JPS62174576A - Electron impact type ion thruster - Google Patents

Electron impact type ion thruster

Info

Publication number
JPS62174576A
JPS62174576A JP1474686A JP1474686A JPS62174576A JP S62174576 A JPS62174576 A JP S62174576A JP 1474686 A JP1474686 A JP 1474686A JP 1474686 A JP1474686 A JP 1474686A JP S62174576 A JPS62174576 A JP S62174576A
Authority
JP
Japan
Prior art keywords
gas
baffle
hollow
ion thruster
type ion
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
JP1474686A
Other languages
Japanese (ja)
Inventor
Hideki Yoshida
英樹 吉田
Toru Sugawara
亨 菅原
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP1474686A priority Critical patent/JPS62174576A/en
Publication of JPS62174576A publication Critical patent/JPS62174576A/en
Pending legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F03MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
    • F03HPRODUCING A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
    • F03H1/00Using plasma to produce a reactive propulsive thrust
    • F03H1/0006Details applicable to different types of plasma thrusters
    • F03H1/0012Means for supplying the propellant
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F03MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
    • F03HPRODUCING A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
    • F03H1/00Using plasma to produce a reactive propulsive thrust
    • F03H1/0006Details applicable to different types of plasma thrusters
    • F03H1/0031Thermal management, heating or cooling parts of the thruster

Landscapes

  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Physics & Mathematics (AREA)
  • Plasma & Fusion (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Particle Accelerators (AREA)

Abstract

PURPOSE:To reduce deterioration in the strength of a baffle by means of gas cooling by providing said baffle in which plural holes are provided in a hollow conductor, in a discharge room and making a gas flow in said hollow conductor. CONSTITUTION:A baffle 7 is formed with a hollow conductor on which plural holes are provided and placed in a discharge room, and an Xe gas is introduced into a hollow part and blown out of the holes. The distribution of ionized plasma produced by the collision of electrons which are accelerated by an electric field between a hollow cathode 1 and an anode 2 with the Xe gas becomes uniform. The baffle 2 is cooled with the gas while having the function of introducing the gas. Accordingly, the deterioration in the strength of the baffle can be reduced by gas cooling.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は1人工衛星の軌道側−を行なうα子衝撃型イ
オン・スラスタに関する、 〔発明の技術的背景とその面題点〕 従来の電子衝炸型イオン・スラスタの構成を第3図に示
す。ガス導入系からホローカソードl内を通って放電容
器8内に導入されたXeガスに。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to an alpha bombardment type ion thruster for orbiting an artificial satellite. The configuration of the explosive type ion thruster is shown in Figure 3. Xe gas is introduced from the gas introduction system into the discharge vessel 8 through the hollow cathode 1.

ホローカソード1から放出後アノード2によって加速さ
れた電子が衝突して電離プラズマを放′4室内に生成し
、xe+イオンが加速電極(3枚)4によって運動エネ
ルギを与えられ、中和器6から放出される電子によりて
中和化された後放出されてイオン・スラスタの推力とな
る。′電離プラズマの放電容器8の壁面からの損失を小
さくするために。
Electrons accelerated by the anode 2 after being emitted from the hollow cathode 1 collide to generate ionized plasma in the radiation chamber 4, and xe+ ions are given kinetic energy by the accelerating electrodes (3 pieces) 4, After being neutralized by the emitted electrons, they are released and become the thrust of the ion thruster. 'To reduce the loss of ionized plasma from the wall of the discharge vessel 8.

磁石3でカスプ磁場を構成してM1@閉じ込めを行りて
いる。Xe+イオンが3枚の加速電極4の孔を発散角最
小かつ加速電極4に衝突せずに抜けて来る几めには、加
速電極4の放電室11近傍で第2図破4!9で示すよう
なイオン成製密度の均一性が必要である。ところが、放
電室内のガス圧をFげて行くと、ガス導入孔下流側でガ
ス濃度が蔓くなりでイオン電流密度が第2図実線1oの
ように高くなり均一性がなくなる。この破れた均一性を
回′復するためには、ガス導入孔の数を増加させる必要
がある。ガス導入孔の増加は放電容器8の製作を複雑な
ものにするとともに大幅ζ型針増加を伴う欠点がある。
Magnet 3 forms a cusp magnetic field to confine M1@. In order for the Xe+ ions to pass through the holes of the three accelerating electrodes 4 with the minimum divergence angle and without colliding with the accelerating electrodes 4, there is a hole near the discharge chamber 11 of the accelerating electrode 4, as shown in Fig. 2, broken 4!9. Such uniformity of ion formation density is required. However, when the gas pressure in the discharge chamber is increased by F, the gas concentration increases on the downstream side of the gas introduction hole, and the ion current density becomes high as shown by the solid line 1o in FIG. 2, and uniformity is lost. In order to restore this broken uniformity, it is necessary to increase the number of gas introduction holes. The increase in the number of gas introduction holes complicates the manufacture of the discharge vessel 8 and has the drawback of significantly increasing the number of ζ-shaped needles.

