CN102941930A - Surface electrification simulation test system and method for satellite tail regions - Google Patents

Surface electrification simulation test system and method for satellite tail regions Download PDF

Info

Publication number
CN102941930A
CN102941930A CN2012104848415A CN201210484841A CN102941930A CN 102941930 A CN102941930 A CN 102941930A CN 2012104848415 A CN2012104848415 A CN 2012104848415A CN 201210484841 A CN201210484841 A CN 201210484841A CN 102941930 A CN102941930 A CN 102941930A
Authority
CN
China
Prior art keywords
satellite
vacuum chamber
tail region
ion source
plasma
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN2012104848415A
Other languages
Chinese (zh)
Inventor
汤道坦
李得天
杨生胜
秦晓刚
史亮
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
510 Research Institute of 5th Academy of CASC
Original Assignee
510 Research Institute of 5th Academy of CASC
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 510 Research Institute of 5th Academy of CASC filed Critical 510 Research Institute of 5th Academy of CASC
Priority to CN2012104848415A priority Critical patent/CN102941930A/en
Publication of CN102941930A publication Critical patent/CN102941930A/en
Pending legal-status Critical Current

Links

Images

Landscapes

  • Electron Sources, Ion Sources (AREA)

Abstract

The invention relates to a surface electrification simulation test system and a method for satellite tail regions, and belongs to the test field. The system comprises a medium and low energy electronic gun, a three-dimensional transmission mechanism, a surface potentiometer, lamp filaments, a plasma diagnostic system, a Kaufmann ion source, a vacuum-pumping system, a vacuum chamber and a personal computer (PC). The method comprises that a satellite component is placed in the vacuum chamber to vacuumize the vacuum chamber; the Kaufmann ion source and the medium and low energy electronic gun are opened, and grid accelerating voltages, ion beams and electronic beams of the Kaufmann ion source and beam density and energy of the medium and low energy electronic gun are set; the plasma diagnostic system is used for diagnosing produced plasma environments; and the three-dimensional transmission mechanism drives the surface potentiometer to measure surface charging potentials in the satellite tail region. By means of the surface electrification simulation test system and the method for satellite tail regions, plasma environment simulation can be performed on satellite tail region environments, and the charging simulation test of the satellite component tail region can be performed.

