L1 and L2 Observatories in the Post-2010 Era Warren Wiscombe & Jay Herman NASA Goddard Francisco Valero Scripps Oceanography
Dec 14, 2015
L1 and L2 Observatories in the Post-2010 Era
L1 and L2 Observatories in the Post-2010 Era
Warren Wiscombe & Jay HermanNASA Goddard
Francisco ValeroScripps Oceanography
23 Jun IGARSS 2002 2
Multiple Vantage Points(from NASA’s Earth Science Vision)
Multiple Vantage Points(from NASA’s Earth Science Vision)
L1 Observatories
Molniya Orbit
GEO
L2 Observatories
Polesitter
balloons
3
L-2
Lagrange Points L1 and L2: New Planets!Lagrange Points L1 and L2: New Planets!
L-1
At L1 and L2, the sum of the Earth’s and Sun’s gravitational fields gives a net gravitational pull equal to that at Earth. Therefore, a spacecraft at L1 or L2 must orbit the Sun with the same period as the Earth.
23 Jun IGARSS 2002 6
L1 and L2 Observatories as Nerve Centers of the SensorWeb
L1 and L2 Observatories as Nerve Centers of the SensorWeb
“Perhaps Triana’s most important contribution to
Earth science observations is the potential for using
L1 observations of Earth to
integrate data from multiple spaceborne as well as
surface and airborne observation platforms
in a self-consistent global database for study of the
planet and documenting the extent of regional and
global change.”
National Academy of Sciences report on Triana, March 2000
23 Jun IGARSS 2002 7
Unique L1/L2 AttributesUnique L1/L2 Attributes
• Relate and connect all other observational assets
• Synoptic view (all times at once)
• High time resolution (1 min or better)
• Sunrise to sunset coverage
• Stably pull out small, delicate effects over many years– Monthly Moon calibration opportunities
– Looong integrations for higher accuracy
• Assist field programs
• Much simpler data processing compared to LEO, GEO
• A true global change observing location!
23 Jun IGARSS 2002 8
Low Earth Orbit (LEO) and L1 ViewsLow Earth Orbit (LEO) and L1 Views
45-min LEO swath
LEO view of Earth takes ~45 min to paint one swath covering ~1/14th of the planet — 11 hr to paint whole planet.
From L1, can do same in less than 1 min (over 600x faster).
Sunrise to sunset instantly
23 Jun IGARSS 2002 9
Geostationary (GEO) Satellite ViewsGeostationary (GEO) Satellite Views
Each GEO takes 15-30 min to paint its covered area.
23 Jun IGARSS 2002 10
Spatio-Temporal Domain of a LEO Satellite vs. an L-1 Observatory
Spatio-Temporal Domain of a LEO Satellite vs. an L-1 Observatory
L1 DOMAIN
LEO DOMAIN
23 Jun IGARSS 2002 11
Electrostatic Analyzer /Magnetometer Boom
Faraday CupNISTAR
EPIC
The Triana SatelliteThe Triana Satellite
23 Jun IGARSS 2002 15
EPIC Science ObjectivesEPIC Science Objectives
• Ozone
• Aerosols
• Cloud phase (ice, water) and particle shape
• Column water vapor
• UV at the surface
• Stratospheric dynamics
• “Hotspot” — vegetation direct backscatter
23 Jun IGARSS 2002 16
Solar Occultation from Lagrange point L2 using Fourier Transform Imaging Spectrometer with 10 Meter telescope
Wavelength Range: 1 – 4 m
Resolution: 5 cm-1 or better
Spatial Resolution: 1–2 km in altitude
Available Solar Flux ~ 12 - 15% of Total Sun
L2 Earth Atmosphere Solar-Occultation ImagerL2 Earth Atmosphere Solar-Occultation Imager
L2–EASISun
23 Jun IGARSS 2002 17
Detector rotates around Earth limb– 2 km altitude resolution– 1 to 4 m spectrum
Exposed Sun: – 15% of solar area – 4% of solar radius
NightsideEarth
440 km in Earthcoordinates;53,500 km on Sun
Sun Eclipsed by Earth from L-2Sun Eclipsed by Earth from L-2
23 Jun IGARSS 2002 18
L2–EASI: Science GoalsL2–EASI: Science Goals
• Measure greenhouse gases at sunrise, sunset...
– CO2, CH4, H2O, O3, O2, N2O
• and get their first 3-D Mapping with resolution
– Height, 2 km: Latitude, 1o Longitude, 2o
23 Jun IGARSS 2002 20
Other L2 Science GoalsOther L2 Science Goals
• Magnetotail• Cosmic rays• Lightning• Aurora• Airglow• Incoming bolides
23 Jun IGARSS 2002 21
L1 and L2 Synergy: Two Examples
(1) Day and night observations of clouds
(2) dynamic observations of solar disturbances outside of the bowshock and within the magnetotail
L1
L2
23 Jun IGARSS 2002 22
Technical Challenges at L1 and L2Technical Challenges at L1 and L2
• Large apertures (10 meter)• Communications back to Earth (at all!)• Data rate back to Earth• Orbit design• Power at L2• Rotation of Earth• Thermal control (L2)
23 Jun IGARSS 2002 24
26,000 km 14,000 km 400 km
Halo OrbitsHalo Orbitscan have anyradius (more fuel to insert into tighter orbit)...
but period is always 6 months.
orbits are 3D; planar projections are Lissajous figures (orbit evolves from one quasi-ellipse to another over several years)
stationkeeping once/month or more