CN111383873A - A Novel Tunable Magnetic Focusing System for Ribbon Beam TWT - Google Patents
A Novel Tunable Magnetic Focusing System for Ribbon Beam TWT Download PDFInfo
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- CN111383873A CN111383873A CN202010150361.XA CN202010150361A CN111383873A CN 111383873 A CN111383873 A CN 111383873A CN 202010150361 A CN202010150361 A CN 202010150361A CN 111383873 A CN111383873 A CN 111383873A
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
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Abstract
Description
技术领域technical field
本发明属于真空电子技术领域,具体涉及一种适用于毫米波及太赫兹频段的带状注行波管的磁聚焦系统。The invention belongs to the technical field of vacuum electronics, and in particular relates to a magnetic focusing system of a band-shaped injection traveling wave tube suitable for millimeter wave and terahertz frequency bands.
背景技术Background technique
带状电子注具有大的横截面尺寸、高的直流功率、低的空间电荷效应等显著优点,采用带状电子注作为电子源的毫米波及太赫兹频段真空电子器件具有更高的输出功率。因此,带状电子注在毫米波及太赫兹真空电子器件领域得到了广泛的关注。带状电子注成形可以由经典的皮尔斯电子枪实现,在均匀磁场或者周期会切磁场的聚焦作用下传输,从而为真空电子器件的信号产生或放大提供了稳定的直流功率。带状注行波管是一种具有高功率、宽带宽、高效率、高增益等特点的一类新型真空电子器件,有着广阔的应用前景,但是它面临带状电子注更难聚焦这一挑战。随着工作频率的提高,如0.22THz、0.34THz等,真空电子器件的尺寸减小,所需的带状注电子枪和磁聚焦系统的加工和装配精度要求特别高(微米量级),这将导致带状电子注的成形与传输更加困难。Ribbon electron beams have significant advantages such as large cross-sectional size, high DC power, and low space charge effect. Vacuum electronic devices in millimeter-wave and terahertz frequency bands using ribbon electron beams as electron sources have higher output power. Therefore, ribbon electron injection has received extensive attention in the field of millimeter-wave and terahertz vacuum electronic devices. The strip electron injection molding can be realized by a classic Pierce electron gun, which is transmitted under the focusing action of a uniform magnetic field or a periodically tangential magnetic field, thereby providing stable DC power for signal generation or amplification of vacuum electronic devices. Ribbon injection traveling wave tube is a new type of vacuum electronic device with the characteristics of high power, wide bandwidth, high efficiency and high gain. . With the increase of the operating frequency, such as 0.22THz, 0.34THz, etc., the size of the vacuum electronic device is reduced, and the required processing and assembly precision of the strip electron gun and magnetic focusing system is particularly high (micron order), which will This makes the formation and transmission of the ribbon-shaped electron beam more difficult.
在毫米波及太赫兹频段,关于带状注行波管的热测实验鲜有报道,国内外研制成功的两支带状注行波管分别为电子科技大学的Ka波段带状注行波管(X.Shi et.al.,“Theoretical and experimental research on a novel small tunable PCM system instaggered double vane TWT,”IEEE Transactions on Electron Devices,vol.62,no.12,pp.4258-4264,Dec.2015.)和美国加州大学戴维斯分校的G波段带状注行波管(A.Baig et al.,“Performance of a Nano-CNC machined220-GHz traveling wave tubeamplifier,”IEEE Transactions on Electron Devices,vol.64,no.5,pp.2390-2397,May2017.),热测实验结果均有100W功率输出。带状注行波管较难研制的原因之一是适用于带状注行波管的电子光学系统难于实现。电子光学系统由电子枪、磁聚焦系统和收集极组成,行波管所采用的磁聚焦系统一般为均匀磁场聚焦系统或者周期永磁聚焦系统,其作用在于利用磁场提供的聚焦力来平衡电子注的空间电荷力,从而实现带状电子注的稳定传输。因此,解决带状电子注传输的关键在于设计磁聚焦系统。如果采用均匀永磁聚焦带状电子注,形成均匀磁场的永磁体组件相对周期磁场采用的永磁体的体积更大,不利于器件的小型化。另外,由于带状注电子枪的阴极组件的制作和枪的装配等误差均可能导致带状电子注的注腰位置和层流性发生变化。由于带状电子注的截面尺寸发生变化,则注电流密度改变,即空间电荷力发生改变,所需的聚焦磁场应该做相应变化,即磁聚焦系统应该可调。因此,研究一种基于永磁体产生周期会切磁场的带状电子注行波管所用的可调磁聚焦系统,包括磁聚焦系统和磁聚焦系统的装配设计,对高频率、高功率、小型化带状注器件的研制及推动毫米波及太赫兹辐射源的发展具有极其重要的意义。