The global S 1 tide and Earth s nutation

Similar documents
Geodätische Woche The global radiational S1 tide - current Earth rotation research at TU Wien. September 17, 2015

Anna Korbacz 1, Aleksander Brzeziński 1 and Maik Thomas 2. Journées Systèmes de référence spatio-temporels.

Tests on the validity of atmospheric torques on Earth computed from atmospheric model outputs

State-of-the-art physical models for calculating atmospheric pressure loading effects

Earth orientation parameters: excitation by atmosphere, oceans and geomagnetic jerks

Coupled data assimilation for climate reanalysis

OBSERVING AND MODELING LONG-PERIOD TIDAL VARIATIONS IN POLAR MOTION

Remaining error sources in the nutation at the submilliarc second level

Inverse Barometer correction comparison for TOPEX/Poseidon mission between Corrections based on JRA-55 and ERA-Interim atmospheric reanalyses

On assessing temporal variability and trends of coupled arctic energy budgets. Michael Mayer Leo Haimberger

Re-dimensioned CFS Reanalysis data for easy SWAT initialization

17. SIGNATURE OF EL NINO IN LENGTH OF DAY AS MEASURED BY VLBI

Analysis of the Relationship between a Change in Wind Field Curl Rate and Sea Surface Height within the Beaufort Gyre Region of the Arctic

Atmospheric Effects in Space Geodesy

Contribution of non-tidal oceanic mass variations to Earth rotation determined from space geodesy and ocean data

The Canadian approach to ensemble prediction

CHAPTER 2 DATA AND METHODS. Errors using inadequate data are much less than those using no data at all. Charles Babbage, circa 1850

ATMOSPHERIC AND OCEANIC EXCITATION OF EARTH ROTATION

MOTIVATION. New view of Arctic cyclone activity from the Arctic System Reanalysis

An Overview of Atmospheric Analyses and Reanalyses for Climate

Global reanalysis: Some lessons learned and future plans

The ECMWF prototype for coupled reanalysis. Patrick Laloyaux

Evaluation of the accuracy of the IAU 2006/2000 precession-nutation

Innovation, increments, and residuals: Definitions and examples. Patrick Heimbach MIT, EAPS, Cambridge, MA

Atmospheric angular momentum time-series: characterization of their internal noise and creation of a combined series

Global Mapping Function (GMF): A new empirical mapping function based on numerical weather model data

The JRA-55 Reanalysis: quality control and reprocessing of observational data

GPC Exeter forecast for winter Crown copyright Met Office

Ocean data assimilation for reanalysis

ERA-CLIM: Developing reanalyses of the coupled climate system

Surface Mass Loads from GRACE, GPS, and Earth Rotation

ECMWF global reanalyses: Resources for the wind energy community

WRF MODEL STUDY OF TROPICAL INERTIA GRAVITY WAVES WITH COMPARISONS TO OBSERVATIONS. Stephanie Evan, Joan Alexander and Jimy Dudhia.

Yuqing Wang. International Pacific Research Center and Department of Meteorology University of Hawaii, Honolulu, HI 96822

What brings new MERRA2 Half-step forward towards new Reanalysis generation

Earth rotation and Earth gravity field from GRACE observations. Lucia Seoane, Christian Bizouard, Daniel Gambis

The Global Mapping Function (GMF): A new empirical mapping function based on numerical weather model data

ECMWF: Weather and Climate Dynamical Forecasts

3. Carbon Dioxide (CO 2 )

Investigation on the use of NCEP/NCAR, MERRA and NCEP/CFSR reanalysis data in wind resource analysis

Steven Feldstein. The link between tropical convection and the Arctic warming on intraseaonal and interdecadal time scales

Summary of the 2012 Global Geophysical Fluid Center Workshop

Recent Developments in Climate Information Services at JMA. Koichi Kurihara Climate Prediction Division, Japan Meteorological Agency

SUPPLEMENTARY INFORMATION

The PRECIS Regional Climate Model

The Scientific Value of Stratospheric Wind Measurements

Tropical stratospheric zonal winds in ECMWF ERA-40 reanalysis, rocketsonde data, and rawinsonde data

