CN109751212B - Pulsed plasma thruster with microporous insulated anode - Google Patents
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Abstract
Description
技术领域technical field
本发明涉及微小卫星推进器技术领域,具体涉及一种带有微孔绝缘阳极的脉冲等离子推进器。The invention relates to the technical field of microsatellite thrusters, in particular to a pulsed plasma thruster with a microporous insulating anode.
背景技术Background technique
随着微小卫星技术的发展,对其推进系统提出了新的要求,需要其能够实现高比冲,高效率的输出。电推进系统由于自身结构及功能上的优势逐渐取代了传统的化学推进系统而成为微小卫星系统的主要推进方式。由于脉冲等离子体推进器具有结构简单,质量轻,比冲高等特点,受到全世界越来越多的关注。With the development of microsatellite technology, new requirements are put forward for its propulsion system, which requires it to achieve high specific impulse and high efficiency output. The electric propulsion system has gradually replaced the traditional chemical propulsion system due to its advantages in structure and function, and has become the main propulsion method of the microsatellite system. Due to its simple structure, light weight and high specific impulse, pulsed plasma thrusters have attracted more and more attention around the world.
传统的脉冲等离子体推进器采用裸金属放电电极结构。但是生成的大部分等离子体在外电场的作用下进入金属电极,形成了电路电流。只有少部分等离子体从电极外喷射出去形成推力。因此,基于前期研究,本文提出了一种带有微孔绝缘阳极的脉冲等离子体推进器。微孔的存在不影响等离子体生成,并且减小了进入阳极的带电粒子数量,使更多的带电粒子形成定向喷射,提高了脉冲等离子体推进器的效率。Conventional pulsed plasma thrusters use a bare metal discharge electrode structure. However, most of the generated plasma enters the metal electrode under the action of an external electric field, forming a circuit current. Only a small part of the plasma is ejected from the electrode to form thrust. Therefore, based on the previous research, this paper proposes a pulsed plasma thruster with a microporous insulating anode. The existence of micropores does not affect the plasma generation, and reduces the number of charged particles entering the anode, allowing more charged particles to form a directional jet, improving the efficiency of the pulsed plasma thruster.
文献“田甲,刘文正,崔伟胜,高永杰.Generation characteristics of a metalion plasma jet in vacuum discharge[J].Plasma Science and Technology,2018,20:1-7.”中提出了一种全绝缘阳极电极结构,阻碍了放电生成的带电粒子运动到电极的通道,从而使得更多的等离子体沿绝缘套筒喷射出去,提高了等离子体源的密度和传播速度。但是,与传统的裸金属阳极电极结构相比,采用全绝缘阳极电极结构放电生成的阴极电流幅值减小。从放电现象上来看,等离子的喷射长度没有明显增加。The literature "Tian Jia, Liu Wenzheng, Cui Weisheng, Gao Yongjie. Generation characteristics of a metalion plasma jet in vacuum discharge[J]. Plasma Science and Technology, 2018, 20: 1-7." proposed a fully insulated anode electrode structure, The passage of the charged particles generated by the discharge is hindered from moving to the electrode, so that more plasma is ejected along the insulating sleeve, and the density and propagation speed of the plasma source are increased. However, compared with the traditional bare metal anode electrode structure, the cathode current amplitude generated by the discharge with the fully insulated anode electrode structure is reduced. From the discharge phenomenon point of view, the plasma jet length does not increase significantly.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于提供一种能够不影响等离子体生成的前提下,提高等离子体源的密度和喷射速度的带有微孔绝缘阳极的平板型脉冲等离子推进器,以解决上述背景技术中存在的在真空放电过程中等离子体源的密度不高,能量低的技术问题。The purpose of the present invention is to provide a flat-plate pulsed plasma thruster with a microporous insulating anode, which can improve the density and ejection speed of the plasma source without affecting the plasma generation, so as to solve the problems existing in the above-mentioned background technology. In the process of vacuum discharge, the density of the plasma source is not high and the energy is low.
