an anode resonant cavity.
Since magnetrons can oscillate high-power microwaves efficiently in a simple configuration, they have been used in a variety of applications and devices. Among those, examples of devices in which an oscillation frequency needs to be tuned precisely include radars that execute detection by changing a frequency precisely to avoid interference and Linac that puts precisely-tuned microwaves into a narrow band resonator with a high Q factor to apply an accelerating electric field to an electron. Magnetrons used in such applications and devices need to have a mechanism that can mechanically change frequencies. Coaxial magnetrons are put into practical use as one option.
The pole piece 7b is provided as a part of an upper structure 12, and the upper structure 12 is joined to the cylindrical side body 6, thus assembling the magnetron. The anode cylinder 3 is joined to the input side structure 14 but not to the upper structure 12, and is cantilevered.
In this configuration, the resonance frequency and oscillation frequency of the magnetron can be adjusted by moving the position of the tuning piston 8 from outside and changing the reactance of the outer cavity 60. As a result, the oscillation frequency of the magnetron can be changed precisely, and tuned to a frequency required for an application or a device. The magnetron can oscillate high-power microwaves, and can be designed to generate high-power microwaves with the peak output of several MW and the average output of several kW.
While a high oscillation efficiency can be achieved in such an exceedingly high-power magnetron, it is important to design a cooling function for heat generated by anode dissipation. In addition, since the vanes 2 are made of a thin metal finely, when an overheat happened, there was a case where deformation was caused, thereby affecting oscillation characteristics or melting deformation was caused, thereby deteriorating the function of the magnetron. Therefore, for high-power magnetrons, there was a proposal of a design such that a coolant is run in the vicinity of an anode structure for cooling. In the case of
JP 2004-134160 A describes a magnetron using a coolant, though it is not a coaxial magnetron, In this example, a cooling jacket is provided along the circumferential direction of the outer wall surface of an anode cylinder to which vanes are joined, and a coolant is run through the cooling jacket. This configuration enables heat generated around the vanes by anode dissipation to be exchanged with the coolant efficiently, which leads to the decrease of the temperature of the anode including the vanes.
However, as can be seen from the configurations shown in JP 10-269953 A and JP 10-302655 A, the coaxial magnetrons as shown in
Meanwhile, in the coaxial magnetrons, the anode cylinder 3 is joined to only the input side structure 14 and is cantilevered as described above. Therefore, there was a problem that heat release to the outside from the anode cylinder 3 cannot be carried out satisfactorily. In other words, in order to strictly secure the distance between the opposing pole pieces 7a and 7b, as shown in
In the drawings of the above-mentioned JP 10-269953 A and other references, an anode cylinder is in contact with upper and lower pole pieces. However, one end of the anode cylinder needs to be free when the distance between the pole pieces is set precisely, as described above.
To reduce heat resistance in the anode part and facilitate cooling, enlarging the cross-sectional area of the anode components such as the vanes 2 and the anode cylinder 3 can be considered. However, this affects a high frequency characteristic, and thus there is a limit in doing so. For example, there occurs a problem that the degree of coupling with the outer cavity 60 through the slot 4 becomes inadequate if the anode cylinder 3 is thickened. Therefore, the peak oscillation output generated by the magnetron is limited due to the limit of heat release of the anode part.
For the above reasons, to achieve heat release as much as possible, it is proposed that the cooling passage 11 is provided at the base of the anode cylinder 3 on the side of the input side structure 14 to run a coolant therethrough for cooling, as shown in
The presently disclosed embodiment has been made in the light of the above-mentioned problems, and an object of the presently disclosed embodiment is to provide a coaxial magnetron that can facilitate heat release from the anode part, improve an overall cooling efficiency, and enhance a peak oscillation output.
To achieve the above object, a first aspect of the coaxial magnetron of the presently disclosed embodiment comprises a cathode, an anode having an anode cylinder and vanes for forming an anode resonant cavity around the cathode, a cylindrical side body forming an outer cavity coaxial with the anode resonant cavity around the anode cylinder, a pair of end sealing structures joined to both ends of the cylindrical side body, and an input part connected to the cathode through one of the end sealing structures, wherein one end of the anode cylinder is joined to one of the end sealing structures, and the other end of the anode cylinder is joined to a groove or a step of the other of the end sealing structures, the groove or the step being formed on the inner surface of the other of the end sealing structures.
A second aspect of the coaxial magnetron of the presently disclosed embodiment comprises a cathode, an anode having an anode cylinder and vanes for forming an anode resonant cavity around the cathode, a cylindrical side body forming an outer cavity coaxial with the anode resonant cavity around the anode cylinder, a pair of end sealing structures joined to both ends of the cylindrical side body, and an input part connected to the cathode through one of the end sealing structures, wherein one end of the anode cylinder is joined to one of the end sealing structures, and the other end of the anode cylinder is joined to a gap of the other of the end sealing structures the gap being formed between a central member and an outer periphery member of the other of the end sealing structures so as to insert the anode cylinder.