Global Response to the Major Volcanic Eruptions in 9 Reanalysis Datasets

Climate Variables for Energy: WP2

23. EL NINO IMPACT ON ATMOSPHERIC AND GEODETIC EXCITATION FUNCTIONS OF POLAR MOTION

Dynamical coupling between the middle atmosphere and lower thermosphere

Towards a Consistent Conventional Treatment of Surface-Load Induced Deformations

Dynamics of the Atmosphere

General Circulation. Nili Harnik DEES, Lamont-Doherty Earth Observatory

On the Causes of and Long Term Changes in Eurasian Heat Waves

An Introduction to Coupled Models of the Atmosphere Ocean System

Note: This is the accepted manuscript and may marginally differ from the published version.

Ensemble-variational assimilation with NEMOVAR Part 2: experiments with the ECMWF system

SUPPLEMENTARY INFORMATION

2. DYNAMICS OF CLIMATIC AND GEOPHYSICAL INDICES

Ensemble-variational assimilation with NEMOVAR Part 2: experiments with the ECMWF system

THE FREE CORE NUTATION

Global reference systems and Earth rotation

Recent advances in modeling precession-nutation

The Dynamics of Atmospherically Driven Intraseasonal Polar Motion

Hilbert analysis unveils inter-decadal changes in large-scale patterns of surface air temperature variability

Lecture #1 Tidal Models. Charles McLandress (Banff Summer School 7-13 May 2005)

Characteristics of Storm Tracks in JMA s Seasonal Forecast Model

Status of Atmospheric Winds in Relation to Infrasound. Douglas P. Drob Space Science Division Naval Research Laboratory Washington, DC 20375

The Energy Balance Model

SUPPLEMENTARY INFORMATION

Principles of the Global Positioning System Lecture 18" Mathematical models in GPS" Mathematical models used in GPS"

How well do we know the climatological characteristics of the North Atlantic jet stream? Isla Simpson, CAS, CDG, NCAR

Introduction to geodetic VLBI

COMBINING GPS AND VLBI MEASUREMENTS OF CELESTIAL MOTION OF THE EARTH S SPIN AXIS AND UNIVERSAL TIME. Jan VONDRÁK* and Cyril RON

Concurrent simulation of the eddying general circulation and tides in a global ocean model

PCIC SCIENCE BRIEF: STORM SURGES AND PROJECTED

D.Carvalho, A, Rocha, at 2014 Applied Energy. Report person:zhang Jiarong. Date:

The Quasi-Biennial Oscillation Analysis of the Resolved Wave Forcing

Diagnosing the Climatology and Interannual Variability of North American Summer Climate with the Regional Atmospheric Modeling System (RAMS)

Sub-seasonal predictions at ECMWF and links with international programmes

Validating Atmospheric Reanalysis Data Using Tropical Cyclones as Thermometers

An update on the NOAA MSU/AMSU CDR development

The Maritime Continent as a Prediction Barrier

Climate Validation of MERRA

2 Observing the Ocean Ships Navigation The Electronics Era 16

Surface Observations Including from the 2012 Mars Curiosity Rover. Martian Atmosphere

EFFECTIVE ATMOSPHERIC ANGULAR MOMENTUM FUNCTIONS AND RELATED PARAMETERS COMPUTED AT THE U.S. NATIONAL METEOROLOGICAL CENTER AAM(AER) 87 * Ol

Progress in embedding global tides into HYCOM simulations. Brian K. Arbic Institute for Geophysics The University of Texas at Austin

5. General Circulation Models

Introduction to Climate ~ Part I ~

Collabora've REAnalysis Technical Environment Intercomparison Project CREATE- IP

Near-surface observations for coupled atmosphere-ocean reanalysis

IMPORTANCE OF SATELLITE DATA (FOR REANALYSIS AND BEYOND) Jörg Schulz EUMETSAT

Climate System. Sophie Zechmeister-Boltenstern

Monsoon Activities in China Tianjun ZHOU

Mesoscale meteorological models. Claire L. Vincent, Caroline Draxl and Joakim R. Nielsen

