Radiation Shielding Simulation For Interplanetary Manned Missions

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Radiation Shielding Simulation For Interplanetary Manned Missions S. Guatelli 1, B. Mascialino 1, P. Nieminen 2, M.G. Pia 1 Credit: ESA 1 INFN Genova, Italy 2 ESA-ESTEC, The Netherlands Credit: ESA IPRD 06 10th Topical Seminar on Innovative Particle and Radiation Detectors 1-5 October, 2006 Siena, Italy

Context Planetary exploration has grown into a major player in the vision of space science organizations like ESA and NASA AURORA: European long term plan for the robotic and human exploration of the solar system with Mars, the Moon and the asteroids as the most likely targets

Human missions to Mars The effects of space radiation on astronauts are an important concern 6 month transit from the Earth to Mars Mission to Mars ~ 2.5 year total duration 1.5 year stay on the Martian surface 6 month return to the earth The crew is exposed to the space radiation environment Radiation sickness Damage to the central nervous system Cancer Optimize trajectories Shielding Credit: ESA Credit: ESA

This project In the framework of the AURORA programme of ESA Scope Quantitative evaluation of the physical effects of space radiation in interplanetary manned missions Transfer vehicles On planetary surface First quantitative evaluation of the shielding properties of conceptual designs Comparison among different shielding options Guidelines for future mission design and concrete engineering studies

Strategy Risk assessment Sound physics results Advanced technology Transparency Reliable model to evaluate acceptable risk (risk is not measured, it is predicted by a model) Distinguish physical and biological effects Validation of the physics modelling components Control systematics Quantitative mathematical analysis of results Object Oriented technology Rigorous software process Software tools based on modern technology Open source software tools Publicly distributed software All the features above are relevant to a mission-critical long-range space science project

Uncertainties and systematics Large uncertainties Modelling hadronic interactions Radiation environment Mission trajectories and duration Characteristics of spacecrafts Biological effects of radiation exposure Intrinsic complexity of the underlying theory Scarce and imprecise experimental data Monte Carlo codes still evolving in this domain Focus on physics in the 1 st study cycle Biological effects on top of sound physics in a following cycle Relative comparison of shielding configurations Relative Instead of absolute dose calculations Multiple hadronic models to evaluate systematics

Software Strategy Software Development Process Iterative and incremental model Based on the Unified Process Specifically tailored to the project Mapped onto ISO 15504 Object Oriented Technology Openness to extensions and evolution Maintainability over a long time scale Monte Carlo simulation Physical Analysis Statistical Analysis Model radiation environment Model shielding configuration Track particles in matter Evaluate energy deposited in the astronaut Compare shielding options quantitatively Functionality (geometry, physics, interactivity) OO technology Rigorous validation Abstract Interfaces for Data Analysis Independence from any specific analysis tools Richest collection of goodness-of-fit tests for data comparison AIDA compliant

Architecture of the Geant4 application Component-based architecture Each component has a specific responsibility Flexibility, extensibility and maintainability

Geometry and materials Decorator Design Pattern Dynamically configure the simulation with Habitat type Shielding geometry Material Astronaut s location

CREME96 Primary particle generation Conservative assumptions for risk assessment Radiation environment models ECSS standard Galactic Cosmic Rays 1 AU Galactic Cosmic Rays 1977 solar minimum Anti-correlation with solar activity Solar Particle Events October 1989 event 99% worst case 1 MeV < E < 100 GeV Solar Particle Events 1 MeV < E < 100 GeV 1 AU

Electromagnetic physics Geant4 Low Energy Package for: p, α, ions (model based on ICRU49 parameterisation) photons and electrons (model based on the Livermore Libraries) Geant4 Standard Package for positrons and muons Low Energy Electromagnetic Package overall better accuracy Demonstrated by validation studies Hadronic Physics Elastic and inelastic hadronic scattering Alternative models of the inelastic scattering of protons, neutrons, pions: Hadronic inelastic process Binary set Bertini set Low energy range (cascade + preequilibrium + nuclear deexcitation) Intermediate energy range ( up to E = 25 GeV) High energy range ( 20. GeV < E < 100. GeV ) α inelastic scattering Low Energy Parameterized model up to E = 100 MeV Binary Ion model Binary Cascade + Precompound + Deexcitation ( up to 10. GeV ) Physics modelling Low Energy Parameterised Quark Gluon String Model Bertini Cascade ( up to 3.2 GeV )

