CN113690118B - Novel helix slow wave structure with variable pitch and variable inner diameter - Google Patents

Novel helix slow wave structure with variable pitch and variable inner diameter Download PDF

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CN113690118B
CN113690118B CN202110865762.8A CN202110865762A CN113690118B CN 113690118 B CN113690118 B CN 113690118B CN 202110865762 A CN202110865762 A CN 202110865762A CN 113690118 B CN113690118 B CN 113690118B
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wave structure
inner diameter
attenuator
pitch
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CN113690118A (en
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段兆云
张潽
黄思隆
王传超
江胜坤
张宣铭
王少萌
巩华荣
宫玉彬
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University of Electronic Science and Technology of China
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/16Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
    • H01J23/24Slow-wave structures, e.g. delay systems
    • H01J23/26Helical slow-wave structures; Adjustment therefor
    • H01J23/27Helix-derived slow-wave structures
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/16Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
    • H01J23/24Slow-wave structures, e.g. delay systems
    • H01J23/30Damping arrangements associated with slow-wave structures, e.g. for suppression of unwanted oscillations

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Abstract

The invention provides a variable-pitch and variable-inner-diameter helical line slow wave structure, and belongs to the technical field of vacuum electronics. The slow wave structure enables return wave oscillation and higher harmonics to be restrained by specifically changing the inner diameter and the thread pitch of the spiral line, and obtains higher efficiency of the traveling wave tube, the electronic efficiency can reach 16% when the output power of a Q wave band is saturated, and the electronic efficiency can reach 4% when the output power is backed off by 6 dB.

Description

一种变螺距变内径的新型螺旋线慢波结构A novel helical slow-wave structure with variable pitch and variable inner diameter

技术领域technical field

本发明属于真空电子技术领域,具体涉及一种变螺距变内径的新型螺旋线慢波结构。The invention belongs to the technical field of vacuum electronics, and in particular relates to a novel helical slow wave structure with variable pitch and variable inner diameter.

背景技术Background technique

随着电子通信技术的快速发展,通信系统对功率放大器件的频率和效率的要求越来越高,半导体器件由于自身散热问题、频率、效率、功率等的限制,目前难于满足未来通信系统的迫切需求,而行波管这类真空电子器件在这方面具有较大的优势。行波管作为一种末级功率放大器,广泛应用在雷达、电子对抗、通信、精确制导等电子装备中。With the rapid development of electronic communication technology, communication systems have higher and higher requirements on the frequency and efficiency of power amplifier devices. Semiconductor devices are currently difficult to meet the urgent needs of future communication systems due to their own heat dissipation, frequency, efficiency, and power limitations. demand, and vacuum electronic devices such as traveling wave tubes have great advantages in this regard. As a final stage power amplifier, traveling wave tube is widely used in electronic equipment such as radar, electronic countermeasures, communication, and precision guidance.

衡量行波管性能好坏的一个重要标准为行波管效率的高低。在未来通信系统中,由于功率放大器一般工作在线性区而不是饱和点,因此需要高频功率放大器在输出功率回退6dB时应同样具有高效率。研究者们采取了一系列不同的技术来提高行波管的效率。就目前而言,主要有以下两种方法:第一种是速度再同步技术;第二种是降压收集极技术。速度再同步技术指的是注波互作用趋于稳定时,通过改变相速度或者电子注速度来减小电子注与高频行波场之间必要的速度差,以此重新激励起有效注波互作用的一种技术。目前这种技术主要通过相速渐变法、相速跳变法和电压跳变法三种方法实现,考虑到加工实现的难度,尤其是在高频段情况下,相比于电压跳变,相速跳变和渐变是更加有效且容易实现的速度再同步方式。An important criterion for measuring the performance of the traveling wave tube is the efficiency of the traveling wave tube. In the future communication system, since the power amplifier generally works in the linear region rather than the saturation point, it is required that the high-frequency power amplifier should also have high efficiency when the output power is backed by 6dB. The researchers employed a series of different techniques to improve the efficiency of the TWT. For now, there are mainly the following two methods: the first is the speed resynchronization technology; the second is the step-down collector technology. Velocity resynchronization technology refers to reducing the necessary velocity difference between the electron beam and the high-frequency traveling wave field by changing the phase velocity or the electron beam velocity when the beam interaction tends to be stable, so as to re-excite the effective beam wave. A technique of interaction. At present, this technology is mainly realized by three methods: phase speed gradient method, phase speed jump method and voltage jump method. Considering the difficulty of processing, especially in the case of high frequency band, compared with voltage jump, phase speed jump and fades are a more efficient and easy way to resynchronize tempo.