Modeling the Arctic Climate System

High-Resolution MPAS Simulations for Analysis of Climate Change Effects on Weather Extremes

High initial time sensitivity of medium range forecasting observed for a stratospheric sudden warming

Transcription:

Journées 2014 St. Petersburg 22 24 September Michael SCHINDELEGGER Johannes BÖHM, David SALSTEIN The global S 1 tide and Earth s nutation Session 4: Earth s rotation and geodynamics

Motivation & Background IAU2000A nutation model, Mathews et al. (MHB): MHB noticed a distinct gap of about 100 µas between their theory and VLBI data at the prograde annual frequency Residual from solar S 1 tide, subtracted prior to adjustment Postfit correction term Present-day circulation models Radiational or thermal tides: Caused by the daily cycle of solar heating; stratospheric O 3 and tropospheric H 2 0 absorb solar radiation Excited waves propagate to the ground; diurnal variations in surface parameters dominated by Sunsynchronous or migrating oscillations, e.g in 2

Radiational Tides Surface pressure: Global maps of S 1 (p) Amplitude (Pa) Phase lag (deg) Signature of migrating wave: equatorial belt of ~60 Pa in amplitude / westward increase in phase Non-migrating waves: strong oscillations over continents, repercussions of the local heat transfer from the ground 3

Radiational Tides S 1 and nutation, important notes: Air pressure loads the oceans and induces oceanic angular momentum = indirect atmospheric excitation Only the second-order tesseral spherical harmonic of pressure (~10 Pa mode) can couple to Earth rotation variations Wind tide effect features a better signal-to-noise ratio, e.g. in terms of S 1 retrograde atmospheric angular momentum (AAM): motion : mass contribution = 7:1 Presence of the 1 ψψ 1 normal mode, cf. Brzeziński et al. (2002) 4

Atmospheric Model Data Time line of atmospheric reanalyses (with fixed model configuration): National Centers for Environmental Prediction Reanalyses I and II ECMWF 40-year Reanalysis Japanese Meteorological Agency 25-year Reanalysis NCEP RI 1 1995 210 NCEP RII 1 1995 210 ERA-40 2 2001 125 JRA-25 2 2002 120 MERRA 3 2004 60 Mapped to nutation by Koot Bizouard & de et Viron al. (1998) (2011), fair agreement found NCEP CFSR 3 2004 40 ERA-Interim 3 2006 80 5

Atmospheric Model Data Probing the 3 rd generation reanalyses: (1) MERRA* of NASA s Global Modeling and Assimilation Office: *Modern Era-Retrospective Analysis for Research and Applications (2) NCEP CFSR: Climate Forecast System Reanalysis (3) ERA-Interim of ECMWF Key numbers Temporal resolution: 3 h, analysis & forecast data Time span: 1994.0 2010.12 0.5 grid Horizontal spacing: 1.25 2.5 (pressure level data), 0.5 (surface pressure, except for MERRA) 6

Surface Pressure & AAM Crosscheck of surface pressure with empirical S 1 solution: ~7000 in situ estimates 1 x 1 multiquadric interpolation Tibetan Plateau, W-China Schindelegger & Ray (2014) ERA-Interim amplitude snippet: almost non-existent S 1 tide Barometers suggest variations > 100 Pa 7

Surface Pressure & AAM Crosscheck of surface pressure with empirical S 1 solution: Tibetan Plateau anomaly : global numerical models (0.5 or less) too coarse to resolve the topography & associated physics: RMS differences in S 1 pressure cycle almost linearly dependent on HH = HH bbbbbbbbbbbbbbbbbb HH mmmmmmmmmm Barometer below model Gradient -100 Pa/km Strong diurnal oscillations in valleys entailed by mountain-valley breezes 8

Surface Pressure & AAM Implications of possible inadequacies in S 1 surface pressure for nutation estimates? Quick assessment based on S 1 Fourier coefficients of mass angular momentum Oceanic contributions diverge Enhanced amplitude of in situ AAM due to W-China S 1 tide _ Land Ocean cells contribution 9

