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GRACE & The Global Water Cycle GRACE & The Global Water Cycle Jianli Chen Jianli Chen Center for Space Research, University of Texas at Austin Center for Space Research, University of Texas at Austin E-mail: chen@csr.utexas.edu


  1. GRACE & The Global Water Cycle GRACE & The Global Water Cycle Jianli Chen Jianli Chen Center for Space Research, University of Texas at Austin Center for Space Research, University of Texas at Austin E-mail: chen@csr.utexas.edu E-mail: chen@csr.utexas.edu

  2. Outline Outline GRACE  About GRACE  Time-Variable Gravity Time-Variable Gravity   The Global Water Cycle The Global Water Cycle   GRACE & The Global Water Cycle GRACE & The Global Water Cycle 

  3. GRACE MISSION GRACE MISSION Science Goals High resolution, mean and time variable gravity field for Earth System Science applications. Mission Systems Instruments • HAIRS (JPL/SSL/APL) • SuperSTAR (ONERA) • Star Cameras ( � DTU) • GPS Receiver (JPL) Satellite (JPL/Astrium) Launcher (DLR/Eurockot) Operations (DLR/GSOC) Science (CSR/JPL/GFZ) Orbit Launched: March 17, 2002 Initial Altitude: 500 km Inclination: 89 deg Eccentricity: ~0.001 Separation Distance: ~220 km Nominal Mission : 5 (extended to 8) years

  4. Progress in Gravity Field Resolution Progress in Gravity Field Resolution Decades of tracking to geodetic satellites 111 days of GRACE data 13 months of GRACE data

  5. GRACE Main Products GRACE Main Products  Time-variable gravity field solutions at approximately Time-variable gravity field solutions at approximately  monthly intervals. monthly intervals.  Static mean gravity fields (e.g., GGM01C, GGM02C, Static mean gravity fields (e.g., GGM01C, GGM02C, … …). ).   In forms of fully normalized spherical harmonics (or Stokes In forms of fully normalized spherical harmonics (or Stokes  coefficients) up to degree and order 120. coefficients) up to degree and order 120.  From three processing centers, CSR, GFZ, and JPL. From three processing centers, CSR, GFZ, and JPL.   Supporting data products, GAC, GAB, GAA, and etc. Supporting data products, GAC, GAB, GAA, and etc. 

  6. Example Product Example Product CSR constrained RL01 solutions. CSR constrained RL01 solutions.   44 monthly solutions, covering the period Apr 2002 - Mar 2006. 44 monthly solutions, covering the period Apr 2002 - Mar 2006.   The longest GRACE time series so far. The longest GRACE time series so far.   Month Jan Feb Mar Apr May Jun Jul Aug Sep Oct Nov Dec 2002 2003 2004 2005 2006

  7. Outline Outline GRACE  About GRACE  Time-Variable Gravity Time-Variable Gravity   The Global Water Cycle The Global Water Cycle   GRACE & The Global Water Cycle GRACE & The Global Water Cycle 

  8. The Earth’ ’s Time-Variable Gravity s Time-Variable Gravity The Earth The geopotential field is determined by mass distribution within the Earth’s system, and is conveniently expressed in a spherical harmonic expansion as,   l l ∞   U ( r , φ , λ ) = GM e R e   1 + ⋅ ( C lm cos m λ + S lm m λ ) P lm (sin φ ) ∑ ∑   r r     l = 2 m = 0   where, r, φ , λ are the geocentric distance, latitude, and longitude; G is the gravitational constant; M e , R e are the mass and equatorial radius of the Earth; C lm , S lm are the spherical harmonics of degree l and order m; are the Legendre polynomials of degree l and order m. P lm (sin φ )

  9. The Earth’ ’s Time-Variable Gravity s Time-Variable Gravity The Earth C lm & S lm are computed from mass changes as 1 (2 − δ 0 m )( l − m )! r l ⋅ P C lm = lm (sin φ ) ⋅ cos m λ ⋅ dM ∫ l ( l + m )! M e R e M 1 (2 − δ 0 m )( l − m )! r l ⋅ P S lm = lm (sin φ ) ⋅ sin m λ ⋅ dM ∫ l ( l + m )! M e R e M Monthly changes of C lm & S lm are provided by GRACE, which can be used to infer mass variations in the Earth system.

  10. Three Representations: Three Representations:  Spherical Spherical Harmonics Harmonics Δ C lm & Δ S lm  Surface Surface mass mass load load change change ∆ σ l ∞ Δ σ ( θ , φ ) = R e ρ ave 2 l + 1 W l ˜ P lm (cos θ ) × [ Δ C lm cos( m φ ) + Δ S lm sin( m φ )] ∑ ∑ 3 1 + k l l = 0 m = 0 change ∆ N  Geoid Geoid height height change l ∞ W l ˜ Δ N ( θ , φ ) = R e P lm (cos θ ) × [ Δ C lm cos( m φ ) + Δ S lm sin( m φ )] ∑ ∑ l = 0 m = 0 W l = W l ( r ) is the Gaussian weighting as a function of spatial radius, r .