又、ホローカソード1から放出される電子を放電室内に
ばらまく九めに設けたバックル7はホローカソード1か
ら1000 ’C程度の輻崎寸を受けて強度劣化を起こ
す。上記欠点は低ガス玉数′4を行なう大型イオン・ス
ラスタに於て大キナ問題である。
Further, the buckle 7 provided at the ninth position to scatter electrons emitted from the hollow cathode 1 into the discharge chamber is subjected to a convergence dimension of about 1000'C from the hollow cathode 1, causing strength deterioration. The above drawback is a large kina problem in large ion thrusters operating with low gas ball counts.

〔発明の目的〕[Purpose of the invention]

本発明は、このような事情に鑑みてなされ几もので、ガ
ス導入孔を放電容器につけないで破れた均一性を回復す
るとともに、バッフルを冷却して強度劣化を小さくした
電子衝撃型イオン・スラスタを提供することを目的とす
る。
The present invention has been made in view of these circumstances, and is an electron impact type ion thruster that restores the broken uniformity without attaching gas inlet holes to the discharge vessel, and reduces strength deterioration by cooling the baffle. The purpose is to provide

〔発明の概要〕[Summary of the invention]

本発明は、バッフルにガス導入機能を持たせて。 In the present invention, the baffle has a gas introduction function.

放゛シ室内に持ち込んだことを特徴とする電子衝撃型イ
オン・スラスタである。
It is an electron impact type ion thruster that is unique in that it was brought into the radiation chamber.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、放電容器の複雑化及び大幅な重量増加
を伴なわずに低ガス圧放電時の均一性を満足させるとと
もにガス冷却によりてバッフルの強度劣化を小さくする
ことができる。
According to the present invention, it is possible to satisfy uniformity during low gas pressure discharge without complicating the discharge vessel or significantly increasing its weight, and to reduce deterioration in strength of the baffle by gas cooling.

(発明の実施例〕 以下本発明の実施例を詳細に説明する。なお従来装作と
その構成が同一の部分については同一符号を附けてその
説明を省略する。第1図に示すように、バッフル7を中
空導体にして、適当な位置に多数の孔を設けて放電室内
に持ち込む。バッフル7の中空部分VCXeガスを導入
すると、Xeガスは孔のあい九方向にふき出す。孔の形
状及び位置を調整することにより放電室内のガス分布を
均一化する。ガス導入孔の数が多い分、均一化の程度F
i高い。ガス分布が均一である念め、ホローカソード1
とアノード2の間の電場によって加逮された電子がXe
ガスに衝突して生成される′ト離プラズマの分布は均一
になる。第1図のガス導入孔の数、形状及び位置は放電
室内のガス分布が均一になるようなものであれば何でも
よく、第1図のものに限定するものではuい。又、バッ
フルの形状も中空導体であればよく第1図のものに限?
するものではない。バッフル7へのガス4人管も第1図
では2本あるが、1本でも、3本以上でもよい。このよ
うに構成することによりバッフル7はガス冷却されると
伴にガス導入機能を持つことになる。導入ガスとしてX
eを用いているが、Xeガスに限定するものではない。
(Embodiments of the Invention) Embodiments of the present invention will be described in detail below.The same reference numerals will be given to parts that are the same in structure as the conventional equipment, and the explanation thereof will be omitted.As shown in FIG. The baffle 7 is made into a hollow conductor, and a large number of holes are provided at appropriate positions to bring it into the discharge chamber. When the VCXe gas is introduced into the hollow part of the baffle 7, the Xe gas blows out in the nine directions of the holes. The gas distribution inside the discharge chamber is made uniform by adjusting the position.The degree of uniformity F is increased due to the large number of gas introduction holes.
iIt's expensive. Hollow cathode 1 to ensure uniform gas distribution
The electrons modified by the electric field between Xe and anode 2
The distribution of the separated plasma generated by colliding with the gas becomes uniform. The number, shape, and position of the gas introduction holes shown in FIG. 1 may be any number as long as the gas distribution within the discharge chamber is uniform, and the gas introduction holes are not limited to those shown in FIG. 1. Also, is the shape of the baffle limited to the one shown in Figure 1 as long as it is a hollow conductor?
It's not something you do. Although there are two gas pipes to the baffle 7 in FIG. 1, it may be one, three or more. With this configuration, the baffle 7 is gas-cooled and has a gas introduction function. X as introduced gas
Although Xe gas is used, it is not limited to Xe gas.

