New "quite time" concept: application to Champ lithospheric field modelling Nils Olsen, Jesper Gjerløv & Co.

Slides:



Advertisements
Similar presentations
30140 Geophysics Part 2: Solid Earth Physics
Advertisements

4/18 6:08 UT 4/17 6:09 UT Average polar cap flux North cap South cap… South cap South enter (need to modify search so we are here) South exit SAA Kress,
Repeat station crustal biases and accuracy determined from regional field models M. Korte, E. Thébault* and M. Mandea, GeoForschungsZentrum Potsdam (*now.
Coestimating models of the large-scale internal, external, and corresponding induced Hermean magnetic fields Michael Purucker and Terence Sabaka Raytheon.
Separating internal geomagnetic secular variation and long-term magnetospheric field variations Monika Korte Deutsches GeoForschungsZentrum GFZ.
SuperDARN Workshop May 30 – June Magnetopause reconnection rate and cold plasma density: a study using SuperDARN Mark Lester 1, Adrian Grocott 1,2,
Monitoring of auroral oval location and geomagnetic activity based on magnetic measurements from satellites in low Earth orbit. S. Vennerstrom Technical.
Abstract Since the ionosphere is the interface between the Earth and space environments and impacts radio, television and satellite communication, it is.
Ionospheric Electric Field Variations during Geomagnetic Storms Simulated using CMIT W. Wang 1, A. D. Richmond 1, J. Lei 1, A. G. Burns 1, M. Wiltberger.
1 Geomagnetic/Ionospheric Models NASA/GSFC, Code 692 During the early part of April 6, 2000 a large coronal “ejecta” event compressed and interacted with.
Geomagnetic field Inclination
4 th Swarm QWG Meeting 2 – 5 December 2014GFZ Potsdam/D On Calibrating the Magnetometry Package Data Nils Olsen, DTU Space.
J. Ebbing & N. Holzrichter – University of Kiel Johannes Bouman – DGFI Munich Ronny Stolz – IPHT Jena SPP Dynamic EarthPotsdam, 03/04 July 2014 Swarm &
Swarm Data Processing and First Scientific Results
Comparison of Field-Aligned Currents calculated by single spacecraft and dual spacecraft methods. Yulia V. Bogdanova, Malcolm W. Dunlop RAL Space, STFC,
Physics 114: Lecture 15 Probability Tests & Linear Fitting Dale E. Gary NJIT Physics Department.
4 th Swarm QWG Meeting 2 – 5 December 2014GFZ Potsdam/D Data Selection Model Parameterization Results: Statistics, Lithospheric Field, Core Field Perspective.
Kick off meeting, swarm E2E study, nio #1 8-Sep-15 Development Approach Task 1: Industrial Module –to be used by industry for their system simulation –Output:
Secular variation in Germany from repeat station data and a recent global field model Monika Korte and Vincent Lesur Helmholtz Centre Potsdam, German Research.
7.2 Types of variation. Learning objectives Students should understand the following: The need for random sampling, and the importance of chance in contributing.
Ørsted Results The perpetually changing geomagnetic field The geomagnetic field An artist’s concept of the geomagnetic field illustrated by field lines.
Comparison of Polar Cap (PC) index calculations. P. Stauning Danish Meteorological Institute ( + 45
New Unifying Procedure for PC index calculations. P. Stauning Danish Meteorological Institute ( + 45
© NERC All rights reserved UK Repeat Station Report T J G Shanahan and S Macmillan June 2009 MagNetE Workshop Helsinki, Finland.
Final Presentation, Swarm E2E study, June 18, 2004, ESTEC, nio #1 1-Nov-15 Swarm End-To-End Mission Performance Study Final Presentation The Swarm E2E.
Introducing POMME Potsdam Magnetic Model of the Earth Star camera calibration Ring current field Static and annually varying external fields Internal field.
GP33A-06 / Fall AGU Meeting, San Francisco, December 2004 Magnetic signals generated by the ocean circulation and their variability. Manoj,
An assessment of the NRLMSISE-00 density thermosphere description in presence of space weather events C. Lathuillère and M. Menvielle The data and the.
