CN108301997A - Pulsed plasma thruster based on Z-PINCH no-spark plugs - Google Patents
Pulsed plasma thruster based on Z-PINCH no-spark plugs Download PDFInfo
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F03—MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03H—PRODUCING A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03H1/00—Using plasma to produce a reactive propulsive thrust
- F03H1/0087—Electro-dynamic thrusters, e.g. pulsed plasma thrusters
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F03—MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03H—PRODUCING A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03H1/00—Using plasma to produce a reactive propulsive thrust
- F03H1/0006—Details applicable to different types of plasma thrusters
- F03H1/0018—Arrangements or adaptations of power supply systems
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Abstract
Description
技术领域technical field
本发明涉及的是一种空间电推进技术和电推力器设计领域的技术,具体是一种基于Z-PINCH无火花塞的脉冲等离子体推力器。The invention relates to a technology in the field of space electric propulsion technology and electric thruster design, in particular to a pulsed plasma thruster based on Z-PINCH without spark plug.
背景技术Background technique
脉冲等离子体推力器是利用脉冲放电,烧蚀、分解、电离推进剂,使之成为等离子体。传统脉冲等离子体推力器通常采用固态聚四氟乙烯作为推进剂结合弹簧供给,也有学者研究了气体和液体推进剂。从结构上来讲,传统脉冲等离子体推力器为平行板电极结合火花塞实现点火和产生脉冲电弧,也有人提出过同轴脉冲等离子体推力器,但点火和产生推力的原理均为等离子体在磁场与放电电流共同作用下受到广义洛仑兹力的作用而加速喷出产生推力。传统平行板电极脉冲等离子体推力器工作时,首先将储能电容器充电至所需电压,然后半导体火花塞点火,电容器沿着工质聚四氟乙烯表面放电,电流形成于工质表面,热流将聚四氟乙烯表面的分子解聚、分裂、电离,随后在广义洛仑兹力和气动压力的共同作用下,等离子体被加速,膨胀喷出产生推力。电容器放电完毕后,推力器停止工作或进入下一个循环。由于热量传递的滞后性,每次放电后仍会有部分推进剂升华为气体但却无法电离,导致推进剂利用率非常低。The pulse plasma thruster uses pulse discharge to ablate, decompose, and ionize the propellant to make it into plasma. Traditional pulsed plasma thrusters usually use solid polytetrafluoroethylene as the propellant combined with spring supply, and some scholars have studied gas and liquid propellants. From a structural point of view, the traditional pulsed plasma thruster uses parallel plate electrodes combined with a spark plug to achieve ignition and pulsed arc generation. Some people have also proposed a coaxial pulsed plasma thruster, but the principle of ignition and thrust is that the plasma is in the magnetic field and Under the joint action of the discharge current, it is accelerated by the generalized Lorentz force to generate thrust. When the traditional parallel plate electrode pulse plasma thruster works, the energy storage capacitor is first charged to the required voltage, and then the semiconductor spark plug is ignited, the capacitor discharges along the surface of the working medium PTFE, the current is formed on the working medium surface, and the heat flow will gather Molecules on the surface of tetrafluoroethylene depolymerize, split, and ionize. Then, under the joint action of generalized Lorentz force and pneumatic pressure, the plasma is accelerated, and the plasma is expanded and ejected to generate thrust. After the capacitor is discharged, the thruster stops working or enters the next cycle. Due to the hysteresis of heat transfer, part of the propellant will still be sublimated into gas after each discharge but cannot be ionized, resulting in a very low utilization rate of the propellant.
发明内容Contents of the invention
本发明针对现有脉冲等离子体推力器依赖火花塞导致结构部件较多体积过大的同时增加安全隐患,并且推进剂利用率低等缺陷,提出一种基于Z-PINCH无火花塞的脉冲等离子体推力器,无需火花塞辅助点火,实现了推进剂点火和放电一体化,降低了点火电压;无需弹簧进行推进剂供给,没有任何活动部件,结构简单;独特的结构设计能有效地提高推进剂的利用效率,推功比更高;尺寸没有特殊限制。The present invention aims at defects such as existing pulsed plasma thrusters relying on spark plugs, resulting in many structural components that are too large in size, increasing potential safety hazards, and low propellant utilization, and proposes a pulsed plasma thruster based on Z-PINCH without spark plugs , no need for spark plug to assist ignition, realize the integration of propellant ignition and discharge, and reduce the ignition voltage; no spring for propellant supply, no moving parts, simple structure; unique structural design can effectively improve the utilization efficiency of propellant, Higher thrust-to-power ratio; no special restrictions on size.