本発明は、カスプi場で放電室を履り*’g子衝撃型の
イオン・スラブ、夕を用いて説明したが、電子衝S型の
放゛亀室を使用しているfe!であればよく、例えば1
俵融合で望用されるプラズマ加熱用中性粒子入射装置の
電子衝撃型のイオン源についても全く同じように適用で
きる。
The present invention has been explained using an ion slab of the electron bombardment type, using a discharge chamber in the cusp I field, but an fe! For example, 1
The same applies to the electron impact type ion source of the neutral particle injection device for plasma heating, which is desired in bale fusion.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明の実施クリを示す概要図、第2図はイオ
ン成製密度の分布特性の概要図、第3図は従来の′4電
子撃型イオン・スラスタの構成1図である。 l・・・ホローカソード、2・・・アノード、3・・・
磁石、4・・・加速′a他、5・・・ケース、6・・・
中和器、7・・・バッフル、8・・・放電容器。 代理人 弁理士  則 近 考 右 同     竹 花 喜久男 ブ1π”ス 第1図 第2図 乙 第3図
FIG. 1 is a schematic diagram showing the implementation of the present invention, FIG. 2 is a schematic diagram of the distribution characteristics of the ion production density, and FIG. 3 is a diagram of the configuration of a conventional '4 electron bombardment type ion thruster. l...Hollow cathode, 2...Anode, 3...
Magnet, 4... Acceleration 'a, etc., 5... Case, 6...
Neutralizer, 7... Baffle, 8... Discharge vessel. Agent Patent Attorney Nori Chika Kou Takehana Kikuo 1π"S Figure 1 Figure 2 Figure B Figure 3

Claims (1)

【特許請求の範囲】[Claims] ガス導入系と放電容器とホローカソードとバッフルと加
速電極と中和器と電源等で構成されるイオン・スラスタ
に於いて、中空導体に複数個の穴を設けたバッフルを放
電室内に設けて、中空導体内にガスを流したことを特徴
とする電子衝撃型イオン・スラスタ。
In an ion thruster consisting of a gas introduction system, a discharge vessel, a hollow cathode, a baffle, an accelerating electrode, a neutralizer, a power supply, etc., a baffle with multiple holes in a hollow conductor is installed inside the discharge chamber. An electron impact type ion thruster characterized by flowing gas inside a hollow conductor.
JP1474686A 1986-01-28 1986-01-28 Electron impact type ion thruster Pending JPS62174576A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1474686A JPS62174576A (en) 1986-01-28 1986-01-28 Electron impact type ion thruster

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1474686A JPS62174576A (en) 1986-01-28 1986-01-28 Electron impact type ion thruster

Publications (1)

Publication Number Publication Date
JPS62174576A true JPS62174576A (en) 1987-07-31

Family

ID=11869676

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1474686A Pending JPS62174576A (en) 1986-01-28 1986-01-28 Electron impact type ion thruster

Country Status (1)

Country Link
JP (1) JPS62174576A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007288466A (en) * 2006-04-17 2007-11-01 Meidensha Corp Pulse power supply
JP2007289436A (en) * 2006-04-25 2007-11-08 Newgin Corp Game ball intake device and game machine having the same

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007288466A (en) * 2006-04-17 2007-11-01 Meidensha Corp Pulse power supply
JP4702156B2 (en) * 2006-04-17 2011-06-15 株式会社明電舎 Pulse power supply
JP2007289436A (en) * 2006-04-25 2007-11-08 Newgin Corp Game ball intake device and game machine having the same

Similar Documents

Publication Publication Date Title
US5763989A (en) Closed drift ion source with improved magnetic field
JPH04229996A (en) Plasma accelearator having closed electron drift
US4894546A (en) Hollow cathode ion sources
US4739214A (en) Dynamic electron emitter
Weidmann et al. The polarized ion source for COSY
JPS61290629A (en) Electron beam excitation ion source
WO1995030235A2 (en) Inertial-electrostatic confinement particle generator
Tsai et al. Plasma studies on a duoPIGatron ion source
Kistemaker On ion sources with high efficiency and intensity
JPS62174576A (en) Electron impact type ion thruster
Hill Ion and electron sources
US5152956A (en) Neutron tube comprising an electrostatic ion source
JP3350186B2 (en) Ion beam generator
US3032490A (en) Destruction of neutral particles in a device for producing a high density plasma
US4931698A (en) Ion source
JPS62174573A (en) Electron impact type ion thruster
JPH06310297A (en) Generating method and device of low energy neutral particle beam
JPH01310179A (en) Ecr type ion thruster
JPH08190995A (en) High speed atomic beam source
JPS62180942A (en) High-speed atomic beam source
Poeschel et al. Study and optimization of 15-cm Kaufman thruster discharges
JPH10275566A (en) Ion source
JPS63124876A (en) Electronic impact type ion thruster
JP2627420B2 (en) Fast atom beam source
JPS62174574A (en) Rf type ion thruster