The present disclosure relates to the technical field of controlling of magnetrons, and in particularly, to an injection-locked magnetron system based on filament injection.
A magnetron is an important industrial microwave source. However, it has poor output characteristics, such as a wide output frequency band, and an uncontrollable phase. The magnetron injection frequency-locking technology can efficiently improve the output characteristics of a magnetron. The magnetron injection frequency-locking technology refers to injecting a high-stability low-power external signal into a low-stability high-power magnetron. When the power and frequency of the injected external signal meet a certain condition, the frequency and phase of the magnetron's output will follow the frequency and phase of the injected external signal. This technology can control the phase and frequency of a high-power oscillator through a small signal, and reduce the sideband noise of the magnetron's output. In 1947, Adler made a theoretical research on oscillator injection locking, and proposed the condition that the injected external signal should meet, that is, Δf≤2f0ρ/Qext, where Δf represents the frequency difference between the injected external signal and magnetron's output, ρ represents an injection ratio, that is, a square root of a power ratio of the injected external signal to the output microwave of the magnetron, f0 represents the free-running frequency of the magnetron, and Qext represents an external quality factor of the magnetron. This condition is called “Adler condition”.
At present, an existing technical solution is to use a waveguide circulator to isolate an injection signal source from a magnetron, and introduce the injected external signal into the output port of the magnetron through the waveguide circulator. After passing through the waveguide circulator, the injected external signal is coupled into the magnetron's resonant cavity through its output antenna, so as to achieve injection locking.
In 1989, William C. Brown proposed a prototype of an injection-locked magnetron system. The system compared the phase of reference signal and magnetron's output, and compensated the magnetron's output phase by a phase shifter to achieve accurate frequency-locking. Many additional investigations on the magnetron injection-locking technology have been conducted. In Japan, N. Shinohara et al. have studied 2.45 GHz injection-locked magnetron using the loop feedback technology, which adopted a phase-locked loop to improve performance of the magnetron by controlling its anode current. In 2005, T. Tahir et al. used a similar technology to realize an injection-locked magnetron by a digital injected signal. In 2008, Hae Jin kim et al. proposed a self-injection locking technology to improve the quality of the magnetron's output. In 2020, Xiaojie Chen proposed a novel magnetron injection locking and power combining system, which replaced a waveguide circulator with a magic-Tee. The magic-Tee can simultaneously realize the injection locking and power combining of two magnetrons, and reduce the loss caused by the waveguide circulators.
In the existing injection locking technology, a large-volume waveguide isolator is required to isolate external signal sources from magnetrons' output, such as a waveguide circulator or a magic-Tee. The volume and weight of waveguide isolators are very large and its manufacturing cost is high, which makes the whole injection locking system huge and expensive. Furthermore, the introduction of the waveguide circulator or the magic-Tee can also increase the loss of the whole system.
In view of this, the purpose of the present disclosure is to provide a novel injection-locked magnetron system based on filament injection to solve the problems of large occupied space, high manufacturing cost and high insertion loss in the related technology, which caused by the large-volume waveguide isolator for isolating external signal sources from magnetrons' output.
The present disclosure is implemented through the following technical solutions.
An embodiment of the present disclosure provides a novel injection-locked magnetron system based on filament injection, which includes: a magnetron, an excitation cavity, and a load; where the magnetron is installed on the excitation cavity and connected to the excitation cavity, the excitation cavity is detachably connected to the load, the magnetron is provided with an injection antenna, and the injection antenna is used to receive an injected external signal and couple the injected external signal into the magnetron to realize injection locking of the magnetron.
In an embodiment of the present disclosure, the magnetron includes a magnetron filament, a magnetron filament cavity, a magnetron resonant cavity, and a magnetron power supply terminal; the magnetron power supply terminal and a part of the injection antenna are installed outside the magnetron filament cavity.
In an embodiment of the present disclosure, the magnetron filament cavity is provided with a through hole through which the injection antenna penetrates, the injection antenna is used to extend into the magnetron filament cavity through the through hole, and the magnetron filament is installed in the magnetron resonant cavity.
In an embodiment of the present disclosure, the injection antenna is connected to a coaxial transmission line.
In an embodiment of the present disclosure, an input voltage of the magnetron power supply terminal is a direct current (DC) voltage of 4000 volts (V).
In an embodiment of the present disclosure, the excitation cavity and the load are fixedly connected by flanges, and the magnetron is integrally connected to the excitation cavity by bolts.
In an embodiment of the present disclosure, the injection antenna includes at least one of a monopole antenna, a dipole antenna, and a loop antenna.
In summary, due to the above technical solutions, the present disclosure has at least the following beneficial effects.