本发明是通过以下技术方案实现的:The present invention is achieved through the following technical solutions:
本发明包括依次设置于基座和外层绝缘体之间的盘式结构的阴极、固体推进剂和锥形结构的阳极,其中:阴极和阳极分别设置于固体推进剂的两端,外层绝缘体套置于固体推进剂的外部并与基座相连。The present invention comprises a disc structure cathode, a solid propellant and an anode of a conical structure arranged between the base and the outer layer insulator in sequence, wherein: the cathode and the anode are respectively arranged at two ends of the solid propellant, and the outer layer insulator covers Placed on the exterior of the solid propellant and attached to the base.
所述的阴极优选为金属铜制的圆盘结构,顶部设有用于连接外部电路的圆形小孔。The cathode is preferably a disc structure made of metal copper, with a small circular hole on the top for connecting to an external circuit.
所述的阳极优选为金属铜制的圆锥结构,底部设有用于连接外部电路的圆形小孔。The anode is preferably a conical structure made of metal copper, and a small circular hole is provided at the bottom for connecting to an external circuit.
所述的固体推进剂优选为圆柱腔体结构,进一步优选为渗透有导电材料的聚四氟乙烯制成。The solid propellant is preferably a cylindrical cavity structure, more preferably made of polytetrafluoroethylene impregnated with conductive material.
所述的基座和外层绝缘体优选为聚碳酸酯制成。The base and the outer insulator are preferably made of polycarbonate.
技术效果technical effect
与现有技术相比,本发明给推力器阴阳两极充电至给定电压,在推进剂表面,圆柱形电流片迅速形成,烧蚀聚四氟乙烯,径向加速烧蚀产物,电流开始在两个电极之间流动。最初电流分布于绝缘体表面,形成圆柱形电流片。电流片在腔的最大半径处形成,这是由于该位置回路阻抗最小。随着电流的增大,在电流片的外侧产生磁场。磁场和电流片相互作用,产生向内放射状的电磁力。这种力造成电流片向腔中心瓦解,但是电流片并不是完全以圆柱形向中心移动,而是产生了倾斜,该现象被称为拉链效应。在电流片的作用下,推进剂最初被径向加速;当电流片完全收缩时,小孔的存在会导致较大的轴向压力梯度。因此,等离子体会沿着轴向加速喷出。等离子体在径向力的作用下受到挤压而发生膨胀,沿轴向扩散。Compared with the prior art, the present invention charges the positive and negative poles of the thruster to a given voltage. On the surface of the propellant, a cylindrical current sheet is rapidly formed, ablates the polytetrafluoroethylene, accelerates the ablation product in the radial direction, and the current starts to flow between the two poles. flow between electrodes. Initially, the current is distributed on the surface of the insulator, forming a cylindrical current sheet. The current sheet forms at the largest radius of the cavity, since this is where the loop impedance is the smallest. As the current increases, a magnetic field is generated on the outside of the current sheet. The magnetic field interacts with the current sheet to produce an electromagnetic force that radiates inward. This force causes the current sheet to collapse toward the center of the cavity, but instead of moving toward the center in a completely cylindrical shape, the current sheet tilts, a phenomenon known as the zipper effect. Under the action of the current sheet, the propellant is initially accelerated radially; when the current sheet is fully contracted, the presence of small holes leads to a large axial pressure gradient. As a result, the plasma is ejected with acceleration along the axial direction. The plasma is squeezed and expanded under the action of radial force, and spreads along the axial direction.