Description

A kind of satellite tail region surface charging simulation experiment system and method
Technical field
The present invention relates to a kind of satellite tail region surface charging simulation experiment system and method, particularly for the system and method for simulation Low Earth Orbit (LEO) plasma environment and aurora electronic environment Satellite tail region surface charging effect test, belong to field tests.
Background technology
When satellite transit is in low temperature high-density plasma environment, form one obvious " flight path " in its tail region, this is a unequal electronics and ion depletion region, since satellite orbit speed greater than the hot speed of ion less than Electron Heat speed, therefore thereby electronics can enter relatively easily this zone and form a negative potential potential barrier, Here it is so-called " tail region charged effect ", and its obvious effect to satellite is that the tail region dielectric surface will charge to a higher negative potential.Especially, when polar region aurora electronic injection was arranged, the tail region current potential of satellite can reach thousands of volts.Usually, the surface charging that forms because of " tail region effect " of satellite is to affect particularly one of the major issue of polar-orbiting satellite safe operation of low orbit.
Document " Wakes and differential charging of large bodies in low earth orbit " studies show that, the substantially proportional relations such as tail region charging potential and satellite velocities (Mach speed), satellite size.The size of the low orbit investigation satellite of present stage design has reached tens of rice, and simultaneously, polar region aurora sedimentation electronic beam current reaches as high as 100 times of geosynchronous orbit, and flux is about 30nA/cm 2, will produce at Large-scale satellite and parts afterbody thereof the current potential of thousands of volts, and because charging capacitor is large, and discharge energy is also large, the Induced by Space Electrostatic Discharges of generation with serious threat satellite electron system in rail safety.Therefore, be necessary to develop a kind of apparatus and method that are fit to carry out satellite tail region band electric analogy testing.
But, in satellite tail region charged effect analogue test, also there is following main difficulty at present:
(1) ground is difficult to real simulation tail region plasma band electrical environment;
(2) ground is difficult to carry out the charged analogue test in full-size(d) satellite tail region.
Therefore, setting up the charged simulation experiment method in a kind of actv. tail region studies significant to carrying out the low-orbit satellite surface charging.
Summary of the invention
For achieving the above object, technical scheme of the present invention is as follows.
A kind of satellite tail region surface charging simulation experiment system, described system comprises: middle low-energy electron rifle, three dimensional transmission mechanism, surface potential meter, filament, plasma diagnostics system, Kaufman ion source, pumped vacuum system, vacuum chamber, PC.
Wherein, at internal vacuum chamber, the filament symmetry is installed on the upper lower wall surface of vacuum chamber; Satellite component vertically is suspended on the center of vacuum chamber by metal filament; Kaufman ion source is installed in respectively on two relative sidewalls of vacuum chamber with middle low-energy electron rifle, and wherein Kaufman ion source is positioned at the satellite component left side, and middle low-energy electron rifle is positioned at the satellite component right side; Being centered close on the straight line of Kaufman ion source, satellite component, middle low-energy electron rifle; Plasma diagnostics system and three dimensional transmission mechanism are positioned at internal vacuum chamber, at three dimensional transmission mechanism the surface potential meter are installed;
Outside at vacuum chamber, PC is connected with the plasma diagnostics system; Pumped vacuum system is connected with vacuum chamber;
Preferred described plasma diagnostics system is the Langmuir probe.
Preferred described filament is tungsten filament.
Distance between preferred described satellite component and the Kaufman ion source is 30 ~ 40cm.
A kind of satellite tail region surface charging simulation experiment method, described method step is as follows:
Step 1, in vacuum chamber, put into satellite component, open pumped vacuum system vacuum chamber is vacuumized, make degree of vacuum in the vacuum chamber≤10 -3Pa;
Step 2, open Kaufman plasma source and middle low-energy electron rifle, set Kaufman ion source grid accelerated voltage, ion beam current, electronic beam current, and the beam current density of middle low-energy electron rifle and energy; Utilize the plasma diagnostics system that the plasma environment that produces is diagnosed;
Step 3, drive the surface potential meter by three dimensional transmission mechanism and move on the satellite component right side, measure the surface charging current potential in the satellite component tail region;
Behind the end of test, shutdown system, size or the Kaufman ion source grid accelerated voltage of transposing satellite component structure, repeating step one~three obtains the scantling of structure of satellite component and the relation of satellite motion speed and tail region charging potential.
