Your SlideShare is downloading. ×
  • Like
Space Radiation & It's Effects On Space Systems & Astronauts Technical Training Course Sampler
Upcoming SlideShare
Loading in...5
×

Thanks for flagging this SlideShare!

Oops! An error has occurred.

×

Now you can save presentations on your phone or tablet

Available for both IPhone and Android

Text the download link to your phone

Standard text messaging rates apply

Space Radiation & It's Effects On Space Systems & Astronauts Technical Training Course Sampler

  • 591 views
Published

This course is designed for technical and management personnel who wish to gain an understanding of the fundamentals and the effects of space radiation on space systems and astronauts. The radiation …

This course is designed for technical and management personnel who wish to gain an understanding of the fundamentals and the effects of space radiation on space systems and astronauts. The radiation environment imposes strict design requirements on many space systems and is the primary limitation to human exploration outside of the Earth's magnetosphere. The course specifically addresses issues of relevance and concern for participants who expect to plan, design, build, integrate, test, launch, operate or manage spacecraft and spacecraft subsystems for robotic or crewed missions. The primary goal is to assist attendees in attainment of their professional potential by providing them with a basic understanding of the interaction of radiation with non-biological and biological materials, the radiation environment, and the tools available to simulate and evaluate the effects of radiation on materials, circuits, and humans

Published in Technology
  • Full Name Full Name Comment goes here.
    Are you sure you want to
    Your message goes here
    Be the first to comment
    Be the first to like this
No Downloads

Views

Total Views
591
On SlideShare
0
From Embeds
0
Number of Embeds
1

Actions

Shares
Downloads
5
Comments
0
Likes
0

Embeds 0

No embeds

Report content

Flagged as inappropriate Flag as inappropriate
Flag as inappropriate

Select your reason for flagging this presentation as inappropriate.