In a third aspect of the presently disclosed embodiment, a passage for running a coolant therethrough is provided in the vicinity of the anode cylinder in the end sealing structure in which the input part pass through, and a passage for running a coolant therethrough is also provided in the vicinity of the anode cylinder in the end sealing structure in which the input part is not disposed.
In a fourth aspect of the presently disclosed embodiment, the central members are separated from the outer periphery members in the end sealing structures at the both ends, and the central members of the end sealing structures are joined to the outer periphery members respectively after the outer periphery members of the end sealing structures are joined to the cylindrical side body.
According to the configuration of the first aspect, for example, provided that the end sealing structures are an input side (base side) structure having an input part and an upper structure disposed on the upper side (tip side), the other end of the anode cylinder is disposed in the groove or step provided on the inner side of the upper structure, that is, there is a clearance gap between the other end (end face) of the anode cylinder and the groove or step, thereby enabling the distance between the input side structure and the upper structure to be adjusted precisely. As a result, the characteristic of the magnetron is set to a desired value. The outer periphery members of the two end sealing structures are joined to the cylindrical side body and the groove or step of the upper structure is joined to the anode cylinder, thus assembling the magnetron. At this time, the side(s) of the anode cylinder are joined to the side(s) of the groove or step of the upper structure.
According to the configuration of the second aspect, the other end of the anode cylinder is inserted into the gap formed in the upper structure, thereby enabling the distance between the input side structure and the upper structure to be adjusted precisely, and joining the sides of the anode cylinder to the sides of the gap of the upper structure. The groove or step or gap can be defined as a side space part including the side(s) and a space contacting the side(s). The side(s) of the anode cylinder are joined to the side(s) of the side space part (i.e. the side(s) of the groove, the step or the gap) provided in the upper structure.
According to the configuration of the third aspect, the cooling passages are provided in both the input side structure and the upper structure, for example, along the circumference of and in the vicinity of the anode cylinder, which enables the anode part to be cooled efficiently.
According to the configuration of the fourth aspect, before the cathode is disposed, the cylindrical side body is joined to the outer periphery members of the input side structure and the upper structure together with the anode cylinder and so on, for example, by brazing or the like, and then the central member of the input side structure to which the cathode has been fixed via an insulator is joined to the outer periphery member of the input side structure while maintaining the concentric position of the cathode to the anode cylinder. This joining is carried out by arc welding or any other method, which has less effect of temperature on the cathode (less increase in temperature), and then the central member of the upper structure is joined to the outer periphery member thereof by arc welding or the like.
The coaxial magnetron of the presently disclosed embodiment can facilitate heat release from the anode part and increase the peak oscillation output by setting the distance between the end sealing structures at both ends of the anode cylinder precisely and carrying out heat release from both ends of the anode cylinder (both upper and lower ends), even though the outer cavity for tuning is provided outside the anode resonant cavity.
According to the third aspect, cooling passages not only in one end sealing structure (input side structure) but also in the other end sealing structure (upper structure) can improve the overall cooling efficiency, while facilitating the cooling of the anode part.
According to the fourth aspect, the concentric position of the cathode to the anode cylinder can be secured well and satisfactory assembling can be carried out while the deterioration of the cathode due to heat at the time of joining is prevented.
In the aspect, on the inner surface of an upper structure (end sealing structure) 16, an annular groove 17 for inserting the anode cylinder 3 is provided along the side of upper part of the anode cylinder 3 in a circle. As shown in
In the coaxial magnetron, since the outer cavity 60 is surrounded by the input side structure 14 and the upper structure 16, a change of the distance La between the input side structure 14 and the upper structure 16 causes deviation of the resonance frequency of the outer cavity 60. Furthermore, a change of the distance Lb between the pole pieces 7a and 7b causes a decrease in the withstanding voltage of the cathode and a change of magnetic flux density distribution. Therefore, it is important to set the distances La and Lb correctly.
At the time of assembling the magnetron, the distance La between the input side structure 14 and the upper structure 16 can be adjusted well, and the La and the distance Lb between the pole pieces 7a and 7b can be maintained precisely by moving the anode cylinder 3 in the groove 17 in the direction of its cylindrical axis and setting the upper end face of the anode cylinder 3 not to come into contact with the upper structure 16 (the bottom of the groove).
The magnetron of the first aspect is assembled by joining the upper structure 16 to the input side (base) structure 14, on which the cathode 1 and the input part 9 have been mounted, through the anode cylinder 3 and the cylindrical side body 6, and the joining is carried out for example, by brazing in a high temperature furnace. That is, joining the anode cylinder 3 to the groove 17 is carried out by putting brazing filler metals therebetween and in the vicinity thereof and raising the temperature. As shown in a joint part 100 of
According to the configuration of the first aspect, joining the anode cylinder 3 to the upper structure 16 (joining having low heat resistance), which could not be carried out conventionally, can be performed, and heat release from the anode cylinder 3 to the upper structure 16 (heat release to end sealing structures at both ends) can be performed, which results in improvement of cooling efficiency.
