Space environmental study for ASTROD I

Slides:



Advertisements
Similar presentations
Variations in the Radiation Environment
Advertisements

How Does the Sun Affect Earth? Unit 1 Key Concepts 6th Grade GEMS Space and Science Sequence.
Radiation Environment in a Human Phantom aboard the International Space Station during the Minimum of 23-rd Solar Cycle Semkova J. 1, Koleva R. 1, Maltchev.
THREE-DIMENSIONAL ANISOTROPIC TRANSPORT OF SOLAR ENERGETIC PARTICLES IN THE INNER HELIOSPHERE CRISM- 2011, Montpellier, 27 June – 1 July, Collaborators:
Mike Lockwood STFC/Rutherford Appleton Laboratory & Southampton University Our life-giving star: the flow of energy from the Sun to the Earth BA Festival.
S. Della Torre 1,2, P. Bobik 5, G. Boella 1,3, M.J. Boschini 1,4, C. Consolandi 1, M. Gervasi 1,3, D. Grandi 1, K. Kudela 5, F. Noventa 1,3, S. Pensotti.
ACTIVITY ON THE SUN: Prominences Sunspots Solar Flares CME’s – Coronal Mass Ejections Solar Wind Space Weather.
Flare Luminosity and the Relation to the Solar Wind and the Current Solar Minimum Conditions Roderick Gray Research Advisor: Dr. Kelly Korreck.
Yihua Zheng and Rebekah M. Evans Solar Energetic Particles (SEPs) Goals: identify SEPs in data, connect to drivers, identify characteristics of SEPs June.
A particle monitor for LISA Pathfinder and Gravity Probe-B gyroscope charging in LEO Peter Wass, Henrique Araújo, Tim Sumner Imperial College London, UK.
Results from the GIOVE-A CEDEX Space Radiation Monitor B Taylor 1, C Underwood 1, H Evans 2, E Daly 2, G Mandorlo 2, R Prieto 2, M Falcone 2 1. Surrey.
The Solar Corona and Solar Wind Steven R. Cranmer Harvard-Smithsonian Center for Astrophysics.
The Cosmic R A y Telescope for the Effects of Radiation.
Solar Energetic Particle Production (SEPP) Mission Primary Contacts: Robert P. Lin (UC Berkeley), John L. Kohl (Harvard-Smithsonian CfA) Primary Science.
Danish Space Research Institute Danish Small Satellite Programme FH Space_Environment.ppt Slide # 1 Flemming Hansen MScEE, PhD Technology Manager.
SPACE WEATHER Definition used by the US National Space Weather Plan: Conditions on the Sun and the solar wind, magnetosphere, ionosphere, and thermosphere.
Gravitational waves LIGO (Laser Interferometer Gravitational-Wave Observatory ) in Louisiana. A laser beam is.
What are the Forms of Hazardous Radiation? Stanley B. Curtis Fred Hutchinson Cancer Research Center, ret. & Dept. of Environmental Health University of.
From Geo- to Heliophysical Year: Results of CORONAS-F Space Mission International Conference «50 Years of International Geophysical Year and Electronic.
GEANT-4/Spenvis User Meeting November 2006 Solar Energetic Particle Modelling Activities at ESA A.Glover 1, E. Daly 1,A. Hilgers 1, SEPEM Consortium 2.
National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology A New JPL Interplanetary Solar High- Energy.
Magnetospheric Morphology Prepared by Prajwal Kulkarni and Naoshin Haque Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global.
Solar Activity and VLF Prepared by Sheila Bijoor and Naoshin Haque Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global AWESOME.
EFFECTS of the TERRESTRIAL MAGNETOSPHERE on RADIATION HAZARD on MOON MISSIONS R. Koleva, B. Tomov, T. Dachev, Yu. Matviichuk, Pl. Dimitrov, Space and Solar-Terrestrial.
The Dangers of Solar Storms and Solar Cycles.  For every 1 million atoms of hydrogen in the entire sun  98,000 atoms of helium  850 of oxygen  360.
Spacecraft Instruments. ► Spacecraft instrument selection begins with the mission description and the selected primary and secondary mission objectives.
The Sun and the Heliosphere: some basic concepts…
Centre de Toulouse Radiation interaction with matter 1.
Radiation conditions during the GAMMA-400 observations:
NEEP 541 Radiation Interactions Fall 2003 Jake Blanchard.
Solar Weather and Tropical Cyclone Activity Abstract Worldwide tropical cyclone energy and frequency data was obtained from the Unisys Weather database.
NASA/NSTA Web Seminar: Radiation – Can’t Live With It, Can’t Live Without It LIVE INTERACTIVE YOUR.
System for Radiation Environment characterization (fluxes, doses, dose equivalents at Earth, Moon and Mars) on hourly thru yearly time frame Example: Snapshots.
Evaluation of the flux of CR nuclei inside the magnetosphere P. Bobik, G. Boella, M.J. Boschini, M. Gervasi, D. Grandi, K. Kudela, S. Pensotti, P.G. Rancoita.
Yihua Zheng Solar Energetic Particles (SEPs) Goals: identify SEPs in data, connect to drivers, identify characteristics of SEPs June 2, 2015SW REDI Boot.
The Sun.
STEREO: Beyond 3D. Why the Sun? The sun provides energy for the development of life on our planet. Our orbit looks calm and peaceful, but there is nothing.
Is the Terrestrial Magnetosphere a Natural Radiation Shield on Moon Space Missions ? R. Koleva, B. Tomov, T. Dachev, Yu. Matviichuk, Pl. Dimitrov, Space.
The Dangers of Solar Storms and Solar Cycles.  Radius = 696,000 km  Mass = 2E30 kg  Luminosity = 3.8E26 W  Rotation Rate  25 days at the equator.
Earth-Moon-Mars Radiation Environment Model N. A. Schwadron, K. Kozarev, L. Townsend, M. Desai, M. A. Dayeh, F. Cucinotta, D. Hassler, H. Spence, M. Pourars,
Radiation Storms in the Near Space Environment Mikhail Panasyuk, Skobeltsyn Institute of Nuclear Physics of Lomonosov Moscow State University.
Solar and Cosmic Ray Energetic Particle Models : Space Weather Aspects
Solar weather consists of the Sun’s effects upon its planetary system and the solar activities it causes. Solar activities, such as flares and CMEs, form.
The Suprathermal Tail Properties are not well understood; known contributors Heated solar wind Interstellar and inner source pickup ions Prior solar and.
16-20 Oct 2005SSPVSE Conference1 Galactic Cosmic Ray Composition, Spectra, and Time Variations Mark E. Wiedenbeck Jet Propulsion Laboratory, California.
Approaches to forecasting radiation risk from Solar Energetic Particles Silvia Dalla (1), Mike Marsh (2) & Timo Laitinen (1) (1) University of Central.
Voyager Observations of Galactic Cosmic Ray Transport in the Heliosheath and their Reacceleration at the Termination Shock F.B. McDonald 1, W.R. Webber.
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.
Pulkkinen, A., M. Kuznetsova, Y. Zheng, L. Mays and A. Wold
Elemental Abundance variations of the Suprathermal Heavy Ion Population over solar cycle 23 M. Al Dayeh, J.R. Dwyer, H.K. Rassoul Florida Institute of.
Multispacecraft observation of solar particle events contribution in the space radiation exposure on electronic equipment at different orbits Vasily S.
The Transition Radiation Detector for the PAMELA Experiment
35th International Cosmic Ray Conference
The most challenging consequences of Earth’s space environment occur in the inner radiation belt So far you have been hearing about sensational new results.
Martian Radiation Env. Modelling Tools (QinetiQ)
SPACE RADIATION DOSIMETRY
Solar Activity and Space Weather
Solar and Heliospheric Physics
Ulysses COSPIN High Energy Telescope observations of cosmic ray and solar energetic particles intensities since its distant Jupiter flyby in 2004 R.B.
CRaTER Science Requirements
SMALL SEP EVENTS WITH METRIC TYPE II RADIO BURSTS
Forbush and GCRDs First rigorous experimental observation of Cosmic Ray Flux Decrease was obtained by S. E. Forbush in , after deep statisitcal.
The Centre of the Solar System Earth Science 11
Toshiyuki Kurino, WMO Space Programme
Grades 9-12: Introduction
Chapter 26: Stars and Galaxies
The Layered Atmosphere:
CORONAL MASS EJECTIONS
Presentation transcript:

Space environmental study for ASTROD I Zhang Qingxiang Wangli Shi Wanglin Hou Xinbin Song Zhenji Deep Space Exploration & Space Science Technology Division Research & Development Center,CAST

Outline Introduction Space environment for ASTROD1 Preliminary space environment effect analysis Suggestion for space environment monitor onboard ASTROD1 Conclusion

1. Introduction 2004.10---- CAST setup Deep Space Exploration & Space Science Technology Division at R&D center to promote space science missions. 2006.3 ----- DESSTD began to work together with ASTROD team 2006.6 -----DESSTD took parting in a ASTROD workshop at Purple Mountain Observatory ...

ASTROD 1(Mini -ASTROD) Two-Way Interferometric and Pulse Laser Ranging between Spacecraft and Ground Laser Station Testing relativistic gravity 3-order-of-magnitude improvment in sensitivity; Astrodynamics & solar-system parameter determination improved by 1-3 orders of magnitude; Improving gravitational-wave detection compared to radio Doppler tracking (Auxiliary goal). Wei-Tou Ni(1,2) and Diana N A Shaul(3) Solar, COsmic Ray and Environmental physics for/with ASTROD and ASTROD I

ASTROD 1 Orbit For ASTROD I the distance from the Sun is 0.5 AU to 1.04 AU; The orbit of ASTROD I is out of magnetosphere of Earth ASTROD and ASTROD I: Progress Report

Key technology for ASTROD 1 Tree dimensions sensing capacitive proof masses μN proportional thrusters (Electric Propulsion thrusters ) lasers and optics (5 lasers onboard ASTROD 1 ) …… longevity and reliability of these technologies in the space environment is vital to success for ASTROD I.