Cancel
    No notes for slide

Transcript

  • 1. SPACE RADIATION AND ITS EFFECTS ON SPACE SYSTEMS AND ASTRONAUTS Instructor: Dr. Vincent L. Pisacane Course Schedule: http://www.ATIcourses.com/schedule.htm Course Oultine: http://www.aticourses.com/Space_Radiation_Effects_On_Systems_Astronaughts.htm
  • 2. www.ATIcourses.com Boost Your Skills with On-Site Courses Tailored to Your Needs 349 Berkshire Drive Riva, Maryland 21140 Telephone 1-888-501-2100 / (410) 965-8805 Fax (410) 956-5785 Email: ATI@ATIcourses.com The Applied Technology Institute specializes in training programs for technical professionals. Our courses keep you current in the state-of-the-art technology that is essential to keep your company on the cutting edge in today’s highly competitive marketplace. Since 1984, ATI has earned the trust of training departments nationwide, and has presented on-site training at the major Navy, Air Force and NASA centers, and for a large number of contractors. Our training increases effectiveness and productivity. Learn from the proven best. For a Free On-Site Quote Visit Us At: http://www.ATIcourses.com/free_onsite_quote.asp For Our Current Public Course Schedule Go To: http://www.ATIcourses.com/schedule.htm
  • 3. SOLAR WIND Introduction  Solar wind is the flow of plasma from the Sun's corona, the outermost atmosphere of the Sun  In vicinity of the Earth the solar wind has – – – – – Temperature of ~150,000 K Sonic velocity of ~45 km s-1 Average velocity ~400 km s-1, supersonic Average density ~1-10 particles cm-3 Composition of ~95 % electrons and protons in near equal numbers, ~4 % helium nuclei (alpha particles), remainder heavy nuclei and is electrically neutral  Termination Shock at ~95 AU is where the velocity transitions from supersonic to subsonic (Illustrated next slide)  Heliopause at ~ 120 AU is the interface between the solar wind and the constituents of the galaxy (Illustrated next slide) From: http://www.mps.mpg.de/projects/sun-climate/se_body.html ©vpisacane, 2014
  • 4. MAGNETIC FIELD and MAGNETOSPHERE Introduction to Interplanetary Fields  The interplanetary magnetic field is driven by the Sun  Upper Figure Ecliptic Plane Inclined 7.25o – It is essentially a dipole field tilted with respect to the ecliptic plane as illustrated in the upper figur  Lower Figure http://www.astro.cornell.edu/~berthoud/alpsat/chapter3a.html – In the ecliptic plane, the plane of the Earth’s orbit, the interplanetary magnetic field is spiral in shape as illustrated in the figure due to the rotation of the Sun about an axis inclined to within 7.25 degrees of normal to the ecliptic plan http://ase.tufts.edu/cosmos/print_images.asp?id=34 ©vpisacane, 2014
  • 5. CUTOFF RIGIDITY Earth Cutoff Contours at 450 km Altitude  Contour maps of computed vertical cutoff rigidities at 450-km altitude for quiet magnetic conditions (Kp = 0 on left), and disturbed (Kp = 8 on right)  Cutoff rigidity contours are in GV increments  Maximum cutoff rigidities are along the magnetic equator and the minimum cutoff rigidity is at the magnetic poles. From DF Smart *, MA Shea, A review of geomagnetic cutoff rigidities for earth-orbiting spacecraft, Advances in Space Research 36 (2005) 2012–2020 ©vpisacane, 2014
  • 6. INTRODUCTION Summary Motion  Motion of the trapped radiation as illustrated in Figure 6.4 consists of three primary components: – Gyration ~ milliseconds • Particles rotating around field lines – Mirroring ~0.1 ─ 1.0 s • Particles traveling from one hemisphere to the other and back – Longitudinal drift ~ 1 ─ 10 min • Particles driting east or west Figure 6.4 Motion of charged particles trapped in the Earth’s magnetic field, ©vpisacane, 2014
  • 7. GUIDING CENTER MOTION Motion in Uniform Magnetic Field  General motion of proton and electron in a constant magnetic field with an initial velocity along the field line results in the direction of the magnetic field results in helical motion g g ©vpisacane, 2014
  • 8. MIRRORS POINTS Equatorial Loss Cone  Equatorial Loss Cone is a cone of velocities of charged particle whose apex is on the equator and axis along a magnetic field line that represents the charged particles that will be lost due to interaction with the atmosphere or the surface in a dipole field  Loss-cone angle for intersection with the Earth depends solely on L-shell value and not on particle mass, charge or energy where sin lc  4L6  3L5  1 / 4 http://www-spof.gsfc.nasa.gov/Education/wtrap2.html  lc Loss -one geometry ©vpisacane, 2014
  • 9. AE8 AND AP8 MODELS Example Electron Flux at Max Sunspot Number AE-8 MAX integral electron flux >1 MeV AE-8 MAX integral electron flux >1 MeV at 500 km altitude From: http://www.spenvis.oma.be/help/background/traprad/traprad.html ©vpisacane, 2014
