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Earth Moon Libration Point (L1) Gateway Station –

Earth Moon Libration Point (L1) Gateway Station – Libration Point Transfer Vehicle Kickstage Disposal Options. Presented to the International Conference On Libration Point Orbits and Applications June 10-14, 2002, Parador d’Aiguablava, Girona, Spain.

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Earth Moon Libration Point (L1) Gateway Station –

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  1. Earth Moon Libration Point (L1) Gateway Station – Libration Point Transfer Vehicle Kickstage Disposal Options Presented to the International Conference On Libration Point Orbits and Applications June 10-14, 2002, Parador d’Aiguablava, Girona, Spain G. L. Condon, NASA – Johnson Space Center / EG5, 281-483-8173, gerald.l.condon1@jsc.nasa.gov C. L. Ranieri, NASA – Johnson Space Center S. Wilson, Elgin Software, Inc.

  2. Acknowledgements • Chris Ranieri* – orbit lifetime analysis • Joey Broome# – STK/Astrogator validation/movie • Sam Wilson+ – software development / analysis • Daniel M. Delwood + – analysis * JSC Co-op # JSC Engineer + Elgin Software, Inc.

  3. Outline • Introduction • Expeditionary vs. Evolutionary Missions • Libration Point Transfer Vehicle (LTV) Kickstage Disposal Options • Geocentric Orbit Lifetime • Conclusion

  4. Introduction The notion of human missions to libration points has been proposed for more than a generation The Gateway concept supports an Evolutionary vs. Expeditionary approach to exploration … • A human-tended Earth-Moon (EM) libration point (L1) Gateway Station could support an infrastructure expanding human presence beyond low Earth orbit and serve as a staging location for human missions to: • The lunar surface • Mars • Asteroids, comets • Other libration point locations (NGST, TPF) • …

  5. Expeditionaryvs. Evolutionary • Single mission or mission set • Completed mission satisfies mission objectives • Closed-end missions Examples Apollo Skylab Apollo-Soyuz Test Project Columbus’ voyage of discovery to the new world

  6. Expeditionaryvs. Evolutionary • Ongoing missions • Open-end missions on which other missions can build • Greater initial capital investment Examples • International Space Station program • Voyages of Prince Henry the Navigator of Portugal • The man chiefly responsible for Portugal’s age of exploration

  7. Earth-Moon L1 – Gateway for Lunar Surface Operations • Celestial park-n-ride • Close to home (3-4 days) • Staging to: • Moon • Sun-Earth L2 • Mars • Asteroids • … NGST TPF Mars Sun-Earth L2 Near Earth Asteroids

  8. Gateway Operations – LTV Kickstage Disposal • Ongoing Gateway operations require robust capability for delivery & retrieval of a crew • Human occupation of the Gateway Station requires a human transfer system in the form of a Libration Point Transfer Vehicle (LTV) designed to ferry the crew between low Earth orbit and the Gateway Station. A key element of such a system is the proper and safe disposal of the LTV kickstage

  9. Purpose • Identify concepts concerning the role of humans in libration point space missions • Examine mission design considerations for an Earth-Moon libration point (L1) gateway station • Assess delta-V (DV) cost to retarget Earth-Moon L1 Gateway-bound LTV spacecraft kickstage to a selected disposal destination

  10. LTV Kickstage Disposal Options LTV/Kickstage Injection Toward L1 LTV / Kickstage Separation Options considered for LTV kickstage disposal: • Lunar Swingby to Heliocentric Orbit (HO) • Lunar Vertical Impact (LVI), typifies any lunar impact • Direct Return to Remote Ocean Area (DROA) • Lunar Swingby to Remote Ocean Area (SROA) • Transfer to Long Lifetime Geocentric Orbit (GO) LTV Crew Cab Continues to L1 LTV Kickstage Diverted to Disposal Destination

  11. Lunar Orbit Inclination = 28.6o (max. ever) Maximum L1 Arrival Wedge Angle @ Libration Point Arrival = 80.2o Earth Equator Lunar Orbit Inclination Earth Parking Orbit Earth Moon 28.6o Earth Equator 51.6o 80.2o L1 (Between Earth And Moon) Methodology • Evaluation Timeframe - 2006 Mission Year Chosen • Survey two week period of L1 arrivals yielding max (80.2o) and min (23.0o) plane changes ever possible at L1 for crewed spacecraft • 28.6o lunar orbit inclination; coplanar departure from 51.6o ISS orbit • Moon goes from perigee to apogee during the chosen 2-week period; begins and ends on the equator • Combine max and min plane changes with arrivals at L1 perigee and apogee by looking at both choices of arrival velocity azimuth (northerly and southerly) for every arrival date (requires arbitrary ISS orbit nodes)

