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Space Propulsion - IAP/TU Wien

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<strong>Space</strong> <strong>Propulsion</strong><br />

• a fixed total mass M of propellant is available for<br />

….acceleration of a payload of mass m L<br />

• compare the velocity gains, when the propellant is<br />

….consumed in a single – stage or a multi – stage rocket<br />

Assumptions:<br />

• initial / final mass ratios identical = R for all stages<br />

• mass of supporting structure in each stage is same fraction φ<br />

….of propellant mass of respective stage (φ = „tankage factor“)<br />

1. St.<br />

2. St.<br />

3. St.<br />

( + φ)<br />

mL<br />

+ m1 1<br />

R =<br />

mL<br />

+ φm1<br />

mL<br />

+<br />

R =<br />

m +<br />

R =<br />

m<br />

L<br />

L<br />

m<br />

+<br />

( m1<br />

+ m2<br />

)( 1+<br />

φ)<br />

m1( 1+<br />

φ) + φm2<br />

L<br />

+ ( m1<br />

+ m2<br />

+ m3<br />

)<br />

( m1<br />

+ m2<br />

)( 1+ φ ) + φm3<br />

m<br />

1<br />

R −1<br />

=<br />

1−φ<br />

m<br />

L<br />

( R −1)<br />

)<br />

R −1<br />

m2 =<br />

L<br />

1 φ<br />

1−φ<br />

[ m + ( + ) m1<br />

]<br />

( R −1)<br />

)<br />

R −1<br />

m3 =<br />

L<br />

1 φ +<br />

1−<br />

φ<br />

[ m + ( + )( m1<br />

m2<br />

)]<br />

( R −1)<br />

R −1<br />

ρ =<br />

1−φ<br />

( R −1)<br />

ψ = ( 1+ φ)ρ<br />

m<br />

i<br />

= ρmL<br />

+ ψ . Si−1<br />

propellant mass for i th stage;<br />

S i<br />

… sum of propellant masses m 1<br />

,<br />

m 2<br />

, …, m i

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