  • 10. AE8 AND AP8 MODELS Low Altitude Simulation 2/2  World map of electron and proton fluxes > 1 MeV Electron flux AE8-Min Proton flux AP8-Min Spenvis simulation ©vpisacane, 2014
  • 11. CHARACTERISTICS Gamma Ray Energy Spectrum  Image is the EGRET gamma ray all-sky survey  EGRET is instrument on NASA's Compton Gamma Ray Observatory satellite  Energies > 1 x 108 eV  Some cosmic rays interact with the interstellar medium and produce gamma rays Picture Credit: NASA, Compton Gamma Ray Observatory ©vpisacane, 2014
  • 12. MODEL EVALUATIONS Differential Flux Geostationary Spacecraft  Integral flux comparisons  Models – ISO-15390-Standard Model – CREME96 Solar Minimum – CREME86 M=2 • Galactic and anomalous – Nymmik et al Solar Minimum  Mission – Altitude 35,786 km Geostationary – Inclination 0o – Eccentricity 0 – 21 March 2012, 12h UT Spenvis simulation ©vpisacane, 2014
  • 13. CHARACTERISTICS Anisotropy of SPE  Upper Figure – Particles propagating along the “favorable path” will be anisotropic at Earth  Lower Figure (From Shea, 1988) – Measured longitude distribution of propagation times of solar particles from coronal mass ejections to Earth – The various symbols indicate data from different studies From Smart and Shea, 1985, and Barouch et al., 1971 ©vpisacane, 2014
  • 14. CHARACTERISTICS Observed Solar Proton Spectra  Solar proton fluence for extremely large solar cycle 22 event on August 1972 and other events  Dashed line is common interpolation between 8/72 event and the USSR balloon measurement MA Xapsos, JL Barth and EG Stassinopoulos, EA Burke, GB Gee, Space Environment Effects: Model for Emission of Solar Protons (ESP)— Cumulative and Worst-Case Event Fluences, NASA/TP--1999-209763, December 1999 ©vpisacane, 2014
  • 15. MARS SURFACE MODEL Martian Surface Radiation Models  Martian Energetic Radiation Environment Models (MEREM) developed to simulate the Martian radiation environment  Two models – eMEREM ─ engineering model – dMEREM ─ more detailed model  Takes into account – Solar minimum and maximum conditions – Solar particle events – Cosmic rays – Secondaries from surface and atmosphere From: P Goncalves, et al, MarsREM:The Mars Energetic Radiation Environment Models, Proceedings of the 31st ICRC, Ł´OD´Z 2009 Spectrum due to GCR protons on Mars surface, for given location and epoch. ©vpisacane, 2014
  • 16. INTRODUCTION Hazards of Radiation http://holbert.faculty.asu.edu/eee560/spacerad.html ©vpisacane, 2014
  • 17. PHOTON RADIATION Aluminum Mass Attenuation Coefficient 1.E+04 Mass Attenuation Coefficient, cm2 g-1 Aluminum 1.E+03 1.E+02 Coherent Incoherent Photoelectric Pair Production Total 1.E+01 1.E+00 1.E-01 1.E-02 1.E-03 1.E-03 1.E-02 1.E-01 1.E+00 1.E+01 1.E+02 Energy, MeV 1.E+03 1.E+04 1.E+05 aluminum, r = 2.7 g cm-3 From XCOM available from NIST ©vpisacane, 2014
  • 18. CHARGED PARTICLE RADIATION Proton and Electron Penetration Depth ©vpisacane, 2014
  • 19. CHARGED PARTICLE RADIATION SRIM 1/3 2 1 Alpha particl e 4 ©vpisacane, 2014
  • 20. EFFECTS ON ELECTRONICS Total Ionization Dose (TID) NPN MOSFET  Example, when gate to source voltage is positive, current flows between drain and source  Gate oxide insulates gate from source and drain and is made of silicon dioxide  When exposed to radiation, holes not as mobile as electrons, become trapped in the gate oxide  With sufficient radiation accumulated trapped holes build to a positive charge that acts the same as if a positive voltage were applied inducing an n+ conducting channel  Positive voltage from the trapped holes – Changes the operating characteristics – Reduces voltage to turn on device – Eventually turns device on permanently leading to failure Cross section of an NMOS transistor showing the gate oxide and conducting n+ channel formed between the source and drain The trapped charges shown in the inset are responsible for the threshold voltage shift, ultimately leading to failure From TR Oldham, Total Ionizing Dose Effects in MOS Oxides and Devices, IEEE Transactions On Nuclear Science, VOL. 50, NO. 3, JUNE 2003 483 ©vpisacane, 2014
  • 21. EFFECTS ON ELECTRONICS UoSAT-2 Spacecraft Single Event Upsets Figure 9.20 ©vpisacane, 2014
  • 22. EFFECTS ON ELECTRONICS Single Event Latchup (SEL) GATE  High-energy charged particle can cause an ionized low impedance path between the power lines and ground or between power lines SOURCE OUTPUT DRAIN P-MOSFET GATE DRAIN SOURCE N-MOSFET  Typically occurs in CMOS circuits wit intrinsic Bipolar Junction Transistors as illustrated  If power is limited, condition will persist and state will not change, called a Single Event Latchup Figures from: Aerospace Corp, http://www.aero.org/capabilities/seet/otherSEE.html  If power is high or not removed quickly, catastrophic failure may occur due to excessive heating of metallization or bond wire failure  Power reset will often correct the problem Top= PNP Bottom= NPN Zero gate voltage would cause no current to flow From NASA ©vpisacane, 2014