为了实现上述目的,本发明采取了如下技术方案:In order to achieve the above object, the present invention has adopted the following technical solutions:
一种带有微孔绝缘阳极的脉冲等离子推进器,包括阴极、套设在所述阴极上的绝缘套筒、以及固定套设在所述绝缘套筒前端的阳极;A pulsed plasma thruster with a microporous insulating anode, comprising a cathode, an insulating sleeve sleeved on the cathode, and an anode fixed sleeved on the front end of the insulating sleeve;
所述阴极的前端设有放电端,所述阳极包括直筒部和喇叭开口部;The front end of the cathode is provided with a discharge end, and the anode includes a straight cylinder portion and a horn opening portion;
所述直筒部的内表面与所述绝缘套筒的外表面相连接;所述阳极上未与所述绝缘套筒相接触的部分包裹有阳极绝缘层;The inner surface of the straight cylindrical portion is connected with the outer surface of the insulating sleeve; the part of the anode that is not in contact with the insulating sleeve is wrapped with an anode insulating layer;
所述喇叭开口部内表面的绝缘层上设有微孔;Micro-holes are provided on the insulating layer on the inner surface of the horn opening;
所述阴极的平板端电连接外电路负高压端子,所述阳极接地。The flat plate end of the cathode is electrically connected to the negative high-voltage terminal of the external circuit, and the anode is grounded.
优选地,所述阴极为板状。Preferably, the cathode is plate-shaped.
优选地,所述放电端为设于所述板状阴极前端的突起形状。Preferably, the discharge end is in the shape of a protrusion provided at the front end of the plate-shaped cathode.
优选地,所述阴极的平板端表面与所述绝缘套筒的内壁相接触。Preferably, the flat plate end surface of the cathode is in contact with the inner wall of the insulating sleeve.
优选地,所述微孔位于所述喇叭开口部内表面的绝缘层的几何中心。Preferably, the micro-hole is located at the geometric center of the insulating layer on the inner surface of the horn opening.
优选地,所述阴极由导磁金属材料制成,所述放电端由铅制成。Preferably, the cathode is made of magnetic conductive metal material, and the discharge end is made of lead.
优选地,所述阳极由铜材料制成。Preferably, the anode is made of copper material.
优选地,所述绝缘套筒由陶瓷材料制成。Preferably, the insulating sleeve is made of ceramic material.
优选地,所述阳极绝缘层由特氟龙材料制成。Preferably, the anode insulating layer is made of Teflon material.
优选地,所述微孔为圆形。Preferably, the micropores are circular.
本发明有益效果:通过绝缘套筒对阴极生成的等离子体进行阻挡及束缚,提高了等离子体定向喷射的能力;在阳极内表面设置有微孔,微孔的存在不影响等离子体生成条件下,减小了进入阳极的带电粒子数量,使更多的带电粒子形成定向喷射出去形成推力,提高了脉冲等离子体推进器的效率。The beneficial effects of the invention are as follows: the plasma generated by the cathode is blocked and bound by the insulating sleeve, which improves the ability of directional spraying of the plasma; the inner surface of the anode is provided with micropores, and the existence of the micropores does not affect the plasma generation conditions, The number of charged particles entering the anode is reduced, so that more charged particles are ejected in a directional manner to form thrust, and the efficiency of the pulse plasma thruster is improved.
本发明附加的方面和优点将在下面的描述中部分给出,这些将从下面的描述中变得明显,或通过本发明的实践了解到。Additional aspects and advantages of the present invention will be set forth in part in the following description, which will be apparent from the following description, or may be learned by practice of the present invention.
附图说明Description of drawings
为了更清楚地说明本发明实施例的技术方案,下面将对实施例描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to illustrate the technical solutions of the embodiments of the present invention more clearly, the following briefly introduces the accompanying drawings used in the description of the embodiments. Obviously, the drawings in the following description are only some embodiments of the present invention. For those of ordinary skill in the art, other drawings can also be obtained from these drawings without any creative effort.
图1为本发明实施例所述的带有微孔绝缘阳极的脉冲等离子推进器结构图。FIG. 1 is a structural diagram of a pulsed plasma thruster with a microporous insulating anode according to an embodiment of the present invention.
图2为本发明实施例所述的带有微孔绝缘阳极的脉冲等离子推进器的放电电路图。FIG. 2 is a discharge circuit diagram of a pulsed plasma thruster with a microporous insulating anode according to an embodiment of the present invention.
图3为本发明实施例所述的没有包裹阳极绝缘层的非绝缘阳极等离子推进器结构图。FIG. 3 is a structural diagram of a non-insulated anode plasma thruster without an anode insulating layer wrapped according to an embodiment of the present invention.