Geology 5660/6660 Applied Geophysics 28 Mar 2014 © A.R. Lowry 2014 For Mon 31 Mar: Burger (§7.4–7.6) Last Time: Earth’s Main Magnetic Field Earth’s.
Swarm ASM-VFM meeting 9-10 Apr 2015ESTEC (NL) Ideas for improving the disturbance model or Welcome to the Null-Space! Nils Olsen, Lars Tøffner-Clausen,
Wavelet Based Estimation of the Hurst Exponent for the Horizontal Geomagnetic Field at MAGDAS Equatorial Stations G. Gopir1,2,*, N. S. A. Hamid1,2, N.
Mapping high-latitude TEC fluctuations using GNSS I.I. SHAGIMURATOV (1), A. KRANKOWSKI (2), R. SIERADZKI (2), I.E. ZAKHARENKOVA (1,2), Yu.V. CHERNIAK (1),
Testing the Equipotential Magnetic Field Line Assumption Using SuperDARN Measurements and the Cluster Electron Drift Instrument (EDI) Joseph B. H. Baker.
Guan Le NASA Goddard Space Flight Center Challenges in Measuring External Current Systems Driven by Solar Wind-Magnetosphere Interaction.
Study on the Impact of Combined Magnetic and Electric Field Analysis and of Ocean Circulation Effects on Swarm Mission Performance by S. Vennerstrom, E.
Study of an Improved Comprehensive Magnetic Field Inversion Analysis for Swarm MTR, E2Eplus Study Work performed by Nils Olsen, Terence J. Sabaka, Luis.
Future China Geomagnetism Satellite Mission (CGS) Aimin Du Institute of Geology and Geophysics, CAS 2012/11/18 Taibei.
Earth’s Dynamic Magnetic Field: The State of the Art Comprehensive Model Terence J. Sabaka Geodynamics Branch NASA/GSFC with special thanks to Nils Olsen.
Sensitivity Analysis and Building Laterally-Variable Ocean Conductivity Grid 1 N. R. Schnepf (UoC/CIRES) C. Manoj (UoC/CIRES) A. V. Kuvshinov (ETHZ)
STSE Tides to Sense Earth, MTR 25 January 2016DTU, Lyngby/DK REPORT ON WP2X00: TIDAL SIGNAL RECOVERY USING THE COMPREHENSIVE INVERSION (CI) RESULTS FROM.
5 th Swarm Data Quality Workshop 7 – 10 September 2015IPG Paris/F PRELIMINARY NEW VERSION OF THE COMPREHENSIVE INVERSION (CI) LEVEL-2 PRODUCTS Terence.
1 NSSC National Space Science Center, Chinese academy of Sciences FACs connecting the Ionosphere and Magnetosphere: Cluster and Double Star Observations.
Geology 5660/6660 Applied Geophysics 30 Mar 2016
© NERC All rights reserved A case for look-up tables for magnetic field error Susan Macmillan ISCWSA error sub-committee meeting 19 March, London.
CWR 6536 Stochastic Subsurface Hydrology Optimal Estimation of Hydrologic Parameters.
Magnetic Measurement Expert Group10-11 March 2016Warsaw / PL MAGNETOMETER – STAR-IMAGER ALIGNMENT: APPARENT EULER ANGLE VARIATION DUE TO MAGNETOSPHERIC.
Summary of Session 2M Swarm 5th Data Quality Workshop
Physics 114: Lecture 13 Probability Tests & Linear Fitting
Magnetic Splinter Meeting
Rapid core field variations just before Swarm
Danish National Space Center, Copenhagen, Denmark
Point and interval estimations of parameters of the normally up-diffused sign. Concept of statistical evaluation.
Hiroko Watanabe (Kyoto Univ.)
High-latitude Neutral Density Maxima
Summary of part of L2 session
swarm End-To-End Mission Performance Study Working meeting on Task 2
Effects of Dipole Tilt Angle on Geomagnetic Activities
Carrington Rotation 2106 – Close-up of AR Mr 2106 Bt 2106
Formosat3 / COSMIC The Ionosphere as Signal and Noise
Ionospheric Effect on the GNSS Radio Occultation Climate Data Record
First Validation of Level 2 Cat-2 products: EEF
Formosat3 / COSMIC The Ionosphere as Signal and Noise
Summary & recommendations multi-mission synergies session 9
~130 Years of Solar Wind Data: The Floor and More
P. Stauning: The Polar Cap (PC) Index for Space Weather Forecasts
Grey Level Enhancement
Effects and magnitudes of some specific errors
Representation of Color Stimuli in Awake Macaque Primary Visual Cortex
Session 5: Higher level products (Internal)
by Andreas Keiling, Scott Thaller, John Wygant, and John Dombeck
Presentation transcript:

New "quite time" concept: application to Champ lithospheric field modelling Nils Olsen, Jesper Gjerløv & Co.

