1 - Nuclear Sciences and Applications - IAEA

More documents

Recommendations

Info

236 KAUFMANN et al. -1 -2-- -3- + with Pellets o without Pellets 1 1 -1 -2 -1 FIG. 8. Comparison of measured and estimated TE. As the above analyses revealed electron transport to be dominating the global energy confinement a statistical investigation of the dependences of the electron temperature profile was started. Gas puff as well as pellet fuelled discharges, Ohmically heated as well as neutral beam heated discharges can be described unformly (2.5 • 10 19 m~ 3 ^ nc 1.2 • 10 20 m- 3 ,0.3 MW
IAEA-CN-50/A-IV-2 237 finement. The improvement lessens with rising heating power. The ion confinement becomes neoclassical in agreement with r7i-mode theory. Tlie global energy confinement, however, remains controlledby electron transport and is characterized by a nearly self-similar electron temperature profile. This leads to a picture where the energy confinement is nearly determined by the boundary temperature and the density profile. High-Z impurities accumulate in the centre according to neoclassical theory. REFERENCES [1] NOTERDAEME, J.-M., et al., Paper IAEA-CN-50/E-H-2, these Proceedings, Vol. 1. [2] NIEDERMEYER, H., Plasma Phys. Controll. Fusion, to be published. [3] KAUFMANN, M., et al., Nucl. Fusion 28 (1988) 827. [4] FUSSMANN, G., et al., in Plasma-Surface Interactions in Controlled Fusion Devices (Proc. 8th Int. Conf. Jiilich, 1988), and references therein. [5] GRUBER, O., et al., in Controlled Fusion and Plasma Heating (Proc. 15th Eur. Conf. Dubrovnik, 1988), Vol. 12B, Part I, European Physical Society (1988) 23.
Page 2:
The cover picture shows the inside
Page 6 and 7:
AFGHANISTAN ALBANIA ALGERIA ARGENTI
Page 8 and 9:
PLASMA PHYSICS AND CONTROLLED NUCLE
Page 10 and 11:
EDITORIAL NOTE The Proceedings have
Page 12 and 13:
A. Kaminaga, T. Kaneko, T. Kato, M.
Page 14 and 15:
Improved confinement regimes with O
Page 16 and 17:
Tokamak with strong magnetic field
Page 18 and 19:
Resonant island divertor experiment
Page 20 and 21:
Particle removal capabilities of th
Page 22 and 23:
Inside launch electron cyclotron he
Page 24 and 25:
T. Hjima, S. Ishida, K. Itami, T. I
Page 26 and 27:
T. Yamauchi, I. Nakazawa, K. Hasega
Page 29 and 30:
ARTSIMOVICH MEMORIAL LECTURE C. MAI
Page 31 and 32:
IAEA-CN-50/A-0 5 ceptible to fast r
Page 33 and 34:
IAEA-CN-50/A-0 7 fusion power plant
Page 35 and 36:
FIRST EXPERIMENTS IN TORE SUPRA EQU
Page 37 and 38:
IAEA-CN-50/A-I-1 11 Supra is the fi
Page 39 and 40:
IAEA-CN-50/A-I-1 13 poloidal field
Page 41 and 42:
nee id interfere >res an j-> 1 O E
Page 43 and 44:
i I •O OJ) — '5 c IS 2 HI 1ZI _
Page 45 and 46:
5.' ' *[Wbl t. 3. 2. 1. _ _ X IAEA-
Page 47 and 48:
nl 30 .29 .28 .27 26 .25 .24 .23 22
Page 49 and 50:
IAEA-CN-50/A-I-1 However, reasonabl
Page 51 and 52:
IAEA-CN-50/A-I-1 25 will make it po
Page 53 and 54:
IAEA-CN-50/A-I-2 AN OVERVIEW OF TFT
Page 55 and 56:
IAEA-CN-50/A-I-2 29 inner belt limi
Page 57 and 58:
IAEA-CN-50/A-I-2 31 0 10 20 TOTAL P
Page 59 and 60:
5 DC LU LU 3 - 1 - Q Q A 1 A IAEA-C
Page 61 and 62:
IAEA-CN-50/A-I-2 35 The question ar
Page 63 and 64:
0.20 0.15 0.10 Rp= 2.45 m a = 0.79
Page 65 and 66:
: . • • 1 IAEA-CN-50/A-I-2 39 1
Page 67 and 68:
LATEST JET RESULTS AND FUTURE PROSP
Page 69 and 70:
Parameter Plasma major radius (Ro)
Page 71 and 72:
1500 IAEA-CN-50/A-I-3 45 2 4 I, (MA
Page 73 and 74:
IAEA-CN-50/A-I-3 47 3.0 3.5 Major r
Page 75 and 76:
I 15 10 5 0 IAEA-CN-50/A-I-3 49 V \
Page 77 and 78:
IAEA-CN-50/A-I-3 51 Magnetic measur
Page 79 and 80:
0.8 0.6 IAEA-CN-50/A-I-3 53 -0.2 12
Page 81 and 82:
10 0.5 Pulse No: 15376 n(He')/ne=1.
