Need for a mission to understand the Earth- Venus-Mars difference in Nitrogen M. Yamauchi 1, I. Dandouras 2, and NITRO proposal team (1) Swedish Institute.

Slides:



Advertisements
Similar presentations
Locations of Boundaries of the Outer and Inner Radiation Belts during the Recent Solar Minimum, as Observed by Cluster and Double Star Natalia Ganushkina.
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.
Climates of Terrestrial Planets Dave Brain LASP / CU Boulder Do magnetic fields affect planet surfaces? Do magnetic fields affect atmospheres? Do magnetic.
Searching for N 2 And Ammonia In Saturn's Inner Magnetosphere Polar Gateways Arctic Circle Sunrise 2008 Polar Gateways Arctic Circle Sunrise January.
M. Yamauchi, I. Dandouras, H. Rème, and the NITRO Proposal Team ESWW-11, Liège, November 2014 Planetary Space Weather Session Nitrogen Ion TRacing Observatory.
PRECIPITATION OF HIGH-ENERGY PROTONS AND HYDROGEN ATOMS INTO THE UPPER ATMOSPHERES OF MARS AND VENUS Valery I. Shematovich Institute of Astronomy, Russian.
Fine-scale 3-D Dynamics of Critical Plasma Regions: Necessity of Multipoint Measurements R. Lundin 1, I. Sandahl 1, M. Yamauchi 1, U. Brändström 1, and.
Martian Pick-up Ions (and foreshock): Solar-Cycle and Seasonal Variation M. Yamauchi(1); T. Hara(2); R. Lundin(3); E. Dubinin(4); A. Fedorov(5); R.A. Frahm(6);
Sudden appearance of sub- keV structured ions in the inner magnetosphere within one hour: drift simulation M. Yamauchi 1, Y. Ebihara 2, I. Dandouras 3,
Budget and Roles of Heavy Ions in the Solar System M. Yamauchi, I. Sandahl, H. Nilsson, R. Lundin, and L. Eliasson Swedish Institute of Space Physics (IRF)
Solar wind interaction with the comet Halley and Venus
Earth’s Radiation Belt Xi Shao Department of Astronomy, University Of Maryland, College Park, MD
1 Update and functional test results for SWIM David McCann Solar system physics and space technology IRF, Kiruna Supervisor: Professor Stas Barabash David.
From Geo- to Heliophysical Year: Results of CORONAS-F Space Mission International Conference «50 Years of International Geophysical Year and Electronic.
Crustal Fields in the Solar Wind: Implications for Atmospheric Escape Dave Brain LASP University of Colorado July 24, 2003.
International Colloquium and Workshop "Ganymede Lander: scientific goals and experiments"
How do gravity waves determine the global distributions of winds, temperature, density and turbulence within a planetary atmosphere? What is the fundamental.
Earth’s Atmosphere Ch. 22.
Cusp O+ H+ e- "SPI" event #1 event #2 MLT energy ratio = 15~20 O+ H+ 68°CGLat66°CGLat 63°CGLat #1) Mono-energetic ion injection with O+ faster.
Electrons at Saturn’s moons: selected CAPS-ELS results A.J. Coates 1,2. G.H. Jones 1,2, C.S.Arridge 1,2, A. Wellbrock 1,2, G.R. Lewis 1,2, D.T. Young 3,
Computer Simulations in Solar System Physics Mats Holmström Swedish Institute of Space Physics (IRF) Forskarskolan i rymdteknik Göteborg 12 September 2005.
Terrestrial Atmospheres Solar System Astronomy Chapter 8.
The EUV impact on ionosphere: J.-E. Wahlund and M. Yamauchi Swedish Institute of Space Physics (IRF) ON3 Response of atmospheres and magnetospheres of.
Finite Gyroradius Effect in Space and Laboratory 1. Radiation belt (Ring current) 2. Auroral phenomena (Substorm current) 3. Shock acceleration and upstream.
Space Science MO&DA Programs - August Page 1 SS Polar Quantifies Magnetospheric Drivers of Upper Atmospheric Chemistry Changes High resolution global.
Fate of cold ions in the inner magnetosphere: energization and drift inferred from morphology and mass dependence M. Yamauchi 1, I. Dandouras 2, H. Reme.
Hot He + events in the inner magnetosphere observed by Cluster M. Yamauchi 1, I. Dandouras 2, H. Reme 2, H. Nilsson 1 (1) Swedish Institute of Space Physics.
The PLANETOCOSMICS Geant4 application L. Desorgher Physikalisches Institut, University of Bern.
29 August, 2011 Beijing, China Space science missions related to ILWS in China
1 Mars Micro-satellite Mission Japanese micro-satellite mission to Mars to study the plasma environment and the solar wind interaction with a weakly-magnetized.
JAXA’s Exploration of the Solar System Beyond the Moon and Mars.