In the millimeter-wave and terahertz frequency bands, there are few reports on the thermal measurement experiments of the band-shaped traveling wave tube. X.Shi et.al.,“Theoretical and experimental research on a novel small tunable PCM system instaggered double vane TWT,”IEEE Transactions on Electron Devices,vol.62,no.12,pp.4258-4264,Dec.2015. ) and the G-band strip traveling wave tube at the University of California, Davis (A. Baig et al., "Performance of a Nano-CNC machined220-GHz traveling wave tubeamplifier," IEEE Transactions on Electron Devices, vol.64 , no.5, pp.2390-2397, May2017.), the thermal test results have a power output of 100W. One of the reasons why it is difficult to develop the strip-beam TWT is that it is difficult to realize the electron optical system suitable for the strip-beam travel-wave tube. The electron optical system consists of an electron gun, a magnetic focusing system and a collector. The magnetic focusing system used in the traveling wave tube is generally a uniform magnetic field focusing system or a periodic permanent magnet focusing system. Its function is to use the focusing force provided by the magnetic field to balance the electron injection. space charge force, thereby achieving stable transport of banded electron beams. Therefore, the key to solving the band-shaped electron injection transport lies in the design of the magnetic focusing system. If a uniform permanent magnet is used to focus the band-shaped electron beam, the volume of the permanent magnet assembly forming a uniform magnetic field is larger than that of the permanent magnet used in the periodic magnetic field, which is not conducive to the miniaturization of the device. In addition, due to errors in the manufacture of the cathode assembly of the strip electron injection gun and the assembly of the gun, the injection waist position and laminar flow properties of the strip electron injector may change. Due to the change of the cross-sectional size of the strip electron injection, the injection current density changes, that is, the space charge force changes, and the required focusing magnetic field should be changed accordingly, that is, the magnetic focusing system should be adjustable. Therefore, a tunable magnetic focusing system for a strip electron injection traveling wave tube based on a permanent magnet to generate a periodically tangential magnetic field is studied, including the magnetic focusing system and the assembly design of the magnetic focusing system. The development of strip injection devices and the development of millimeter wave and terahertz radiation sources are of great significance.
发明内容SUMMARY OF THE INVENTION
针对背景技术所存在的带状电子注在带状注行波管中较难稳定传输的问题,本发明的目的在于提供一种适用于带状注行波管的新型可调磁聚焦系统。该发明基于永磁体产生周期会切磁场和设计的磁聚焦系统固定装置,使得磁聚焦系统具有一定的可调范围,从而应用于带状注行波管实现带状电子注的稳定传输。Aiming at the problem that the band-shaped electron injection is difficult to transmit stably in the band-shaped traveling wave tube in the background art, the purpose of the present invention is to provide a novel tunable magnetic focusing system suitable for the band-shaped traveling wave tube. The invention is based on a permanent magnet generating a periodic tangential magnetic field and a designed fixing device for the magnetic focusing system, so that the magnetic focusing system has a certain adjustable range, so that the invention can be applied to the band-shaped electron beam tube to realize the stable transmission of the band-shaped electron beam.