  11. Surface Mass Changes from GRACE Surface Mass Changes from GRACE Main issues to solve: Main issues to solve: Spatial smoothing is needed as high degree and order terms are Spatial smoothing is needed as high degree and order terms are   dominated by noise. dominated by noise. Appropriate treatments of low degree harmonics (e.g., the large Appropriate treatments of low degree harmonics (e.g., the large   uncertainty of C20 in RL01 solutions, and the missing geocenter, uncertainty of C20 in RL01 solutions, and the missing geocenter, degree-1 terms in GRACE data). degree-1 terms in GRACE data). How to validate GRACE estimates? How to validate GRACE estimates?   How to minimize leakage effects due to the spatial smoothing? How to minimize leakage effects due to the spatial smoothing?   What is the effective spatial resolution of GRACE? What is the effective spatial resolution of GRACE?  

  12. The Challenge of Spatial Smoothing The Challenge of Spatial Smoothing

  13. The Challenge of Low Degree Terms The Challenge of Low Degree Terms

  14. Outline Outline GRACE  About GRACE  Time-Variable Gravity Time-Variable Gravity   The Global Water Cycle The Global Water Cycle   GRACE & The Global Water Cycle GRACE & The Global Water Cycle 

  15. The Global Water Cycle The Global Water Cycle

  16. The Global The Global Water Water Cycle Cycle The The Global Global Water Water Cycle Cycle (Courtesy of NASA Water and Energy Cycle Project)

  17. The Global Water Cycle The Global Water Cycle Hydrological Cycle - Hydrological Cycle - Precipitation (P) Precipitation (P)   Evapotranspiration (E)  Runoff (R) Runoff (R)   P E Water storage change ( Water storage change ( Δ Δ S) S)   Basic Conservation Equation Basic Conservation Equation Δ Δ S = P - E - R S = P - E - R   R Δ S S Δ

  18. Hydrological Interests Hydrological Interests Terrestrial water storage change ( Δ S) - soil moisture & ground water soil moisture & ground water Terrestrial water storage change ( Δ S) -     Δ Δ S = P - E - R S = P - E - R Polar ice sheet mass balance ( Δ S) Polar ice sheet mass balance ( Δ S)   Δ S = P - E - R   Δ S = P - E - R Snow water equivalent ( Snow water equivalent ( Δ Δ SWE) SWE)   Δ SWE = P - E - R - Δ S   Δ SWE = P - E - R - Δ S Evapotranspiration (E)   E = P - R - Δ S Δ S Runoff (R) Runoff (R)    R = P - E - Δ S Δ S

  19. OB World Major River Basins Mississippi Amazon Bay of Bengal

  20. Antarctica Ice Sheet Antarctica Ice Sheet The Antarctic ice sheet has a total area of ~ 14,000,000 km 2 2 and averaged ice sheet thickness of and averaged ice sheet thickness of The Antarctic ice sheet has a total area of ~ 14,000,000 km ~ 2.16 km, accounts for 90% of the world’ ~ 2.16 km, accounts for 90% of the world ’s ice and 75% of the world s ice and 75% of the world’ ’s fresh water resources, s fresh water resources, and has the potential to raise the global sea level by over 70 meters if completely melt. and has the potential to raise the global sea level by over 70 meters if completely melt.

  21. Greenland Ice Sheet Greenland Ice Sheet The Greenland ice sheet is the 2 nd nd largest ice cap on Earth, and contains ~ largest ice cap on Earth, and contains ~ The Greenland ice sheet is the 2 2.5 million cubic kilometers or 10% of total global ice mass. The glacial 2.5 million cubic kilometers or 10% of total global ice mass. The glacial complex in southeast Greenland is among the most active glaciers. complex in southeast Greenland is among the most active glaciers.

  22. Mountain Glaciers Mountain Glaciers Mountain glaciers (e.g., those in the Gulf of Alaska region) only hold a small portion of Mountain glaciers (e.g., those in the Gulf of Alaska region) only hold a small portion of the world’ the world ’s ice. However, they are more vulnerable to the global warming and regional s ice. However, they are more vulnerable to the global warming and regional climate change, and thus may have comparable amount of melting (as compared with climate change, and thus may have comparable amount of melting (as compared with polar ice sheets) and contribute significantly to the global sea level rise. polar ice sheets) and contribute significantly to the global sea level rise.

  23. Outline Outline GRACE  About GRACE  Time-Variable Gravity Time-Variable Gravity   The Global Water Cycle The Global Water Cycle   GRACE & The Global Water Cycle GRACE & The Global Water Cycle 

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