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S.1 Spacecraft Propulsion Systems Chapter 1: Introduction to ...

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Kinetic energy in the expelled mass<br />

- 19-<br />

Electric propulsion leads <strong>to</strong> higher exhaust velocities achieved by chemical propulsion (ve<br />

< 5000 m/s), by this saving mass of propellant.<br />

Power Input<br />

Since power is the major constrain for electric thrusters on spacecraft, the following example will<br />

illustrate the impact of power on limiting of thrust levels for electric propulsion.<br />

The power input <strong>to</strong> a thruster system is:<br />

ve<br />

P = F [W]<br />

2η<br />

F<br />

2η<br />

= P [N]<br />

ve<br />

With the assumption:<br />

P = 1000W power input<br />

η = 1 (<strong>to</strong> simplify)<br />

ve = 30 000 m/s typically for electric thrusters<br />

The resulting thrust will be:<br />

2 ⎡W ≡ Nm / s⎤<br />

F = 1000 = 0.<br />

067<br />

30000 ⎢<br />

⎣ m / s ⎥<br />

⎦<br />

[ N ]<br />

Conclusion: Thrust levels of electric propulsion will be

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