The Swarm D NanoMagSat project Latest News

Slides:



Advertisements
Similar presentations
Lightning Imager and its Level 2 products Jochen Grandell Remote Sensing and Products Division.
Advertisements

Towards Low-cost Swedish Planetary Missions S. Barabash 1, O. Norberg 2, J.-E. Wahlund 3, M. Yamauchi 1, S. Grahn 4, S. Persson 4, and L. Blomberg 5 1.
Status update of ASM on Swarm Charlie Swarm 4th DATA QUALITY WORKSHOP 2 December 2014 GFZ Potsdam Jean-Michel Léger.
Geospace Electrodynamic Connections (GEC) Mission The GEC mission has been in the formulation phase as part of NASA’s Solar Terrestrial Probe program for.
Repeat station crustal biases and accuracy determined from regional field models M. Korte, E. Thébault* and M. Mandea, GeoForschungsZentrum Potsdam (*now.
Paul T.M. Loto’aniu 1,2 and H.J. Singer 1 NOAA Space Environment Center 1 CIRES, University of Colorado 2 Paul T.M. Loto’aniu 1,2 and H.J. Singer 1 NOAA.
C. Papadimitriou 1,2,G. Balasis 1, I. A. Daglis 2,1 R. Haagmans 3 1 Institute for Astronomy, Astrophysics, Space Applications and Remote Sensing, National.
GLOBAL POSITIONING SYSTEM FOR ENVIRONMENTAL MANAGEMENT.
The DEMETER satellite: Payload, Operations and Data
VENUS (Vegetation and Environment New µ-Spacecraft) A demonstration space mission dedicated to land surface environment (Vegetation and Environment New.
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:
→ Potential ESA- Roscosmos Cooperation in Education Activities.
Solar Orbiter. Contents The mission The mission The orbit The orbit The instruments The instruments VIM: Visible-light Imager and Magnetograph VIM: Visible-light.
Brief introduction of YINGHUO-1 Micro-satellite for Mars environment exploration J. Wu, G. Zhu, H. Zhao, C. Wang, L. Lei, Y. Sun, W. Guo and S. Huang Center.
T SPP1788 “DynamicEarth“ Workshop, GFZ Potsdam, 3 July 2014 No. 1 Calibration/Validation of Swarm Data Products: German activities Hermann Lühr and Cal/Val.
Cubesats A spacecraft concept to provide advances in international cooperation From: Doug Rowland, NASA GSFC Alexi Glover, ESA.
The Intrinsic Magnetic Field of Saturn: A Special One or an Averaged One? H. Cao, C. T. Russell, U. R. Christensen, M. K. Dougherty Magnetospheres of the.
Molecular Gas and Dust in SMGs in COSMOS Left panel is the COSMOS field with overlays of single-dish mm surveys. Right panel is a 0.3 sq degree map at.
Workshop - November Toulouse Absolute scalar magnetometer controller design Jean BERTRAND, Jérémie POULY – CNES Axel BONESS, François BERTRAND –
Graz, June 2007 The DEMETER mission: Objectives and first results M. Parrot LPCE/CNRS 3A, Avenue de la Recherche Orléans cedex 2, France
3D Current Topology in the Vicinity of an Evening Arc O. Marghitu (1,3), G. Haerendel (2), B.Klecker (3), and J.P. McFadden (4) (1)Institute for Space.
DSL Distributed Systems Laboratory ATC 23 August Model Mission: Magnetospheric Multiscale (MMS) Mission Goal “To study the microphysics of three.
Observing ion cyclotron waves M. R. Lessard, M. Widholm, P. Riley, H. Kim M. J. Engebretson University of New Hampshire Augsburg College NSF Workshop on.
A. Vaivads, M. André, S. Buchert, N. Cornilleau-Wehrlin, A. Eriksson, A. Fazakerley, Y. Khotyaintsev, B. Lavraud, C. Mouikis, T. Phan, B. N. Rogers, J.-E.