  12. Methodology (continued) • HO, LVI, DROA, SROA, and GO maneuver times designed to minimize DV for stage disposal subject to imposed constraints • Solutions considered to be a practical attempt to minimize these maneuver DVs (e.g.: coplanar kickstage deflection maneuver assumed optimal for some disposal options) and not rigorous global optimizations Analysis • Analysis Tools • Earth Orbit to Lunar Libration (EOLL) scanner* • Four-body model • Earth, moon, sun, spacecraft • Jean Meeus's analytic lunar and solar ephemerides • Overlapped conic split boundary value solutions individually calibrated to multiconic accuracy • Validation with STK/Astrogator * Developed and updated by Sam Wilson

  13. Option 1. Lunar Swing-By to Heliocentric Orbit (HO) 6. Kickstage flies behind trailing limb of Moon to achieve geocentric C3>0 (hence departure from Earth-Moon system) Moon 3.5 day transfer L1 5. Spacecraft arrives at L1 84 • Nominal crew vehicle trajectory to Earth-Moon L1 • Trip time = 3.5 days (84 hours) • Braking maneuver at L1 1. Libration Point Transfer Vehicle (LTV) spacecraft with Kickstage in initial 407 x 407 km parking orbit Earth 4. Jettisoned kickstage performs maneuver to achieve close encounter with moon 3. Coast phase; Kickstage jettison 2. . Kickstage injects spacecraft & kickstage onto transfer trajectory toward L1

  14. Option 1. Lunar Swing-By to Heliocentric Orbit (HO) Video

  15. Moon at Moon at Perigee Apogee Option 1. Lunar Swing-By to Heliocentric Orbit (HO)

  16. Option 1. Lunar Swing-By to Heliocentric Orbit (HO) • Advantages • No Earth or Lunar disposal issues (e.g., impact location, debris footprint, litter) • Relatively low disposal DV cost • Disadvantages • Heliocentric space litter (kickstage heliocentric orbit near that of the earth) • Periodic possibility of re-contact with Earth

  17. Option 2. Lunar Vertical Impact (LVI) 6. Kickstage impacts Lunar surface Moon L1 5. Spacecraft arrives at L1 1. Lunar Transfer Vehicle (LTV) spacecraft with Kickstage in initial 407 x 407 km parking orbit Earth 4. Jettisoned kickstage performs maneuver to achieve lunar impact 3. Coast phase Kickstage jettison 2. Kickstage injects spacecraft & kickstage onto transfer trajectory toward L1

  18. Option 2. Lunar Vertical Impact (LVI)Video

  19. Moon at Moon at Perigee Apogee Option 2. Lunar Vertical Impact (LVI)

  20. Option 2. Lunar Vertical Impact (LVI) • Advantages • No Earth disposal issues (e.g., impact location, debris footprint, litter, possible recontact) • Disadvantage • Lunar litter • Relatively high disposal DV cost

  21. Option 3. Direct Return to Remote Ocean Area (DROA) 5. Spacecraft arrives at L1 Moon L1 1. Lunar Transfer Vehicle (LTV) spacecraft with Kickstage in initial 407 x 407 km parking orbit • Kickstage returns to Earth for ocean impact Earth 4. Jettisoned kickstage performs maneuver to achieve 20° atmospheric entry angle and mid-ocean impact 2. Kickstage injects spacecraft & kickstage onto transfer trajectory toward L1 3. Coast phase; Kickstage jettison

  22. Option 3. Direct Return to Remote Ocean Area (DROA)DV Budget Gives 240o Longitude Control • Entry flight path angle = -20o selected • Confines surface debris footprint • Impact latitude is determined by: • Spacecraft date of arrival at L1 and • Choice of northerly or southerly velocity azimuth at L1 arrival • From an established (e.g., ISS) earth orbit, these two degrees of freedom typically yield two or three transfer opportunities to L1 every month. • Impact longitude depends on (1.) and (2.) above, plus 3. Atmospheric entry time chosen for the kickstage • Minimizing the kickstage deflection DV determines an unique (and essentially random) impact longitude for an arbitrary transfer opportunity. • Kickstage budget gives 240 degrees of longitude control • If kickstage disposal is not to constrain the primary mission, the kickstage DV budget must be sufficient to allow the impact point to be moved from its minimum-DV location to an Atlantic or a Pacific mid-ocean line. • At any latitude, the maximum longitude difference between the chosen mid-ocean lines is 240 degrees (see next chart).

