System and safety studies of accelerator driven transmutation ... - SKB

More documents

Recommendations

Info

OPECST,Public Hearing, January 20, 2005 ..nor dr Strangelove being non- critically fascinated with nuclear… 3
….nor I am a Nobel Prize Winner OPECST,Public Hearing, January 20, 2005 …yet… However, I have done transmutation related research since 1991 and conducted a lot of large research projects in this field 4
Page 1 and 2:
System and safety studies of accele
Page 3 and 4:
Preface The research on safety of A
Page 5 and 6:
coolant fraction allows for decay h
Page 7 and 8:
To dispose the spent fuel as it is
Page 9 and 10:
SAMMANFATTNING Resultaten från for
Page 11 and 12:
Detaljerade analyser av neutronkine
Page 13 and 14:
Modellering av de termo-kemiska ege
Page 15 and 16:
LIST OF APPENDICES 1. Carl-Magnus P
Page 17 and 18:
ABBREVIATIONS AND ACRONYMS EUROPEAN
Page 19 and 20:
FCC Face Centered Cubic - type of a
Page 21 and 22:
1 SYSTEM AND SAFETY STUDIES OF ADS
Page 23 and 24:
pin. The full core void worth was c
Page 25 and 26:
Figure 2.1 The 1180-loading of Yali
Page 27 and 28:
Counts Counts 10 5 10 4 10 3 10 2 1
Page 29 and 30:
Figure 2.4 Ion source interruption
Page 31 and 32:
New 1 g 232 Th, 238 U (ultra pure)
Page 33 and 34:
3.1.2 System descriptions The PDS-X
Page 35 and 36:
4 NUCLEAR FUEL CYCLE ANALYSIS 4.1 E
Page 37 and 38:
will be calculated using MCB, the M
Page 39 and 40:
irradiation, the spent fuel assembl
Page 41 and 42:
4.1.3 Results The calculations has
Page 43 and 44:
4.2 ANALYSIS OF THE SWEDISH NUCLEAR
Page 45 and 46:
Mass [tons] 300 250 200 150 100 50
Page 47 and 48:
5 POTENTIAL OF REACTOR BASED TRANSM
Page 49 and 50:
due to a partial insertion, the inf
Page 51 and 52:
irradiation to maintain the core as
Page 53 and 54:
configuration allowed the reactor t
Page 55 and 56:
6.2 THERMOCHEMISTRY OF ADVANCED FUE
Page 57 and 58:
Figure 7.1 Positions of Cr atoms in
Page 59 and 60:
8 DEVELOPMENT OF CODES AND METHODS
Page 61 and 62:
Let us assume the neutron flux is p
Page 63 and 64:
waste repository notes which year t
Page 65 and 66:
9 INTERNATIONAL INTERACTIONS, SEMIN
Page 67 and 68:
Janne Wallenius Oct 2005 Participat
Page 69 and 70:
[11] Sylvie Pillon and Janne Wallen
Page 71 and 72:
Nuclear Instruments and Methods in
Page 73 and 74:
376 fraction, beff, have been calcu
Page 75 and 76:
378 Fig. 3. Fit of exponentials to
Page 77 and 78:
380 Table 6 Experimental estimation
Page 79 and 80:
382 dominating closer to criticalit
Page 81 and 82:
12th International Conference on Em
Page 83 and 84:
2.2 Yalina Booster Yalina and Yalin
Page 85 and 86:
Yalina and Yalina Booster Λ 1 ⎛
Page 87 and 88:
Yalina and Yalina Booster Table III
Page 89 and 90:
Yalina and Yalina Booster 7 REFEREN
Page 91 and 92:
1720 A. Talamo, W. Gudowski / Annal
Page 93 and 94:
Page 95 and 96:
Page 97 and 98:
Page 99 and 100:
Page 101 and 102:
Page 103 and 104:
Page 105 and 106:
Page 107 and 108:
Page 109 and 110:
Page 111 and 112:
Page 113 and 114:
Page 115 and 116:
Page 117 and 118:
Page 119 and 120:
Page 121 and 122:
Journal of NUCLEAR SCIENCE and TECH
Page 123 and 124:
1042 A. TALAMO and W. GUDOWSKI Tabl
Page 125 and 126:
Page 127 and 128:
1046 A. TALAMO and W. GUDOWSKI 237
Page 129 and 130:
1048 A. TALAMO and W. GUDOWSKI 1) 2
Page 131 and 132:
Page 133 and 134:
1052 A. TALAMO and W. GUDOWSKI IX.
Page 135 and 136:
Abstract Annals of Nuclear Energy 3
Page 137 and 138:
Table 1 Technical data of the power
Page 139 and 140:
Page 141 and 142:
Page 143 and 144:
Page 145 and 146:
Page 147 and 148:
Page 149 and 150:
Page 151 and 152:
Page 153 and 154:
Page 155 and 156:
Page 157 and 158:
Page 159 and 160:
Page 161 and 162:
Page 163 and 164:
Page 165 and 166:
Page 167 and 168:
Abstract Technical note Managing th
Page 169 and 170:
86 A. Talamo / Annals of Nuclear En
Page 171 and 172:
Page 173 and 174:
Page 175 and 176:
Page 177 and 178:
Page 179 and 180:
Page 181 and 182:
Page 183 and 184:
Westlén and Wallenius HEAT REMOVAL
Page 185 and 186:
Page 187 and 188:
Page 189 and 190:
Page 191 and 192:
Page 193 and 194:
Accelerator-driven Systems: Safety
Page 195 and 196:
Abstract The accelerator-driven sys
Page 197 and 198:
Acknowledgements I owe thanks to ma
Page 199 and 200:
“A grad student in procrastinatio
Page 201 and 202:
specify the meaning of the term “
Page 203 and 204:
that three fast breeder reactors (F
Page 205 and 206:
emitting properties and its relativ
Page 207 and 208:
TABLE 8 Effective dose coefficients
Page 209 and 210:
Fig. 1 Radiotoxic inventory of the
Page 211 and 212:
prior to disposal. The most commonl
Page 213 and 214:
often used in repository safety ana
Page 215 and 216:
separations process is also known a
Page 217 and 218:
Spent Fuel U Pu PUREX FP + An Np Tc
Page 219 and 220:
Fig. 6 Schematic picture of the pyr
Page 221 and 222:
From the viewpoint of reducing the
Page 223 and 224:
Chapter 3: Transmutation Strategies
Page 225 and 226:
from reprocessing is sent into stor
Page 227 and 228:
adiotoxicity in the spent fuel afte
Page 229 and 230:
In order to overcome the safety iss
Page 231 and 232:
79 Se (T1/2=6.5·10 4 years) and 12
Page 233 and 234:
Source multiplication in a subcriti
Page 235 and 236:
given by the source multiplication
Page 237 and 238:
Fig. 16 Delayed neutron spectra vs.
Page 239 and 240:
offers low void worths. For tight l
Page 241 and 242:
smaller than classical MOX-fuel sur
Page 243 and 244:
Responsiveness of the ADS The kinet
Page 245 and 246:
Fig. 19 compares the response in a
Page 247 and 248:
design parameters. The reference co
Page 249 and 250:
indefinitely. The burst limit is ap
Page 251 and 252:
maintain the reactor in the subcrit
Page 253 and 254:
value (-$18.5), the power increases
Page 255 and 256:
() β ( ) Λ () dck t k t = p t −
Page 257 and 258:
(a) (b) (c) (d) Fig. 25 Source over
Page 259 and 260:
Accelerator reliability In accelera
Page 261 and 262:
Conclusions The thesis analysed and
Page 263 and 264:
Appendix A: Reactor Kinetics Equati
Page 265 and 266:
The definition of F(t) is: ρ () t
Page 267 and 268:
Bibliography 1 R. G. Cochran and N.
