Orbit Selection for the WATER HM Mission R. S. Nerem CCAR, CIRES, University of Colorado D. P. Chambers Center for Space Research, University of Texas.

Slides:



Advertisements
Similar presentations
Global Ocean Tide Models – Assesment of Errors and their Impact on GRACE gravity fields Roman Savcenko and Wolfgang Bosch Deutsches Geodätisches Forschungsinstitut.
Advertisements

Surface Water and Ocean Topography (SWOT) Satellite Mission
WaTER/Hydrosphere Mapper: A wide swath altimetry mission for hydrology and oceanography Lee-Lueng Fu Douglas Alsdorf Nelly Mognard OSTST Meeting, March.
ECCO-2 and NASA Satellite Missions Lee-Lueng Fu Jet Propulsion Laboratory January 22-23, ECCO-2 Meeting.
Preliminary SWOT Orbit Design Study R. Steven Nerem, Ryan Woolley, George Born, James Choe Colorado Center for Astrodynamics Research, University of Colorado.
Effect of Surface Loading on Regional Reference Frame Realization Hans-Peter Plag Nevada Bureau of Mines and Geology and Seismological Laboratory University.
Coastal Altimetry Workshop February 5-7, 2008 Organized by: Laury Miller, Walter Smith: NOAA/NESDIS Ted Strub, Amy Vandehey: CIOSS/COAS/OSU With help from.
MR P.Durkee 5/20/2015 MR3522Winter 1999 MR Remote Sensing of the Atmosphere and Ocean - Winter 1999 Active Microwave Radar.
2-3 November 2009NASA Sea Level Workshop1 The Terrestrial Reference Frame and its Impact on Sea Level Change Studies GPS VLBI John Ries Center for Space.
Essentials of Oceanography 7th Edition
Unit 3 Lesson 2 Moon Phases and Eclipses
WATER HM maating, Washington, DC 2007 Tidal corrections for the WATER mission F. Lyard LEGOS, CNRS, Toulouse.
Surface Water and Ocean Topography Mission (SWOT)
Sea Level Change Observation Status on the elements of the puzzle Christian Le Provost LEGOS / CNRS Toulouse, France.
The Four Candidate Earth Explorer Core Missions Consultative Workshop October 1999, Granada, Spain, Revised by CCT GOCE S 59 Performance.
Coastal Altimetry Ted Strub Corinne James, Martin Saraceno, Remko Scharoo and many colleagues.
Remote Sensing: John Wilkin Active microwave systems (1) Satellite Altimetry IMCS Building Room 214C ext
Spaceborne Weather Radar
Integration Tide Gauge and Satellite Altimetry for Storm Surge and Sea Level change prediction. Ole B. Andersen and Y. Cheng (DTU, Denmark) Xiaoli Deng,
ODINAFRICA/GLOSS Sea Level Training Course
Hosted by: Lee-Lueng Fu, Hydrosphere Mapper Doug Alsdorf, WATER Funding from CNES, JPL, and NASA Welcome to a Joint Meeting of Ocean Sciences and Surface.
1 Assessment of Geoid Models off Western Australia Using In-Situ Measurements X. Deng School of Engineering, The University of Newcastle, Australia R.
OC3522Summer 2001 OC Remote Sensing of the Atmosphere and Ocean - Summer 2001 Active Microwave Radar.
Satellite Altimetry - possibilities and limitations
How Does GPS Work ?. Objectives To Describe: The 3 components of the Global Positioning System How position is obtaining from a radio timing signal Obtaining.
Sea Level Change Measurements: Estimates from Altimeters Understanding Sea Level Rise and Variability June 6-9, 2006 Paris, France R. S. Nerem, University.
Mapping Ocean Surface Topography With a Synthetic-Aperture Interferometry Radar: A Global Hydrosphere Mapper Lee-Lueng Fu Jet Propulsion Laboratory Pasadena,
(a) Pre-earthquake and (b) post-earthquake Advanced Spaceborne Thermal Emission and Reflection Radiometer (ASTER) images of North Sentinel Island. The.
A SATELLITE CONSTELLATION TO OBSERVE THE SPECTRAL RADIANCE SHELL OF EARTH Stanley Q. Kidder and Thomas H. Vonder Haar Cooperative Institute for Research.
2007 OSTST meeting Y. Faugere (CLS) J. Dorandeu (CLS) F. Lefevre (CLS) Long period errors observed at Envisat crossovers and possible impact of tides.
MERIS US Workshop, Silver Springs, 14 th July 2008 MERIS US Workshop, 14 July 2008, Washington (USA) Henri LAUR Envisat Mission Manager.
Physical Oceanography. RAP Barrier Island Major Oceans The three major oceans are : 1._______-largest, deepest, coldest, least salty. 2.__________-
Bell work If the moon had the mass of a golf ball, the approximate mass of the sun would be about 110 school busses! Even though the moon is smaller than.
–wave –crest –trough –breaker Objectives Describe the physical properties of waves. Explain how tides form. Compare and contrast various ocean currents.
REMOTE SENSING IN EARTH & SPACE SCIENCE