According to the third aspect, heat from the anode part (vanes 2 and anode cylinder 3) or the pole pieces 7a and 7b can be reduced by running a coolant through the upper and lower cooling passages 11 and 20, which results in improvement of the overall cooling efficiency as well as cooling efficiency of the anode part. That is, since in conventional magnetrons, the upper structure 16 is not joined to the anode cylinder 3, even if a cooling passage is provided in the upper structure 16, effective cooling cannot be achieved. However, in the aspect, the anode cylinder 3 is joined to the upper structure 16 and heat generated from the vanes 2 and the anode cylinder 3 can be transferred well from the upper structure 16 to the coolant in the cooling passage 20. This effective heat transfer enables the temperatures of the vanes 2 and the anode cylinder 3 to be reduced efficiently.
In the aspect, the cooling passages 11 and 20 are provided along the side of the anode cylinder 3 in a circle, but the upper and lower cooling passages may be provided linearly or partially in the vicinity of the anode cylinder 3.
In the aspect, firstly, the outer periphery member 14c of the input side structure 14 having the cooling passage 11 and the outer periphery member 16c of the upper structure 16 having the cooling passage 20 are assembled so as to cover the anode cylinder 3 and the cylindrical side body 6 and joined by brazing. Simultaneously, as described above, the upper part of the anode cylinder 3 is joined to the groove 17 by brazing (joint part 100). After that, the pole piece 22a, on which the cathode 1 and the input part 9 have been mounted, is inserted into the inside of the anode cylinder 3 and between the vanes 2. The pole piece 22a is then joined to the outer periphery member 14c while checking the concentric position of the cathode 1 relative to the vanes 2 from the opening of the central part of the upper structure 16 on which the pole piece 22b is not mounted. This joining is carried out by arc welding or other method, which has less effect of temperature on the cathode (less increase in temperature), but not by brazing. Finally, the pole piece 22b of the upper structure 16 is joined to the outer periphery member 16c by arc welding or other method similarly, and thus the magnetron that is sealed in a vacuum internally is assembled. The arc welding is a method for welding and joining by subjecting the outer surfaces of the pole piece 22a and the outer periphery member 14c to local heating and the outer surfaces of the pole piece 22b and the outer periphery member 16c to local heating.
According to the fourth aspect, the pole pieces 22a and 22b which are the central members of the end sealing structures are separated from the outer periphery members 14c and 16c, respectively and assembled later, which enables the concentric position of the cathode 1 relative to the vanes 2 to be checked. Further, deterioration of the cathode 1 can be prevented effectively since the pole pieces can be joined by a joining method such as arc welding or the like in which temperature rise is low after the outer periphery members 14c and 16c including the cooling passages 11 and 20 have been joined to the cylindrical side body 6 and the anode cylinder 3 by a joining method such as brazing or the like in which temperature rise is high and the cathode 1 has been disposed.
Also, in the fifth aspect, the pole piece 22a as the central member of the input side structure 14 may be so designed as to be separated from the outer periphery member, and also the pole piece 22b as the central member of the upper structure 16 may be so designed as to be separated (e.g., at the part indicated by two-dot chain line) from the outer periphery member, like the fourth aspect.
The input side structure 14 and the upper structure 16 of each of the aspects are covers of the cylindrical anode, and are in a circular form along the anode cylinder 3, and thus can be processed together with the anode cylinder 3 and others at the time of processing with a lathe, which enables high work efficiency to be obtained in processing each part.
In each aspect, the groove 17 or the step 18 or the gap 26 is provided on the side of the upper structure 16, but the joining of the anode cylinder 3 to the end sealing structures at both ends may be reversed, that is, the groove 17 or the step 18 or the gap 26 may be provided on the side of the input side structure 14.
According to the coaxial magnetron of the presently disclosed embodiment, since cooling efficiency is improved, deformation and melting of the anode components mostly of the vanes 2 due to overheating at the time of generation of high output can be prevented, and such a high microwave output that has not been obtained before can be obtained. In applications and devices using microwaves such as radars and Linac, in many cases, a higher output enables a bigger effect to be obtained, and according to the presently disclosed embodiment, it is not necessary to design a larger size of magnetrons for the purposes of high cooling efficiency and high output, which has a large effect on the industries. In high-frequency coaxial magnetrons, the size of the cavity resonator is smaller depending on wavelengths, but in this case, the sizes of the anode components become smaller, and heat capacity decreases and heat resistance increases, which leads to a more disadvantageous thermal condition. However, the presently disclosed embodiment can provide an efficient cooling effect, and thus there is an advantage that high frequency coaxial magnetrons generating high output can be designed.
The presently disclosed embodiment can be applied in applications and devices using microwaves such as radars and Linac, and can also be applied in high-frequency and high-power coaxial magnetrons.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2013000512 | Jan 2013 | JP | national |