为实现上述目的,本发明的技术方案如下:For achieving the above object, technical scheme of the present invention is as follows:
一种适用于带状注行波管的新型可调磁聚焦系统,包括磁聚焦系统和磁聚焦系统固定装置,其特征在于,所述磁聚焦系统包括n个单周期磁体组件和一对极靴,所述单周期磁体组件由两组磁体单元组成,所述磁体单元对称设置,所述一组磁体单元包括两个第一永磁体和两个第二永磁体,所述两个第一永磁体并排设置,所述两组磁体单元中第一永磁体相互排斥,所述两个第二永磁体通过磁性吸引力交错吸附于并排设置的两个第一永磁体表面,且该表面为两组磁体单元中第一永磁体相互排斥面的相对面,所述极靴设置于第一永磁体靠近电子枪一侧;A new type of tunable magnetic focusing system suitable for strip-shaped traveling wave tube, comprising a magnetic focusing system and a fixing device for the magnetic focusing system, characterized in that the magnetic focusing system includes n single-period magnet assemblies and a pair of pole pieces , the single-period magnet assembly consists of two sets of magnet units, the magnet units are symmetrically arranged, the set of magnet units includes two first permanent magnets and two second permanent magnets, the two first permanent magnets Arranged side by side, the first permanent magnets in the two groups of magnet units repel each other, and the two second permanent magnets are alternately adsorbed on the surfaces of the two first permanent magnets arranged side by side through magnetic attraction, and the surfaces are two groups of magnets the opposite surface of the mutually repelling surface of the first permanent magnet in the unit, the pole piece is arranged on the side of the first permanent magnet close to the electron gun;
所述磁聚焦系统固定装置包括第一磁聚焦系统支架、第二磁聚焦系统支架、磁聚焦系统支架条和连接板;所述第一磁聚焦系统支架和第二磁聚焦系统支架均为L型,L型的第一磁聚焦系统支架和第二磁聚焦系统支架的第一侧面结构相同,均设置有通孔,用于放置磁聚焦系统中的第二永磁体;通孔上方设置有圆形螺钉孔,与所述磁聚焦系统支架条上的圆形螺钉孔配合,通过支架条固定单周期磁体组件;所述连接板位于磁聚焦系统支架条上方,连接板上设置有一对圆形螺钉孔和一对U型螺钉孔,其中,圆形螺钉孔与第一磁聚焦系统支架连接固定,U型螺钉孔和第二磁聚焦系统支架连接固定;所述第一磁聚焦系统支架的第二侧面设置有定位块,所述两组磁体单元关于定位块对称,定位块上方用于放置高频结构;所述第二聚焦系统支架的第二侧面通过U型螺钉孔固定连接第一磁聚焦系统支架的第二侧面。The magnetic focusing system fixing device includes a first magnetic focusing system bracket, a second magnetic focusing system bracket, a magnetic focusing system bracket strip and a connecting plate; the first magnetic focusing system bracket and the second magnetic focusing system bracket are both L-shaped , the L-shaped first magnetic focusing system bracket and the second magnetic focusing system bracket have the same first side structure, and both are provided with through holes for placing the second permanent magnet in the magnetic focusing system; above the through holes is a circular The screw holes are matched with the circular screw holes on the magnetic focusing system bracket strip, and the single-period magnet assembly is fixed by the bracket strip; the connecting plate is located above the magnetic focusing system bracket strip, and a pair of circular screw holes are arranged on the connecting plate and a pair of U-shaped screw holes, wherein the circular screw holes are connected and fixed with the first magnetic focusing system bracket, and the U-shaped screw holes are connected and fixed with the second magnetic focusing system bracket; the second side surface of the first magnetic focusing system bracket A positioning block is provided, the two groups of magnet units are symmetrical about the positioning block, and the high-frequency structure is placed above the positioning block; the second side of the second focusing system bracket is fixedly connected to the first magnetic focusing system bracket through U-shaped screw holes the second side.
进一步地,所述n为正整数。Further, the n is a positive integer.
进一步地,所述第二磁聚焦系统支架的第一侧面的U型螺钉孔和第二侧面的U型螺钉孔联合用于调节磁聚焦系统中两组磁体单元的间距。Further, the U-shaped screw holes on the first side and the U-shaped screw holes on the second side of the second magnetic focusing system bracket are combined to adjust the distance between the two groups of magnet units in the magnetic focusing system.
进一步地,所述通孔的高度大于第二永磁体高度,便于调节第二永磁体相对于第一永磁体的位置。Further, the height of the through hole is greater than the height of the second permanent magnet, which facilitates adjustment of the position of the second permanent magnet relative to the first permanent magnet.