Q波段螺旋线行波管由于其频率高、带宽宽、信号传输速率高的优点,将在未来通信系统中具有重要应用前景。针对螺旋线慢波结构,传统方法主要是通过螺距跳变和渐变,使得高频电磁场相速产生相应跳变和渐变来实现速度再同步,从而提高行波管的效率。然而,单纯的螺距变化的螺旋线慢波结构一方面很难抑制行波管存在的大功率返波振荡,无法保证行波管稳定工作;另一方面,该方法在提升行波管效率方面仍然不能满足未来通信系统对于输出功率回退6dB的效率需求。如专利CN20669744U公开了一种包含多渐变段的螺旋线行波管的慢波结构及其高频结构,其输入段和输出段的螺距均有改变,但其在Q波段43.5-46.5GHz的饱和电子效率为10.11%;2016年电子科技大学王凡的硕士学位论文“8-18GHz大功率螺旋线行波管的研究”中讨论了一种变螺距且变内径的螺旋线行波管,但其频段较低,仅是利用变内径结构来抑制返波振荡,而且与本专利所提出的变螺距变内径的办法完全不同。Due to its advantages of high frequency, wide bandwidth and high signal transmission rate, the Q-band helical traveling wave tube will have important application prospects in future communication systems. For the helical slow-wave structure, the traditional method mainly uses pitch jumps and gradients, so that the phase velocity of the high-frequency electromagnetic field produces corresponding jumps and gradients to achieve velocity resynchronization, thereby improving the efficiency of the traveling wave tube. However, the helical slow-wave structure with simple pitch change is difficult to suppress the high-power back-wave oscillation existing in the TWT, and cannot guarantee the stable operation of the TWT; on the other hand, this method still can improve the efficiency of the TWT. It cannot meet the efficiency requirement of the future communication system for the output power backoff of 6dB. For example, patent CN20669744U discloses a slow-wave structure and high-frequency structure of a helical traveling wave tube including multi-gradient sections. The electron efficiency is 10.11%; in 2016, Wang Fan's master's thesis "Research on 8-18GHz high-power helical traveling wave tube" discussed a variable pitch and variable inner diameter helical traveling wave tube, but its The frequency band is relatively low, and the variable inner diameter structure is only used to suppress the back wave oscillation, which is completely different from the method of changing the pitch and changing the inner diameter proposed in this patent.

因此,能够用于实现Q波段行波管高效率且有效抑制返波振荡的螺旋线慢波结构是亟需解决的关键问题。Therefore, the helical slow-wave structure that can be used to realize the high efficiency of the Q-band traveling wave tube and effectively suppress the back-wave oscillation is a key problem that needs to be solved urgently.

发明内容SUMMARY OF THE INVENTION

针对背景技术所存在的技术问题,本发明的目的在于提供一种变螺距变内径的新型螺旋线慢波结构。该慢波结构通过变化螺旋线的内径和螺距,使得返波振荡和高次谐波被抑制,并得到了较高的行波管效率,同时在输出功率回退6dB时也具有较高的效率。In view of the technical problems existing in the background art, the purpose of the present invention is to provide a novel helical slow-wave structure with variable pitch and variable inner diameter. By changing the inner diameter and pitch of the helix, the slow-wave structure suppresses the back-wave oscillation and higher harmonics, and obtains a higher efficiency of the traveling wave tube. At the same time, it also has a higher efficiency when the output power is backed by 6dB. .