Preferably in step 2, Kaufman ion source grid accelerated voltage is that 100V, ion beam current are that 32mA, electronic beam current are 35mA; The energy of middle low-energy electron rifle is 1.0 ~ 100keV, and beam current density is 1 ~ 10nA/cm 2The density of the plasma in the vacuum chamber is 10 9/ m 3~10 12/ m 3
Beneficial effect
1. the invention provides a kind of satellite tail region surface charging simulation experiment system, described system can carry out the environment plasma environment simulation of satellite tail region, can carry out satellite component tail region charging analogue test.
2. the invention provides the test method of described satellite tail region surface charging simulation experiment system, can carry out the environment plasma environment simulation of satellite tail region, be specially: utilize Kaufman ion source to produce high density low-power plasma body, simultaneously, relative motion effect for analog satellite, ion accelerating grid electrode at Kaufman ion source applies accelerated voltage to ion current, produced the plasma flow of directed flow, therefore, the afterbody at the object of directional plasma stream can produce the tail region effect.
3. described method can be carried out the simulation of aurora electronic environment, is specially on the opposite of Kaufman ion source and places a middle low-energy electron rifle, and its electron energy is 1.0 ~ 100keV, and beam current density is 1 ~ 10nA/cm 2
Description of drawings
Fig. 1 is satellite of the present invention tail region surface charging simulation experiment system structural representation.
Among the figure: 1 is satellite component, and 2 is middle low-energy electron rifle, and 3 is three dimensional transmission mechanism, and 4 is the surface potential meter, and 5 is filament, and 6 is the plasma diagnostics system, and 7 is Kaufman ion source, and 8 is pumped vacuum system, and 9 is vacuum chamber, and 10 is PC.
The specific embodiment
Below the invention will be further described.
Embodiment
A kind of satellite tail region surface charging simulation experiment system as shown in Figure 1, described system comprises: middle low-energy electron rifle 2, three dimensional transmission mechanism 3, surface potential meter 4, filament 5, plasma diagnostics system 6, Kaufman ion source 7, pumped vacuum system 8, vacuum chamber 9, PC 10.
Wherein, in vacuum chamber 9 inside, filament 5 symmetries are installed on the upper lower wall surface of vacuum chamber; Satellite component 1 vertically is suspended on the center of vacuum chamber 9 by metal filament; Kaufman ion source 7 is installed in respectively on 9 two relative sidewalls of vacuum chamber with middle low-energy electron rifle 2, and wherein Kaufman ion source 7 is positioned at satellite component 1 left side, and middle low-energy electron rifle 2 is positioned at satellite component 1 right side; Being centered close on the straight line of Kaufman ion source 7, satellite component 1, middle low-energy electron rifle 2; Plasma diagnostics system 6 and three dimensional transmission mechanism 3 are positioned at vacuum chamber 9 inside, at three dimensional transmission mechanism 3 surface potential meter 4 are installed;
Have through hole at vacuum chamber 9 walls, the PC 10 of vacuum chamber 9 outsides is connected with plasma diagnostics system 6 by wire; Pumped vacuum system 8 is connected with vacuum chamber 9;
Wherein, described plasma diagnostics system 6 is the Langmuir probe.Described filament 5 is tungsten filament.Distance between described satellite component 1 and the Kaufman ion source 7 is 30cm.The electron energy of middle low-energy electron rifle is 1.0 ~ 100keV, and beam current density is 1 ~ 10nA/cm 2
A kind of satellite tail region surface charging simulation experiment method, described method step is as follows:
Step 1, in vacuum chamber 9, put into satellite component 1, open 8 pairs of vacuum chambers 9 of pumped vacuum system and vacuumize, make degree of vacuum in the vacuum chamber 9≤8.0 * 10 -4Pa;
Step 2, open Kaufman plasma source 7 and middle low-energy electron rifle 2, setting Kaufman ion source 7 grid accelerated voltages is that 100V, ion beam current are that 32mA, electronic beam current are slightly larger than ion beam current, is 35mA; The beam current density of middle low-energy electron rifle 2 is 2nA/cm 2, energy is 50keV, by the afterbody charging of 2 pairs of satellite component 1 of electron gun; Utilize the plasma environment of 6 pairs of generations of plasma diagnostics system to diagnose, the plasma density of generation is controlled at 10 9~ 10 11/ m 3
Step 3, drive surface potential meters 4 by three dimensional transmission mechanism 3 and move on satellite component 1 right side, measure the surface charging current potential in satellite component 1 tail region;
Behind the end of test, shutdown system, regulating Kaufman ion source 7 grid accelerated voltages is 120V, repeating step one~three, the relation of acquisition satellite motion speed and tail region charging potential.Then change the size of satellite component 1, repeating step one~three obtains the size of satellite component 1 and the relation of tail region charging potential.
In sum, more than be preferred embodiment of the present invention only, be not for limiting protection scope of the present invention.Within the spirit and principles in the present invention all, any modification of doing, be equal to replacement, improvement etc., all should be included within protection scope of the present invention.