进一步地,所述交错设置的第二永磁体之间的垂直间距为w,当w值由小变大时,带状电子注的宽边由过聚焦由到聚焦不足。Further, the vertical spacing between the staggered second permanent magnets is w, and when the value of w increases from small to large, the broad side of the band-shaped electron beam changes from over-focusing to under-focusing.
进一步地,所述第一永磁体和第二永磁体的材料均为钕铁硼;所述极靴材料为纯铁;所述磁聚焦系统固定装置材料均为无磁金属。Further, the materials of the first permanent magnet and the second permanent magnet are both NdFeB; the material of the pole piece is pure iron; the material of the fixing device of the magnetic focusing system is non-magnetic metal.
进一步地,所述无磁金属优选为铝。Further, the non-magnetic metal is preferably aluminum.
综上所述,由于采用了上述技术方案,本发明的有益效果是:To sum up, due to the adoption of the above-mentioned technical solutions, the beneficial effects of the present invention are:
1.本发明设计的适用于带状注行波管的新型可调磁聚焦系统,通过在第一永磁体1-1的Y方向上吸附交错的第二永磁体1-2,从而在带状电子注通道产生By磁场,用以抵消带状电子注在X方向的空间电荷力;并且加载的第二永磁体1-2可以在竖直X方向进行调节,即当交错的两个第二永磁体之间的间距w越大时,产生的By磁场越小,反之越大。1. The novel adjustable magnetic focusing system designed by the present invention is suitable for the strip-shaped injection traveling wave tube. By adsorbing the staggered second permanent magnets 1-2 in the Y direction of the first permanent magnet The electron injection channel generates By magnetic field to counteract the space charge force of the band-shaped electron injection in the X direction; and the loaded second permanent magnet 1-2 can be adjusted in the vertical X direction, that is, when the two second permanent magnets are staggered. When the spacing w between the magnets is larger, the generated By magnetic field is smaller, and vice versa.
2.本发明所设计的可调磁聚焦系统,相对于其它均匀磁场形式的磁聚焦系统具有小型化、成本低等优点,对高频率、高功率、小型化带状注器件的研制及推动毫米波及太赫兹辐射源的发展具有极其重要的意义。2. The adjustable magnetic focusing system designed by the present invention has the advantages of miniaturization and low cost compared with other magnetic focusing systems in the form of uniform magnetic field. The development of terahertz radiation sources is of great significance.
附图说明Description of drawings
图1为本发明磁聚焦系统整体结构示意图。FIG. 1 is a schematic diagram of the overall structure of the magnetic focusing system of the present invention.
图2为本发明磁聚焦系统固定装置示意图。FIG. 2 is a schematic diagram of the fixing device of the magnetic focusing system of the present invention.
图3为本发明磁聚焦系统示意图。FIG. 3 is a schematic diagram of the magnetic focusing system of the present invention.
图4为本发明的磁聚焦系统单周期结构及磁化方向示意图;4 is a schematic diagram of the single-period structure and magnetization direction of the magnetic focusing system of the present invention;
其中,(a)为磁聚焦系统单周期结构(n=1)示意图;(b)为磁聚焦系统单周期结构Y向视图;(c)为磁聚焦系统单周期结构Z向视图;(d)为磁聚焦系统单周期结构永磁体磁化方向示意图。Among them, (a) is the schematic diagram of the single-period structure of the magnetic focusing system (n=1); (b) is the Y-direction view of the single-period structure of the magnetic focusing system; (c) is the Z-direction view of the single-period structure of the magnetic focusing system; (d) It is a schematic diagram of the magnetization direction of the permanent magnet with a single-period structure of the magnetic focusing system.
图5为本发明实施例1模拟计算得到的磁聚焦系统轴向磁感应强度沿Z轴的分布图。FIG. 5 is a distribution diagram of the axial magnetic induction intensity of the magnetic focusing system along the Z axis obtained by the simulation calculation in
图6为本发明实施例1中带状电子注在磁聚焦系统作用下的窄边传输轨迹(Y-Z截面)。6 is the narrow-side transmission track (Y-Z section) of the band-shaped electron injection under the action of the magnetic focusing system in the first embodiment of the present invention.
