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The Complete Book of Spaceflight: From Apollo 1 to Zero Gravity

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120 electrostatic propulsion<br />

electrothermal propulsion<br />

electric propulsion electrostatic propulsion<br />

electromagnetic propulsion<br />

electric propulsion <strong>The</strong> various types <strong>of</strong> electric propulsion.<br />

and popular is the heavy inert gas xenon, which is used in<br />

the XIPS (xenon-ion propulsion system). <strong>The</strong> gas propellant<br />

enters a discharge chamber at a controlled rate. A hot<br />

cathode (negative electrode) at the center <strong>of</strong> the chamber<br />

emits electrons, which are attracted <strong>to</strong> a cylindrical anode<br />

(positive electrode) around the walls <strong>of</strong> the chamber.<br />

Some <strong>of</strong> the electrons collide with and ionize a<strong>to</strong>ms <strong>of</strong><br />

the propellant, creating positively-charged ions. <strong>The</strong>se<br />

ions are then drawn <strong>to</strong>ward a high-voltage electric field<br />

set up between two closely spaced grids at the downstream<br />

end <strong>of</strong> the chamber. <strong>The</strong>se grids contain numerous<br />

tiny lined-up holes so that they serve as porous<br />

electrodes. <strong>The</strong> ions are drawn through the first grid (the<br />

screen grid), are accelerated in the narrow gap between<br />

the first and second grid (the accelera<strong>to</strong>r grid), and then<br />

pass through the second grid as a fast-moving ion beam.<br />

On the downstream side <strong>of</strong> the accelera<strong>to</strong>r grid, electrons<br />

are injected back in<strong>to</strong> the beam before it is expelled so<br />

that the spacecraft remains electrically neutral. If only<br />

positively-charged ions were allowed <strong>to</strong> escape, the vehicle<br />

would become more and more negatively-charged<br />

until it prevented the thruster working at all.<br />

ion propulsion<br />

arcjet thrusters<br />

resis<strong>to</strong>jet thrusters<br />

microwave plasma thrusters<br />

electron bombardment thrusters<br />

contact ion thrusters<br />

field emission/colloid thrusters<br />

Hall-effect thrusters<br />

pulsed-plasma thrusters<br />

magne<strong>to</strong>plasmadynamic thrusters<br />

helicon thrusters<br />

electrostatic propulsion<br />

A form <strong>of</strong> electric propulsion in which the thrust is produced<br />

by accelerating charged particles in an electrostatic<br />

field. It includes three types <strong>of</strong> device: electron bombardment<br />

thrusters, ion contact thrusters, and field<br />

emission/colloid thrusters. Of these, the first two<br />

involve the production and acceleration <strong>of</strong> separate ions<br />

and are therefore forms <strong>of</strong> ion propulsion. <strong>The</strong> third<br />

type involves the production and acceleration <strong>of</strong> charged<br />

liquid droplets. Only electron bombardment thrusters<br />

have been used operationally aboard spacecraft.<br />

electrothermal propulsion<br />

A form <strong>of</strong> electric propulsion in which electrical energy<br />

is used <strong>to</strong> heat a suitable propellant, causing it <strong>to</strong> expand<br />

through a supersonic nozzle and generate thrust. Two<br />

basic types <strong>of</strong> electrothermal thruster are in use <strong>to</strong>day:<br />

the resis<strong>to</strong>jet and the arcjet. In both, material characteristics<br />

limit the effective exhaust velocity <strong>to</strong> values similar<br />

<strong>to</strong> those <strong>of</strong> chemical rockets. A third, experimental type is<br />

the microwave plasma thruster, which potentially could<br />

achieve somewhat higher exhaust velocities.

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