Page 83 and 84:
IAEA-CN-50/A-I-3 57 5 10 15 [Pt-dW/
Page 85 and 86:
10 E X 4 H-mode y 0.2 0.4 0.6 0.8 1
Page 87 and 88:
IAEA-CN-50/A-I-3 61 where V is the
Page 89 and 90:
IAEA-CN-50/A-I-3 63 confinement deg
Page 91:
IAEA-CN-50/A-I-3 65 References [1 ]
Page 94 and 95:
68 JT-60 TEAM T. TANAKA, Y. TANAKA,
Page 96 and 97:
Ip = 3.2 MA lp = 2.7 MA JT-60TEAM R
Page 98 and 99:
72 JT-60TEAM E5695 0 1 2 3 4 5 6 7
Page 100 and 101:
74 JT-60TEAM 3 : LIH *3.1HA 2.8HA A
Page 102 and 103:
76 JT-60TEAM 4.5 5.0 5.5 6.0 6.5 7.
Page 104 and 105:
78 JT-60TEAM 250 "(a) 200 150 50 n
Page 106 and 107:
80 JT-60 TEAM The further developme
Page 109 and 110:
STABILITY OF HIGH BETA DISCHARGES I
Page 111 and 112:
IAEA-CN-50/A-II-l 85 a typical plas
Page 113 and 114:
0.5- 0- 0.8- 0.4- 0.0- IAEA-CN-50/A
Page 115 and 116:
IAEA-CN-50/A-IM 89 absence of the l
Page 117 and 118:
s.o • .5 (a) IAEA-CN-50/A-II-l 91
Page 119 and 120:
IAEA-CN-50/A-II-l 93 stability limi
Page 121:
IAEA-CN-50/A-II-l 95 [6] STAMBAUGH,
Page 124 and 125:
98 OKABAYASHI et al. PBX-M maximall
Page 126 and 127:
100 1 .0 .6 .0 -.2 -.4 -.6 1.11 CO
Page 128 and 129:
102 0.5 OKABAYASHI et al. Indentati
Page 130 and 131:
104 OKABAYASHI et al. 40 30 I I I I
Page 132 and 133:
106 OKABAYASHI et al. §1 •a J i
Page 134 and 135:
108 OKABAYASHI et al. -2 1 • •
Page 137 and 138:
MHD ACTIVITIES AND RELATED IMPURITY
Page 139 and 140:
0.5 IAEA-CN-50/A-H-3 113 FIG. 1. St
Page 141 and 142:
0) a. II E IAEA-CN-50/A-H-3 115 1 1
Page 143 and 144:
IAEA-CN-50/A-II-3 117 These observa
Page 145:
6. CONCLUSIONS IAEA-CN-50/A-II-3 11
Page 148 and 149:
122 GAO et al. With hydrogen plasma
Page 150 and 151:
124 GAO et al. P—3.0 r—8.5 SHOT
Page 152 and 153:
126 GAO et al. a) M >
Page 154 and 155:
128 GAO et al. 0.6 0.3 0.0 50 100 r
Page 157 and 158:
SUPERLOW DENSITY EXPERIMENT ON HT-6
Page 159 and 160:
IAEA-CN-50/A-n-S-l 133 (b) Hard X-r
Page 161 and 162:
IAEA-CN-SO/A-n-5-l 135 0 0.2 0.4 0:
Page 163 and 164:
IAEA-CN-50/A-D-5-2 INVESTIGATION OF
Page 165 and 166:
0.14 0.10 0.09 0.08 0.05 0.04 0.03
Page 167 and 168:
TABLE I. REDUCTION OF Xe (m 2 -s')
Page 169:
IAEA-CN-50/A-II-5-2 143 (3) The lin
Page 172 and 173:
146 FUSSMANN et al. Abstract IMPROV
Page 174 and 175:
148 FUSSMANN et al. 150- 100- 50- 0
Page 176 and 177:
150 FUSSMANN et al. UJ 100- 50- + 2
Page 178 and 179:
152 FUSSMANN et al. In both regimes
Page 180 and 181:
154 FUSSMANN et al. reduced. With c
Page 182 and 183:
156 FUSSMANN et al. and consequentl
Page 185 and 186:
THE JET H-MODE AT HIGH CURRENT AND
Page 187 and 188:
IAEA-CN-50/A-IH-2 achieve an H-mode
Page 189 and 190:
6.0 40 2.0 (a) 0l=. 5.0 (c) 0 Pulse
Page 191 and 192:
IAEA-CN-50/A-III-2 165 reduced in t
Page 193 and 194:
IAEA-CN-50/A-HI-2 167 near the firs
Page 195 and 196:
IAEA-CN-50/A-III-2 169 plasmas with