Surface Pressure & AAM Implications of possible inadequacies in S 1 surface pressure for nutation estimates? Quick assessment based on S 1 Fourier coefficients of mass angular momentum Oceanic contributions diverge Enhanced amplitude of in situ AAM due to W-China S 1 tide ERA-Interim AAM with inserted in situ grid over W-China increases by ~0.2 10 23 kgm 2 s -1 13 µas in nutation _ Land Ocean cells contribution 10

Nutation: Atmospheric Excitation S 1 nutation estimates obtained from standard procedure: 1) Demodulation to celestial AAM functions 2) Low-pass filtering CFSR deviation: S 1 (p) anomaly of ~35 Pa in Subantarctic Ocean 3) Fit of in- and out-ofphase components w.r.t. fundamental arguments 4) Convolution (Brzezińksi transfer function) Good agreement with 1 st /2 nd generation reanalyses but amplitude reduction for ERA and MERRA 11

Nutation: Atmospheric Excitation S 1 nutation estimates, temporal variability: Partition between mass & motion effects in ERA and MERRA about 55:45 Estimation repeated with 3-year sliding window Interannual variability of up to 40 µas Is this noise or a real physical signal? 12

Nutation: Atmospheric Excitation S 1 nutation estimates, temporal variability arguments for noise: Little coherence among all three reanalyses No residual pattern of the same size (40 µas) at the prograde annual frequency in celestial pole offsets: IERS series, Morlet wavelet analysis MHB fitting period T = +365 d Amplitude (µas) Atmospheric contribution rather harmonic and well-covered by the MHB empirical correction term (?) 13

Nutation: Oceanic Excitation Substantial contribution of radiational S 1 oceanic tide: FES2012 tidal heights (1 cm = 100 Pa) Collection of estimates from heights & currents, or already published papers: phase (µas): in out-of FES2012-11.7 51.9 FES: Finite Element Solution CLIO: Coupled Large-Scale Ice- Ocean Model OMCT: Ocean Model for Circulation and Tides (1.875 ) Ray & Egbert (2004) de Viron et al. (2004): CLIO Brzeziński et al. (2012): OMCT 11.6 62.3 8 57-29.4 30.3 14

Atmospheric + Oceanic Excitation Superposition of atmospheric & oceanic effects: Not fully consistent w.r.t. surface pressure forcing fields In terms of RMS differences at sea surface, MERRA fits well to ECMWF input data of both Ray & Egbert (2004) and FES2012 phase (µas): in out-of ERA -30.2 51.4 MERRA -38.3 40.6 (CFSR -42.7 85.6) phase (µas): in out-of MERRA + FES -50.0 92.5 MERRA + Ray -26.7 102.9 VLBI observ. -10.4 108.2 Similar conclusion in de Viron et al. (2004): CLIO + NCEP, but apparent anomaly (40 µas) in atmospheric out-of-phase estimate 15

S 1 and Earth s nutation Summary and conclusion: Atmospheric pressure term probably the bottleneck in explaining the observed prograde annual nutation, even if examined by aid of 3 rd generation reanalyses Total (mass + motion) excitation varies with time in a rather spurious manner Critical role of averaging period Uncertainty in atmospheric contribution therefore likely to be in the range of 20 µas accuracy of VLBI estimates 16

The End Thank you for your attention! e-mail: michael.schindelegger@tuwien.ac.at ASPIRE (I1479) is funded by the Austrian Science Fund (FWF) and the German Science Foundation (DFG) 17

Back-Up Slides ψ 1 retrograde annual nutation: mean estimates 1994.0 2010.12 Inter-model disparities of about 100 µas (!) Large formal errors indicative of noise-like character of the ψ 1 tide: Amplitude (Pa) in surface pressure 18

Back-Up Slides ψ 1 retrograde annual nutation: temporal variability Estimation repeated with 3-year sliding window Large-magnitude fluctuations, probably non-physical Partition between mass & motion effects about 95:5 19