图7为本发明实施例1中带状电子注在磁聚焦系统作用下的宽边传输轨迹(X-Z截面)。FIG. 7 is the broad-side transmission track (X-Z section) of the band-shaped electron injection under the action of the magnetic focusing system in Example 1 of the present invention.
图8为本发明实施例2模拟计算得到的磁聚焦系统的轴向磁感应强度沿Z轴的分布图。FIG. 8 is a distribution diagram of the axial magnetic induction intensity of the magnetic focusing system along the Z axis obtained by the simulation calculation in
图9为本发明实施例2中带状电子注在磁聚焦系统作用下的窄边传输轨迹(Y-Z截面)。FIG. 9 is the narrow-side transmission track (Y-Z section) of the band-shaped electron injection under the action of the magnetic focusing system in
图10为本发明实施例2中带状电子注在磁聚焦系统作用下的宽边传输轨迹(X-Z截面)。FIG. 10 is the broadside transmission track (X-Z section) of the band-shaped electron injection under the action of the magnetic focusing system in Example 2 of the present invention.
图中磁聚焦系统1包括:第一永磁体1-1、第二永磁体1-2和极靴1-3;第一磁聚焦系统支架2包括:矩形通孔2-1和矩形定位块2-2;第二磁聚焦系统支架3包括:矩形通孔3-1、第一U形螺钉孔3-2和第一圆形螺钉孔3-3;磁聚焦系统支架条4包括第二圆形螺钉孔4-1;连接板5包括:第三圆形螺钉孔5-1和第二U形螺钉孔5-2。In the figure, the
具体实施方式Detailed ways
为使本发明的目的、技术方案和优点更加清楚,下面结合实施方式和附图,对本发明作进一步地详细描述。In order to make the objectives, technical solutions and advantages of the present invention clearer, the present invention will be further described in detail below with reference to the embodiments and accompanying drawings.
本实施方式以G波段带状注行波管电子光学系统为例,说明本发明中的新型可调磁聚焦系统可用于实现带状电子注的稳定传输。本发明中带状注电子枪已在中国发明专利CN201910870119.7作过描述:带状电子注的注腰尺寸约为0.4mm×0.1mm,注电流和阴极发射电流密度分别为130mA和26A/cm2,压缩比为12.5:1,在注腰处的注电流密度为325A/cm2。This embodiment takes the G-band band-shaped electron beam tube electron optical system as an example to illustrate that the novel tunable magnetic focusing system in the present invention can be used to realize the stable transmission of the band-shaped electron beam. The strip electron injection gun in the present invention has been described in Chinese invention patent CN201910870119.7: the injection waist size of the strip electron injector is about 0.4mm×0.1mm, and the injection current and cathode emission current density are respectively 130mA and 26A/cm 2 , the compression ratio is 12.5:1, and the injection current density at the injection waist is 325A/cm 2 .
实施例1Example 1
一种适用于带状注行波管的新型可调磁聚焦系统整体结构示意图如图1所示,包括磁聚焦系统1和磁聚焦系统固定装置;所述磁聚焦系统为周期会切磁场聚焦系统,提供聚焦磁力,用于平衡带状电子注的空间电荷力,使得带状电子注能够稳定传输。A schematic diagram of the overall structure of a new type of tunable magnetic focusing system suitable for strip-shaped TWT , which provides a focusing magnetic force for balancing the space charge force of the banded electron beams, so that the banded electron beams can be transported stably.