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:

一种变螺距变内径的螺旋线慢波结构,包括螺旋线、衰减器、夹持杆和管壳;其中,螺旋线由三根分布均匀的夹持杆固定,夹持杆另一端固定于管壳上;A helical slow wave structure with variable pitch and variable inner diameter, comprising a helix, an attenuator, a clamping rod and a tube shell; wherein the helix is fixed by three evenly distributed clamping rods, and the other end of the clamping rod is fixed to the tube shell superior;

所述螺旋线包括输入段、输出段和切断区;所述切断区位于输入段与输出段之间,用于切断反馈途径;The spiral line includes an input section, an output section and a cut-off area; the cut-off area is located between the input section and the output section for cutting off the feedback path;

所述衰减器包括集中衰减器和分布衰减器;其中,集中衰减器设置于切断区的两侧,用于吸收反射波以及返波,分布衰减器设置于输入段区间,其作用为吸收反射波和返波;The attenuator includes a centralized attenuator and a distributed attenuator; wherein, the centralized attenuator is arranged on both sides of the cut-off area for absorbing reflected waves and returning waves, and the distributed attenuator is arranged in the input section, and its function is to absorb reflected waves and return waves;

所述输入段的螺距固定,内径渐变,且起始端处内径S1与切断区内径S2满足关系式S1=1.0769S2,电子注经过输入段的速度调制和密度调制后在输入段末端实现电子群聚,建立增长波;The pitch of the input segment is fixed, the inner diameter is gradually changing, and the inner diameter S 1 at the starting end and the diameter S 2 in the cut-off area satisfy the relationship S 1 =1.0769S 2 , and the electronic injection is at the end of the input segment after the speed modulation and density modulation of the input segment. To achieve electronic clustering and establish growth waves;

所述输出段的内径渐变,螺距跳变,输出段依次划分为相速增加段、负跳变段、正跳变段和相速降低段,各段的螺距对应为P1、P2、P3和P4,轴向长度分别为L2、L3、L4和L5,相速增加段用于对电子相位进行补偿,并对输入段末端的群聚电子进一步群聚,相速降低段将电子注的能量尽可能交给电磁场,完成能量输出;其中,P2=0.974P1,P3=1.026P1,P4=0.962P1,L2=0.22L,L3=0.08L,L4=0.2L,L5=0.087L;The inner diameter of the output section changes gradually, the pitch jumps, and the output section is divided into a phase speed increase section, a negative jump section, a positive jump section and a phase speed reduction section in turn, and the pitch of each section corresponds to P 1 , P 2 , P 3 and P 4 , the axial lengths are L 2 , L 3 , L 4 and L 5 respectively, the phase velocity increasing segment is used to compensate the electron phase, and the clustered electrons at the end of the input segment are further clustered, and the phase velocity decreases The segment transfers the energy of the electron injection to the electromagnetic field as much as possible to complete the energy output; among them, P 2 =0.974P 1 , P 3 =1.026P 1 , P 4 =0.962P 1 , L 2 =0.22L, L 3 =0.08L , L 4 =0.2L, L 5 =0.087L;

输入段和输出端螺旋线的内径在切断区相同,且两端处也相同,输入段和相速增加段的螺距相同,均为P1The inner diameter of the input section and the output end helix are the same in the cut-off area and at both ends, and the pitches of the input section and the phase velocity increasing section are the same, both of which are P 1 .

进一步地,所述输入段的轴向长度L1应满足关系式:L1=0.4L-0.413L,其中,L为慢波结构整体长度,为80-100mm。Further, the axial length L 1 of the input section should satisfy the relation: L 1 =0.4L-0.413L, where L is the overall length of the slow-wave structure, which is 80-100 mm.

进一步地,螺距P1的的长度优选为0.3-0.5mm。Further, the length of the pitch P1 is preferably 0.3-0.5 mm.