Page 197 and 198:
I 3s H-mode 8
Page 199 and 200:
IAEA-CN-50/A-HI-2 173 The steep tem
Page 201 and 202:
IAEA-CN-50/A-III-2 175 available),
Page 203 and 204:
IAEA-CN-50/A-III-2 177 (xi0 19 m 3
Page 205 and 206:
IAEA-CN-50/A-III-2 179 APPENDIX I T
Page 207:
IAEA-CN-50/A-IH-2 181 [16] Bishop,
Page 210 and 211:
184 ZARNSTORFT et al. Abstract TRAN
Page 212 and 213: 186 ZARNSTORFF et al. X-ray spectro
Page 214 and 215: 188 ZARNSTORFF et al. 8 CM e CM E 2
Page 216 and 217: 190 ZARNSTORFF et al. 1.5 2.0 2.5 n
Page 219 and 220: IAEA-CN-50/A-III-4 ENERGY CONFINEME
Page 221 and 222: o O •
Page 223 and 224: 0.3 0.2- 0.1- 0.0 0.8 0.6 0.4 0.2 0
Page 225 and 226: 00 d f CM I- CQ i o o o IAEA-CN-50/
Page 227 and 228: E m F LU LJU Z o N_ CE UU o / UJ q
Page 229 and 230: IAEA-CN-50/A-m-4 203 The TB values
Page 231: IAEA-CN-50/A-HM 205 [7] OHYABU, N.,
Page 234 and 235: 208 SUZUKI et al. favourable in a c
Page 236 and 237: 210 SUZUKI etal. As the neutral bea
Page 238 and 239: 212 SUZUKI et al. 3. FOUR-PELLET IN
Page 241 and 242: HEATING OF PEAKED DENSITY PROFILES
Page 243 and 244: Yd o g a> - c 4 _n ...— 0) n 12 t
Page 245 and 246: 1.3 I" 1 |03 C 0.5 i: 12 8 4 n - Te
Page 247 and 248: IAEA-CN-50/A-IV-l 221 1 2 3 Q,_-2ff
Page 249 and 250: 2 q(o) 1- 10 1 U • O • IAEA-CN-
Page 251 and 252: 0.3 f0.2 1 5" 0.1 IAEA-CN-50/A-IV-l
Page 253 and 254: IAEA-CN-50/A-IV-l 227 APPENDIX I TH
Page 255 and 256: IAEA-CN-50/A-IV-2 PELLET INJECTION
Page 257 and 258: 3 - 2 - 1 - IAEA-CN-50/A-IV-2 231 1
Page 259 and 260: 0 FIG. 4. ONI O £ at o ID c IC 15
Page 261: IAEA-CN-50/A-IV-2 0.35 MW 2.6 MW Ga
Page 266 and 267: 240 AZIZOV et al. TABLE I. TSP PARA
Page 268 and 269: 242 AZIZOV et al. 65 75 85 95 105 1
Page 270 and 271: 244 AZIZOV et al. 30 40 50 60 Ip =
Page 273 and 274: HIGH TEMPERATURE EXPERIMENTS AND FU
Page 275 and 276: IAEA-CN-50/A-IV-4 249 FIG. 1. Data
Page 277 and 278: P ICRHV 2 IAEA-CN-50/A-IV-4 251 FIG
Page 279 and 280: IAEA-CN-SO/AIV-4 253 FIG. 4. (a) Di
Page 281: IAEA-CN-50/A-IV-4 255 The fusion pe
Page 284 and 285: 258 STRACHAN et al. - Z - 1, Steady
Page 286 and 287: 260 STRACHAN et al. 10' 10' Classic
Page 288 and 289: 262 STRACHAN et al. _ 1 s 10* I : 1
Page 291 and 292: ENERGY CONFINEMENT WITH AUXILIARY H
Page 293 and 294: E6950(Bi=4.0T) E6956(Bt = 2.7T) °4
Page 295 and 296: E7558 • IMPROVED 5 6 TIME (S) IAE
Page 297 and 298: 7.0 E - 1 0.0 7.0 0.0 =— \ n; - T
Page 299: IAEA-CN-50/A-V-1 273 [9] SHIMOMURA,
Page 302 and 303: 276 ASHRAF et al. However, the conv
Page 304 and 305: 278
Page 306 and 307: 280 ASHRAF et al. Modulation amplit
Page 308 and 309: 282 KIMet al. (a) (b) 410 420 TIME
Page 310 and 311: 284 KIM et al. (b) o 3
Page 312 and 313:
286 KIM et ah In summary, we observ
Page 314 and 315:
288 KAWAHATA et al. TEXT tokamak, t
Page 316 and 317:
