AAWSAP DIRD, Aneutronic Fusion Propulsion I, November 2010
DOW-UAP-D145 · page 11 of 50
Text
This text came with the file. It may have mistakes. When the text and the image disagree, the image is right.
UNCLASSIFIED//POlt Offl@IAL WS& &NkY Specific Impulse To compare various propulsion systems and their fuel, rocket efficiency can be represented by the amount of momentum that can be obtained per unit weight of the propellant that is used. This is defined as the "specific impulse" (lsp) and is measured in units of seconds: I = Li(m v • . ,1w 11s,) = v ,x/11111S/ (1.5) ,.,, ( ) • Li ni gearth g ea1·1/t Here, earth's gravitational acceleration, gearth, is 9.81 m/s2. As described earlier, the best propulsion system is typically one that has the highest possible exhaust or propellant velocity. High specific impulse, or correspondingly high exhaust velocity, also produces low energy efficiency. Table 1: Specific Impulse for Various Rocket Engine Types En<1ine Tvpe Ve (m/s) Isa (s) Saturn V Rocket 2nd and 3rd Staqes 4 130 421 LH2/LOX Liquid Fuel Solid Rocket 2,500 255 Best Chemical Rocket Tested 5 320 542 F2/Li/H2 Chemical Rocket Nuclear Thermal Rocket 8 340 850 Ion Thruster 29 000 3 000 VASIMR 290,000 30,000 The efficiency of a rocket can be defined as the ratio of rocket thrust to the power required to generate the thrust. The resulting equations follow: Power = dE 2 (1.6) = ½(dm) V dt 2 dt e Thrust = (1.7) (dm)V dt ' UNCLASSIFIED/fF&A &FFI&I:.l.k W&li &NkY 3