进一步地,所述切断区的轴向长度为1-2mm。Further, the axial length of the cutting area is 1-2 mm.

进一步地,所述分布衰减器设置一个或多个,使电子注经过输入段后的增益不超过26dB。Further, one or more distributed attenuators are set so that the gain of the electronic injector after passing through the input section does not exceed 26dB.

进一步地,所述分布衰减器和集中衰减器的衰减量不同。Further, the attenuation amounts of the distributed attenuator and the centralized attenuator are different.

本发明的机理为:输入段是利用其半径变化使高频场的相速变化,电子注经过这一段的速度调制和密度调制后在输入段末端实现电子群聚,建立增长波;输出段在螺旋线内径上都是渐变段,在螺距上进行跳变,对电子相位进行补偿并对输入段末端的群聚电子进一步群聚,并同时使电子注的能量尽可能交给电磁场,完成能量输出。考虑到行波管工作时电子注半径会在慢波结构后端逐渐增大,而电子注的填充比需要保持在一定范围内才能获得最佳的注波互作用效果,因此将慢波结构内径与电子注半径在某些区域同步增大,有利于高频场从电子注中获得更多的能量,从而提高效率。The mechanism of the invention is as follows: the input section uses its radius change to change the phase velocity of the high-frequency field, and the electron injection achieves electron clustering at the end of the input section after the speed modulation and density modulation of this section to establish a growing wave; the output section is in the The inner diameter of the helix is a gradient segment, and the pitch is jumped to compensate for the electron phase and further cluster the clustered electrons at the end of the input segment, and at the same time, the energy of the electron injection is given to the electromagnetic field as much as possible to complete the energy output. . Considering that the electron injection radius will gradually increase at the back end of the slow-wave structure when the TWT is working, and the filling ratio of the electron injection needs to be kept within a certain range to obtain the best injection-wave interaction effect, so the inner diameter of the slow-wave structure is Synchronized with the increase of the electron beam radius in some regions, it is beneficial for the high-frequency field to obtain more energy from the electron beam, thereby improving the efficiency.

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.本发明输出段的相速增加段设置为螺距负跳变后接正跳变的结构,这种结构有效抑制了高次谐波分量,使得群聚效果更好,极大地提高了行波管的电子效率。1. The phase velocity increasing section of the output section of the present invention is set to a structure with a negative pitch jump followed by a positive jump. This structure effectively suppresses high-order harmonic components, makes the clustering effect better, and greatly improves the traveling wave. Electronic efficiency of the tube.

2.本发明通过采用变螺距变内径的螺旋线慢波结构,其产生的变化相速使得返波振荡起振长度增加,从而有效抑制了行波管中的返波振荡,确保行波管在高增益下稳定工作。同时,输出段慢波结构内径在电子注半径逐渐增大的区域也相应增大,使得填充比保持在一个注波互作用效果较好的范围内,有利于得到更好的注波互作用效果从而提高行波管的电子效率。2. The present invention adopts a helical slow-wave structure with variable pitch and variable inner diameter, and the change of phase velocity generated by the variable phase speed increases the start-up length of the back-wave oscillation, thereby effectively suppressing the back-wave oscillation in the traveling wave tube and ensuring that the traveling wave tube is in Stable operation at high gain. At the same time, the inner diameter of the slow-wave structure in the output section also increases correspondingly in the region where the electron injection radius gradually increases, so that the filling ratio is kept within a range with a better injection-wave interaction effect, which is beneficial to obtain a better injection-wave interaction effect. Thus, the electronic efficiency of the traveling wave tube is improved.

3.本发明提出的螺旋线慢波结构适用于Q波段,即频率为36-40GHz,输出功率饱和时电子效率能达到16%,输出功率回退6dB时电子效率能达到4%。3. The spiral slow-wave structure proposed by the present invention is suitable for the Q-band, that is, the frequency is 36-40 GHz, the electronic efficiency can reach 16% when the output power is saturated, and the electronic efficiency can reach 4% when the output power is backed by 6dB.