图4为本发明实施例所述的在阳极绝缘层未设置微孔等离子推进器结构图。FIG. 4 is a structural diagram of the plasma thruster without microporous provided in the anode insulating layer according to the embodiment of the present invention.
图5为本发明实施例测得的用非绝缘阳极和带有微孔的绝缘阳极生成的等离子体密度分布情况图。FIG. 5 is a graph showing the distribution of plasma density generated by using a non-insulated anode and an insulated anode with micropores measured in an embodiment of the present invention.
图6为本发明实施例测得的用非绝缘阳极和带有微孔的绝缘阳极生成的等离子体传播速度图。FIG. 6 is a graph of the propagation velocity of plasma generated by using a non-insulated anode and an insulated anode with micropores measured in an embodiment of the present invention.
图7为本发明实施例测得的不同绝缘微孔下的等离子体密度分布情况图。FIG. 7 is a graph showing the distribution of plasma density under different insulating micropores measured in an embodiment of the present invention.
图8为本发明实施例测得的不同绝缘微孔下的等离子体传播速度分布情况图。FIG. 8 is a graph showing the distribution of plasma propagation velocity under different insulating micropores measured in an embodiment of the present invention.
其中:1-阴极;2-绝缘套筒;3-阳极;31-直筒部;32-喇叭开口部;4-阳极绝缘层;5-微孔;6-放电端。Wherein: 1-cathode; 2-insulating sleeve; 3-anode; 31-straight cylinder part; 32-horn opening part; 4-anode insulating layer; 5-micropore; 6-discharge end.
具体实施方式Detailed ways
下面详细叙述本发明的实施方式,所述实施方式的示例在附图中示出,其中自始至终相同或类似的标号表示相同或类似的元件或具有相同或类似功能的元件。下面通过附图描述的实施方式是示例性的,仅用于解释本发明,而不能解释为对本发明的限制。Embodiments of the present invention are described in detail below, examples of which are illustrated in the accompanying drawings, wherein the same or similar reference numerals refer to the same or similar elements or elements having the same or similar functions throughout. The embodiments described below through the accompanying drawings are exemplary and are only used to explain the present invention, but not to be construed as a limitation of the present invention.
本技术领域技术人员可以理解,除非特意声明,这里使用的单数形式“一”、“一个”、“所述”和“该”也可包括复数形式。应该进一步理解的是,本发明的说明书中使用的措辞“包括”是指存在所述特征、整数、步骤、操作、元件和/或组件,但是并不排除存在或添加一个或多个其他特征、整数、步骤、操作、元件和/或它们的组。应该理解,这里使用的“连接”或“耦接”可以包括无线连接或耦接,使用的措辞“和/或”包括一个或更多个相关联的列出项的任一单元和全部组合。It will be understood by those skilled in the art that the singular forms "a", "an", "the" and "the" as used herein can include the plural forms as well, unless expressly stated otherwise. It should be further understood that the word "comprising" used in the description of the present invention refers to the presence of stated features, integers, steps, operations, elements and/or components, but does not exclude the presence or addition of one or more other features, Integers, steps, operations, elements and/or groups thereof. It should be understood that "connected" or "coupled" as used herein can include wirelessly connected or coupled, and that use of the term "and/or" includes any and all combinations of one or more of the associated listed items.
本技术领域技术人员可以理解,除非另外定义,这里使用的所有术语(包括技术术语和科学术语)具有与本发明所属领域中的普通技术人员的一般理解相同的意义。还应该理解的是,诸如通用字典中定义的那些术语应该被理解为具有与现有技术的上下文中的意义一致的意义,并且除非像这里一样定义,不会用理想化或过于正式的含义来解释。It will be understood by those skilled in the art that, unless otherwise defined, all terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this invention belongs. It should also be understood that terms such as those defined in general dictionaries should be understood to have meanings consistent with their meanings in the context of the prior art and, unless defined as herein, are not to be taken in an idealized or overly formal sense. explain.
为便于理解本发明,下面结合附图以具体实施例对本发明作进一步解释说明,且具体实施例并不构成对本发明实施例的限定。In order to facilitate the understanding of the present invention, the present invention will be further explained and described below with reference to the accompanying drawings with specific embodiments, and the specific embodiments do not constitute limitations to the embodiments of the present invention.
本领域技术人员应该理解,附图只是实施例的示意图,附图中的部件并不一定是实施本发明所必须的。Those skilled in the art should understand that the accompanying drawings are only schematic diagrams of the embodiments, and the components in the accompanying drawings are not necessarily necessary to implement the present invention.