Page 269 and 270:
38 M. Bunn, S. Fetter, J. P. Holdre
Page 271 and 272:
75 R. J. Puigh and M. L. Hamilton,
Page 273 and 274:
74 Paper I
Page 275 and 276:
chemical reactions. An “inherentl
Page 277 and 278:
temperature with irradiation time e
Page 279 and 280:
and compressible pool volumes with
Page 281 and 282:
comparison, the FFTF reactor, which
Page 283 and 284:
CerMet and nitride. The reason is t
Page 285 and 286:
failure, which leaves small safety
Page 287 and 288:
XII.B. Transient results The result
Page 289 and 290:
programme,” Nucl. Sci. Eng., Acce
Page 291 and 292:
277, American Nuclear Society, LaGr
Page 293 and 294:
Neutronics of minor actinide burnin
Page 295 and 296:
TABLE I: Fuel Doppler constant KD (
Page 297 and 298:
nitric acid. Therefore, we may not
Page 299 and 300:
(e.g. SS316) on the other hand have
Page 301 and 302:
FIG. 4: Example of core map with 24
Page 303 and 304:
TABLE X: BOL temperature coefficien
Page 305 and 306:
[18] M.A. Smith, E.E. Morris, and R
Page 307 and 308:
76 Paper III
Page 309 and 310:
II. REACTOR KINETICS EQUATIONS In t
Page 311 and 312:
The model pertains to an accelerato
Page 313 and 314:
V.A. Variations in Source Strength
Page 315 and 316:
TABLE VI Calculations of the core c
Page 317 and 318:
pressure, starting at t=1 sec. The
Page 319 and 320:
14. R. E. ALCOUFFE, F. W. BRINKLEY,
Page 321 and 322:
Safety Analysis of Na and Pb-Bi Coo
Page 323 and 324:
Neutronics analysis Table 1. Design
Page 325 and 326:
stoichiometric oxide fuel. The fuel
Page 327 and 328:
4000 3500 3000 2500 2000 Peak fuel
Page 329 and 330:
Figure 7. Sodium (left) and lead/bi
Page 331 and 332:
78 Paper V
Page 333 and 334:
1690 M. Eriksson, J.E. Cahalan / An
Page 335 and 336:
Page 337 and 338:
Page 339 and 340:
Page 341 and 342:
Page 343 and 344:
Page 345 and 346:
Page 347 and 348:
Page 349 and 350:
Page 351 and 352:
RELIABILITY ASSESSMENT OF THE LANSC
Page 353 and 354:
calculations are based on operation
Page 355 and 356:
Figure 3 is interesting in that sen
Page 357 and 358:
The database is for practical reaso
Page 359 and 360:
Failure analysis Analysis of failur
Page 361 and 362:
Source efficiency and high-energy n
Page 363 and 364:
Abstract Transmutation of plutonium
Page 365 and 366:
The following papers are not includ
Page 367 and 368:
ERALIB1 ERAnos LIBrary ERANOS Europ
Page 369 and 370:
TRU TRansUranic elements TRUEX TRan
Page 371 and 372:
Contents 1 Introduction 1 2 Transmu
Page 373 and 374:
Chapter 1 Introduction The growing
Page 375 and 376:
objectives of the present thesis ha
Page 377 and 378:
n+ 238U → 239U + γ → 239Np + e
Page 379 and 380:
natural uranium is typically needed
Page 381 and 382:
ate step when an even-N nuclide is
Page 383 and 384:
the atomic mass of a specific eleme
Page 385 and 386:
χ (Ε) 0.4 0.3 0.2 0.1 0.0 0 1 2 3
Page 387 and 388:
UOX- LWR 1. Once-through 2. Pu-burn
Page 389 and 390:
2.2.4 Radiotoxicity reduction The t
Page 391 and 392:
onstrated that recovery yields of 9
Page 393 and 394:
advantage, thanks to the radiation
Page 395 and 396:
As was mentioned earlier, a fast ne
Page 397 and 398:
3.3 Coolant options Since the neutr
Page 399 and 400:
3.4.1 Heavy liquid metal target Two
Page 401 and 402:
In a single spallation reaction, ab
Page 403 and 404:
for this purpose, since it allows f
Page 405 and 406:
technical reasons. One is that larg
Page 407 and 408:
concepts, developed by different EU
Page 409 and 410:
Evaluated Nuclear Data Libraries (e
Page 411 and 412:
SATURNE experiments that the Bertin
Page 413 and 414:
4. Number of neutrons appearing as
Page 415 and 416:
The eigenfunctions of hermitian ope
Page 417 and 418:
( , , ) + ∫∫∫ Φ ( , , ) =
Page 419 and 420:
ks FˆΦ FˆΦ = = AˆΦFˆΦ + S ,
Page 421 and 422:
S Fˆ Φ AˆΦ − FˆΦ AˆΦ 1−
Page 423 and 424:
the second-step calculation. This i
Page 425 and 426:
⎛1−kˆ eff ⎞ FΦ ψ * = ⎜
Page 427 and 428:
Moreover, replacing ϕ * ⋅ Z by
Page 429 and 430:
6.3.3 Varying the target radius Bot
Page 431 and 432:
6.3.4 Required proton beam current