附图说明Description of drawings

图1为实施例的单周期螺旋线慢波结构的视图;1 is a view of a single-period helical slow-wave structure of an embodiment;

其中,(a)为左视图,(b)为主视图,(c)为部分结构三维模型图。Among them, (a) is the left view, (b) is the main view, and (c) is the 3D model of the partial structure.

图2为本发明的慢波结构中螺旋线的示意图。FIG. 2 is a schematic diagram of the helix in the slow-wave structure of the present invention.

图3为实施例在39GHz工作时的波形图和频谱图;3 is a waveform diagram and a spectrogram of the embodiment when working at 39 GHz;

其中,(a)为波形图,(b)为频谱图。Among them, (a) is a waveform diagram, and (b) is a spectrogram.

图4为实施例中变螺距变内径的螺旋线行波管的输出功率示意图和电子效率示意图;4 is a schematic diagram of the output power and a schematic diagram of the electronic efficiency of the helical traveling wave tube with variable pitch and variable inner diameter in the embodiment;

其中,(a)为饱和时的输出功率和电子效率,(b)为输出功率回退6dB时的输出功率和电子效率。Among them, (a) is the output power and electron efficiency at saturation, (b) is the output power and electron efficiency when the output power is backed by 6dB.

图5为实施例中变螺距变内径的螺旋线行波管的增益示意图。FIG. 5 is a schematic diagram of the gain of the helical traveling wave tube with variable pitch and variable inner diameter in the embodiment.

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.

一种变螺距变内径的螺旋线慢波结构,包括螺旋线、衰减器、夹持杆和管壳;其结构视图如图1所示,其中,螺旋线由三根分布均匀的夹持杆固定,夹持杆另一端固定于管壳上,如图1中的(a)所示;A helical slow-wave structure with variable pitch and variable inner diameter, including a helix, an attenuator, a clamping rod and a tube shell; its structural view is shown in Figure 1, wherein the helix is fixed by three evenly distributed clamping rods, The other end of the clamping rod is fixed on the tube shell, as shown in (a) in Figure 1;

所述螺旋线包括输入段、输出段和切断区,其结构示意图如图2所示;The spiral line includes an input section, an output section and a cut-off area, and its schematic diagram is shown in Figure 2;

输入段,用于电子的速度调制和密度调制,其内径为渐变结构,用来抑制返波振荡,电子注经过输入段的速度调制和密度调制后在输入段末端实现电子群聚,建立增长波;The input segment is used for the velocity modulation and density modulation of electrons, and its inner diameter is a gradual structure to suppress the back-wave oscillation. After the velocity modulation and density modulation of the input segment, the electron injection realizes electron clustering at the end of the input segment and establishes a growing wave. ;

输出段,包括相速增加段、负跳变段、正跳变段和相速降低段;其中,相速增加段对电子相位进行补偿,并对进入输出段的群聚电子继续进行群聚,相速降低段将电子注的能量尽可能交给电磁场,完成能量输出;The output section includes a phase velocity increase section, a negative transition section, a positive transition section and a phase velocity reduction section; wherein, the phase velocity increase section compensates the electron phase, and continues to cluster the clustered electrons entering the output section, The phase velocity reduction section transfers the energy of the electron injection to the electromagnetic field as much as possible to complete the energy output;

切断区,位于输入段与输出段之间,其作用为切断反馈途径,抑制反射振荡。The cut-off area is located between the input section and the output section, and its function is to cut off the feedback path and suppress the reflection oscillation.

所述衰减器包括集中衰减器和分布衰减器;其中,集中衰减器设置于切断区的两侧,用于吸收反射波以及返波,分布衰减器设置于输入段区间,其作用也为吸收反射波和返波;衰减器为夹持杆上喷碳形成,其厚度和范围决定衰减量大小。The attenuator includes a centralized attenuator and a distributed attenuator; wherein, the centralized attenuator is arranged on both sides of the cut-off area to absorb reflected waves and returning waves, and the distributed attenuator is arranged in the input section, and its function is also to absorb reflections Wave and return wave; the attenuator is formed by spraying carbon on the clamping rod, and its thickness and range determine the amount of attenuation.