实施例Example
如图1所示,本发明实施例提供了一种带有微孔绝缘阳极的脉冲等离子推进器,包括阴极1、套设在所述阴极上的绝缘套筒2、阳极3、阳极绝缘层4以及微孔5,所述阴极1为平板状,所述阴极1的前端设有放电端6,所述阳极3为固定套设于所述绝缘套筒2外壁上的立方体筒状结构,所述阳极3的前端制成喇叭口状,形成喇叭开口部32,阳极3的直筒部31的内表面与绝缘套筒2的外表面接触。阳极3表面由阳极绝缘层4包裹,只有在喇叭开口部32绝缘层内表面设置有微孔5。As shown in FIG. 1 , an embodiment of the present invention provides a pulsed plasma thruster with a microporous insulating anode, including a
所述阴极1的平板端电连接外电路负高压端子,所述阳极3接地。The flat plate end of the
所述放电端6为设于所述板状阴极1前端的突起形状。The
在实际应用中,所述放电端6的形状可以为楔形、弧形、立方体形等有突起的形状。所述放电端6的具体形状并不受上述形状的限制,其形状由本领域技术人员可根据实际情况具体设置。In practical applications, the shape of the
所述阴极1的平板端表面与所述绝缘套筒2的内壁相接触。The flat end surface of the
所述微孔5位于所述喇叭开口部32内表面的绝缘层4的几何中心。The micro-hole 5 is located at the geometric center of the insulating
所述阴极1由导磁金属材料制成,所述放电端6由铅制成。The
在实际应用中,所述放电端6并不受上述铅材料的限制,本领域技术人员可根据实际情况具体选择放电端6的制作材料。In practical applications, the
所述阳极3由铜材料制成。The
所述绝缘套筒2由陶瓷材料制成。The insulating
所述阳极绝缘层4由特氟龙材料制成。The
所述微孔5为圆形。The micropores 5 are circular.
如图1所示,本发明实施例所述的带有微孔绝缘阳极的脉冲等离子推进器包括平板型阴极1,阴极1的前端放电端6制成楔形,用来束缚生成的等离子体的绝缘筒2和包裹阳极3的带有微孔5的阳极绝缘层4,以及阳极3。As shown in FIG. 1 , the pulsed plasma thruster with a microporous insulating anode according to the embodiment of the present invention includes a
阴极放电端6的长度和厚度之比为4:3-1:1,本实施例中具体为长度/厚度=2:1。所述阴极1的平板状部分的材质采用铁质良导磁特性金属。The ratio of the length to the thickness of the
所述板状阳极3通过金属导线连接到地,且阳极3被带有微孔5的阳极绝缘层包裹。The plate-shaped
为便于理解,下面给出一组放电电极的详细尺寸。阴极1的放电端采用铅金属,阴极总长为24mm,阴极1的平板状部分的长度:宽度:厚度=20mm:5mm:2mm,楔形放电端的长度为4mm,放电端顶端的宽度:厚度=:5mm:2mm。阳极3的平板状部分的长度:宽度:厚度=4mm:5mm:2mm,喇叭状部分的长度为10mm,开口角度是30度,材料为金属铜。阳极绝缘层的厚度为2mm。微孔5位于喇叭状阳极内表面的几何中心处,微孔5为圆柱型,半径为0.5mm。For ease of understanding, detailed dimensions of a set of discharge electrodes are given below. The discharge end of the
阴极1与外部放电电路的负高压端子相连接。放电电源采用脉冲放电形式,其具体放电电路如图2所示。220V交流电源,经过变压器升压,倍压整流电路变换后给电容C2充电。当给三点间隙施加点火脉冲时,三点间隙导通,经C2、27Ω电阻、240μH电感和真空间隙构成回路,真空间隙击穿产生放电现象。阴极通过接线柱接电源高压端,阳极通过导线接地。The
图5为采用如图3所示的非绝缘阳极电极和微孔直径为1mm时的微孔绝缘阳极电极放电生成的等离子体的密度分布图。由图5可知,与非阳极绝缘型电极相比,采用微孔绝缘阳极电极生成的等离子体密度较大。说明利用微孔绝缘阳极电极结构可以获得更高密度的等离子体源。FIG. 5 is a graph showing the density distribution of plasma generated by discharge using the non-insulated anode electrode shown in FIG. 3 and the microporous insulated anode electrode with a microporous diameter of 1 mm. It can be seen from Fig. 5 that the plasma density generated by the microporous insulating anode electrode is higher than that of the non-anodic insulating electrode. It shows that a higher density plasma source can be obtained by using the microporous insulating anode electrode structure.