Europe: IRF-Kiruna (Sweden), IRAP (Toulouse, France), UCL/MSSL (London, UK), LPP (Paris, France), FMI (Helsinki, Finland), Inst Space Sci. (Bucharest,
PAPER I. ENA DATA ANALYSIS RESULTS. The Imager for Magnetopause-to- Aurora Global Exploration (IMAGE) missionis the first NASA Mid-size Explorer (MIDEX)
Initial Measurements of O-ion and He-ion Decay Rates Observed from the Van Allen Probes RBSPICE Instrument Andrew Gerrard, Louis Lanzerotti et al. Center.
Scott M. Bailey, LWS Workshop March 24, 2004 The Observed Response of the Lower Thermosphere to Solar Energetic Inputs Scott M. Bailey, Erica M. Rodgers,
Cold plasma: a previously hidden solar system particle population Mats André and Chris Cully Swedish Institute of Space Physics, Uppsala.
Oxygen Injection Events observed by Freja Satellite M. Yamauchi 1, L. Eliasson 1, H. Nilsson 1, R. Lundin 1, and O. Norberg 2 1.Swedish Institute of Space.
M. Yamauchi 1, H. Nilsson 1, I. Dandouras 2, H. Reme 2, R. Lundin 3, Y. Ebihara 4 (1) Swedish Institute of Space Physics (IRF), Kiruna, Sweden (2) CNRS.
Escaping ions over polar cap. Inner magnetosphere, Bow shock/Foreshock, and Ancient magnetosphere.
1 MAVEN PFP ICDR May 23-25, 2011 Mars Atmosphere and Volatile EvolutioN (MAVEN) Mission Particles and Fields Science Critical Design Review May ,
Understanding the Earth- Venus-Mars difference in Nitrogen M. Yamauchi 1, I. Dandouras 2, and NITRO proposal team EANA-2012 (P4.30, ) (1) Swedish.
NASA NAG Structure and Dynamics of the Near Earth Large-Scale Electric Field During Major Geomagnetic Storms P-I John R. Wygant Assoc. Professor.
CRRES observations indicate an abrupt increase in radiation belt fluxes corresponding to the arrival of a solar wind shock. The processes(s) which accelerate.
Hot He + events in the inner magnetosphere observed by Cluster 1 Yamauchi, et al. (2014), JGR, doi: /2013JA Inner magnetosphere: Majority.
IRF (Kiruna, Sweden), IRAP (Toulouse, France), UCL/MSSL (London, UK), NASA/GSFC (USA), FMI (Helsinki, Finland), Inst Space Sci. (Bucharest, Romania), UNH.
© 2009 W.W. Norton Earth Liquid water on its surface Oxygen atmosphere Only planet known to support life 4.6 billion years old 71% covered by H 2 O Oblate.
What are the Inner planets?
M. Yamauchi 1, H. Lammer 2, J.-E. Wahlund 3 1. Swedish Institute of Space Physics (IRF), Kiruna, Sweden 2. Space Research Institute (IWF), Graz, Austria.
Morphology of Inner Magnetospheric low- energy ions M. Yamauchi 1, I. Dandouras 2, H. Reme 2, R. Lundin 3, L.M. Kister 4, F. Mazouz 5, Y. Ebihara 6 (1)
24 January, 20011st NOZOMI_MEX Science Workshop, Jan, 2001 R. Lundin, M. Yamauchi, and H. Borg, Swedish Institute of Space Physics H. Hayakawa, M.
Lunar Surface Atmosphere Spectrometer (LSAS) Objectives: The instrument LSAS is designed to study the composition and structure of the Lunar atmosphere.
NITRO for M4: IRF (Kiruna, Sweden), IRAP (Toulouse, France), OHB-Sweden (Kista, Sweden), NASA/GSFC (USA), UNH (Durham, USA), LATMOS/IPSL (Guyancourt, France),
Techniques for mass resolution improvement achieved by typical plasma analyzers: Modeling and simulations 1 G. Nicolaou, 1 M. Yamauchi, 1 M. Wieser, 1.
A Global Hybrid Simulation Study of the Solar Wind Interaction with the Moon David Schriver ESS 265 – June 2, 2005.
Gyeongbok Jo 1, Jongdae Sohn 2, KyeongWook Min 2, Yu Yi 1, Suk-bin Kang 2 1 Chungnam National University 2 Korea Advanced Institute of Science.
Post-Cluster: Need for a mission to understand Nitrogen in space
Plasma Wave Excitation Regions in the Earth’s Global Magnetosphere
Mass-loading effect in the exterior cusp and plasma mantle
M. Yamauchi1, I. Dandouras2, H. Reme2,
Sub-keV Phenomena of Dayside Ring Current
Oxygen Injection Events observed by Freja Satellite
Energetic Neutral Atom Imaging of
The Wakes and Magnetotails of Venus and Mars
1G. Nicolaou, 1M. Yamauchi, 1,2H. Nilsson, 1M. Wieser, 3A. Fedorov, 1D
R. Bucˇık , K. Kudela and S. N. Kuznetsov
Nitrogen and Oxygen Budget ExpLoration (NOBEL)
Primordial Atmosphere
Satellite mission ideas using EISCAT_3D
NITRO A Mission to "Planet Earth"
M. Yamauchi1, A. Schillings1,2, R. Slapak3, H. Nilsson1, I. Dandouras3
Presentation transcript:

Need for a mission to understand the Earth- Venus-Mars difference in Nitrogen M. Yamauchi 1, I. Dandouras 2, and NITRO proposal team (1) Swedish Institute of Space Physics (IRF), Kiruna, Sweden, (2) Institut de Recherche en Astrophysique et Planétologie (IRAP), CNRS and U. Toulouse, Toulouse, France R125 (EGU )

(A) Nitrogen is an essential element of life: Formation of many pre-biotic molecules is most likely related to the amount and the oxidation state of N (reduced form like NH 3, neutral form like N 2, and oxidized form like NO x ) near the surface in the ancient Earth (Miller and Urey, 1959). One cannot use the present abundance of N, O, H as the ancient value because of the significant escape of ions from the ionosphere that are observed (Chappell et al., 1982, Nilsson, 2011). (B) N/O ratio is quite different between the brother plants Earth: 75% of atmospheric mass (the amount in the soil, crust, and ocean are small) Venus ~ 2.5 times as much as Earth (3% of P atom.Venus = 90 x P atom.Earth ) Titan ~ 1.5 times as much as Earth (98% of P atom.Titan ) Mars ~ only 0.01% of the Earth (note: M Mars ~ 10% of M Earth ): This is a mystery because (1) O is abundant in all three planets (Martian case, exist in the crust as oxidized rocks); (2) N is much more difficult to be ionized than O due to triple chemical binding (i.e., more difficult to escape). Why study Nitrogen (& N/O ratio) in space?  Need to understand the dynamic of N (& its difference from O) at different solar conditions for whatever the planet. 2 (C) But past instruments failed to separate N/O for keV

Increase inFUV (or T)P sw B sun MeV e - Pick-up (small)unchange(+?)unchange Large-scale(unchange?)+++(+++?)(unchange?) Non-thermal heating+++ ++(+?) Jeans & photo-chemical+++ for H+unchange (+?) O + /H + ratio of escape??+++++(++?) N + /O + ratio of escape(+?) (?)(++?) Unmagnetized (Mars/Venus/ Ancient Earth) Magnetized (Earth) Increase inFUV (or T)P sw B sun MeV e - Pick-up (important)++ +(unchange?) Large-scale(+?)(++?) (unchange?) Non-thermal heating(++?) Jeans & photo-chemical+++ for H+unchange (+?) O + /H + ratio of escape??(+++?)(+?)(++?) N + /O + ratio of escape(?) (++?) Table 1&2: Escape estimate: Expected change in the escape of H, O, N (increase level +, ++, or +++) in response to enhanced input from the sun. Inside parenthesis () means no relevant observation, and the increase is guessed from physical consideration. The effect of FUV increase is mainly through heating at upper atmosphere (increase in T). Increase in solar B causes increase in |B| and variation dB (latter is largely influenced by the sunspot activities). 3

