John Company

AAWSAP DIRD, Aneutronic Fusion Propulsion II, November 2010

DOW-UAP-D146 · page 24 of 36

Page 24 of 36 of DOW-UAP-D146

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Figure 14. Comparison of Fusion, Nuclear-Thermal, and Chemical Propulsion
for Same Payload.
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Thrust-to-weight ratio
Figure 15. Thrust-to-Weight Ratio and Exhaust Velocity Regimes for Various
Long-Range Space Propulsion Options.
INTERSTELLAR
The ability of fusion propulsion to carry payloads or travelers to a habitable star tens of
light-years away will be limited by the amount of fusion fuel it can transport or gather
along its route. A simple calculation of the amount of energy to move a space-shuttle­
sized veh icle (100 Mg) to the nearest star, Alpha Centauri, indicates a minimum
amount of energy in the mass equivalent of 106 kg. However, in 1960 Robert Bussard
proposed the use of magnetic fields to scoop interstellar hydrogen to fuel a fusion
rocket to propel a spacecra~ now know as the Bussard Ram Jet (shown in Figure 16).20
Although interstellar hydrogen does not fuse, Bussard proposed the use of the stellar
carbon-nitrogen-oxygen (CNO) cycle in which carbon is used as a catalyst to burn
hydrogen through the strong nuclear reaction. However, the size of the scoops and the
fusion power required to maintain them makes this concept unlikely to be realized.
UNCLASSIFIED//fOfl Offl@IAk l:ISE 8HkY
19