Page 433 and 434:
multiplication process from the ext
Page 435 and 436:
Three sub-critical configurations,
Page 437 and 438:
have energy close to 14.1 MeV. Howe
Page 439 and 440:
and can from this point of view be
Page 441 and 442:
1.E+00 Neutron flux (normalised) 10
Page 443 and 444:
7.2.3 Distribution of the spallatio
Page 445 and 446:
equal or slightly larger than 1, wh
Page 447 and 448:
eactivity indicator can be obtained
Page 449 and 450:
Chapter 8 The Yalina experiments In
Page 451 and 452:
8.2 Dynamic experiments performed a
Page 453 and 454:
fundamental decay rate, determined
Page 455 and 456:
ρ n1 − n0 = β n eff 1 . (64) Th
Page 457 and 458:
for this is the fluctuations of the
Page 459 and 460:
above the bottom of the active part
Page 461 and 462:
perimental results. Experience from
Page 463 and 464:
Core power [kW] 300 200 100 0 0 0.9
Page 465 and 466:
29). As expected, it appears that t
Page 467 and 468:
ficients together with the specific
Page 469 and 470:
personnel is 12 µSv/h. However, pr
Page 471 and 472:
High-energy contribution As was sho
Page 473 and 474:
Fig. 46. Vertical cross-sectional v
Page 475 and 476:
there is a fraction of leakage neut
Page 477 and 478:
ψ∗/Ep 40 30 20 10 0 Energy gain
Page 479 and 480:
ψ∗ 40 30 20 10 ZrN matrix YN mat
Page 481 and 482:
Table 20. Proton source efficiency,
Page 483 and 484:
Fig. 56. Horizontal cross-sectional
Page 485 and 486:
Chapter 11 Abstracts of papers 11.1
Page 487 and 488:
11.5 Paper V Different reactivity d
Page 489 and 490:
source response have been investiga
Page 491 and 492:
Table A2. Production facts for oper
Page 493 and 494:
Eq. (B.5) expresses the energy prod
Page 495 and 496:
Table C1 (cont.) Neutrons Photons P
Page 497 and 498:
13 R. Soule, “Neutronic Studies i
Page 499 and 500:
45 H. A. Abderrahim, P. Kuoschus, M
Page 501 and 502:
78 F. Atchison, Proc. of a Speciali
Page 503 and 504:
108 I. Koprivnikar, E. Schachinger,
Page 505 and 506:
The basic idea of ADS is to supply
Page 507 and 508:
equilibrium (Prael, 1998) Models ar
Page 509 and 510:
two dips in the neutron fluxes caus
Page 511 and 512:
4.3 Calculations of ϕ* for the MUS
Page 513 and 514:
Instead of plotting the ratio ϕ* /
Page 515 and 516:
have already been multiplied in the
Page 517 and 518:
APPENDIX A Table 3 Material Composi
Page 519 and 520:
Definition and Application of Proto
Page 521 and 522:
is the best way to define the neutr
Page 523 and 524:
TABLE I Relative Fraction of Actini
Page 525 and 526:
compared to 0.8% for r=50 cm). When
Page 527 and 528:
Proton Source Efficiency ψ * 40 30
Page 529 and 530:
16. L. S. WATERS, “MCNPX TM User
Page 531 and 532:
314 spallation reactions. The produ
Page 533 and 534:
316 current of3.0 mA (1.9 10 13 pro
Page 535 and 536:
318 between 0.1 and 10 MeV, while m
Page 537 and 538:
320 would be very thin, only the un
Page 539 and 540:
322 Relative effective dose 1.E+01
Page 541 and 542:
324 12 mSv h 1 , which is about 15
Page 543 and 544:
326 originates from neutrons with e
Page 545 and 546:
328 [17] Internal SAD document at t
Page 547 and 548:
affecting ψ* - the macroscopic fis
Page 549 and 550:
nected to an increase in ψ*. Preli
Page 551 and 552:
fission and capture cross-sections
Page 553 and 554:
Relative fission probability, σf/(
Page 555 and 556:
F φ >=< Fφ > + < Fφ > + < Fφ >
Page 557 and 558:
tions. Three parameters - the avera
Page 559 and 560:
Nuclear Instruments and Methods in
Page 561 and 562:
fraction, beff, have been calculate
Page 563 and 564:
satisfactory statistical agreement,
Page 565 and 566:
and combining the values of a obtai
Page 567 and 568:
dominating closer to criticality, t
Page 569 and 570:
Abstract Elsevier Science 1 Journal
Page 571 and 572:
adjusted to give a keff close to 0.
Page 573 and 574:
Elsevier Science 5 f Σ Σ c Core F
Page 575 and 576:
Table 6 shows how the differences i
Page 577 and 578:
Transmutation of nuclear waste in g
Page 579 and 580:
ii Abstract The actinides in spent
Page 581 and 582:
iv VI D. Westlén, J. Cetnar and W.