下面对本发明中各个部分进行具体介绍。Each part of the present invention will be described in detail below.

本发明中输入段,对应图2中的AB1段,该段进行电子的速度调制和密度调制,实现电子群聚,建立增长波。整段内径渐变从S1变化至S2,用以抑制返波振荡,内径S1与切断区内径S2满足如下关系式:S1=1.0769S2。AB1段螺距为P1,为使得电子注在AB1段得到良好的电子群聚效果,同时抑制返波振荡,输入段的轴向长度L1满足如下关系式:L1=0.4L-0.45L,经过仿真优化,本实施例取值为L1=0.4108L;In the present invention, the input section corresponds to the AB 1 section in FIG. 2 , and this section performs electron velocity modulation and density modulation to realize electron clustering and establish a growing wave. The inner diameter of the whole section is gradually changed from S 1 to S 2 to suppress the back-wave oscillation. The inner diameter S 1 and the diameter S 2 in the cut-off area satisfy the following relationship: S 1 =1.0769S 2 . The pitch of the AB 1 section is P 1 . In order to make the electron injection in the AB 1 section get a good electron clustering effect and suppress the return wave oscillation, the axial length L 1 of the input section satisfies the following relationship: L 1 =0.4L-0.45 L, after simulation optimization, the value of this embodiment is L 1 =0.4108L;

本发明中输出段对应B2F段,包括相速增加段,对应B2E段和相速降低段,对应EF段,其中相速增加段内设置有一螺距负跳变后接正跳变的结构,即B2C,CD,DE段,其作用是:抑制高次谐波分量,提高电子效率;其中,相速增加段变化的螺距和分布决定电子注与空间电荷波的耦合程度,B2C,CD,DE段对应螺距分别为:P1,P2,P3,轴向长度分别为:L2,L3,L4,满足如下关系式:P2=0.974P1,P3=1.026P1,L2=0.22L,L3=0.08L,L4=0.2L;In the present invention, the output section corresponds to the B 2 F section, including the phase velocity increasing section, corresponding to the B 2 E section and the phase velocity decreasing section, corresponding to the EF section, wherein the phase velocity increasing section is provided with a pitch negative jump followed by a positive jump. structure, namely B 2 C, CD, DE segments, its function is to suppress high-order harmonic components and improve electron efficiency; among them, the pitch and distribution of changes in the phase velocity increase segment determine the degree of coupling between electron injection and space charge wave, B 2 The corresponding pitches of C, CD and DE sections are: P 1 , P 2 , P 3 , and the axial lengths are: L 2 , L 3 , L 4 , which satisfy the following relationship: P 2 =0.974P 1 , P 3 =1.026P 1 , L 2 =0.22L, L 3 =0.08L, L 4 =0.2L;

输出段中的相速降低段对应EF段,其螺距为P4,轴向长度为L5,满足如下关系式:P4=0.962P1,L5=0.087L;The phase velocity reduction section in the output section corresponds to the EF section, the pitch is P 4 , and the axial length is L 5 , which satisfies the following relationship: P 4 =0.962P 1 , L 5 =0.087L;

切断区位于输入段与输出段之间,为1mm,作用是切断反馈途径,抑制自激振荡,包括反射振荡和返波振荡。The cut-off area is located between the input section and the output section, and is 1 mm in size. The function is to cut off the feedback path and suppress the self-excited oscillation, including reflection oscillation and return oscillation.

输入段和输出端的螺旋线的内径在切断区相同,且两端处也相同,输入段和相速增加段的螺距相同,均为P1,其中,L为80-100mm,P1为0.3-0.5mm。The inner diameter of the helix at the input section and the output end is the same in the cut-off area and at both ends. The pitch of the input section and the phase velocity increasing section are the same, both are P 1 , where L is 80-100mm, and P 1 is 0.3- 0.5mm.