VenusEarthMars rich in N N <0.01% of Earth/Venus 4 N/O ratio is very low at Mars compared to the Earth, Venus, Titan Fig. 1

(a) Dependence on geomagnetic activities is larger for N + than O + for both 30 keV (Hamilton et a., 1988). (b) + at <10 keV range is abundant in the magnetosphere. (c) N/O ratio at Mars and C/O ratio at Moon are extremely low compared to the other planets. But, all magnetospheric mission failed to separate hot N + from O + at 0.05~10 keV range. This is because the time-of-flight instrument did not perform the promised M/∆M > 8 due to high cross-talk and scattering by start surface. Present knowledge on N + MEX/IMA detected C + /N + /O + group in 4 mass channels (ch.10, 11, 12, 13) out of total 32 channels. * IMA uses only 5 cm magnet to separate mass-per-charge, and by doubling the magnet to 10 cm, we may separate CNO. However, the technology is within reach! 5

Science QuestionWhat and where should we measure?requirement N + escape history compared to O + or H + N +, O + and H + at different solar and magnetospheric conditions. #1, ∆t<1min Ion filling route to the inner magnetosphere N +, O + and H + at different solar and magnetospheric conditions. #1, ∆t<1min N-O difference in energy re- distribution in the ionosphere N +, O +, H +, J //, and e - at different solar conditions. #1, precipitating e -, J //, outflowing ions Ion energization mechanisms energy difference (including cutoff energy) among N +, O + and H + at different altitude #1, ∆t<1min #1: N + -O + separation (M/∆M ≥ 8 for narrow mass) and H + -He + -O + separation (M/∆M ≥ 2 for wide mass) at  and // directions at eV (11 km/s~9 eV for N) with ∆E/E ≤ 7% ((E O+ - E N+ )/E N+ =15%)  Nitro Mission Table 3: scientific questions related to the N and N/O ratio measurement (a) the history of oxydation state of the atmospheric N, (b) Mars mystery on N/O ratio, (c) acceleration mechanism, (d) re-distribution of energy in the upper ionosphere, (e) ion injection and dynamics in response to substorm injections (can be monitored by ENA) 6 First-time measurement of N + and N + /O + ratio of the escape (>50 eV) to understand

SI mass (*a) functionresolutionG-factor & ∆t for full E ICA-N <5.5 kg Magnetic ion mass seperation ∆E/E=7%, eV/q m/∆m=8 (only m/q > 8) 3.5·10 -4 cm 2 sr 1 <6s, (2kbps) IMS <6.0kg Ion: Time-of-flight with start-surface ∆E/E=7%, eV/q, m/∆m~4 (m/q ≥ 1) cm 2 sr 1 <1s, 7kbps PRIMA <2.4kg Ion: Time-of-flight with start-shutter ∆E/E = 15%, eV/q m/∆m=8 (m/q ≥ 1) 0.5·10 -4 cm 2 sr 1 <1s, (0.5kbps) MAG <2.3kg Ion cyclotron wave (can be simplified) < 35 pT (SC cleanness limits to < 0.5 nT) <0.1s, 1.5kbps PEACE <4.0kg Electron∆E/E= 13%, eV/q 6·10 -4 cm 2 sr 1 <0.2s, 5kbps STEIN <2.4kg Energetic Neutral Atoms (no mass) ∑ eV/q2·10 -2 cm 2 sr 1 <60s, 7kbps Nitro scientific instruments (*a) mass includes shielding against radiation belt particles Orbit: 3~6 R E x 800~2000 km polar (inc=90°) orbit, with total payload of about 21 kg including shielding against radiation belt particles 7

PrimaIMSICA key SI

(1) Understanding the non-thermal nitrogen escape is essential in modeling both the ancient atmosphere of the Earth and the Martian nitrogen mystery. (2) Unfortunately, past magnetospheric missions could not N + /O+ for < 50 eV because of high cross-talk in TOF instruments. (3) Now, the technology to separate N+ and O+ with light-weight instrument just became available. (4) Therefore, we need a dedicated mission to understand N+. This is the Nitro mission, that was proposed to ESA. Summary 9

Ion circulation in the magnetosphere Appendix 10 ion composition (Hamilton et al., 1988) H + < 50 eV O + < 50 eV ion escape (Cully et al., 2003)