附图说明Description of drawings
图1、图2为本发明的整体结构示意图;Fig. 1, Fig. 2 are overall structural representations of the present invention;
图3为本发明中所述的外层绝缘体示意图;Fig. 3 is a schematic diagram of the outer layer insulator described in the present invention;
图4为本发明中所述的阴极示意图;Fig. 4 is the cathode schematic diagram described in the present invention;
图5为本发明中所述的推进腔示意图;Fig. 5 is a schematic diagram of the propulsion chamber described in the present invention;
图6为本发明中所述的阳极示意图;Fig. 6 is a schematic diagram of the anode described in the present invention;
图7为本发明中所述的基座示意图;Fig. 7 is a schematic diagram of the base described in the present invention;
图8和图9为实施例效果示意图;Fig. 8 and Fig. 9 are the effect schematic diagram of embodiment;
图中:1外层绝缘体、2阴极、3固体推进剂、4阳极、5基座。In the figure: 1 outer insulator, 2 cathode, 3 solid propellant, 4 anode, 5 base.
具体实施方式Detailed ways
如图1和图2所示,为本实施例涉及的基于Z-PINCH原理无火花塞的新型脉冲等离子体推进装置,包括:从上到下依次配合连接的外层绝缘体1、阴极2、固体推进剂3、阳极4和基座5,其中:阴极2顶部圆形小孔用于连接外部电路。所述的阳极4底部圆形小孔用于连接外部电路。As shown in Figure 1 and Figure 2, it is a new type of pulsed plasma propulsion device based on the Z-PINCH principle without spark plugs involved in this embodiment, including: an outer layer insulator 1, a cathode 2, and a solid propulsion device connected sequentially from top to bottom. Agent 3, anode 4 and base 5, wherein: the circular small hole on the top of cathode 2 is used to connect to an external circuit. The circular small hole at the bottom of the anode 4 is used for connecting an external circuit.
如图3、7所示,所述的外层绝缘体1和基座6均由聚碳酸酯制成,聚碳酸酯具有阻燃、耐磨和抗氧化性。As shown in Figures 3 and 7, the outer insulator 1 and the base 6 are both made of polycarbonate, which has flame retardancy, wear resistance and oxidation resistance.
如图4、6所示,所述的阴极2和阳极4均由金属铜制成,铜有良好的导电性,且耐高温,熔点高。阴极2中间有小孔,固体推进剂3被烧蚀后产生的等离子体从孔中喷出。阳极4上部是锥体,当电流片形成时,便于产生径向力。As shown in Figures 4 and 6, both the cathode 2 and the anode 4 are made of metal copper, which has good electrical conductivity, high temperature resistance and high melting point. There is a small hole in the middle of the cathode 2, and the plasma generated after the solid propellant 3 is ablated is ejected from the hole. The upper part of the anode 4 is a cone, which facilitates the generation of radial force when the current sheet is formed.
如图5所示,所述的固体推进剂3由聚四氟乙烯制成,对聚四氟乙烯渗透特定的导电材料。聚四氟乙烯具有耐高温、耐腐蚀且绝缘的特性,烧蚀后产生等离子体。采用圆柱形放电室是为了在给定尺寸条件下,能够最大程度利用空间贮存推进剂。As shown in FIG. 5 , the solid propellant 3 is made of polytetrafluoroethylene, and the polytetrafluoroethylene is infiltrated with a specific conductive material. PTFE has the characteristics of high temperature resistance, corrosion resistance and insulation, and generates plasma after ablation. The purpose of adopting the cylindrical discharge chamber is to maximize the use of space for propellant storage under the condition of given size.
本实施例通过以下方式进行工作:中空圆柱形聚四氟乙烯置于正负电极之间。在推进剂表面,圆柱形电流片迅速形成,烧蚀聚四氟乙烯,径向加速烧蚀产物,电流开始在两个电极之间流动。最初电流分布于绝缘体表面,形成圆柱形电流片。电流片在腔的最大半径处形成,这是由于该位置回路阻抗最小。随着电流的增大,在电流片的外侧产生磁场。磁场和电流片相互作用,产生向内放射状的电磁力。这种力造成电流片向腔中心瓦解,但是电流片并不是完全以圆柱形向中心移动,而是产生了倾斜,该现象被称为拉链效应。在电流片的作用下,推进剂最初被径向加速;当电流片完全收缩时,小孔的存在会导致较大的轴向压力梯度。因此,等离子体会沿着轴向加速喷出。等离子体在径向力的作用下受到挤压而发生膨胀,沿轴向扩散。This embodiment works in the following way: A hollow cylindrical polytetrafluoroethylene is placed between the positive and negative electrodes. On the surface of the propellant, a cylindrical current sheet is formed rapidly, ablating the PTFE, accelerating the ablation products radially, and the current begins to flow between the two electrodes. Initially, the current is distributed on the surface of the insulator, forming a cylindrical current sheet. The current sheet forms at the largest radius of the cavity, since this is where the loop impedance is the smallest. As the current increases, a magnetic field is generated on the outside of the current sheet. The magnetic field interacts with the current sheet to generate an electromagnetic force that radiates inward. This force causes the current sheet to collapse toward the center of the cavity, but instead of moving toward the center in a completely cylindrical shape, the current sheet tilts, a phenomenon known as the zipper effect. Under the action of the current sheet, the propellant is initially accelerated radially; when the current sheet is fully contracted, the presence of small holes leads to a large axial pressure gradient. Therefore, the plasma is ejected with acceleration along the axial direction. The plasma is compressed and expanded under the action of radial force, and spreads along the axial direction.