图2为本发明磁聚焦系统固定装置示意图,所述磁聚焦系统固定装置包括第一磁聚焦系统支架2、第二磁聚焦系统支架3、磁聚焦系统支架条4以及连接板5。FIG. 2 is a schematic diagram of a magnetic focusing system fixing device of the present invention. The magnetic focusing system fixing device includes a first magnetic
所述第一磁聚焦系统支架2和第二磁聚焦系统支架3均为L型,并排设置,所述L型的第一磁聚焦系统支架2和第二磁聚焦系统支架3的第一侧面结构相同,对称设置有上下两排交错的通孔2-1和3-1,用于放置磁聚焦系统中的交错的第二永磁体1-2;通孔上方设置有第一圆形螺钉孔3-3,磁聚焦系统支架条4上设置有第二圆形螺钉孔4-1,所述第一磁聚焦系统支架侧面设置的圆形螺钉孔与同侧磁聚焦系统支架条4设置的第二圆形螺钉孔4-1配合固定单周期磁体组件,防止双排的第一永磁体1-1在沿第一侧面竖直方向(X方向)的移动;所述连接板位5于磁聚焦系统支架条4上方,连接板5上设置有一对第三圆形螺钉孔5-1和一对第二U型螺钉孔5-2,其中,第三圆形螺钉孔5-1与第一磁聚焦系统支架2连接固定,第二U型螺钉孔5-2和第二聚焦系统支架3连接固定;所述第一磁聚焦系统支架2的第二侧面设置有定位块2-2,用于对带状注行波管X方向的定位,两组磁体单元关于定位块对称;所述第二聚焦系统支架3的第二侧面通过第一U型螺钉孔3-2固定连接第一磁聚焦系统支架2的第二侧面;第一U形螺钉孔3-2和第二U形螺钉孔5-2联合用于调节磁聚焦系统双排永磁体1-1的间距d,距离越近,轴向磁场越强。The first magnetic focusing
所述的圆形螺钉孔和U形螺钉孔,适用M2螺钉,如图所示;其中,第一磁聚焦系统支架的第一侧面与第二侧面的连接处的凹槽、两个磁聚焦系统支架第一侧面靠近通孔处的台阶,均为加工工艺限制,与技术方案的实现效果无关。The circular screw holes and U-shaped screw holes are suitable for M2 screws, as shown in the figure; among them, the groove at the connection between the first side and the second side of the first magnetic focusing system bracket, the two magnetic focusing systems The steps on the first side of the bracket close to the through holes are all limitations of the processing technology and have nothing to do with the realization effect of the technical solution.
图3为本发明磁聚焦系统示意图,所述磁聚焦系统包括4个单周期磁体组件和一对极靴1-3,所述单周期磁体组件由两组磁体单元组成,所述磁体单元对称设置,所述磁体单元包括两个第一永磁体1-1和两个第二永磁体1-2,第一永磁体1-1和第二永磁体1-2分别磁化;所述极靴1-3设置于第一永磁体1-1靠近电子枪一侧;该磁聚焦系统可应用于中等功率输出的G波段带状注行波管。3 is a schematic diagram of the magnetic focusing system of the present invention, the magnetic focusing system includes four single-period magnet assemblies and a pair of pole pieces 1-3, the single-period magnet assemblies are composed of two sets of magnet units, and the magnet units are symmetrically arranged , the magnet unit includes two first permanent magnets 1-1 and two second permanent magnets 1-2, the first permanent magnet 1-1 and the second permanent magnet 1-2 are magnetized respectively; the pole piece 1- 3 is arranged on the side of the first permanent magnet 1-1 close to the electron gun; the magnetic focusing system can be applied to the G-band band injection traveling wave tube with medium power output.
图4为本发明的磁聚焦系统单周期结构及磁化方向示意图。图4(a)为本发明磁聚焦系统一对磁体单元结构示意图,所述磁体单元包括两个第一永磁体1-1和两个第二永磁体1-2,第二永磁体1-2交错吸附于第一永磁体1-1XOY表面;图4(b)为本发明磁聚焦系统单周期结构Y向视图;图4(c)为本发明磁聚焦系统单周期结构Z向视图;图4(d)为本发明磁聚焦系统单周期结构永磁体磁化方向示意图,箭头指向代表磁钢的N极,且在单周期中加载的交错的第二永磁体1-2与对应加载位置处的第一永磁体1-1的磁化方向相同。FIG. 4 is a schematic diagram of the single-period structure and magnetization direction of the magnetic focusing system of the present invention. 4(a) is a schematic structural diagram of a pair of magnet units in the magnetic focusing system of the present invention, the magnet units include two first permanent magnets 1-1 and two second permanent magnets 1-2, and the second permanent magnet 1-2 It is staggered and adsorbed on the surface of the first permanent magnet 1-1XOY; Fig. 4(b) is a Y-direction view of the single-period structure of the magnetic focusing system of the present invention; Fig. 4(c) is a Z-direction view of the single-period structure of the magnetic focusing system of the present invention; Fig. 4 (d) is a schematic diagram of the magnetization direction of the permanent magnet with a single-cycle structure of the magnetic focusing system of the present invention, the arrow points to the N-pole representing the magnetic steel, and the staggered second permanent magnets 1-2 loaded in a single cycle and the first permanent magnet at the corresponding loading position The magnetization directions of one permanent magnet 1-1 are the same.