”Quiet Times” and Internal Field Modeling ”Quiet times” means reduced external (ionospheric and magnetospheric) contributions Does not necessarily mean absence of external contributions Important for field modeling: the remaining external “noise” should have “zero mean” … … and thus hopefully averages out and leads to an unbiased internal field model, although it will increase the rms misfit.

Test of SMDL indices with Lithospheric Field Modeling CHAOS-4h: Field model derived from 2 years of low-altitude CHAMP data (Sept 2008 – Sept 2010), 30 sec sampling rate Non-polar regions (|QD lat| < 55°): |dDst/dt| < 2 nT/hr Kp ≤20 Fulfilled for 57 % of time Polar regions (|QD lat| > 55°): |dDst/dt| < 2 nT/hr Em ≤ 0.8 mV/m Fulfilled for 42 % of time Only data from ”dark regions” (sun at least 10° below horizon) Model parameterization Crustal (static) field up to SH degree N = 100 Quadratic Secular Variation up to N = 16 Co-estimation of large-scale magnetospheric field parameterized by RC index and of Euler angles (of VFM – STR rotation) in bins of 10 days Replace these selection criteria with SMDL criteria, with thresholds such that 57% of non-polar and 42% of polar data are chosen

Histogram of SMDL indices (2008-2010)

Cumulative Distribution 0.57 Slo < 6.2 for 57% of time Shi < 48 for 42% of time 0.42 ”SMDL field model”

Cumulative Distribution 0.57 Slo < 6.2 for 57% of time Shi < 48 for 42% of time ”SMDL field model”

Cumulative Distribution Modified Threshold values 0.57 + 10% 0.57 similar threshold modifications for Shi 0.57 - 10% ”SMDL” ”SMDL-10%” ”SMDL+10%” … and compare with CHAOS-4

Model Misfit Lower rms misfit with equal amount of data points Non-polar rms [nT] Polar rms [nT # data Br Bq Bf F CHAOS-4 275311 1.95 2.93 2.26 103463 3.72 SMDL 274376 1.93 2.64 2.03 102887 SMDL-10% 247317 1.90 2.56 1.99 95295 3.63 SMDL+10% 305537 1.96 2.74 2.10 115810 3.91 Lower rms misfit with equal amount of data points

Crustal Field Spectra But only very small change of field model

Maps of DBr at ground MF7 – CHAOS-4

Maps of DBr at ground MF7 - SMDL

Maps of DBr at ground MF7 – SMDL-10%

Maps of DBr at ground MF7 – SMDL+10%

Maps of DBr at ground CHAOS-4 - SMDL

Maps of DBr at ground CHAOS-4 – SMDL-10%

Maps of DBr at ground CHAOS-4 – SMDL+10%

Conclusions SMDL selection criteria work – somehow! Same amount of data selected using SMDL rather than dDst/dt and Kp leads to smaller model misfit, in particular at non-polar latitudes (10% reduction in Bq, Bf) Difference maps of Br (wrt MF7) indicate larger differences at polar latitudes but smaller differences at non-polar latitudes

Bias vs misfit: Contamination of Magnetic Field Model due to Polar-Cap Currents In Summer 1999: Determination of IGRF 2000 from Ørsted satellite data. Only few geomagnetic quiet days with vector data available (May and Sept 1999) Determination of two models: Model a: 6 quiet days in May (10 May - 22 May) Model b: 3 quiet days in Sept (23 Sept - 25 Sept) Zero mean residuals in Northern polar cap for both models Smaller misfit for Model b (Sept data) - better model?

Bias vs misfit: Contamination of Magnetic Field Model due to Polar-Cap Currents

Bias vs misfit: Contamination of Magnetic Field Model due to Polar-Cap Currents

Bias vs misfit: Contamination of Magnetic Field Model due to Polar-Cap Currents

”Quiet Times” and Internal Field Modeling ”Quiet times” means reduced external (ionospheric and magnetospheric) contributions Does not necessarily mean absence of external contributions Important for field modeling: the remaining external “noise” should have “zero mean” … … and thus hopefully averages out and leads to an unbiased internal field model, although it will increase the rms misfit. Perhaps SMDL selection results in ”reduced” external contributions, but of preferred (i.e. biased) magnetic field direction of the remaining part?