Ion Energetics of the Modes of the CubeSat Ambipolar Thruster Timothy A. Collard 1, J. P. Sheehan 1, and Alec D. Gallimore 1 1 Aerospace Engineering, University.
1 MAVEN PFP ICDR May 23-25, 2011 Mars Atmosphere and Volatile EvolutioN (MAVEN) Mission Particles and Fields Science Critical Design Review May ,
Guan Le NASA Goddard Space Flight Center Challenges in Measuring External Current Systems Driven by Solar Wind-Magnetosphere Interaction.
Dec 1, FIELDS Top Level Requirements Review S. Harris (UCB)
William Liu Canadian Space Agency June 12, 2007, Uppsala, Sweden CSA Report to the 5 th ILWS Working Group Meeting.
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.
STSE Tides to Sense Earth, MTR 25 January 2016DTU, Lyngby/DK REPORT ON WP2X00: TIDAL SIGNAL RECOVERY USING THE COMPREHENSIVE INVERSION (CI) RESULTS FROM.
TRIO-CINEMA 1 UCB, 2/08/2010 ACS Dave Auslander, Dave Pankow, Han Chen, Yao-Ting Mao, UC Berkeley Space Sciences Laboratory University of California, Berkeley.
Double Star Active Archive - DWP/STAFF 1 Double Star Active Archive STAFF/DWP Keith Yearby and Hugo Alleyne University of Sheffield Nicole Cornilleau-Wehrlin.
LISA Laser Interferometer Space Antenna: The Mission Mike Cruise For the LISA Team.
Summary of Session 2M Swarm 5th Data Quality Workshop
Astronomical Institute AS CR, Ondřejov Observatory, Czech Republic
Simulation-to-Flight 1 Additional Resources:
The 3rd Swarm Science Meeting, June 2014, Copenhagen, Denmark
INPE Agency Report.
Summary of Swarm L2 and swarm science The Swarm Team
Forecasting the Perfect Storm
Summary of part of L2 session
The Europa Initiative for ESA’s M5 mission JEM SCIENCE PLAN
Introduction to geodesy & accelerometry with Swarm
swarm End-To-End Mission Performance Study Working meeting on Task 2
First validation of Level 2 CAT-2 products: FAC/IBI/TEC
Cianchini, F. J. Pavon-Carrasco, C. Cesaroni, L. Spogli
Upcoming Facilities of IIA
Operational Description
THEMIS INSTRUMENT TRAINING
ACS UC Berkeley Space Sciences Laboratory
Meteoroids 2016, ESTEC, Noordwijk, the Netherlands, June 6-10, 2016
Requirements for microwave inter-calibration
5th Workshop on "SMART Cable Systems: Latest Developments and Designing the Wet Demonstrator Project" (Dubai, UAE, April 2016) Contribution of.
First Validation of Level 2 Cat-2 products: EEF
Oerstedt+Champ+Swarm → Empirical models →New parameters/knowledge
Summary & recommendations multi-mission synergies session 9
Recent Activities of Ocean Surface Topography Virtual Constellation (OST-VC) Remko Scharroo (EUMETSAT)
Objectives and Requirements of SWOT for Observing the Oceanic Mesoscale Variability (based on a workshop held at Scripps Institution of Oceanography, April.
Task Group Report: Ionosphere-Thermosphere
In flight calibration of the experimental ASM vector mode on board the Swarm satellites Thomas Jager, François Bertrand, Viviane Cattin & Jean-Michel.
CubeSat vs. Science Instrument Complexity
Future Opportunities in Geomagnetism and Electromagnetism:
Session 6 Aeronomy/ Novel applications
Charging of the PICASSO CubeSat
Rocketry Trajectory Basics
Satellite mission ideas using EISCAT_3D
5. Conclusions and future work
Prof. Leonardo M. Reyneri
Presentation transcript:

The Swarm D NanoMagSat project Latest News G. Hulot1, J.-M. Léger2 1Institut de Physique du Globe de Paris, Sorbonne Paris Cité, Université Paris Diderot - CNRS, France 2CEA-Léti, MINATEC, Grenoble, France 6th Swarm Data Quality Workshop, 26-29/09/2016, University of Edinburgh, Scotland

Goals of the Swarm D NanoMagSat project Build a nanosatellite (NanoMagSat) for absolute magnetometry by taking advantage of the fact that: The ASM on board Swarm have proven their ability to deliver science class vector mode and burst mode data ASMs (and other instruments) can be made smaller with improved accuracy Use this nanosatellite to improve the Swarm constellation: addition of a D satellite Lead the path to the extension of the INTERMAGNET network to space with cheap nanosatellites (~10 M€ needed to develop NanoMagSat, possibly as little as 2-3 M€ for building recurrent models)

ASM-V core field at core surface Br component at core surface Comparison between ASM-V and VFM core field (n=1-13) models at central epoch (22/04/2014) reveals the impact of the disagreement in the information provided by the ASM-V and early L1b nominal data.

VFM core field at core surface Br component at core surface Comparison between ASM-V and VFM core field (n=1-13) models at central epoch (22/04/2014) reveals the impact of the disagreement in the information provided by the ASM-V and early L1b nominal data.

ASM-V lithospheric field at Earth’s surface Br component at Earth’s surface Comparison between ASM-V and VFM lithospheric field (n=15-45) reveals the impact of the disagreement in the information provided by the ASM-V and early L1b nominal data.

VFM lithospheric field at Earth’s surface Br component at Earth’s surface Comparison between ASM-V and VFM lithospheric field (n=15-45) reveals the impact of the disagreement in the information provided by the ASM-V and early L1b nominal data.

Example of plasma bubble type of signals detected with the ASM burst mode

Example of low frequency “whistler” type of signals detected with the ASM burst mode

Progress on the ASM instrument The instrument is currently being miniaturized (Rutkowski et al., Sensors Actuators, 2014). Issues identified on Swarm (see Léger et al., EPS, 2015; Fratter et al. AA, 2016) are currently being solved. The instrument could be run in a permanent dual mode so as to simultaneously provide 1Hz scalar + vector data AND 250 Hz scalar data, with improved performance.

NanoMagSat 12U Cubesat (20cmx20cmx30cm) with a 2m boom for the magnetometry payload Miniaturised ASM magnetometer in dual vector/burst mode, with two star cameras. Possibility of miniaturized VFM or search coils (possibly based on Tunnel Magneto Resistance, TMR) to also measure high frequency vector field fluctuations (up to 500 Hz or further) Langmuir Probes (Te, Ne) Dual frequency GPS (TEC) Little attitude control: gravitationally stabilized (requirement: spin < 40°/mn swing < 30°/mn to keep bias below 0.2nT) No propulsion

Making the science return of Swarm even better by adding just one satellite Swarm has already been proven to be a great success, thanks, in particular, to its constellation/gradient design There are weaknesses, however, in the Swarm constellation: - Local time separation could still be improved - Orbits only cross each other at the poles

Local time separation of Swarm satellites End of April 2014 3 hrs: April 2016 6 hrs: April 2018 It will take almost another three years to reach 6 hrs local time separation, and only four different local times would then be sampled.

Time needed to cover all local times It currently takes roughly four months for the Swarm constellation to cover all local times. This will decrease to two months when full separation of Alpha/Charlie with respect to Bravo will be reached (April 2018) This is very nice, but could still be improved

A NanoMagSat satellite on an orbit at (say) 60° inclination would provide the missing local times fast One day of local time and geographic coverage

A NanoMagSat satellite on an orbit at (say) 60° inclination would provide the missing local times fast Geographic coverage after 36 days (1 point every 100 s)

A NanoMagSat satellite on an orbit at (say) 60° inclination would provide the missing local times fast Combined Days 1, 9, 18 and 27 of local time and geographic coverage

A NanoMagSat satellite on an orbit at (say) 60° inclination would also provide crossing orbits (tie points) Combined Days 1, 9, 18 and 27 of local time and geographic coverage

Benefits NanoMagSat on such an orbit would bring for investigation of magnetic field sources Higher temporal resolution for ionospheric Sq field models (down to one month) Improved reconstruction of fast changes (sub-annual) of the core field The lithospheric field could also be improved, also thanks to the 60° crossing of the orbits (providing tie points) But also: Improved understanding of local ionospheric currents Improved spatial description of the magnetospheric field Improved input for investigations of the electrical conductivity of the Deep Earth

Aiming at a launch before 2021 Swarm’s constellation is complete up to 2022, at least Higher Bravo satellite could stay even longer in orbit, likely well beyond 2024

Next steps Extension of the NanoMagSat Phase 0 study within CNES has just been approved Run a set of complete end-to-end simulations with the help of the Swarm science community (and assistance from CNES and ESA) Present the mission to the next level within CNES (Fall 2017 ?) Start considering moving towards an “InterMagSat” network of orbiting magnetic observatories (space extension of the “Intermagnet” network of ground magnetic observatories)

Space magnetometry and nanosatellites, important technical facts 1 Hz (or higher frequency) magnetometry does not need severe orbit or attitude control, this translates into: -> no intrinsic need for thrusters -> only a recovery mode is needed for attitude control, which would rarely be used Only needs accurate: -> orbit knowledge -> time control -> attitude reconstruction