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UTILIZING SPENVIS FOR EARTH ORBIT ENVIRONMENTS ASSESSMENTS: RADIATION EXPOSURES, SEE, and SPACECRAFT CHARGING Brandon Reddell and Bill Atwell THE BOEING COMPANY NASA Systems Houston, TX 77059 USA SPENVIS & GEANT4 Workshop Leuven, Belgium 3 - 7 October 2005 ABSTRACT The SPENVIS, developed by the Belgium Institute of Aeronomy (BIRA), Brussels, Belgium, has been utilized to generate trapped proton and electron particle spectra for low-earth (LEO), mediumearth (MEO) and geostationary orbits (GEO) and to perform comparisons/benchmarking for several high-energy particle transport codes. A discussion of the proton and electron spectra and transport codes used in this study is presented. Results of the absorbed dose calculations and code comparisons using aluminum shielding are presented and discussed in detail. An example of a single event effects (SEE) analysis for the International Space Station (ISS) internal and external computers is discussed. Additionally, the application of SPENVIS to calculate spacecraft charging is also discussed in relation to the ISS. A comparison of the SPENVIS predicted structure potential with the Boeing ISS Plasma Interaction Model (PIM) prediction and measured data from the Floating Potential Probe (FPP) is shown. 2 Outline of Talk Application of SPENVIS to generate trapped electron and proton spectra for various near-Earth orbits Present dose comparisons for benchmarking radiation transport codes MULASSIS/GEANT4, FLUKA, MCNPX, Shieldose 2, CEPXS Other SPENVIS options under consideration/or being used by the Boeing ISS Environments Group Single Event Effects ISS vehicle structure charging predictions Comparison with Boeing ISS Plasma Interaction Model predictions and on-orbit data Conclusions 3 NEAR-EARTH REGIONS LOW-EARTH ORBIT (LEO) – Typical ISS orbit ~ 400 km X 51.6 deg MEDIUM-EARTH ORBIT – Global Positioning Satellite (GPS) Orbit 20,200 km x 55 deg GEOSTATIONARY ORBIT – 160 deg W long. ~36,000 km x ~0 deg 4 LEO PROTON & ELECTRON SPECTRA AP-8MIN PROTON INTEGRAL & DIFFERENTIAL SPECTRA ISS ORBIT: 400 KM X 51.6 DEG EPOCH: JUNE 2007 AE-8MAX ELECTRON INTEGRAL & DIFFERENTIAL ISS ORBIT: 400 KM X 51.6 DEG EPOCH: JAN. 2012 5 LEO AP-8MIN PROTON INTEGRAL & DIFFERENTIAL SPECTRA LEO AP-8MIN Proton Spectra 400 km x 51.6 deg - Epoch: June 2007 1.E+09 1.E+08 Integral & Diff. Flux, / day Integral Differential 1.E+07 1.E+06 1.E+05 1.E+04 1.E+03 1.E+02 0 100 200 Proton Energy, MeV 300 6 LEO AE-8MAX ELECTRON INTEGRAL & DIFF. SPECTRA LEO AE-8MAX Electron Spectra 400 km x 51.6 deg - Epoch: Jan. 2012 1.E+11 Integral & Diff. Flux, / day 1.E+10 Integral 1.E+09 Differential 1.E+08 1.E+07 1.E+06 1.E+05 1.E+04 1.E+03 0 1 2 3 4 5 6 Electron Energy, MeV 7 MEO AE-8MAX ELECTRON DIFFERENTIAL SPECTRUM Diff. Flux, #/cm2-MeV-day MEO AE-8MAX Electron Diff. Spectrum GPS Orbit - 20,200 km x 55 deg 1.E+14 1.E+13 1.E+12 1.E+11 1.E+10 1.E+09 1.E+08 1.E+07 1.E+06 1.E+05 1.E+04 1.E+03 0 2 4 Electron Energy, MeV 6 8 MEO AP-8MIN PROTON DIFFERENTIAL SPECTRUM Diff. Flux, #/cm2-MeV/day MEO AP-8MIN Proton Diff. Spectrum GPS Orbit 1.E+14 1.E+13 1.E+12 1.E+11 1.E+10 1.E+09 1.E+08 1.E+07 1.E+06 1.E+05 1.E+04 0 1 2 3 4 Proton Energy, MeV 5 6 7 9 GEO AE-8MAX INTEGRAL & DIFF. ELECTRON SPECTRA 160 deg W long. – Epoch: Jan. 2012 GEO AE-8MAX Electron Spectra 160 deg W long. - Epoch Jan. 2012 1.E+14 Integral & Diff. Flux, #/cm 2-day & #/cm 2-MeV/day Integral 1.E+13 Differential 1.E+12 1.E+11 1.E+10 1.E+09 1.E+08 1.E+07 1.E+06 1.E+05 0 1 2 3 Electron Energy, MeV 4 5 10 COMPUTER CODES MULASSIS / GEANT 4 3-D Monte-Carlo transport code Hadronic, Electromagnetic, Low-Energy Neutron Physics FLUKA 3-D Monte-Carlo transport code Precision Physics Default, with electromagnetic and low energy neutrons SHIELDOSE 2 Uses pre-calculated, mono-energetic depth-dose data for an isotropic, broad-beam fluence of radiation incident on uniform aluminum plane media. Proton transport considers Coulomb interactions only (no nuclear interaction), electron transport with bremsstrahlung MCNPX 3-D Monte-Carlo transport code For this study, only electron transport considered, including electromagnetic