DELTA-V BUDGET
'Delta-''v'' budget' (or 'velocity change budget') is a term used in astrodynamics and aerospace industry for velocity change (or delta-''v'') requirements for the various propulsive tasks and orbital maneuvers over phases of the space mission.
Sample delta-''v'' budget will enumerate various classes of manoeuvres, delta-''v'' per manoeuvre, number of manoeuvres required over the time of the mission.
In the absence of an atmosphere and landings where the ground is hit with some speed, the delta-''v'' is the same for changes in orbit the other way around: gaining and losing speed cost an equal effort.
★ Launch to LEO — this not only requires an increase of velocity from 0 to 7.8 km/s, but also typically 1.5–2 km/s for atmospheric drag and gravity drag
★ Re-entry from LEO — no delta-v is required, there is only atmospheric drag
Delta-v needed to move inside Earth Moon system (speeds lower than escape velocity) in km/s
[2]
[3]
According to Marsden and Ross, "The energy levels of the Sun-Earth L1 and L2 points differ from those of the Earth-Moon system by only 50 m/s (as measured by maneuver velocity)."[5]

★ Bi-elliptic transfer
★ Gravity assist
★ Hohmann transfer
★ The Oberth effect
★ Tsiolkovsky rocket equation
1. Frozen lunar orbits
2. list of delta-v
3. L2 Halo lunar orbit
4. NEO list
5.
New methods in celestial mechanics and mission design
6. table of cislunar/mars delta-vs
7. cislunar delta-vs
★ Delta V pages at Caltech
★ Javascript Delta V calculator
Sample delta-''v'' budget will enumerate various classes of manoeuvres, delta-''v'' per manoeuvre, number of manoeuvres required over the time of the mission.
In the absence of an atmosphere and landings where the ground is hit with some speed, the delta-''v'' is the same for changes in orbit the other way around: gaining and losing speed cost an equal effort.
| Contents |
| Launch/landing budget |
| Stationkeeping budget |
| Earth-Moon space budget |
| Interplanetary budget |
| Delta-vs around the Solar System |
| Abbreviations used |
| See also |
| References |
| External links |
Launch/landing budget
★ Launch to LEO — this not only requires an increase of velocity from 0 to 7.8 km/s, but also typically 1.5–2 km/s for atmospheric drag and gravity drag
★ Re-entry from LEO — no delta-v is required, there is only atmospheric drag
Stationkeeping budget
| Maneuver | Average delta-''v'' per year [m/s] | Maximum per year [m/s] | |||
|---|---|---|---|---|---|
| Drag compensation in 400–500 km LEO | <25 | <100 | |||
| Drag compensation in 500–600 km LEO | < 5 | < 25 | |||
| Drag compensation in > 600 km LEO | < 7.5 | ||||
| Station-keeping in geostationary orbit | 50 – 55 | ||||
| Station-keeping in L1/L2 | 30 – 100 | ||||
| Station-keeping in Moon orbit | 0 [1] – 400 | ||||
| Attitude control (3-axis) | 2 – 6 | ||||
| Spin-up or despin | 5 – 10 | ||||
| Stage booster separation | 5 – 10 | ||||
| Momentum wheel unloading | 2 – 6 | ||||
Earth-Moon space budget
Delta-v needed to move inside Earth Moon system (speeds lower than escape velocity) in km/s
| FromTo | LEO-Ken | LEO-Eq | GEO | EML-1 | EML-2 | EML-4/5 | LLO | Moon | C3 |
|---|---|---|---|---|---|---|---|---|---|
| Earth | 9.30 - 10.00 | ||||||||
| Low Earth Orbit (LEO-Ken) | 4.24 | 4.33 | 3.77 | 3.43 | 3.97 | 4.04 | 5.93 | 3.22 | |
| Low Earth Orbit (LEO-Eq) | 4.24 | 3.90 | 3.77 | 3.43 | 3.99 | 4.04 | 5.93 | 3.22 | |
| Geostationary Orbit (GEO) | 2.06 | 1.63 | 1.38 | 1.47 | 1.71 | 2.05 | 3.92 | 1.30 | |
| Lagrangian point 1 (EML-1) | 0.77 | 0.77 | 1.38 | 0.14 | 0.33 | 0.64 | 2.52 | 0.14 | |
| Lagrangian point 2 (EML-2) | 0.33 | 0.33 | 1.47 | 0.14 | 0.34 | 0.64 | 2.52 | 0.14 | |
| Lagrangian point 4/5 (EML-4/5) | 0.84 | 0.98 | 1.71 | 0.33 | 0.34 | 0.98 | 2.58 | 0.43 | |
| Low Lunar orbit (LLO) | 1.31 | 1.31 | 2.05 | 0.64 | 0.65 | 0.98 | 1.87 | 1.40 | |
| Moon (Moon) | 2.74 | 2.74 | 3.92 | 2.52 | 2.53 | 2.58 | 1.87 | 2.80 | |
| Earth Escape velocity (C3) | 0.00 | 0.00 | 1.30 | 0.14 | 0.14 | 0.43 | 1.40 | 2.80 | |
[2]
[3]
Interplanetary budget
| From | To | delta-v in km/s |
|---|---|---|
| Earth Escape velocity (C3) | Mars Transfer Orbit | 0.6 |
| Mars Transfer Orbit | Mars Capture Orbit | 0.9 |
| Mars Capture Orbit | Deimos Transfer Orbit | 0.2 |
| Deimos Transfer Orbit | Deimos surface | 0.7 |
| Deimos Transfer Orbit | Phobos Transfer Orbit | 0.3 |
| Phobos Transfer Orbit | Phobos surface | 0.5 |
| Mars Capture Orbit | Low Mars Orbit | 1.4 |
| Low Mars Orbit | Mars surface | 4.1 |
| Earth Escape velocity (C3) | Closest NEO Asteroids[4] | 0.8 - 2.0 |
According to Marsden and Ross, "The energy levels of the Sun-Earth L1 and L2 points differ from those of the Earth-Moon system by only 50 m/s (as measured by maneuver velocity)."[5]
Delta-vs around the Solar System

Delta-v's in km/s for various orbital manuevers[6][7] using conventional rockets. Red arrows show where optional aerobraking can be performed in that particular direction, black numbers give delta-v in km/s that apply in either direction. Lower delta-v transfers than shown can often be achieved, but involve rare transfer windows or take significantly longer, see: fuzzy orbital transfers. Not all possible links are shown.
Abbreviations used
| C3 | Escape orbit |
| GEO | Geosynchronous orbit |
| GTO | Geostationary transfer orbit |
| L5 | Earth-Moon fifth Lagrangian point |
| LEO-Eq | Low Earth orbit - equatorial |
| LEO-Ken | Low Earth orbit - "Kennedy inclination orbit" |
See also
★ Bi-elliptic transfer
★ Gravity assist
★ Hohmann transfer
★ The Oberth effect
★ Tsiolkovsky rocket equation
References
1. Frozen lunar orbits
2. list of delta-v
3. L2 Halo lunar orbit
4. NEO list
5.
New methods in celestial mechanics and mission design
6. table of cislunar/mars delta-vs
7. cislunar delta-vs
External links
★ Delta V pages at Caltech
★ Javascript Delta V calculator
This article provided by Wikipedia. To edit the contents of this article, click here for original source.
psst.. try this: add to faves

العربية
中国
Français
Deutsch
Ελληνική
हिन्दी
Italiano
日本語
Português
Русский
Español