Fusion Programme - ENEA - Fusione

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Abbreviations and AcronymsITERITGITMIVTIVVSInternational Thermonuclear Experimental Reactorion turbulent gradientIntegrated Tokamak Modellinginner vertical targetin-vessel viewing and ranging systemJJAEAJETJRAJT-60UJT-60SAJapan Atomic Energy Agency - JapanJoint European Torus - Abingdon - U.K.Joint Research ActivitiesJAERI Tokamak 60 Upgrade, Naka, JapanJAERI Tokamak 60 Super AdvancedKKGAMkinetic geodesic acoustic modeLLANLLCALCCALEGLFRLHLHCLHCDLLLL-LiLMFRLNLLOCALTSLos Alamos National Laboratorylife cycle assessmentlife cycle cost analysislow-energy grouplead fast reactorlower hybridLarge Hadran Collider (CERN)lower hybrid current driveliquid lithium limiterliquid lithiumliquid metal fast reactorLegnaro National Laboratoryloss-of-coolant accidentlow-temperature superconductingMMAMARFEMASTminor actinidemultifaceted asymmetric radiation from the edgeMega Ampère Spherical Tokamak196
2007MHDMiAEMITMOD-TFAMQEMSAMSEMSEMSMMSSTMTHMmagnetohydrodynamicmagnetic-isalnd-induced Alfvén eigenmodeMEGAPIE integral testmetal organic deposition trifluoroacetateminimum quench energyModified Source Approximationmotional Stark effectMinistry for Economic Development (Italy)modified source multiplicationMeasurement Simulation Software Toolmetric tons of heavy metalNNACENBINEGNHFMLNNNNSANRGNPLNPPN-VDSNZPVNatural Circulation Experimentneutral beam injectionnon-evaporate getterNational High-Field Magnet Laboratory - Talahassee - U.S.A.neural networksNational Nuclear Security Administrationnon-evaporable getterneutron power loadsIRIS nuclear power plantnormal vent detritiation systemnormal zone propagation velocityOOECD/NEAOREORNLOSTOVTOXIDENPOrganisation for Economic Cooperation and Development/Nuclear Energy Agencyoccupational radiation exposureOak Ridge National Laboratory - Tennessee - U.S.A.Oxford Instruments Superconducting Technologiesouter vertical targetOxidizing Environment Impact on Source TermPAMp-CVDPEPFISPFCPFCPFCIpassive active multijunctionpolycristalline chemical vapour depositionpolyethylenepoloidal field insert sampleplasma-facing componentpoloidal field coilpoloidal field coil insert197
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PROGRESS REPORT2007Nuclear Fusion a
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ContentsPART I - FUSION PROGRAMME 7
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2007PART IV - MISCELLANEOUS 18314.
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2007analyses of the missions to be
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Fusion Programme2007 Progress Repor
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Fusion ProgrammeTable 1.I - Summary
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Fusion ProgrammeFollowing a Europea
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Fusion Programmen e (10 20 m -3 )3.
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Fusion Programmewas not affected by
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Fusion ProgrammeShear Alfvén wavec
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Fusion Programmen H (10 20 /m 3 )0.
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Fusion Programmei.e., typically, ra
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Fusion ProgrammeENEA has provided t
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Fusion Programmennα6 LIF6 LIF9 BeI
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Fusion Programmedifference between
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Fusion ProgrammeIntroductionThe suc
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Fusion ProgrammeMinority ions, acce
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Fusion ProgrammeThe cryostat overal
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Fusion ProgrammeIntroductionThe tec
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Fusion ProgrammeThe main results so
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Fusion ProgrammeInfrared absorption
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Fusion ProgrammeFig. 3.8 - Frascati
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Fusion ProgrammeThe second year of
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250Fusion Programmeflow-rate in the
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Fusion ProgrammeThe aim of the work
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Fusion ProgrammeFig. 3.21 - X-ray s
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Fusion ProgrammeRange (mm)593583573
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Fusion ProgrammeZ (m)6420-2-4-6sour
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Fusion Programmea) b)c)Fig. 3.31 -
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Fusion Programmeactivation. Eight r
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Fusion Programme1×10 -6Tensile cre
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Fusion ProgrammeAcc V Spot Magn Det
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Fusion Programmelubricants cannot b
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Fusion ProgrammeTritium roomTritium
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Fusion ProgrammeImplications for PS
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Fusion ProgrammeThe development and
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Fusion ProgrammeIntroductionDuring
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Fusion Programme19.5Section view B-
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Fusion Programmeresults and particu
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Fusion ProgrammeFollowing the exten
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Fusion Programme4.7 Characterisatio
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Fusion ProgrammeMagnetic moment (em
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Fusion ProgrammeCeO 2YSZCeO 2YBCOMa
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Fusion Programme0 1 10 0 1 100 1 10
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Fusion ProgrammeLoad (mN)0.80.60.40
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Fusion Programme5.1 Outline and Ove
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Fusion Programme(λ D /Δ 0 ) 2Δ 0
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5. Inertial Fusion2007 Progress Rep
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6. Communication and Relationswith
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7. Publications and Events - Fusion
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Fission Technology8.1 Advanced and
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Fission TechnologyAcceleration m/s
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Fission Technology232.73 mm (17 pin
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Fission TechnologyThe Very High Tem
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Fission Technology500Thermocouple t
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Fission Technology0.16 mm 0.16 mm0.
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Fission Technology-4800-85000.00SGU
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Fission Technologythrough calculati
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Fission Technology1.23 e+001.17 e+0
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Fission TechnologyPressure (bar)642
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Fission TechnologyFig. 8.37 - Creep
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Fission TechnologyENEA organised th
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Fission TechnologyTemperature600400
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Fission TechnologyZ(m)1.00.80.60.40
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Fission Technologythat a system is
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Fission TechnologyMaxwellian-averag
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Page 150 and 151: Fission Technology9.1 Boron Neutron
Page 152 and 153: Fission TechnologyIn collaboration
Page 154 and 155: Fission Technologyvolume. Thus the
Page 156 and 157: Fission TechnologyFig. 9.9 - Logger
Page 158 and 159: Fission TechnologyIn relation to EN
Page 160 and 161: Fission TechnologyArticles11.1 Publ
Page 162 and 163: Fission TechnologyArticles incourse
Page 164 and 165: Fission TechnologyF. ROELOFS, B. DE
Page 166 and 167: Fission TechnologyE. BERTHOUMIEUX e
Page 168 and 169: Fission TechnologyInternal reportsR
Page 170 and 171: Fission TechnologyRTI FPN-P815-008
Page 173 and 174: PART IIINUCLEAR PROTECTION171
Page 175 and 176: 12. Radioactive Waste Management an
Page 183: 13. Publications - Nuclear Protecti
Page 186 and 187: Miscellaneous14.1 Advances in the I
Page 188 and 189: Miscellaneoususing a full wave code
Page 190 and 191: MiscellaneousAt present the effect
Page 192 and 193: MiscellaneousSuperAGILE view of the
Page 194 and 195: Abbreviations and AcronymsAacACPADS
Page 196 and 197: Abbreviations and AcronymsEFITEHRSE
Page 200 and 201: Abbreviations and AcronymsPFWPGAPHY
Page 202: Abbreviations and AcronymsVVDEVELLA
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