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