effects. CEPXS 1-D planar-geometry discrete ordinates code for coupled photon-electron transport 11 LEO Proton Dose Comparisons 200 MeV Proton incident on 1.0 g/cm2 Aluminum Slab 1 Mulassis/G4 FLUKA Shieldose 2 Dose Rate, rad (Si) / day 0.1 0.01 0.001 0.0001 0.01 0.1 1 10 Al Shielding Thickness, g/cm2 100 12 LEO Electron Dose Comparisons 1.0 MeV Electron incident on 1.0 g/cm2 Aluminum Slab 100 Mulassis/Geant4 FLUKA Dose Rate, rad (Si) / day 10 Shieldose 2 1 0.1 0.01 0.001 0.01 0.1 1 Al Shielding Thickness, g/cm2 10 13 MEO Electron Dose Comparisons 1.E+05 Mulassis/G4 FLUKA Dose Rate, rad (Si) / day 1.E+04 Shieldose 2 1.E+03 1.E+02 1.E+01 1.E+00 1.E-01 0.01 0.1 1 Al Shielding Thickness, g/cm2 10 14 GEO Electron Dose Comparisons - 1 Geosynchronous Orbit - Electrons 1.00E+05 SD2 MCNPX CEPXS Mulassis/G4 FLUKA Dose Rate, rads Si /day 1.00E+04 1.00E+03 1.00E+02 1.00E+01 1.00E+00 1.00E-01 0.01 0.10 1.00 Al Thickness, g/cm 10.00 2 15 GEO Electron Dose Comparisons - 2 GEO Comparisons 1.00E+05 MCNPX Mulassis/G4 FLUKA 1.00E+04 Dose Rate, rads Si /day 1.00E+03 1.00E+02 1.00E+01 1.00E+00 1.00E-01 1.00E-02 0.01 0.10 1.00 Al Thickness, g/cm 10.00 2 16 Single Event Effects 17 ISS Single Event Upset Observations ISS Orbit 18 ISS Single Event Upset Observations S1-1 MDM-10 S0-1 MDM-10 S1-2 MDM-4 S0-2 MDM-10 P1-1 MDM-4 P1-2 MDM-10 US Laboratory Module MDM-DRAM Measured SEU Count/238 days SEFA SEU Count/238 days FOM SEU Count/238 Days Lab-1 40 g/cm2 488 287 83 Lab-3 40 g/cm2 490 287 83 P1-2: 10 g/cm2 536 6202 1647 S1-1: 10 g/cm2 488 6202 1647 19 ISS Spacecraft Charging 20 ISS Vehicle Charging Various models available to compute floating potential of structure with respect to plasma SOLARC, PIX2, thin sheath, thick sheath models for solar array and structure SOLARC gives best correlation to observed floating potential and Boeing ISS PIM results SOLARC only accounts for solar array charging (i.e. no magnetic induction) FPP Unit 21 FPP Potential Data (April 11, 2001) 25 PEAK 1 FPP Eclipse Sun PEAK 2 PEAK 3 Voltage (-V) 20 PCU OFF 15 PEAK 4 PEAK 5 PEAK 6 10 5 0 12:00 14:00 16:00 18:00 20:00 22:00 Time (GMT) 22 Potential Map for ISS Stage 11A Corresponding to April 11, 2001 (FPP Peak 1) Conditions Potential (V) Vmin = -31.1V Vmax = -18.3V 23 ISS Potential Comparison 30 FPP Data PIM - 23m2 SPENVIS/SOLARC Voltage (-V) 20 10 0 12:30 13:00 13:30 Time (GMT) 14:00 24 Spacecraft Charging For LEO, spacecraft charging is highly dependent on plasma temperature, density, and geomagnetic field For these reasons, a probabilistic approach must be used to address spacecraft charging: Models like the International Reference Ionosphere (IRI-2001) are climatological in nature and provide average properties; not the short transients that occur near eclipse exit The SPENVIS spacecraft charging models allow the user to input plasma temperature and density to compute floating potential – only compute solar array charging SPENVIS will need to access a plasma database of measured/known values to calculate spacecraft charging 25 Spacecraft Charging For predictions, known plasma parameters must used to simulate transient plasma conditions Climatological models do not predict extreme plasma conditions properly PIM Results 26 CONCLUSIONS SPENVIS was utilized to generate trapped electron and proton spectra for LEO, MEO, and GEO Various computer codes were used to transport these spectra to compute absorbed dose Dose rates computed in thin silicon detector behind finite & semiinfinite slab aluminum shielding For all three regimes, the transport codes generally agree to within 10-15% of each other Some deviations at extremely thin and extremely thick regions Can infer differences in radiation transport model physics SPENVIS can be used to study Single Event Effects SPENVIS needs a choice of GCR models so that the user can generate preferred spectra i.e. CREME 96 or Badhwar-O’Neil GCR Model Recommend adding Figure of Merit (FOM) technique to SPENVIS SPENVIS could be used to study spacecraft charging provided user knows a priori plasma conditions SPENVIS needs a geomagnetic field induced potential (vxB·L) option/model. This is important for large spacecraft 27