根据本发明实施例所示的变螺距变内径的螺旋线慢波结构,利用三维PIC仿真软件进行仿真优化,在注电压为8500V,注电流为0.06A,周期聚焦磁场(峰值~0.4T)的条件下,其仿真结果如图3-5所示。图3为本发明慢波结构在39GHz工作时的波形图和频谱图;其中,(a)为波形图,(b)为频谱图。如图3中的(a)所示,输出波形在5ns时基本达到稳定不再有大的波动,对应的频谱图如图3中的(b),表明频谱较为纯净无其他杂波峰值,返波振荡和反射振荡被很好地抑制。图4为实施例中变螺距变内径的螺旋线行波管的饱和输出功率示意图和电子效率示意图,如图所示在36GHz-40GHz的频率范围内,其饱和输出功率大于84W,对应电子效率超过16.47%,输出功率回退至6dB左右时,其输出功率在20W以上,对应电子效率高于4%,实现了高效率。图5为实施例中变螺距变内径的螺旋线行波管的增益示意图,其工作频带内饱和增益超过46.69dB,输出回退6dB时增益超过55.5dB。总的来说,本发明实现了抑制返波振荡和反射振荡,同时具有较高的电子效率和输出功率。According to the spiral slow-wave structure with variable pitch and variable inner diameter shown in the embodiment of the present invention, the three-dimensional PIC simulation software is used for simulation optimization. When the injection voltage is 8500V, the injection current is 0.06A, and the periodic focusing magnetic field (peak value ~ 0.4T) Under the conditions, the simulation results are shown in Figure 3-5. 3 is a waveform diagram and a spectrogram of the slow-wave structure of the present invention when it operates at 39 GHz; wherein (a) is a waveform diagram, and (b) is a spectrogram. As shown in (a) in Figure 3, the output waveform is basically stable at 5ns and no longer has large fluctuations. The corresponding spectrogram is shown in (b) in Figure 3, indicating that the spectrum is relatively pure and has no other clutter peaks. Wave oscillations and reflection oscillations are well suppressed. 4 is a schematic diagram of the saturated output power and the schematic diagram of the electronic efficiency of the spiral traveling wave tube with variable pitch and variable inner diameter in the embodiment. As shown in the figure, in the frequency range of 36GHz-40GHz, the saturated output power is greater than 84W, and the corresponding electronic efficiency exceeds 16.47%, when the output power falls back to about 6dB, the output power is above 20W, and the corresponding electronic efficiency is higher than 4%, achieving high efficiency. 5 is a schematic diagram of the gain of the helical traveling wave tube with variable pitch and variable inner diameter in the embodiment, the saturation gain in the working frequency band exceeds 46.69dB, and the gain exceeds 55.5dB when the output backs off by 6dB. In general, the present invention achieves suppression of back-wave oscillation and reflection oscillation, while having higher electronic efficiency and output power.

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.

Claims (6)