  23. Option 3. Direct Return to Remote Ocean Area (DROA)Shaded Region Contains Max Longitude Difference (240o) Between Mid-Atlantic and Mid-Pacific Target Lines x x x x x x x x x x x x x x x x Ocean Impact demo location x x x x

  24. Option 3. Direct Return to Remote Ocean Area (DROA) Video

  25. Moon at Moon at Perigee Apogee Option 3. Direct Return to Remote Ocean Area (DROA)

  26. Option 3. Direct Return to Remote Ocean Area (DROA) • Data shown represent best of two solution subtypes • Generally there are two local optima for the location of the kickstage maneuver point in the earth-to-L1 transfer trajectory, of which the better one was always chosen • Advantages • Assuming kickstage disposal is not allowed to constrain the primary mission, this option is one of three (HO,DROA,GO) requiring the lowest DV budget that could be found (slightly more than 90 m/s in all three cases) • Avoidance of close lunar encounter, combined with steep entry over wide areas of empty ocean minimizes criticality of navigation and maneuver execution errors • Disadvantages • Not appropriate if kickstage contains radioactive or other hazardous material

  27. Option 4. Lunar Swingby to Remote Ocean Area (SROA) 5. Spacecraft arrives at Earth-Moon L1 L1 • Kickstage passes in front of Moon’s leading limb and returns to Earth for ocean impact 1. Lunar Transfer Vehicle (LTV) spacecraft with Kickstage in initial 407 x 407 km parking orbit 4. Jettisoned kickstage performs maneuver to achieve close encounter with moon 3. Coast phase; Kickstage jettison 2. Kickstage injects spacecraft & kickstage onto transfer trajectory toward L1

  28. Option 4. Lunar Swingby to Remote Ocean Area (SROA)

  29. Moon at Moon at Perigee Apogee Option 4. Lunar Swingby to Remote Ocean Area (SROA)

  30. Option 4. Lunar Swingby to Remote Ocean Area (SROA) • Advantages • None identified • Disadvantages • This option requires a greater DV budget than any other one examined. • The DV values shown are minimum values for impact at an essentially random location. • The DV required for longitude control will be even higher • Inherent sensitivity of this kind of trajectory is almost certain to require extended lifetime of the control system to perform midcourse corrections before and after perisel passage

  31. Option 5. Transfer to Long Lifetime Geocentric Orbit (GO) 4b. Alternatively, kickstage may raise perigee with maneuver at/near apogee of Earth-L1 transfer orbit Moon L1 5. Crew module arrives at L1 1. Lunar Transfer Vehicle (LTV) crew module with Kickstage in initial 407 x 407 km parking orbit • Kickstage continues on parking orbit Earth 4a. Jettisoned kickstage performs retargeted Earth parking orbit maneuver 3. Coast phase Kickstage jettison 2. Kickstage injects crew module & kickstage onto transfer trajectory toward L1

  32. Option 5. Transfer to Long Lifetime Geocentric Orbit (GO) Video

  33. Moon at Moon at Perigee Apogee Option 5. Transfer to Long Lifetime Geocentric Orbit (GO)

  34. Option 5. Transfer to Long Lifetime Geocentric Orbit (GO) • Advantages • Preferable to deliberate ocean impact if kickstage carries hazardous material • In 4 of the 22 cases studied, the DV requirement for GO disposal (into an orbit having a perigee altitude of 6600 km and an apogee altitude in the range of 300000 – 370000 km) was less than 12 m/s, which is much lower than that found for any other option considered. • Assuming the 22 cases represent an unbiased sample of all possible transfers between earth orbit and L1, this implies that a 12 m/s budget would suffice if it were permissable to forgo all but about 20% of the otherwise-available transfer opportunities. • Disadvantages • More orbital debris in the earth-moon system • The 12 m/s budget described above would increase the average interval between usable transfers to something like 50 days, as opposed to 10 days if transfer utilization were not allowed to be constrained by the disposal DV budget (which would then have to be more than 90 m/s). • To achieve acceptable orbit lifetime, lunar and solar perturbations may necessitate a higher perigee and/or lower apogees, either of which will increase the required DV.