Reference numerals: 1. Excitation cavity; 2. Magnetron; 3. Waveguide directional coupler; 4. Load; 201. Magnetron filament; 202. Monopole antenna; 203. Magnetron filament cavity; 204. Magnetron power supply terminal; 205. First cold water supply terminal; 206. Magnetron resonant cavity; 207. Coaxial transmission line; 208. Inductance coil; 209. Lead; 401. Second cold water supply terminal.
All features disclosed in this specification, or steps in all methods or processes disclosed, except mutually exclusive features and/or steps thereof, can be combined in any way.
Unless otherwise stated, any of the all features disclosed in this specification (including any additional claims and abstract) can be replaced by other equivalent features or alternative features with similar purpose. That is to say, unless otherwise stated, each of the all feature is merely one example in a series of equivalent or similar features.
In the description of the present disclosure, it should be understood that orientations or positional relationships indicated by terms “up”, “down”, “left” and “right” are based on the orientations or positional relationships shown in the accompanying drawings, merely for convenience and simplification of the description of the present disclosure, and do not indicate or imply that the referred equipment or elements must have a specific orientation, be constructed and operated in a specific orientation, and therefore cannot be understood as a limitation of the present disclosure.
In addition, terms “first” and “second” are merely used for descriptive purposes, and cannot be understood as indicating or implying relative importance or implicitly indicating the number of indicated technical features. Thus, a feature defined with the term “first”, “second”, or the like may explicitly or implicitly include one or more of the feature.
As shown in
In an embodiment of the present disclosure, the magnetron 2 includes a magnetron filament 201, a magnetron filament cavity 203, a magnetron resonant cavity 206, a magnetron power supply terminal 204, and a first cold water supply terminal 205. The injection antenna 202 is a monopole antenna. The magnetron power supply terminal 204 and a part of the monopole antenna 202 are installed outside the magnetron filament cavity 203.
In an embodiment of the present disclosure, the first cold water supply terminal 205 is installed outside the magnetron resonant cavity 206, and the magnetron power supply terminal 204 and the first cold water supply terminal 205 are respectively installed on same directional side walls of the magnetron filament cavity 203 and the magnetron resonant cavity 206.
In an embodiment of the present disclosure, the magnetron filament cavity 203 is provided with a through hole through which the monopole antenna 202 penetrates, the monopole antenna 202 is used to extend into the magnetron filament cavity 203 through the through hole, and the magnetron filament 201 is installed in the magnetron resonant cavity 206.
In an embodiment of the present disclosure, a cooling assembly is installed outside the magnetron resonant cavity 206. The cooling assembly is installed to surround the magnetron resonant cavity 206. A cooling medium is supplied through the first cold water supply terminal 205 and the cooling assembly to cool the magnetron resonant cavity 206.
In other embodiments of the present disclosure, the cooling assembly is used for cooling the magnetron resonant cavity 206 through a cooling medium, which may be air or other liquids.
In an embodiment of the present disclosure, the monopole antenna 202 is connected to a coaxial transmission line.
In an embodiment of the present disclosure, the load 4 is provided with a second cold water supply terminal 401.
Based on the above structure, the excitation cavity 1 is used to excite the fundamental mode of output energy, and the waveguide directional coupler 3 is used to output spectrum of the magnetron 2. A direct current (DC) voltage of 4000 voltages (V) is input to the magnetron filament cavity 203 through the magnetron power supply terminal 204. Further, in order to prevent the leakage of an RF signal of the magnetron 2, two inductance coils 208 are installed in the magnetron filament cavity 203 and outside the magnetron resonant cavity 206, so components installed in the magnetron filament cavity 203 can be used as a coupling antenna to couple the injected external signal into the magnetron resonant cavity 206, thereby realizing injection locking. Specifically, the two inductance coils 208 are in one-to-one correspondence connected to two leads 209 of the magnetron filament 201, and the two leads 209 of the magnetron filament 201 are positioned in the magnetron filament cavity 203. Therefore, in the technical solution of the present disclosure, the injected external signal is injected by the monopole antenna 202, and coupled into the magnetron resonant cavity 203 through the magnetron filament 201, and the output microwave of the magnetron 2 is output through the excitation cavity 1, and passes through the waveguide directional coupler 3, and is finally absorbed by the load 4, such that the output microwave of the magnetron 2 can be locked by the injected external signal, and the frequency of the output microwave of the magnetron 2 completely follows the frequency of the injected external signal within a locking bandwidth.
In the traditional magnetron injection frequency-locking technology, an injected external signal is injected by a waveguide isolator and then is coupled through the excitation cavity 1 for realizing injection locking. In contrast, in the present disclosure, the monopole antenna 202 is used to extend into the magnetron filament cavity 203 by the through hole drilled in the magnetron filament cavity 203, for realizing injection locking.