1.一种变螺距变内径的螺旋线慢波结构,其特征在于,所述螺旋线慢波结构包括螺旋线、衰减器、夹持杆和管壳;其中,螺旋线由三根分布均匀的夹持杆固定,夹持杆另一端固定于管壳上;1. a helical slow wave structure with variable pitch and variable inner diameter, characterized in that, the helical slow wave structure comprises a helix, an attenuator, a clamping rod and a tube shell; wherein, the helix is composed of three evenly distributed clamps. The holding rod is fixed, and the other end of the clamping rod is fixed on the tube shell; 所述螺旋线包括输入段、输出段和切断区;所述切断区位于输入段与输出段之间,用于切断反馈途径;The spiral line includes an input section, an output section and a cut-off area; the cut-off area is located between the input section and the output section for cutting off the feedback path; 所述衰减器包括集中衰减器和分布衰减器;其中,集中衰减器设置于切断区的两侧,用于吸收反射波以及返波,分布衰减器设置于输入段区间,其作用为吸收反射波和返波;The attenuator includes a centralized attenuator and a distributed attenuator; wherein, the centralized attenuator is arranged on both sides of the cut-off area for absorbing reflected waves and returning waves, and the distributed attenuator is arranged in the input section, and its function is to absorb reflected waves and return waves; 所述输入段的螺距固定,内径渐变,且起始端处内径S1与切断区内径S2满足关系式S1=1.0769S2,电子注经过输入段的速度调制和密度调制后在输入段末端实现电子群聚,建立增长波;The pitch of the input section is fixed, the inner diameter is gradually changing, and the inner diameter S 1 at the starting end and the diameter S 2 in the cut-off area satisfy the relationship S 1 =1.0769S 2 , and the electronic injection is at the end of the input section after the speed modulation and density modulation of the input section. To achieve electronic clustering and establish growth waves; 所述输出段的内径渐变,螺距跳变,输出段依次划分为相速增加段、负跳变段、正跳变段和相速降低段,各段的螺距对应为P1、P2、P3和P4,轴向长度分别为L2、L3、L4和L5,相速增加段用于对电子相位进行补偿,并对输入段末端的群聚电子进一步群聚,相速降低段将电子注的能量尽可能交给电磁场,完成能量输出;其中,P2=0.974P1,P3=1.026P1,P4=0.962P1,L2=0.22L,L3=0.08L,L4=0.2L,L5=0.087L,L为慢波结构整体长度;The inner diameter of the output section changes gradually, the pitch jumps, and the output section is divided into a phase speed increase section, a negative jump section, a positive jump section and a phase speed reduction section in turn, and the pitch of each section corresponds to P 1 , P 2 , P 3 and P 4 , the axial lengths are L 2 , L 3 , L 4 and L 5 respectively, the phase velocity increasing segment is used to compensate the electron phase, and the clustered electrons at the end of the input segment are further clustered, and the phase velocity decreases The segment transfers the energy of the electron injection to the electromagnetic field as much as possible to complete the energy output; among them, P 2 =0.974P 1 , P 3 =1.026P 1 , P 4 =0.962P 1 , L 2 =0.22L, L 3 =0.08L , L 4 =0.2L, L 5 =0.087L, L is the overall length of the slow-wave structure; 输入段和输出端螺旋线的内径在切断区相同,且在两端处也相同,输入段和相速增加段的螺距相同,均为P1The inner diameter of the input section and the output end helix are the same in the cut-off area and at both ends, and the pitches of the input section and the phase velocity increasing section are the same, both P 1 . 2.如权利要求1所述的螺旋线慢波结构,其特征在于,所述输入段的轴向长度L1应满足关系式:L1=0.4L-0.413L,其中,L为慢波结构整体长度,为80-100mm。2 . The helical slow-wave structure according to claim 1 , wherein the axial length L 1 of the input section should satisfy the relation: L 1 =0.4L-0.413L, wherein L is the slow-wave structure. 3 . The overall length is 80-100mm. 3.如权利要求1所述的螺旋线慢波结构,其特征在于,螺距P1的长度为0.3-0.5mm。3 . The helical slow wave structure according to claim 1 , wherein the length of the pitch P 1 is 0.3-0.5 mm. 4 . 4.如权利要求1所述的螺旋线慢波结构,其特征在于,所述切断区的轴向长度为1-2mm。4 . The helical slow wave structure according to claim 1 , wherein the axial length of the cut-off region is 1-2 mm. 5 . 5.如权利要求1所述的螺旋线慢波结构,其特征在于,所述分布衰减器设置一个或多个,用于使电子注经过输入段后的增益不超过26dB。5 . The helical slow-wave structure according to claim 1 , wherein one or more distributed attenuators are provided, so that the gain of the electron injector after passing through the input section does not exceed 26 dB. 6 . 6.如权利要求1所述的螺旋线慢波结构,其特征在于,所述分布衰减器和集中衰减器的衰减量不同。6 . The helical slow wave structure according to claim 1 , wherein the distributed attenuator and the concentrated attenuator have different attenuations. 7 .
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