2. Space environments for ASTROD1 Galaxy Cosmic Ray Solar event particles Solar wind Solar electromagnetic radiation

Galaxy Cosmic Ray All Elements in Periodic Table Energies in GeV Found Everywhere in Interplanetary Space Omnidirectional Mostly Fully Ionized Cyclic Variation in Fluence Levels Lowest Levels = Solar Maximum Peak Highest Levels = Lowest Point in Solar Minimum Single Event Effects Hazard Model: CREME96 Janet Barth: Radiation Environments

GCR energy and LET spectrum at 1AU calculated with CREAM96

GCR Gradients in the Heliosphere Basd on data from IMP, Voyage and Pioneer, GCR flux increased with distance form Sun. The gradient magnitude is 10% per AU at 1AU 4%per AU at 5AU Difference between GCR flux at 0.5AU and 1AU will be less 10%, Using external radiation fluence at 1AU for ASTROD1 is conservative.

Solar event particles CME Solar Flares Increased Levels of Protons & Heavier Ions Energies Protons - 100s of MeV Heavier Ions - 100s of GeV Abundances Dependent on Radial Distance from Sun Partially Ionized - Greater Ability to Penetrate Magnetosphere Number & Intensity of Events Increases Dramatically During Solar Maximum Models Dose - SOLPRO, JPL, Xapsos/NRL Single Event Effects - CREME96 (Protons & Heavier Ions) CME Solar Flares Janet Barth: Radiation Environments

Proton Event Spectra - Cycle 22 time φ0 k α r 1972.8.4 2.45×1010 0.0236 1.108 0.996 1989.8.12 1.622×1011 1.166 0.4015 0.994 1989.9.29 3.631×1010 0.877 0.3841 0.998 1989.10.19 1.230×1012 2.115 0.2815 1991.3.23 1.660×1011 0.972 0.4410 0.993 Total Integral Proton Fluence Janet Barth: Radiation Environments

SEP energy and LET spectrum at 1AU calculated with CREAM96

SEP Gradients in the Heliosphere The gradient in peak intensity was found to be about R-3, and the total fluence gradient as R-2(NASA) a 1/r+ heliocentric scaling is used for SPE, whilst no scaling is used for heliocentric distances greater than 1AU.(ESA) Recommendations of NASA Sun-Solar System Connections(2005) Radiation Exposure and Mission Strategies for Interplanetary Manned Mission – REMSIM(2004) The SEP peak intensity at 0.5AU is 8 times of that at 1AU, total fluence at 0.5AU is 4 times of that at 1AU.

Solar wind Stream of Charged Particles from Sun’s Corona electrons, protons, heavy Ions Magnetized Plasma Detected Out to 10 billion km from Earth by Pioneer 10 Velocity ~ 300 - 900 km/s Energy ~ .5 - 2.0 keV/nuc

Solar wind plasma parameter Electron Density e temperatureTe Ion Velocity vi Ei/Ti density i Debye Lengh 0.5AU(A) 4.27cm-3 10.6eV 702km/s 2573 eV 6m 0.5AU(B) 13.1 cm-3 68.2 eV 863 km/s 3888 eV 17m A:come from Feldman, high speed solar wind environment scaled to 0.5AU B: data from the SWOOPS(Solar Wind Observations Over the Poles of the Sun) instrument onboard Ulysses

Solar electromagnetic radiation Solar electromagnetic radiation diffuses with distance from the sun at a rate of 1/R2.

3 Preliminary space environment effect analysis Total dose effect Displacement damage Single Event Effect Optical darkening and thermal property changes Optical contamination

Total dose effect

The Solar Orbiter will go into the inner heliosphere to 0.21 AU, For a nominally shielded (4mm Al) silicon component is epected to receive a dose of 48 krad over the entire mission(5 years) The effect of Total dose to microelectronic is not very serious for ASTROD1.

Displacement damage CCD and laser LED may be degraded at very low proton fluence by displacement damage. Allan H. JohnstonDisplacement Damage and SpecialIssues for Optoelectronics

Single Event Effect Microelectronics are likely to occur different SEE.

Detectors will be flooded with “noise”. Single event effect will be a major concerns for ASROD1 , especially during large SEP. SOHO/LASCO Images

Effect to exposed material optical darkening and surface thermal property changes due to synergistic effects between radiation, UV, thermal cycling, vacuum and contamination.

4 Suggestion for space environment monitor onboard ASTROD1 */ The space environment definition is not very certain because we don’t have enough data. It’s proposed that space radiation instrument onboard ASTROD1 satellite: To space environment safety management of satellite and charge management of test materials. Collect environment data in inner heliosphere It’s proposed to add space environment measurement as one of the scientific objects of ASTROD1

5.conclusion Studying the space environment and it’s effect as early as possible are very important for space mission success. It’s proposed to add space environment measurement as one of the scientific aims of ASTROD1.

Thanks http://www.cast.cn zhangqingxiang@cast.cn