Space Propulsion - IAP/TU Wien
Space Propulsion - IAP/TU Wien
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