Page 583 and 584:
vi MONJU Japanese experimental fast
Page 585 and 586:
viii CONTENTS 6.5 Summary of the se
Page 587 and 588:
2 CHAPTER 1. BURDENING FUTURE GENER
Page 589 and 590:
Page 591 and 592:
Page 593 and 594:
Page 595 and 596:
10 CHAPTER 2. NUCLEAR REACTIONS Fig
Page 597 and 598:
12 CHAPTER 2. NUCLEAR REACTIONS Fig
Page 599 and 600:
14 CHAPTER 3. FAST REACTORS Reactor
Page 601 and 602:
16 CHAPTER 3. FAST REACTORS reactor
Page 603 and 604:
18 CHAPTER 3. FAST REACTORS Generat
Page 605 and 606:
20 CHAPTER 3. FAST REACTORS Two ent
Page 607 and 608:
22 CHAPTER 3. FAST REACTORS a liqui
Page 609 and 610:
24 CHAPTER 4. PARTITIONING AND TRAN
Page 611 and 612:
Page 613 and 614:
Page 615 and 616:
Page 617 and 618:
Page 619 and 620:
34 CHAPTER 5. FAST SUB-CRITICAL COR
Page 621 and 622:
Page 623 and 624:
Page 625 and 626:
Page 627 and 628:
Page 629 and 630:
Page 631 and 632:
Page 633 and 634:
48 CHAPTER 6. DESIGNING A GAS-COOLE
Page 635 and 636:
Page 637 and 638:
Page 639 and 640:
Page 641 and 642:
Page 643 and 644:
Page 645 and 646:
Page 647 and 648:
Page 649 and 650:
Page 651 and 652:
Page 653 and 654:
Bibliography [1] T. Ginsburg. Die f
Page 655 and 656:
[29] G. Melese-d’Hospital. Perfor
Page 657 and 658:
[58] L.A. Lys et al. Gas turbine po
Page 659 and 660:
Acknowledgements Even though my wor
Page 661 and 662:
PROOF COPY [LY8910B] 088545PRB OLSS
Page 663 and 664:
Page 665 and 666:
Page 667 and 668:
£ ¤¥¦ §¨¨© ¡¢ ¨§¨ ¢¦
Page 669 and 670:
List of Papers I. J. Wallenius, P.
Page 671 and 672:
Chapter 1 Introduction About 16% of
Page 673 and 674:
Figure 1.1: The length and time sca
Page 675 and 676:
2.2. Primary Damage: Vacancies and
Page 677 and 678:
2.2. Primary Damage: Vacancies and
Page 679 and 680:
2.3. Primary Damage Evolution 9 the
Page 681 and 682:
2.3. Primary Damage Evolution 11 20
Page 683 and 684:
2.3. Primary Damage Evolution 13 Im
Page 685 and 686:
3.1. Ab Initio 15 The problem is ad
Page 687 and 688:
3.2. Interatomic Potentials 17 wher
Page 689 and 690:
3.2. Interatomic Potentials 19 3.2.
Page 691 and 692:
3.3. Molecular Dynamics 21 be of th
Page 693 and 694:
3.4. The Monte Carlo Method 23 sele
Page 695 and 696:
4.1. Potential Construction 25 func
Page 697 and 698:
4.2. Verification of Potentials 27
Page 699 and 700:
4.2. Verification of Potentials 29
Page 701 and 702:
4.3. Cascades Using Molecular Dynam
Page 703 and 704:
Chapter 5 Summary and Outlook Befor
Page 705 and 706:
Bibliography [1] http://www.iaea.or
Page 707 and 708:
Bibliography 37 [24] P. Olsson, J.
Page 709 and 710:
Modeling of chromium precipitation
Page 711 and 712:
MODELING OF CHROMIUM PRECIPITATION
Page 713 and 714:
Page 715 and 716:
Page 717 and 718:
Page 719 and 720:
etween EAM and FS type of potential
Page 721 and 722:
leaving other properties untouched.
Page 723 and 724:
1. Introduction Displacement cascad
Page 725 and 726:
(BCA) study [44], to correlate with
Page 727 and 728:
correspondence with the maximum num
Page 729 and 730:
however, that only above 20 keV can
Page 731 and 732:
As explained in what follows, Figs.