The excitation cavity 1, the waveguide directional coupler 4 and the load 4 are fixedly connected to each other by flanges, and the magnetron 2 is in whole connected to the excitation cavity 1 by bolts.
Further, it should be noted that, the injection antenna 202 may also be a dipole antenna or a loop antenna. Moreover, the injection antenna 202 may be more than one in number, and the multiple injection antenna 202 may be at least two of the monopole antennas, the dipole antennas, and the loop antennas.
With respect to the technical solution of the present disclosure, the inventor performed a verification experiment, and filament injection locking of the magnetron 2 is achieved without introducing a waveguide circulator. A final injection locking performance is shown in table 1 below.
A test block view of the present disclosure is shown in
In this test experiment, an injected external signal is provided by a signal source and a high-gain power amplifier. It can be clearly observed by a spectrum analyzer that an output microwave of the magnetron 2 is locked by the injected external signal. With the increase of the power of the injected external signal and the change of the frequency, it can be observed that the periodic pulling spectrum before performing injection locking and the injection locking spectrum after performing injection locking are shown in
The finally measured locking bandwidths at different injection ratios are shown in the table 1 above. The measured results show that the proposed system of the present disclosure is feasible.
The reasons for the narrow locking bandwidth are: 1) the monopole antenna 202 is not well matched; 2) there is a certain transmission loss between the magnetron filament cavity 203 and the magnetron resonant cavity 206, and the signal from the magnetron filament cavity 203 is not completely coupled into the magnetron resonant cavity 206. In the future, after the monopole antenna 202 is completely matched with the magnetron filament 201, it is expected that the locking bandwidth of the present disclosure comparable to that of the traditional solution can be achieved with low system cost and a smaller volume.
The above is merely preferred embodiments of the present disclosure, and are not intended to limit the present disclosure. Any modification, equivalent substitution and improvement made within the spirit and principle of the present disclosure should be included in the scope of protection of the present disclosure.
Number | Date | Country | Kind |
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202111539440.0 | Dec 2021 | CN | national |
Number | Name | Date | Kind |
---|---|---|---|
2710923 | Kern | Jun 1955 | A |
2759099 | Olive | Aug 1956 | A |
2820197 | Donal, Jr. | Jan 1958 | A |
3701020 | De Vito | Oct 1972 | A |
4809004 | Brandao | Feb 1989 | A |
5045814 | English | Sep 1991 | A |
5084651 | Farney | Jan 1992 | A |
5107272 | Joynson | Apr 1992 | A |
5483123 | Walker | Jan 1996 | A |
5598064 | Wallander | Jan 1997 | A |
5680012 | Walker | Oct 1997 | A |
9355808 | Huang | May 2016 | B2 |
10374551 | Kazakevich | Aug 2019 | B2 |
10426022 | Kazakevich | Sep 2019 | B2 |
10477668 | Chase | Nov 2019 | B2 |
10700639 | Kazakevich | Jun 2020 | B2 |
11474201 | Yang | Oct 2022 | B2 |
11525931 | Yonehara | Dec 2022 | B2 |
20040156846 | Daum | Aug 2004 | A1 |
20040156852 | Daum | Aug 2004 | A1 |
20060187114 | Gibson | Aug 2006 | A1 |
20070139247 | Brown | Jun 2007 | A1 |
20150270091 | Huang | Sep 2015 | A1 |
20170094770 | Kephart | Mar 2017 | A1 |
20170250651 | Kazakevich | Aug 2017 | A1 |
20170280549 | Chase | Sep 2017 | A1 |
20180352644 | Kephart | Dec 2018 | A1 |
20190069387 | Kazakevich | Feb 2019 | A1 |
20190182910 | Huang | Jun 2019 | A1 |
20190224751 | Thangaraj | Jul 2019 | A1 |
20200015347 | Kephart | Jan 2020 | A1 |
20200044607 | Kazakevich | Feb 2020 | A1 |
20200084873 | Kazakevich | Mar 2020 | A1 |
20200116821 | Yang | Apr 2020 | A1 |
20200243294 | Neubauer | Jul 2020 | A1 |
Number | Date | Country |
---|---|---|
104241064 | Dec 2014 | CN |
Entry |
---|
CNIPA, Notification of a Second Office Action for CN202111539440.0, dated Nov. 11, 2022. |
Sichuan University (Applicant), Reply to Notification of a Second Office Action for CN202111539440.0, w/ (allowed) replacement claims, dated Nov. 15, 2022. |
CNIPA, Notification to grant patent right for invention in CN202111539440.0, dated Jan. 9, 2023. |
Number | Date | Country | |
---|---|---|---|
20230187164 A1 | Jun 2023 | US |