在本实施例中,结构参数设置如下:a=16mm,b=2.4mm,c=1.5mm,d=2.4mm,e=4mm,h=4.8mm,w=5mm。本实施例中第一永磁体1-1和第二永磁体1-2均采用烧结钕铁硼(Sintered NdFeB)磁性材料,相比于钐钴永磁材料,钕铁硼具有更高的磁能积和矫顽力,更好的机械性能,更有利于毫米波及太赫兹频段磁聚焦系统的实现。In this embodiment, the structural parameters are set as follows: a=16mm, b=2.4mm, c=1.5mm, d=2.4mm, e=4mm, h=4.8mm, w=5mm. In this embodiment, both the first permanent magnet 1-1 and the second permanent magnet 1-2 are made of sintered NdFeB (Sintered NdFeB) magnetic material. Compared with the samarium cobalt permanent magnet material, NdFeB has a higher magnetic energy product And coercivity, better mechanical properties, more conducive to the realization of millimeter-wave and terahertz band magnetic focusing system.
为说明本发明的可调磁聚焦系统提供的聚焦磁力能够较好地平衡上述带状电子注的空间电荷力,对带状注电子枪和新型可调磁聚焦系统进行了联合模拟仿真。由三维电磁仿真软件模拟计算,得到如下结果:In order to illustrate that the focusing magnetic force provided by the adjustable magnetic focusing system of the present invention can better balance the space charge force of the above-mentioned band-shaped electron injection, a joint simulation of the band-shaped electron gun and the new adjustable magnetic focusing system is carried out. The three-dimensional electromagnetic simulation software is used to simulate and calculate, and the following results are obtained:
当磁聚焦系统的周期n为4时,本发明磁聚焦系统适用于中等增益、中等输出功率的G波段带状注行波管。在本情形中,第一永磁体1-1和交错的第二永磁体1-2位于Z=9.3mm~28.5mm范围内。如图5所示,为本发明模拟计算得到4周期长度的磁聚焦系统的中心位置处轴向磁感应强度Bz沿Z轴的分布图,Bz的周期为4.8mm,绝对值最大时约为0.35T。另外,带状电子注的传输轨迹在YZ面(窄边)和XZ面(宽边)的截面视图分别如图6和图7所示,带状电子注通过Z=30mm位置处注电流保持不变,这表明带状电子注在传输过程未被管体截获。When the period n of the magnetic focusing system is 4, the magnetic focusing system of the present invention is suitable for the G-band band injection traveling wave tube with medium gain and medium output power. In this case, the first permanent magnets 1-1 and the staggered second permanent magnets 1-2 are located in the range of Z=9.3mm˜28.5mm. As shown in Figure 5, the distribution diagram of the axial magnetic induction intensity Bz along the Z axis at the center position of the magnetic focusing system with a length of 4 cycles is obtained by the simulation calculation of the present invention. The period of Bz is 4.8mm, and the absolute value is about 0.35T at the maximum . In addition, the cross-sectional views of the transport trajectories of the strip electron beam on the YZ plane (narrow side) and the XZ plane (broad side) are shown in Figures 6 and 7, respectively. changes, which indicates that the banded electron injection was not intercepted by the tube body during the transport process.