Page 733 and 734:
4.2 Clustered fraction While the st
Page 735 and 736:
metals, for example, it has been sh
Page 737 and 738:
Acknowledgements This work required
Page 739 and 740:
[52] W.J. Phytian, A.J.E. Foreman,
Page 741 and 742:
Table 2 - Summary of recoil energie
Page 743 and 744:
Figure captions Figure 1 - Fe-Fe pa
Page 745 and 746:
Number of FP at peak time cascade d
Page 747 and 748:
Number of sub-cascades 4 3 2 1 0 Fi
Page 749 and 750:
SIA clustered fraction Vacancy clus
Page 751 and 752:
SIA clustered fraction Vacancy clus
Page 753 and 754:
* Corresponding author, phone #: +3
Page 755 and 756:
time and the different mechanisms o
Page 757 and 758:
[35]. The use of a large distance c
Page 759 and 760:
SIA clusters have been counted both
Page 761 and 762:
and depleted in SIAs. Isolated vaca
Page 763 and 764:
Figure 3 shows the number of recomb
Page 765 and 766:
potentials predict between 30% and
Page 767 and 768:
To summarize, we expect to see the
Page 769 and 770:
properties. But while in the latter
Page 771 and 772:
[24] H.-E. Schaefer, K. Maier, M. W
Page 773 and 774:
fraction 0.5 0.4 0.3 0.2 0.1 Contri
Page 775 and 776:
Number of defects 20 15 10 5 SIA cl
Page 777 and 778:
Abstract This study is a first step
Page 779 and 780:
Abbreviations ADS Accelerator-drive
Page 781 and 782:
9 ADS and MOX Transmutation Strateg
Page 783 and 784:
Important technological assumptions
Page 785 and 786:
2 Generating nuclear power Fission
Page 787 and 788:
coolants are low neutron capture cr
Page 789 and 790:
steam-generators and other equipmen
Page 791 and 792:
3.3 Conversion At the conversion fa
Page 793 and 794:
3.5.2 Uranium oxide (UOX) The urani
Page 795 and 796:
Table 1. Main elements present in s
Page 797 and 798:
Fig. 4. Fission product yield as fu
Page 799 and 800:
corresponding radioactive decay hal
Page 801 and 802:
4 Swedish Spent Fuel Storage and Di
Page 803 and 804:
Fig. 6. Swedish nuclear waste manag
Page 805 and 806:
handling spent fuel at CLAB. It als
Page 807 and 808:
Secondly it performs an operation o
Page 809 and 810:
6 Nuclear Fuel Cycles studied in th
Page 811 and 812:
7 Advanced Nuclear Fuel Cycles sele
Page 813 and 814:
8 Characterization of the ADS Conce
Page 815 and 816: 9 ADS and MOX Transmutation Strateg
Page 817 and 818: 10.2 Scenario II - LWR + ADS Stabil
Page 819 and 820: ecycling in Scenario III resulted i
Page 821 and 822: 12 Results - Phase-Out Scenarios 12
Page 823 and 824: the time of shut-down only 7 tons o
Page 825 and 826: LWR-park which is doomed to be phas
Page 827 and 828: 22. Working Party on the Physics of
Page 829 and 830: nuclear power reactor under normal
Page 831 and 832: fission in LWRs and other reactors
Page 833 and 834: 238 U microscopic cross sections [b
Page 835 and 836: Appendix B - Transmutation of Nucle
Page 837 and 838: In a fast neutron spectrum the neut
Page 839 and 840: understood it is important to exami
Page 841 and 842: Elsevier Science 1 From Once-throug
Page 843 and 844: Phase-out Reference Scenario The ph
Page 845 and 846: varied from 1800 to 3300 [MWt] depe
Page 847 and 848: plutonium in the system 4 though, w
Page 849 and 850: Elsevier Science 1 The Subcritical
Page 851 and 852: 3. Subcritical assembly The sub-cri
Page 853 and 854: 6. Conclusion The SAD project is in
Page 855 and 856: 2 2. Key parameters of SAD and supp
Page 857 and 858: 4 Fig. 5 Distributions of the 210 P
Page 860 and 861: O FFICE PARLEMENTAIRE D ’ ÉVALUA
Page 862 and 863: Nouvelles Les recherches technologi
Page 864 and 865: OPECST,Public Hearing, January 20,
Page 868 and 869: Some pre-declarations for this talk
Page 880 and 881: Pu can be pretty efficiently (but s
Page 886: I am leaving conclusions to the Hon
show all

System and safety studies of accelerator driven transmutation ... - SKB

Create successful ePaper yourself

Delete template?

Save as template?