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- it is possible to use 8 low level static<br />

magnetic field to rench the resonance<br />

condition, e.g. 36 GausB for resonance at<br />

100 me. A lower thruster mass can be thus<br />

ach ieved :<br />

.. slnco the ~avelcnqht 10 much hiyher thar<br />

the chamber dimensions, problems arisinq<br />

pram energy propagation into plnsna can LU<br />

avoided. In case of VllF oxcitation, plasma<br />

generation Is infact achieved through a<br />

"noar field" mechanism so that no cut-off<br />

frequency exists:<br />

- it is possible to use coupling<br />

olactrodeo. for the VHF RF field, outside<br />

the discharqr? chnmbcr, clue to the lini'ced<br />

rwor losses for irradiation > 1/~, i.6 about 2 UHZ connidcrinq<br />

a pressure of 10'-4 Torr and nn alcctron<br />

energy of 13eV. This condltion ensures<br />

that electrons turns around the magnetic<br />

field many times between consecutive<br />

collisions:<br />

2) R 1 cm, whore R~is the qyration<br />

radius of the electron in presence of a<br />

magnetic field dirocted nlonq tha chamber<br />

axis. This condition enquros that the<br />

electron trajec'ories are conta,iriwl in the<br />

#<br />

+ischarge chamber;<br />

3) EM field wavelcnqht >' 3+5 cm. Tnis<br />

condition avoids propnqation problems in<br />

the plasma.<br />

In summary, the ECR technique IR expccted<br />

to provide substantial Lmprovenenta in low<br />

power ion thrusters pcrformanca, enhancing<br />

the advantages of traditions: RF tcchnlqes<br />

in combination with qthers typical of the<br />

Kaufman technoloqy. The main fotsturcs of<br />

the ECR technique are summarized as<br />

Io1 lows :<br />

- ECR sources do not have components<br />

subjected to wearout, as cathodes or<br />

accelerating electrodes, l.n the plasma<br />

charber. I ,<br />

Problems of sputteriny erosion inside the<br />

chamber are thus eliminated, impac; ing<br />

positively the thruster lifet ime.<br />

Moreover, it is possible to realize the<br />

discharge vessel with materials having<br />

high secondary electron emission<br />

coefficients, scarcely sensitive to<br />

erosion and capable of reducing electron<br />

losses from plasma towards tho vessel<br />

walls.<br />

- T:.e plasma produced by the ECR 1s hiqhly<br />

uniform, both in density and t-mperature.<br />

Achievable ulec'ron densities ar@ of the<br />

order of 10'12 electrons/cm'3 at pressures<br />

in the range of 10--4 + 10A-5 Torr, thus<br />

facilitatinq beam extraction optimization.<br />

- The ECR technique is specially<br />

advantageous for ion thrusters operating<br />

at' low thrust levels ( 2410 mN) where it<br />

reduces considerably the Instability<br />

phenomena inside the plasma. Low thrusts<br />

ere related to small chamber dimensions,<br />

which eimpliliee tho realization of a<br />

uniPom magnetic fielc! in tne dlscharge<br />

vessel, and requires less Dc power.<br />

A small chamber also requires small<br />

electrodes for electroinaqnetic energy<br />

tranwfer, with lower losses due to EU<br />

irradiation and vessel walls absorption.<br />

Furthermore, for constant average beam<br />

current densities, thruster throttling is<br />

accompl isiied keeping the mass flow rate<br />

to beam area ratio constant. A reduced<br />

flow rat& is associated with a pressure<br />

regime within the discharge chamber where<br />

ECR proves more efficient and stable than<br />

other traditional excitation techniques.<br />

- Tho yrid extraction syetcn can be<br />

dcsigncd and optimized on the basis of the<br />

enhanced plasma characteristics typical of<br />

the ECR technique. In this direction PROEL<br />

Is investigatinq also new technoloqies<br />

(patent pcn-llng) for the realization of<br />

qrids with a qcnmstry having a hiqh<br />

transparency factor to ions, while<br />

maintaining good nechanical rcsistnnce and<br />

the capnbillty to survive to sputtering<br />

erosion.<br />

The USQ of ti hiqh melting point refractory<br />

material, coa t ed with sui table<br />

anti?putterlng protcctlon layer, is the<br />

solution to long lifetime requirements.<br />

6,CONCLOS IOttS<br />

Electric propulsion, and in particular<br />

advanced ion propulnlon. is an enablinq<br />

technoloqy for the feasibility of very low<br />

Earth orbit missions, in power-limited<br />

liqhtsats, where drag in the doninant<br />

effect.<br />

Furthermore, low power ion thrusters are a<br />

good system alternattve for propulsion<br />

tasks requirinq tho stoady application of<br />

low thrust levale ovcr extended periods of<br />

time to implement a qiven velocity<br />

correction. Nevertheless very lon9<br />

lifetimes, of the order of 20000 to 40COO<br />

hours, must be reliably demonstrated.<br />

Improvements In mass and power efficiency<br />

of such low power tiiusters wou!d a!so<br />

benefit the liqhtsats design.<br />

Lov power arcjets, in the 1 Kw ranqe, have<br />

also promisinq applications for certain<br />

orbit manoeuvering tasks, and their<br />

development s:iould be further pursued.<br />

REFERENCES<br />

(11 J. Reale "A low altitude Lon-prop-IIf*d<br />

remote sensing spiscecrnft ": 27nd<br />

IEPC; Viaregqio, October 1991:

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