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A simple analytical equation to calculate the atmospheric drag during aerobraking campaigns. Application to Mars. PowerPoint Presentation
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A simple analytical equation to calculate the atmospheric drag during aerobraking campaigns. Application to Mars.

A simple analytical equation to calculate the atmospheric drag during aerobraking campaigns. Application to Mars.

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A simple analytical equation to calculate the atmospheric drag during aerobraking campaigns. Application to Mars.

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  1. A simple analytical equation to calculate the atmospheric drag during aerobraking campaigns. Application to Mars. François Forget & Michel Capderou Laboratoire de Météorologie Dynamique, CNRS 14/12/2010

  2. Atmospheric drag and velocity change Δvduring an orbital pass through the atmosphere

  3. Coupling an orbitography numerical model and an atmospheric model. Here: Mars Climate database (Forget et al. 2006) Ixion orbitography (Capderou 2005) http://climserv.ipsl.polytechnique.fr/ixion.html “Mars aerobraking simulator”

  4. Example : Delta V during a 200 sols (1314 orbits) “drag compensated” aerobraking campaign • - MGS like shape • - Inclination = 75° • - Excentricity = 0.4 • - Initial conditions: • Ls=0° • Periapsis at 0°N, • z=100km Can we calculate Delta V without having to run complex models for quick look estimation and mission strategy design ?

  5. Previous analytical work: very complex equations by King-Hele (1987) on the “contractions of orbit”

  6. Calculation of aerobraking Δv over one orbit • Drag force on spacecraft: • Change of velocity a time t: • Integration over one orbit (period T ) :

  7. v2 ρ

  8. Calculation of aerobraking Δv over one orbit (2) • Assuming that around perihelion the atmosphere is relatively isothermal (scale height H) : • Integration of one orbit (period T ) : • Playing with the Keplerian equations (with simplification and development around periaspis) give the variation of altitude as function of time:

  9. Relative velocity at perisapsis Scale height at periapsis (RT/g) Density at perisapsis

  10. Validation : Delta V during a 200 sols (1314 orbits) “drag compensated” aerobraking campaign • - MGS like shape • - Inclination = 75° • - Excentricity = 0.4 • - Initial conditions: • Ls=0° • Periapsis at 0°N, • z=100km

  11. Validation : Delta V during a 200 sols (1314 orbits) “drag compensated” aerobraking campaign • - MGS like shape • - Inclination = 75° • - Excentricity = 0.4 • - Initial conditions: • Ls=0° • Periapsis at 0°N, • z=100km

  12. Statistics of errors (simple equation – reference model) over one Mars year simulations Orbit Inclination:

  13. Statistics of errors (simple equation – reference model) over one Mars year simulations

  14. Impact of the relative wind • One must take into account the motion of the atmosphere in addition to the spacecraft velocityVspc. • Notice that the transverse component Vt is always negligible, unlike the axial component Va, because V02 ~ (Vspc+Va)2 >> Vt2 Atmospheric motion Vt (transverse component, galilean frame) Spacecraft velocity Vspc (Galilean frame) Atmospheric wind Va (axial component)

  15. Estimation of the relative wind • Case 1 : spacecraft velocity and atmospheric wind known from models: • Case 2: neglect planet rotation and winds • (use only spacecraft velocity in galilean frame) • Case 3: atmosphere rotating like the solid planet

  16. The error resulting from the assumption on winds depends on the orbit inclination Polar orbits

  17. Mean zonal wind predicted by the LMD Global Climate model

  18. Conclusions and perpectives • Velocity change Δv during an orbital pass through the atmosphere can be computed using a simple equation with error < ~5% (better than error on density…) • e.g. : • This should be useful for preliminary mission design by non specialists, simple scaling,to develop autonomous aerobraking system, etc… • Conversely, estimation of the velocity change provide an estimation of density at periapsis in real time. • This equation should be valid on other planets

  19. Thank you