实施例2Example 2
当磁聚焦系统的周期n为18时,本发明磁聚焦系统适用于高增益、高输出功率的G波段带状注行波管,在本情形中,第一永磁体1-1和交错的第二永磁体1-2位于Z=9.3mm~95.7mm范围内。如图8所示,为本发明模拟计算得到18周期长度的磁聚焦系统的中心位置处轴向磁感应强度Bz沿Z轴的分布图,Bz的周期为4.8mm,绝对值最大时约为0.35T。另外,带状电子注的传输轨迹在YZ面(窄边)和XZ面(宽边)的截面视图分别如图9和图10所示,从图中看出,带状电子注在大于90mm长度的传输距离下,宽边和窄边方向的电子注波动幅度都很小,这说明所设计的磁聚焦系统产生的周期磁场足够用于电子注窄边的聚焦。因此,该新型可调磁聚焦系统可用于带状电子注的稳定传输。When the period n of the magnetic focusing system is 18, the magnetic focusing system of the present invention is suitable for the G-band band-shaped TWT with high gain and high output power. In this case, the first permanent magnet 1-1 and the staggered No. The two permanent magnets 1-2 are located in the range of Z=9.3mm˜95.7mm. As shown in Figure 8, the distribution diagram of the axial magnetic induction intensity Bz along the Z axis at the center position of the magnetic focusing system with a length of 18 periods is obtained by the simulation calculation of the present invention. The period of Bz is 4.8mm, and the absolute value is about 0.35T at the maximum. . In addition, the cross-sectional views of the transport trajectories of the banded electron beams on the YZ plane (narrow side) and the XZ plane (broadside) are shown in Figures 9 and 10, respectively. It can be seen from the figures that the banded electron beams are longer than 90mm Under the transmission distance of , the fluctuation amplitudes of electron beams in the broadside and narrowside directions are very small, which indicates that the periodic magnetic field generated by the designed magnetic focusing system is sufficient for the focusing of the electron beams on the narrowside. Therefore, the novel tunable magnetic focusing system can be used for stable transport of ribbon electron beams.
进一步地研究表明,当w值由小变大,由交错的第二永磁体在带状电子注区域产生的By将由大变小,带状电子注的宽边由过聚焦到聚焦不足,因而本发明可以通过调节交错的第二永磁体的间距w改变带状电子注宽边聚焦所需的磁场By。值得注意的是,本发明中模拟计算的采用带状电子注在磁场区域传输距离大于86mm,带状电子注并没有在传输过程中发生崩溃、剧烈发散,在Z=95.7mm位置处通过的电流与发射电流一致,表明该磁聚焦系统提供的聚焦磁力能够较好地抵消带状电子注自身的空间电荷力,从而避免了带状电子注的发散,这说明所设计的新型可调磁聚焦系统能够对带状电子注进行良好地聚焦,对于高增益、高功率毫米波及太赫兹带状注行波管的研制具有重要的价值。Further research shows that when the value of w increases from small to large, the By generated by the staggered second permanent magnets in the band-shaped electron injection area will change from large to small, and the broad side of the band-shaped electron injection will change from over-focusing to under-focusing. The invention can change the magnetic field By required for the broadside focusing of the band-shaped electron beamer by adjusting the spacing w of the staggered second permanent magnets. It is worth noting that, in the simulation calculation of the present invention, the transmission distance of the band-shaped electron injection in the magnetic field area is greater than 86mm, and the band-shaped electron injection does not collapse or diverge violently during the transmission process, and the current passing at the position of Z=95.7mm Consistent with the emission current, it shows that the focusing magnetic force provided by the magnetic focusing system can better offset the space charge force of the band electron beam itself, thereby avoiding the divergence of the band electron beam, which indicates that the designed new tunable magnetic focusing system The ability to focus the band electron beam well is of great value for the development of high-gain, high-power millimeter-wave and terahertz band-beam traveling wave tubes.
以上所述,仅为本发明的具体实施方式,本说明书中所公开的任一特征,除非特别叙述,均可被其他等效或具有类似目的的替代特征加以替换;所公开的所有特征、或所有方法或过程中的步骤,除了互相排斥的特征和/或步骤以外,均可以任何方式组合。The above descriptions are only specific embodiments of the present invention, and any feature disclosed in this specification, unless otherwise stated, can be replaced by other equivalent or alternative features with similar purposes; all the disclosed features, or All steps in a method or process, except mutually exclusive features and/or steps, may be combined in any way.
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