GRACE Mascons and Hydrological Data for the Continents: GRACE ACCESS D. Rowlands (1), F. Lemoine (1), S. Luthcke (1), S. Klosko (2), D. Chinn (2), K. Akoumany.
Progress in Geoid Modeling from Satellite Missions
Physical Oceanography Chapter 15. Major Oceans The three major oceans are : 1._______-largest, deepest, coldest, least salty. 2.__________- second largest,
1 Tides Newton's gravitational force law says that the force of gravitation attraction depends strongly on the separation between two objects. The same.
E. Schrama TU Delft, DEOS Error characteristics estimated from CHAMP, GRACE and GOCE derived geoids and from altimetry derived.
Key RO Advances Observation –Lower tropospheric penetration (open loop / demodulation) –Larger number of profiles (rising & setting) –Detailed precision.
Arctic terrestrial water storage changes from GRACE satellite estimates and a land surface hydrology model Fengge Su a Douglas E. Alsdorf b, C.K. Shum.
Joint OS & SWH meeting in support of Wide-Swath Altimetry Measurements Washington D.C. – October 30th, 2006 Baptiste MOURRE ICM – Barcelona (Spain) Pierre.
Don Chambers Center for Space Research, The University of Texas at Austin Josh Willis Jet Propulsion Laboratory, California Institute of Technology R.
SWOT: A HIGH-RESOLUTION WIDE-SWATH ALTIMETRY MISSION
Satellites Storm “Since the early 1960s, virtually all areas of the atmospheric sciences have been revolutionized by the development and application of.
Combining Altimeter-derived Currents With Aquarius Salinity To Study The Marine Freshwater Budget Gary Lagerloef Aquarius Principal Investigator Yi Chao.
Improved Marine Gravity from CryoSat and Jason-1 David T. Sandwell, Emmanuel Garcia, and Walter H. F. Smith (April 25, 2012) gravity anomalies from satellite.
Orbital Analysis for Inter-Calibration Dave Mac Donnell Brooke Anderson Bruce Wielicki Don Garber NASA Langley Research Center Solar Workshop January 30,
SATELLITE ORBITS The monitoring capabilities of the sensor are, to a large extent, governed by the parameters of the satellite orbit. Different types of.
Don P. Chambers Center for Space Research The University of Texas at Austin Wide-Swath Ocean Sciences and Hydrology Meeting 31 October 2006 Orbit Selection.
Potential for estimation of river discharge through assimilation of wide swath satellite altimetry into a river hydrodynamics model Kostas Andreadis 1,
Interannual Variability and Decadal Change of Solar Reflectance Spectra Zhonghai Jin Costy Loukachine Bruce Wielicki (NASA Langley research Center / SSAI,
1 July 20, 2000 Geosat Follow-On An examination from an operational point of view Impact on operational products Overall system performance (from sensor.
SCM x330 Ocean Discovery through Technology Area F GE.
Climate Science and Satellite Altimetry Meeting of the Committee on a Strategy to Mitigate the Impact of Sensor De-scopes and De-manifests on the NPOESS.
How Does GPS Work ?. The Global Positioning System 24+ satellites 20,200 km altitude 55 degrees inclination 12 hour orbital period 5 ground control stations.
Unit 3 Lesson 2 Moon Phases and Eclipses. Round and Round They Go! How are Earth, the moon, and the sun related in space? Earth spins on its axis and.
Thomas Herring, IERS ACC, MIT
L. Carrère, Y. Faugère, E. Bronner, J. Benveniste
L. Carrère, F. Lyard, M. Cancet, L. Roblou, A. Guillot
5th Workshop on "SMART Cable Systems: Latest Developments and Designing the Wet Demonstrator Project" (Dubai, UAE, April 2016) Contribution of.
Astronomy-Part 10 Notes The Earth-Moon-Sun Systems
Mark A. Bourassa1 Ernesto Rodriguez2 and Sarah Gille3
Section 3: Ocean Movements
Objectives and Requirements of SWOT for Observing the Oceanic Mesoscale Variability (based on a workshop held at Scripps Institution of Oceanography, April.
Corinne James, Martin Saraceno, Remko Scharoo
Tides Tides are daily changes in the elevation of the ocean surface (sea level) Ocean tides result from the gravitational attraction exerted upon Earth.
The next 3 figures are from the Ocean Pathfinder Project at NASA/GSFC The next 3 figures are from the Ocean Pathfinder Project at NASA/GSFC. Compliments.
Physical Oceanography
Presentation transcript:

Orbit Selection for the WATER HM Mission R. S. Nerem CCAR, CIRES, University of Colorado D. P. Chambers Center for Space Research, University of Texas at Austin (with input from Gregg Jacobs, Richard Ray, and John Ries)