  • 23. RADIATION GUIDELINES Steps in Radiation Hardness Assurance Program DESCRIPTION STEPS 1 Identify the radiation exposure 2 Identify acceptable risk 3 Determine margins of safety 4 Identify potentially susceptible parts, maintain parts list 5 Procure rad-hard parts if possible (availability, cost) 6 Identify parts still at risk 7 Establish risk mitigation strategies for parts at risk 8 Confirm hardness of rad-hard parts by analysis and test 9 Confirm risk mitigation strategies for parts at risk by analysis and test 10 Monitor effectiveness of risk mitigation strategies during operations Table 9.6 ©vpisacane, 2014
  • 24. RADIATION DAMAGE COEFFICIENTS EQFLUX Simulation Low Earth Orbit 2/2 Trapped proton equivalent fluences for Pmax as function of cover slide thicknesses Solar proton equivalent fluences for Pmax as function of cover slide thicknesses Trapped proton Equivalent fluences for Voc as function of cover slide thicknesses Solar proton equivalent fluences for Voc as function of cover slide thicknesses Trapped proton equivalent fluences for Isc as function of cover slide thicknesses Solar proton equivalent fluences for Isc as function of cover slide thicknesses ©vpisacane, 2014
  • 25. INTRODUCTION DNA Repair  DNA damage, due to environmental factors and normal metabolic processes inside the cell, occurs at a rate of up to 500,000 DNA modifications per cell per day  If the rate of DNA damage exceeds the capacity of the cell to repair it, the accumulation of errors can overwhelm the cell and result in early apoptosis, senescence, or cancer  Normal apoptosis results in about one million cells dying every second in an adult  Definitions – Senescence • An irreversible state in which the cell no longer divides – Apoptosis • Programmed cell death  DNA Repair  Successful repair  Unsuccessful repair • Mutations • Replication errors • Persistent DNA damage • Genomic instability ©vpisacane, 2014
  • 26. COUNTERMEASURE READINESS LEVELS Introduction 9. Countermeasure fully flight-tested and ready for implementation. 8. Validation with human subjects in actual operational space flight, demonstrate efficacy/operational feasibility. 7. Evaluation with human subjects in controlled laboratory simulating operational space flight environment. 6. Laboratory/clinical testing of potential countermeasure in subjects to demonstrate efficacy of concept. 5. Proof of concept testing and initial demonstration of feasibility and efficacy. 4. Formulation of countermeasures concept based on understanding of phenomenon. 3. Validated hypothesis. Understanding of scientific processes underlying problem. 2. Hypothesis formed, preliminary studies to define parameters. Demonstrate feasibility. 1. Phenomenon observed and reported. Problem defined. ©vpisacane, 2014
  • 27. BACKGROUND EXPOSURE Growth In Exposure to Ionizing Radiation in USA Source: NCRP Report No. 160, 2009 ©vpisacane, 2014
  • 28. BACKGROUND EXPOSURE Radiation Exposure in the US from NCRP-160 Collective effective dose= Total radiation dose incurred by a population Radiation exposure in the United States, from NCRP-160 [NCRP, 2006] ©vpisacane, 2014
  • 29. SPACEFLIGHT EXPOSURE Astronaut Radiation Doses ▲ Absorbed dose ● Effective dose Figure 9.25 Historical radiation doses recorded by astronauts▲ and estimates of effective doses ● for all NASA mission through December 1999, from Cucinotta et al, [2002], ©vpisacane, 2014
  • 30. PARTICLE ACCELERATORS Synchrotron  Synchrotron is a cyclotron where magnetic field is increased as energy increase to maintain constant radius to account for mass increase as speed of light is approached  Formed from straight sections interspaced with bending magnets , accelerating cavities, and drift tubes  Diagram – Group of particles enter at A – Interspaced magnets M bend trajectory – Interspaced acceleration gap G accelerates particle – Magnetic field at M increases as particle energy increases to maintain constant radius  Proton Synchrotron at CERN in Geneva – – – – – Orbit diameter of 172 m Deflecting magnets of 1.4 T Accelerates protons to 28 GeV Each pulse contains ~ 1011 protons Protons travel ~80,000km during acceleration Synchrotron http://www.schoolphysics.co.uk/age1619/Nuclear%20physics/Accelerators/text/Synchrotron_/index.ht ml Spill Synchrotron output ©vpisacane, 2014
  • 31. NASA SPACE RADIATION LABORATORY NSRL Site Pictures NSRL Entrance Tunnel uunder development Tunnel populated ©vpisacane, 2014