Shielding studies Inflatable Habitat Shielding materials Shielding thickness Comparison to rigid habitats Planet surface habitats Shielding with lunar regolith Comparison to a rigid habitat

Inflatable habitat Multilayer structure External thermal protection blanket - Betacloth and mylar Meteoroid and debris protection - Nextel (bullet proof material) and open cell foam Structural layer - Kevlar Rebundant bladder - Polyethylene, polyacrylate, EVOH, kevlar, nomex Experimental set-up Engineering model by ALENIA SPAZIO GCR Simplified geometry Retains the essential characteristics for a shielding characterization Multilayer Z Astronaut Water phantom

Average energy deposit (MeV) GCR p Systematics of hadronic modelling Study of possible systematic effects related to hadronic physics modelling Comparison of the energy deposit in the phantom with different hadronic models Energy deposit profile of GCR proton Multilayer + 10 cm water shielding Bertini Depth in the phantom (cm) Binary Electromagnetic Hadronic contribution is significant Average no. of secondary particles reaching the phantom Counts Bertini Binary Energy of secondary p Bertini White: Bertini set Black: Binary set Binary Different energy deposit profiles and secondary product patterns Kolmogorov Smirnov Test: p-value < 0.05 Physics models Energy deposit in the phantom Electromagnetic 71.9 ± 0.2 MeV Hadronic-Bertini 128.0 ± 0.4 MeV Hadronic-Binary 117.3 ± 0.4 ~10 % difference compatible with experimental validation of Geant4 hadronic models

Shielding thickness Impossible to shield galactic cosmic rays completely! GCR p The shielding modulates the fraction of GCR reaching the phantom Secondary particles are also generated in the shielding material No shielding 10 cm water shielding Average energy deposit of GCR p in the phantom Effect of 5 cm and 10 cm water shielding + inflatable multi-layer % GCR p reaching the phantom 5 cm water 10 cm water EM + Bertini 88.7 ± 0.2 83.3 ± 0.2 EM + Binary 88.0 ± 0.2 82.3 ± 0.2 Average energy deposit (MeV) 10 cm water - Bertini set 5 cm water - Bertini set 10 cm water - Binary set 5 cm water - Binary set Depth in the phantom (cm) Energy deposit in the phantom 5 cm water 10 cm water EM + Bertini 130.2 ± 0.5 128.0 ± 0.5 EM + Binary 119.3 ± 0.4 117.3 ± 0.4 Doubling the shielding thickness results in: Few % difference in the stopped GCR protons ~2 % difference in the total energy deposit

Shielding material for an inflatable habitat Polyethylene Water Average energy deposit (MeV) Average energy deposit of GCR p GCR p 10 cm water - Bertini set 10 cm polyethylene - Bertini set 10 cm water - Binary set 10 cm polyethylene - Binary set Depth in the phantom (cm) Water and polyethylene: equivalent shielding effect Energy deposit in the phantom (MeV) 10 cm polyethylene 10 cm water EM + Bertini 128.4 ± 0.5 128.0 ± 0.5 EM + Binary 117.3 ± 0.5 117.3 ± 0.5 Average number of secondary particles reaching the phantom Counts 10 cm water 10 cm polyethylene Bertini set Energy of secondary n Anderson-Darling test Cramer-von Mises test χ 2 test all borderline p-value