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 General Constraints on Search l No sun-synchronous orbits l Altitudes lower than 1000 km to avoid radiation exposure l Inclinations greater than 75° in order to sample most rivers in Siberia l Repeat period ~ 20-days in order to meet groundtrack spacing requests of mesoscale oceanography and hydrology (~10 days was also considered to meet a request for higher temporal resolution studies)

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Sun Synchronous Orbits

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Why not Sun-Synchronous Orbits? l Prevents Serious Tidal Studies l Tides poleward of 66° l Tides in shallow water and estuaries l Wavelengths shorter than 300 km l Maps Diurnal Errors to Undesirable Periods l Into long-period “climate-like” signals l Into seasonal variations (annual, semi-annual) l Into the mean sea surface

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Calculating Tidal Aliasing P is satellite repeat period T is tide period  p is tide alias period

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Aliasing Considerations l For applications in oceans and estuaries, we desire a satellite orbit that aliases all tides to frequencies greater than 2 cycles-per year l The alias period is shorter than the semi-annual (half-year) signal l Can observe multiple cycles of the alias period within a few years Another important factor to consider is the separation between alias frequencies and between the aliases and annual/semi-annual (  f) l Determines time needed to separate two tides in altimeter observations Time to separate ~ 1/  f l T/P did not have optimal separation for some constituents l K1 aliased to within 0.11 cpy of semi-annual l 9-years to separate

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Tidal Aliasing ~10 Day Repeat

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Tidal Aliasing ~20 Day Repeat

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Tidal Aliasing ~20 Day Repeat

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Orbit 1 Altitude = km Inclination = 78° Repeat Period = days Orbit 2 Altitude = km Inclination = 78° Repeat Period = days Except for K1, these two orbits have very good aliasing properties for 9 major constituents

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 General Observations l Only orbits with an inclination 2 cpy l Retrograde orbits have poor aliasing of solar tides l If we do not require that the K1 alias > 2 cpy l Good orbits do exist up to 80° inclination l This covers more of the Arctic Ocean, all of the Antarctic boundary, and most rivers in Siberia

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Shallow Water Tides l In shallow water (including estuaries) tides are nonlinear and have much smaller wavelength than in the deep ocean l In 40 m, tide wavelength is 10x smaller than in 4000m l Shallow water tides are poorly observed by current altimeter systems l Examine aliasing of select nonlinear tides for potential orbits

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Orbit 1 Altitude = km Inclination = 78° Repeat Period = days Orbit 2 Altitude = km Inclination = 78° Repeat Period = days Some close aliases between nonlinear and primary tides Aliasing of Nonlinear Tides

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Comments on the Orbit “ ….. many coastal locations at mid to high latitudes would be sampled twice in each 10-day orbit, for a repeat of about 5 days. Those interested in coastal applications prefer that this repeat time not be increased. Five days will still not resolve the rapid coastal ocean response to synoptic forcing (periods of 1-5 days), relying on models to assimilate the SSH data and provide the higher temporal resolution needed.” T. Strub “The basic recommendation on orbits for mesoscale is for full coverage. So I would lean toward the longer repeat (~ 20 days) if the swath were 60 km to each side. Tidal aliasing should be considered for mesoscale.” G. Jacobs “Inclination greater than 74°, temporal sampling not critical, but more frequent overpasses desirable.”, D. Alsdorf

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Orbit Repeat Period 11-Day Repeat15-Day Repeat 21-Day Repeat

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 WaTER HM Swath

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 HM sampling (9.95 days) Nadir sampling (9.95 days) Sampling with 200 km Swath

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Groundtrack Separation 140 km 200 km

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Precision Orbit Determination l Availability of GRACE gravity models has significantly reduced gravity-driven orbit error. l GPS has made precise continuous tracking routinely available. l For orbit altitudes in the km range, 2 cm orbit accuracy should be easily obtainable. l Extended antennas and solar arrays may complicate the orbit determination. l Thought should be given to monitoring motion of antenna phase centers with respect to s/c center-of-mass, attitude determination, GPS multipath issues.

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Radial Orbit Errors due to Gravity Predicted using difference between GGM02C-GFZ04C Proposed Wide-Swath OrbitJason Orbit Mean Portion RMS about Mean

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Conclusions l For a 120 km swath, a ~20 day repeat is desired to obtain near global coverage. l A variety of orbits exist with altitudes near 800 km, inclinations of ~ 78°, and repeat periods near 21 days that have good tidal aliasing properties for deep ocean tides and meet other mission requirements l Care must be given to the precision orbit determination, but 2 cm radial accuracy should be possible. l Preliminary Recommendation (Altitude = km, Inclination = 78°, Repeat Period = days) l Will be able to additionally observe the M 4 tide as well as 2MN 2, 2MS 6, and 2MS 2, will not be able to separate MS 4 and M 6 tides l More effort might find an orbit that can sample both MS 4 and M 4 well

The University of Colorado Colorado Center for Astrodynamics Research Nerem 10/29/07 Shallow Water Tides