图6为采用如图3所示的非绝缘阳极电极和微孔直径为1mm时的微孔绝缘阳极电极放电生成的等离子体的传播速度分布图。由图6可知,与非阳极绝缘型电极相比,采用微孔绝缘阳极电极生成的等离子体传播速度较大。说明利用微孔绝缘阳极电极结构可以获得更高能量的等离子体源。FIG. 6 is a graph showing the propagation velocity distribution of plasma generated by discharge using the non-insulated anode electrode as shown in FIG. 3 and the microporous insulated anode electrode when the microporous diameter is 1 mm. It can be seen from Fig. 6 that the propagation velocity of the plasma generated by the microporous insulating anode electrode is higher than that of the non-anodic insulating electrode. It shows that a higher energy plasma source can be obtained by using the microporous insulating anode electrode structure.
对比试验Comparative Test
试验1、带有三种不同阳极的电极结构放电后等离子体生成效果测试试验:
在放电实验过程中,对带有三种不同阳极的电极结构进行了放电实验研究,三种电极结构分别是如图3所示的阳极裸露的非绝缘阳极结构、如图4所示的绝缘阳极结构及如图1所示的微孔绝缘阳极结构。对于裸金属阳极电极结构,阴极1采用铅金属,阴极总长为24mm,阴极1的平板状部分的长度:宽度:厚度=20mm:5mm:2mm,楔形放电端的长度为4mm,放电端顶端的宽度:厚度=:5mm:2mm。阳极3的平板状部分的长度:宽度:厚度=4mm:5mm:2mm,喇叭状部分的长度为10mm,开口角度是30度,材料为金属铜。相比较而言,对于绝缘阳极电极结构,起包裹阳极作用的绝缘层4的材料为EVA,阳极绝缘层的厚度为2mm。而对于微孔绝缘阳极电极结构,微孔5位于喇叭状阳极内表面的几何中心处,微孔5为圆柱型,半径为0.5mm。During the discharge experiment, the electrode structure with three different anodes was studied. The three electrode structures are the non-insulated anode structure with exposed anode as shown in Fig. And the microporous insulating anode structure shown in Figure 1. For the bare metal anode electrode structure, the
采用带有不同阳极结构的脉冲等离子体推进器放电,实验测得的等离子体生成效果对比如表1所示。Using pulsed plasma thrusters with different anode structures to discharge, the experimentally measured plasma generation effects are shown in Table 1.
表1不同阳极结构下的等离子体测量结果Table 1 Plasma measurement results under different anode structures
由表1中的参数可知,在相等的放电电压条件下,非绝缘阳极电极结构放电时的阴极电流幅值为112A,阳极电流幅值为60A。阳极电流幅值只占阴极电流幅值的53%,分析可知,这是由于放电生成的部分电子沿绝缘套筒轴向喷射出去而没有进入阳极所造成的。全绝缘阳极电极结构放电时的阴极电流幅值为86A;由于阳极金属被EVA绝缘材料全部包裹,因而测得的阳极电流幅值为0。而微孔绝缘阳极电极结构放电时的阴极电流幅值为112A,阳极电流幅值为48A。It can be seen from the parameters in Table 1 that under the condition of equal discharge voltage, the cathode current amplitude is 112A and the anode current amplitude is 60A when the non-insulated anode electrode structure discharges. The anode current amplitude only accounts for 53% of the cathode current amplitude. The analysis shows that this is because part of the electrons generated by the discharge are ejected along the axial direction of the insulating sleeve and do not enter the anode. When the fully insulated anode electrode structure discharges, the cathode current amplitude is 86A; since the anode metal is completely wrapped by the EVA insulating material, the measured anode current amplitude is 0. While the microporous insulated anode electrode structure discharges the cathode current amplitude is 112A, the anode current amplitude is 48A.