根据该发明所述的推力器,设计了实验方案验证其性能,具体步骤如下:According to the thruster described in the invention, an experimental scheme is designed to verify its performance, and the specific steps are as follows:
步骤1)将推力器固定在真空舱内的推力测量装置上,调整舱内运动平台的位置,以便于通过舱壁上的观察窗对推力器工作状况进行监控;Step 1) Fix the thruster on the thrust measuring device in the vacuum cabin, adjust the position of the motion platform in the cabin, so as to monitor the working condition of the thruster through the observation window on the bulkhead;
步骤2)对推力测量装置进行调试和静态标定;Step 2) debugging and static calibration of the thrust measuring device;
步骤3)将推力测量装置电定位,抽真空至要求的真空度;Step 3) electrically positioning the thrust measuring device, and evacuating to the required vacuum degree;
步骤4)解除推力测量装置电定位,观察测控仪上示力窗的示值,基本稳定后即可准备实验;Step 4) Release the electric positioning of the thrust measuring device, observe the indication value of the force display window on the measurement and control instrument, and prepare for the experiment after it is basically stable;
步骤5)打开推力器电源系统(包括主电容器充电电源和点火系统电源),同时打开数据采集系统电源,记录当前推力测量装置的零点;Step 5) Turn on the thruster power supply system (including the main capacitor charging power supply and the ignition system power supply), and simultaneously turn on the data acquisition system power supply, and record the zero point of the current thrust measuring device;
步骤6)推力器点火实验,数据采集系统记录推力测量数据。Step 6) Thruster ignition experiment, the data acquisition system records the thrust measurement data.
当给推力器的阴阳两级加上电压之后,如图8所示,推力器便开始工作。When voltage is applied to the yin and yang stages of the thruster, as shown in Figure 8, the thruster starts to work.
如图9所示,为推力器稳定工作过程中一个脉冲的放电特性,根据U-I曲线可以看出,初始时电压为20V,点火电压为480V。充电过程持续时间为1ms,此时电流增大,最大值为24A,随后电流缓慢下降。整个放电过程持续时间为1.04ms。从图中可以计算得出,该新型推力器的运行功率为4.8W。As shown in Figure 9, it is the discharge characteristic of a pulse during the stable operation of the thruster. According to the U-I curve, it can be seen that the initial voltage is 20V, and the ignition voltage is 480V. The duration of the charging process is 1ms. At this time, the current increases, the maximum value is 24A, and then the current decreases slowly. The duration of the entire discharge process is 1.04ms. It can be calculated from the figure that the operating power of the new thruster is 4.8W.
实验结果表明,该推力器能够工作,初步达到了设计要求。推功比为17.83μN/W,比传统脉冲等离子体推力器的推功比要大。上述具体实施可由本领域技术人员在不背离本发明原理和宗旨的前提下以不同的方式对其进行局部调整,本发明的保护范围以权利要求书为准且不由上述具体实施所限,在其范围内的各个实现方案均受本发明之约束。Experimental results show that the thruster can work and meet the design requirements initially. The thrust power ratio is 17.83μN/W, which is larger than that of the traditional pulsed plasma thruster. The above specific implementation can be partially adjusted in different ways by those skilled in the art without departing from the principle and purpose of the present invention. The scope of protection of the present invention is subject to the claims and is not limited by the above specific implementation. Each implementation within the scope is bound by the invention.
Claims (6)
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Application publication date: 20180720 |