  35. Summary Results HO, LVI, DROA, SROA, GO Transfer Delta-V vs. Libration Point Arrival Time V Cost to Deflect LTV Kickstage from L1 Target to Disposal Destination D Moon at Moon at 140 Perigee Apogee 130 SROA N 120 SROA S LVI N 110 LVI S 100 HO N DROA S 90 V (m/s) HO S 80 D 70 GO N Deflection 60 50 DROA N 40 Key: N=North L1 Arrival Azimuth S=South L1 Arrival Azimuth 30 HO = Heliocentric Orbit LVI = Lunar Vertical Impact 20 DROA = Direct Remote Ocean Area SROA = (Lunar) Swingby Remote Ocean Area 10 GO S GO = Geocentric (Parking) Orbit 0 10/6/06 0:00 10/8/06 0:00 10/10/06 0:00 10/12/06 0:00 10/14/06 0:00 10/16/06 0:00 10/18/06 0:00 10/20/06 0:00 Libration Point Arrival Time (mm/dd/yy hh:mm)

  36. Geocentric Orbit Lifetime Study

  37. Geocentric Orbit Lifetime • Spacecraft (kickstage) initial condition – Apogee of LEO to EM L1 transfer orbit • Apogee range: 300,000 km – 371,000 km • Perigee range: 6600 km – 20,000 km • 45 test case runs • Results • 56% of the test cases impacted the Earth within 10 years • Spacecraft cannot be left on transfer orbit • Further study to determine safe Apogee and Perigee Ranges

  38. LTV Orbit Lifetime Note: A negative lifetime indicates LTV kickstage experienced either heliocentric departure from the Earth-Moon system or Lunar impact 45 transfer orbits in sample space

  39. Summary • Recommend Direct Remote Ocean Area impact disposal for cases without hazardous (e.g., radioactive) material on LTV kickstage • Controlled Earth contact • Relatively small disposal DV • Avoids close encounter with Moon • Trajectories can be very sensitive to initial conditions (at disposal maneuver) • DV to correct for errors is small • Recommend Heliocentric Orbit disposal for cases with hazardous material on LTV kickstage • No Earth or Lunar disposal issues (e.g., impact location, debris footprint, litter) • Relatively low disposal DV cost • Further study required to determine possibility of re-contact with Earth

  40. Additional Slides

  41. Summary Results

  42. Earth Moon L1 - Orbit Lifetime Study • Possible future missions to Earth-Moon (EM) L1 Libration Point – Gateway Station • Need to develop safe disposal guidelines for such a mission • Do not want nuclear payloads crashing into Earth

  43. Earth Moon L1 Study • Three orbit lifetime studies using STK/Astrogator: • S/c left on transfer orbit to EM L1 with low perigee and an apogee near EM L1 (343,000 km) • S/c left at EM L1 with no relative velocity to EM L1 and no station keeping • S/c left at EM L1 with a parametric scan of impulsive delta-Vs of varying magnitudes and directions (0 - 360 degrees; 0 - 500 m/s) • Propagation utilizes multiple gravitation sources • Earth (central), Sun, Moon, Mars, and Jupiter • Coordinate System defined with origin at EM L1

  44. Earth-Moon L1 - Orbit Lifetime Spacecraft Initially at L1 • The spacecraft possesses zero initial position and velocity relative to Earth-Moon L1 • With no station-keeping maneuvers, spacecraft drifts from L1 position • EM L1 location shifts as the Earth and Moon positions change • EM L1 Earth distance: 302830 km – 345298 km • No Earth Impacts found – Either lunar impacts or the s/c uses the lunar gravity to go heliocentric • Un-discernable pattern (given data sample space)

  45. L1 Orbit Lifetime vs. EM L1 Position in Lunar Cycle Orbit lifetimes <100 years result in either lunar impact or heliocentric trajectory (via lunar fly-by) No Earth impacts occurred (for these 18 sample propagations)

  46. EM L1 Orbit Lifetime w/ Delta-Vs • Seven Total Earth Impacts • Earth Impact for a case with a Δv as small as 10 m/s • No discernible pattern to results by either magnitude, direction, or epoch for maneuver

  47. Orbit Lifetime for Spacecraft at L1Initial DV of 10-500 m/s; 360o Range Relative to Initial Velocity

  48. 100 Years 100 Years 1.71 Years 0.033 years Earth Impact Lunar Impact Escape to Heliocentric Orbit 0.618 Years 100 Years 0.402 years Maneuver at Earth-Moon L1 (345,187 km apogee)DV = 100 m/s Over 360o Range of Direction 100 Years In Earth Orbit L1 Velocity Direction

  49. EM L1 Orbit Lifetime – Future Work • Further studies to better define safe disposal guidelines for s/c launched to EM L1 • Further examine lifetimes for s/c at or near EM L1 position and velocity • Examine transfers to other disposal orbits, possibly b/w GEO and EM L1 that are less affected by lunar perturbations • Write for paper to be possibly presented in Spain on this work

  50. Human Presence in Space • Demonstrated benefit to human presence • Hubble Space Telescope deploy and repair • Retrieval of Long Duration Exposure Facility • Retrieval of Westar and Palapa satellites

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