Inflatable vs. Rigid Habitat Reference: rigid structures as in the ISS (2-4 cm Al) Average energy deposit of GCR p Average energy deposit (MeV) GCR p Depth in the phantom (cm) 10 cm water - Bertini 4 cm Al - Bertini 10 cm water - Binary 4 cm Al - Binary set 10 cm water EM 4 cm Al EM Kolmogorov-Smirnov test Multi-layer + 10 cm water equivalent to 4 cm Al Multi-layer + 5 cm water equivalent to 2.15 cm Al Shielding Energy deposited in phantom (MeV) material EM Bertini Binary ML + 5 cm water 73.5 ± 0.3 130.2 ± 0.5 119.3 ± 0.4 ML + 10 cm water 71.9 ± 0.3 128.0 ± 0.5 117.3 ± 0.5 4 cm Al 72.9 ± 0.3 127.5 ± 0.5 117.0 ± 0.4 2.15 cm Al 73.9 ± 0.3 130.5 ± 0.5 119.3 ± 0.5 An inflatable habitat exhibits a shielding capability equivalent to a conventional rigid one

Secondary products in inflatable and rigid habitats Counts Average no. of secondary particles reaching the phantom Binary set Multilayer + 10 cm water 4 cm Al Energy spectrum of secondary protons Bertini set 10 cm water 4 cm Al Anderson-Darling test Cramer-von Mises test χ 2 test Different No significant effects on the energy deposit in the phantom

Effects of other cosmic ray components Similar studies of GCR α, C, O, Si and Fe ion components Energy deposited in phantom (MeV) by GCR α Weighted according to the relative flux w.r.t. p Multi-layer + 10 cm water EM 27.2 ± 0.1 EM + Bertini 32.0 ± 0.1 EM + Binary 31.7 ± 0.1 Average energy deposit of GCR ions Weighted according to the relative flux w.r.t. p Multi-layer + 10 cm water shielding EM physics only Dominant contribution derived from electromagnetic interactions First indication The hadronic models for α particles are under development and under validation Main contribution from p and α

Radiation protection from solar particle events A shelter protects the crew from the harmful effects of solar particle events 10 cm water SPE Shelter Z Shelter: limited zone enclosed by an additional shielding layer Alarm of a solar particle event The astronauts recover in the shelter

Solar particle events Fraction of solar event protons reaching the phantom Shelter thickness (cm) % 0 (1.03 ± 0.05) 10-1 20 50 75 Average total energy deposit EM physics Bertini set (1.6 ± 0.2) 10-2 (3.4 ± 0.8) 10-3 (2.0 ± 0.6) 10-3 75 cm shelter Solar event protons spectrum Average total energy deposit (kev) Binary set Shelter thickness (cm) An additional shelter layer is effective at stopping a significant fraction of solar particle events

Radiation shielding on planetary surface Moon: intermediate step to a human mission to Mars Energy deposit in the phantom Shielding: moon soil Average total energy deposit (MeV) GCR p Energy deposit 4cm Al habitat Moon soil heap Cavity GCR SPE Moon soil Regolith layer thickness (cm) Shielding against GCR Lunar regolith shielding is comparable to or better than a conventional Al structure Shielding against SPE 50 cm regolith equivalent to the shielding effectiveness of 50 cm SPE vehicle shelter Moon regolith can be considered as a shielding option

Summary Inflatable Habitat + shielding Hadronic interactions are significant, systematics is under control The shielding capabilities of an inflatable habitat are comparable to a conventional rigid structure Water / polyethylene are equivalent Shielding thickness optimisation involves complex physics effects An additional shielding layer, enclosing a special shelter zone, is effective against SPE Moon Habitat Regolith shielding limits GCR and SPE exposure effectively Its shielding capabilities against GCR can be better than conventional Al structures as in the ISS

Conclusions This project represents the first attempt in the European AURORA programme to estimate the radiation protection of astronauts quantitatively Quantitative evaluations Based on open source, validated software Guidance to space industry The software system developed is publicly available to the scientific community Advanced software technology Open to extension and evolution 1 st development cycle of a long-term project in collaboration with ESA Thanks to all REMSIM team members for their collaboration, in particular to: V. Guarnieri, C. Lobascio, P. Parodi and R. Rampini This project was funded by the European Space Agency