Claims (6)

1. satellite tail region surface charging simulation experiment system, it is characterized in that: described system comprises: middle low-energy electron rifle (2), three dimensional transmission mechanism (3), surface potential meter (4), filament (5), plasma diagnostics system (6), Kaufman ion source (7), pumped vacuum system (8), vacuum chamber (9), PC (10);
Wherein, in vacuum chamber (9) inside, filament (5) symmetry is installed on the upper lower wall surface of vacuum chamber; Satellite component (1) vertically is suspended on the center of vacuum chamber (9) by metal filament; Kaufman ion source (7) is installed in respectively on (9) two relative sidewalls of vacuum chamber with middle low-energy electron rifle (2), and wherein Kaufman ion source (7) is positioned at satellite component (1) left side, and middle low-energy electron rifle (2) is positioned at satellite component (1) right side; Being centered close on the straight line of Kaufman ion source (7), satellite component (1), middle low-energy electron rifle (2); Plasma diagnostics system (6) and three dimensional transmission mechanism (3) are positioned at vacuum chamber (9) inside, at three dimensional transmission mechanism (3) surface potential meter (4) are installed;
In vacuum chamber (9) outside, PC (10) is connected with plasma diagnostics system (6); Pumped vacuum system (8) is connected with vacuum chamber (9).
2. a kind of satellite according to claim 1 tail region surface charging simulation experiment system, it is characterized in that: described plasma diagnostics system (6) is the Langmuir probe.
3. a kind of satellite according to claim 1 tail region surface charging simulation experiment system, it is characterized in that: described filament (5) is tungsten filament.
4. a kind of satellite according to claim 1 tail region surface charging simulation experiment system, it is characterized in that: the distance between described satellite component (1) and the Kaufman ion source (7) is 30 ~ 40cm.
5. satellite tail region surface charging simulation experiment method, it is characterized in that: described method is being carried out such as each described system of claim 1 to 4, and described method step is as follows:
Step 1, in vacuum chamber (9), put into satellite component (1), open pumped vacuum system (8) vacuum chamber (9) is vacuumized, make degree of vacuum in the vacuum chamber (9)≤10 -3Pa;
Step 2, open Kaufman plasma source (7) and middle low-energy electron rifle (2), set grid accelerated voltage, ion beam current, the electronic beam current of Kaufman ion source (7), and beam current density and the energy of middle low-energy electron rifle (2); Utilize plasma diagnostics system (6) that the plasma environment that produces is diagnosed;
Step 3, drive surface potential meter (4) by three dimensional transmission mechanism (3) and move on satellite component (1) right side, measure the surface charging current potential in satellite component (1) tail region;
Behind the end of test, shutdown system, size or Kaufman ion source (7) the grid accelerated voltage of transposing satellite component (1), repeating step one~three obtains the size of satellite component (1) and the relation of satellite motion speed and tail region charging potential.
6. a kind of satellite according to claim 5 tail region surface charging simulation experiment method, it is characterized in that: in step 2, Kaufman ion source (7) grid accelerated voltage is that 100V, ion beam current are that 32mA, electronic beam current are 35mA; The energy of middle low-energy electron rifle (2) is 1.0 ~ 100keV, and beam current density is 1 ~ 10nA/cm 2The density of the plasma in the vacuum chamber (9) is 10 9/ m 3~ 10 12/ m 3
CN2012104848415A 2012-11-25 2012-11-25 Surface electrification simulation test system and method for satellite tail regions Pending CN102941930A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN2012104848415A CN102941930A (en) 2012-11-25 2012-11-25 Surface electrification simulation test system and method for satellite tail regions

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN2012104848415A CN102941930A (en) 2012-11-25 2012-11-25 Surface electrification simulation test system and method for satellite tail regions

Publications (1)

Publication Number Publication Date
CN102941930A true CN102941930A (en) 2013-02-27

Family

ID=47724955

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2012104848415A Pending CN102941930A (en) 2012-11-25 2012-11-25 Surface electrification simulation test system and method for satellite tail regions

Country Status (1)

Country Link
CN (1) CN102941930A (en)

