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Two-stage launcher placing 22 t in a 400 km orbit, then a Hohmann transfer to geostationary orbit: rocket equation, plane change and propellant budget
| Tool | Orbital and Rocket Delta-v |
| Source | Martin Company (1963). Space Flight Handbooks, Volume 1: Orbital Flight Handbook, Part 2, Mission Sequencing Problems. NASA SP-33 Part 2, National Aeronautics and Space Administration, Washington, DC. Page VI-48 (the bi-elliptic ratios); Rickman, S. L. (2020). Introduction to Orbital Mechanics and Spacecraft Attitudes for Thermal Engineers. NASA Engineering and Safety Center. Charts 95 and 152 to 157 (geostationary altitude, Hohmann transfer). |
| Level | Undergraduate |
Problem
An illustrative two-stage launch vehicle (no particular vehicle) lifts a 22,000 kg payload from latitude 28.5 degrees to a 400 km circular orbit about Earth. Find the ideal velocity of the vehicle and compare it with what the ascent needs for entered losses; then find the two burns of a Hohmann transfer from that orbit to geostationary altitude, the cost of the 28.5 degree plane change, and the propellant a 5,400 kg spacecraft with a 320 s engine needs for the transfer.
Inputs to Enter
- Stage 1: dry 25,000 kg, propellant 400,000 kg, I_sp 300 s, thrust 7,600 kN; stage 2: dry 4,500 kg, propellant 100,000 kg, I_sp 348 s, thrust 980 kN; payload 22,000 kg
- Parking orbit 400 km, launch latitude 28.5 deg, gravity loss 1.5 km/s, drag and steering loss 0.2 km/s (entered estimates)
- Final altitude 35,786 km, plane change 28.5 deg, bi-elliptic intermediate altitude 200,000 km
- Budget: 2,398 m/s (1 %), 1,824 m/s (1 %), 50 m/s (10 %); end mass 5,400 kg, I_sp 320 s
- Earth: GM 398,600.4355 km³/s² (JPL DE440), equatorial radius 6,378.137 km, rotation period 23.9345 h (NASA fact sheet); g_0 = 9.80665 m/s²
Answers
- Stage 1: m_0/m_f = 551,500 / 151,500 = 3.6403, Δv = 300 · 9.80665 · ln 3.6403 = 3.8012 km/s, T/W 1.405, burn 154.8 s; stage 2: 126,500 / 26,500 = 4.7736, Δv 5.3344 km/s, T/W 0.790, burn 348.2 s
- Ideal velocity 9.136 km/s; lift-off mass 551,500 kg; payload fraction 3.989 % (4.112 % at the optimum split of the same velocity)
- Required: v_c 7.6686 + 1.5 + 0.2 − 0.4087 (site speed) = 8.960 km/s; reserve 0.176 km/s
- Hohmann 6,778.1 → 42,164.1 km: Δv_1 = 10.0660 − 7.6686 = 2.3975 km/s, Δv_2 = 3.0747 − 1.6182 = 1.4565 km/s, total 3.8540 km/s, transfer time 19,048.6 s = 5.291 h
- With the 28.5 deg plane change: 4.2215 km/s all at the second burn, 4.1963 km/s with 2.23 deg taken at the first burn; a separate plane-change burn would make it 5.3676 km/s
- Radius ratio 6.22 is below 11.939, so the Hohmann transfer beats any bi-elliptic one (4.3492 km/s through 200,000 km altitude); stationary radius 42,164.2 km, altitude 35,786.1 km, speed 3.0747 km/s
- Budget 4,319.2 m/s with margins: mass ratio 3.9605, start mass 21,386.7 kg, propellant 15,986.7 kg; 613 kg inside the 22,000 kg payload
Notes
The tool's default inputs are this case; press Submit. The vehicle and the losses are illustrative, not a printed example. Checked against an independent numerical solution (integration of the two-body equations for the transfer and of the thrust equation for the burns, constrained optimisation for the staging split) and against printed values of public documents: the bi-elliptic ratios 11.939 and 15.582, the geostationary altitude 35,786 km and others listed in test_orbital_rocket_delta_v.php (1,479 checks).