由等离子体测量参数可知,非绝缘阳极电极结构放电生成的等离子体射流的密度峰值最低,传播速度最小;采用绝缘阳极电极结构生成的等离子体的射流长度没有明显提高。与非绝缘阳极电极结构相比,用带有微孔的绝缘层包裹金属阳极后,生成的等离子体射流的密度峰值、传播速度分别提高为原来的8.9倍、1.30倍。综上可知,阳极绝缘层上微孔结构的存在提高了等离子体射流的性能。It can be seen from the plasma measurement parameters that the density peak of the plasma jet generated by the discharge of the non-insulated anode electrode structure is the lowest and the propagation velocity is the smallest; the jet length of the plasma generated by the insulated anode electrode structure is not significantly improved. Compared with the non-insulated anode electrode structure, after wrapping the metal anode with an insulating layer with micropores, the peak density and propagation speed of the generated plasma jet are increased by 8.9 times and 1.30 times, respectively. In conclusion, the existence of the microporous structure on the anode insulating layer improves the performance of the plasma jet.
试验2、微孔尺寸对电极等离子体生成效果影响的测试:
在放电实验过程中。基于微孔绝缘阳极电极结构,探究微孔尺寸对等离子体生成效果的影响,等离子体生成效果如表2所示。during the discharge experiment. Based on the structure of the microporous insulating anode electrode, the effect of the micropore size on the plasma generation effect was explored. The plasma generation effect is shown in Table 2.
表2不同微孔尺寸下的等离子体测量结果Table 2 Plasma measurement results under different micropore sizes
由表2中的参数可知,微孔尺寸对电极间放电电压幅值、阴极电流幅值无明显影响。但是微孔尺寸减小,阳极电流的幅值明显减小。分析可知,采用较小微孔尺寸的绝缘阳极电极结构,减少了进入电极的带电粒子数量。From the parameters in Table 2, it can be seen that the size of the micropores has no significant effect on the amplitude of the discharge voltage between the electrodes and the amplitude of the cathode current. However, the size of the micropores is reduced, and the amplitude of the anode current is significantly reduced. The analysis shows that the use of an insulated anode electrode structure with a smaller pore size reduces the number of charged particles entering the electrode.
结合图7至图8可知,当微孔直径从3.0mm减小为0.2mm时,等离子体的密度、传播速度、射流长度分别增大为原来的3.3倍、3.56倍、228倍。因此,采用较小微孔的绝缘阳极电极结构,提高了生成的等离子体喷射性能。7 to 8, it can be seen that when the diameter of the micropore is reduced from 3.0 mm to 0.2 mm, the density, propagation velocity and jet length of the plasma increase by 3.3 times, 3.56 times and 228 times, respectively. Therefore, the use of an insulated anode electrode structure with smaller micropores improves the resulting plasma spray performance.
综上所述,本发明的带有微孔绝缘阳极的电极结构,在不影响等离子体生成的前提下,减少了进入电极的带电粒子数量,使更多的等离子体喷射出去形成推力源,提高了等离子体的喷射性能。To sum up, the electrode structure with the microporous insulating anode of the present invention reduces the number of charged particles entering the electrode without affecting the generation of plasma, so that more plasma is ejected to form a thrust source, and the the ejection performance of the plasma.
采用较小尺寸的微孔结构,可以进一步减少等离子体的损失,提高等离子体源的密度和传播速度。By adopting a microporous structure with a smaller size, the loss of the plasma can be further reduced, and the density and propagation speed of the plasma source can be improved.
本领域普通技术人员可以理解:本发明实施例中的装置中的部件可以按照实施例的描述分布于实施例的装置中,也可以进行相应变化位于不同于本实施例的一个或多个装置中。上述实施例的部件可以合并为一个部件,也可以进一步拆分成多个子部件。Those of ordinary skill in the art can understand that: the components of the apparatus in the embodiment of the present invention may be distributed in the apparatus of the embodiment according to the description of the embodiment, and may also be located in one or more apparatuses different from this embodiment by making corresponding changes . The components of the above-mentioned embodiments may be combined into one component, or may be further divided into multiple sub-components.
以上所述,仅为本发明较佳的具体实施方式,但本发明的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明揭露的技术范围内,可轻易想到的变化或替换,都应涵盖在本发明的保护范围之内。因此,本发明的保护范围应该以权利要求的保护范围为准。The above description is only a preferred embodiment of the present invention, but the protection scope of the present invention is not limited to this. Substitutions should be covered within the protection scope of the present invention. Therefore, the protection scope of the present invention should be subject to the protection scope of the claims.
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