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103245858A (en) * 2013-04-24 2013-08-14 兰州空间技术物理研究所 Device and method for ground-based simulation experimentation of charging effect of high altitude satellite material
CN103698589A (en) * 2013-11-28 2014-04-02 兰州空间技术物理研究所 Satellite surface potential monitoring device
CN104239620A (en) * 2014-09-03 2014-12-24 兰州空间技术物理研究所 Charging effect simulation method at tail region of spacecraft
CN104260906A (en) * 2014-09-03 2015-01-07 兰州空间技术物理研究所 Spacecraft tail area ion atmosphere ground-based simulation method
CN104340381A (en) * 2014-10-24 2015-02-11 兰州空间技术物理研究所 Experiment system for space lower earth orbit plasma environment simulation
CN105000202A (en) * 2015-07-16 2015-10-28 兰州空间技术物理研究所 Vacuum pumping system of test equipment of ion thrusters
CN105785153A (en) * 2014-12-19 2016-07-20 中国科学院空间科学与应用研究中心 Simulation device of satellite surface charge and discharge phenomena
CN110006776A (en) * 2019-04-12 2019-07-12 哈尔滨工业大学 A kind of evaluation method for the anti-sputtering performance of Hall electric propulsion device channel material
CN112146905A (en) * 2020-09-04 2020-12-29 兰州空间技术物理研究所 Space high-speed charged particle simulation device and simulation method
CN114560109A (en) * 2022-03-17 2022-05-31 中国科学院国家空间科学中心 Space proton deep charging ground simulation device and method

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN86201075U (en) * 1986-03-01 1986-12-31 中国科学院空间中心 High-energy and broad beam divergent field koufmen ion gun for surface modification
JPH03157300A (en) * 1989-11-13 1991-07-05 Natl Space Dev Agency Japan<Nasda> Artificial satellite
CN1917131A (en) * 2005-08-18 2007-02-21 中国科学院半导体研究所 Filament of neutralization cathode in Kaufman ion source, and method
CN101696950A (en) * 2009-10-13 2010-04-21 中国航天科技集团公司第五研究院第五一〇研究所 Spherical Langmuir probe device for measuring low-density cold plasmas
CN102507717A (en) * 2011-10-20 2012-06-20 中国航天科技集团公司第五研究院第五一〇研究所 Device and method for on-orbit monitoring of charging of satellite material surface

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN86201075U (en) * 1986-03-01 1986-12-31 中国科学院空间中心 High-energy and broad beam divergent field koufmen ion gun for surface modification
JPH03157300A (en) * 1989-11-13 1991-07-05 Natl Space Dev Agency Japan<Nasda> Artificial satellite
CN1917131A (en) * 2005-08-18 2007-02-21 中国科学院半导体研究所 Filament of neutralization cathode in Kaufman ion source, and method
CN101696950A (en) * 2009-10-13 2010-04-21 中国航天科技集团公司第五研究院第五一〇研究所 Spherical Langmuir probe device for measuring low-density cold plasmas
CN102507717A (en) * 2011-10-20 2012-06-20 中国航天科技集团公司第五研究院第五一〇研究所 Device and method for on-orbit monitoring of charging of satellite material surface

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
张超等: "卫星内带电效应地面试验技术研究", 《航天器环境工程》 *
秦晓刚等: "卫星尾迹带电数值模拟研究", 《真空与低温》 *

Cited By (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103245858A (en) * 2013-04-24 2013-08-14 兰州空间技术物理研究所 Device and method for ground-based simulation experimentation of charging effect of high altitude satellite material
CN103698589A (en) * 2013-11-28 2014-04-02 兰州空间技术物理研究所 Satellite surface potential monitoring device
CN104239620B (en) * 2014-09-03 2017-04-05 兰州空间技术物理研究所 A kind of spacecraft tail region charged effect emulation mode
CN104260906A (en) * 2014-09-03 2015-01-07 兰州空间技术物理研究所 Spacecraft tail area ion atmosphere ground-based simulation method
CN104260906B (en) * 2014-09-03 2016-05-04 兰州空间技术物理研究所 A kind of spacecraft tail region ionic environment ground simulation method
CN104239620A (en) * 2014-09-03 2014-12-24 兰州空间技术物理研究所 Charging effect simulation method at tail region of spacecraft
CN104340381A (en) * 2014-10-24 2015-02-11 兰州空间技术物理研究所 Experiment system for space lower earth orbit plasma environment simulation
CN104340381B (en) * 2014-10-24 2016-04-06 兰州空间技术物理研究所 A kind of space Low Earth Orbit plasma environment experimental system for simulating
CN105785153A (en) * 2014-12-19 2016-07-20 中国科学院空间科学与应用研究中心 Simulation device of satellite surface charge and discharge phenomena
CN105785153B (en) * 2014-12-19 2019-02-26 中国科学院空间科学与应用研究中心 A kind of simulator of satellite surface charge and discharge phenomena
CN105000202A (en) * 2015-07-16 2015-10-28 兰州空间技术物理研究所 Vacuum pumping system of test equipment of ion thrusters
CN110006776A (en) * 2019-04-12 2019-07-12 哈尔滨工业大学 A kind of evaluation method for the anti-sputtering performance of Hall electric propulsion device channel material
CN110006776B (en) * 2019-04-12 2021-08-24 哈尔滨工业大学 Method for evaluating anti-sputtering performance of Hall electric propeller channel material
CN112146905A (en) * 2020-09-04 2020-12-29 兰州空间技术物理研究所 Space high-speed charged particle simulation device and simulation method
CN114560109A (en) * 2022-03-17 2022-05-31 中国科学院国家空间科学中心 Space proton deep charging ground simulation device and method

Similar Documents

Publication Publication Date Title
CN102941930A (en) Surface electrification simulation test system and method for satellite tail regions
Guan et al. Experimental and numerical investigation of electrohydrodynamic flow in a point-to-ring corona discharge
Sibeck et al. ARTEMIS science objectives
Moreau et al. Electrohydrodynamic force produced by a corona discharge between a wire active electrode and several cylinder electrodes–Application to electric propulsion
Deca et al. Electromagnetic particle-in-cell simulations of the solar wind interaction with lunar magnetic anomalies
Shukla et al. Recent developments in quantum plasma physics
Mochalskyy et al. Towards a realistic 3D simulation of the extraction region in ITER NBI relevant ion source
Lim et al. Plasma parameters and discharge characteristics of lab-based krypton-propelled miniaturized Hall thruster
CN104863811B (en) negative particle thruster
Shang et al. Hypersonic experimental facility for magnetoaerodynamic interactions
Ulmen Formation and extraction of a dense plasma jet from a helicon-plasma-injected inertial electrostatic confinement device
CN105158617A (en) Charge-discharge simulator based on electron induction
Doshi et al. Feasibility study of artificial rainfall system using ion seeding with high voltage source
Takeiri et al. Research progress on ionic plasmas generated in an intense hydrogen negative ion source
Zhang et al. Particle simulation of streamer discharges on surface of DC transmission line in presence of raindrops
Jorns et al. Foundations of plasmas as ion sources
Chen Analysis of energy balance in a helicon coupled to an inertial electrostatic confinement device
Tarantino Determining the evolution and effects of hypervelocity plasma plumes
CN115450875B (en) High-speed neutral airflow generating device
Yu et al. Numerical investigation of atmospheric pressure plasma jet under nonuniform electric field
Kozhevnikov et al. The Electrodynamic Nature of" Anomalous" Ion Transport in Vacuum Discharges
Vladimirov et al. Automated test bench for simulation of radiation electrification of spacecraft structural dielectrics
Tang et al. DC-Augmented Dielectric Barrier Discharge (DCA-DBD)
Tariq et al. Electrodynamic interaction of Ganymede with the Jovian magnetosphere and the radial spread of wake‐associated disturbances
Block Interpretation of laboratory experiments of interest to space physics

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C02 Deemed withdrawal of patent application after publication (patent law 2001)
WD01 Invention patent application deemed withdrawn after publication

Application publication date: 20130227