290 KAWAHATA et al. ^ 30 °- S-200.
Page 318 and 319:
292 KAWAHATA et al. 0 6 12 18 24 ra
Page 320 and 321:
294 WOOTTON et al. 1. Particle tran
Page 322 and 323:
296 10' N 10° E gio- 1 O (a) 10" 0
Page 324 and 325:
298 WOOTTON et al. ne=3xl0 19 m- 3
Page 326 and 327:
300 ZURRO et al. FIG. 1. Variation
Page 328 and 329:
302 ZURRO et al. Mo) 6 (10"cm- 3 )
Page 330 and 331:
304 ZURRO et al. -140 50 100 f(kHz)
Page 333 and 334:
TRANSPORT STUDIES ON TFTR UTILIZING
Page 335 and 336:
IAEA-CN-50/A-V-4 309 uses the TRANS
Page 337 and 338:
5 g 30 20 < 2.0 Q § 1.0 i 0.5 10 1
Page 339 and 340:
IAEA-CN-50/A-V-4 313 the laser-blow
Page 341 and 342:
IAEA-CN-S0/A-V-4 315 on working gas
Page 343 and 344:
I0 7 ! 10' 1.8 IAEA-CN-50/A-V-4 317
Page 345 and 346:
IAEA-CN-50/A-V-4 319 The difference
Page 347:
IAEA-CN-50/A-V-4 321 [12] RADEZTSKY
Page 350 and 351:
324 DONNE et al. E CO o FIG. 1. Sho
Page 352 and 353:
326 DONNE et al. 350 300 250 200 15
Page 354 and 355:
328 DONNE et al. 1.0 0.8 - 0.6 - t
Page 357 and 358:
RECENT TEXTOR RESULTS TEXTOR TEAM (
Page 359 and 360:
IAEA-CN-50/A-VI-l 333 line-radiatio
Page 361 and 362:
IAEA-CN-50/A-VI-l 335 These measure
Page 363 and 364:
q(r] 3- 2- 1- - IAEA-CN-50/A-VI-l 3
Page 365 and 366:
IAEA-CN-50/A-VI-l 339 FIG. 4. Sawto
Page 367 and 368:
IAEA-CN-S0/A-VI-2-1 RESONANT ISLAND
Page 369 and 370:
IAEA-CN-50/A-VI-2-1 343 • «• >
Page 371:
IAEA-CN-50/A-VI-2-1 345 tons. This
Page 374 and 375:
348 EVANS et al. JIPP T-IIU ( minor
Page 376 and 377:
350 EVANS et al. FIG. 3. High speed
Page 378 and 379:
352 EVANS et al. REFERENCES [1] KAR
Page 380 and 381:
354 BAKOS et al. The radiation of t
Page 382 and 383:
356 BAKOS et al. < + s 5 2 1 5 2 10
Page 384 and 385:
358 BAKOS et al. REFERENCES [1] BAK
Page 386 and 387:
360 STfiCKEL et al. A quantitative
Page 388 and 389:
362 STOCKEL et al. This and other f
Page 390 and 391:
364 STOCKEL et al. 15 I 10 "" 5 0 (
Page 393 and 394:
GLOBAL POWER BALANCE AND LOCAL HEAT
Page 395 and 396:
0.5 1 r. (s> Goldston IAEA-CN-50/A-
Page 397 and 398:
IAEA-CN-50/A-VH-l 371 Separate Elec
Page 399 and 400:
IAEA-CN-50/A-VII-l 373 4. SIMULATIO
Page 401 and 402:
6. CONCLUSIONS IAEA-CN-50/A-VII-l 3
Page 403 and 404:
SAWTOOTH ACTIVITY AND CURRENT DENSI
Page 405 and 406:
-0.6 (keV) 6.6 6.4 6.2 6.0 5.8 IAEA
Page 407 and 408:
IAEA-CN-50/A-VII-2 381 #15697 . 0 1
Page 409 and 410:
IAEA-CN-50/A-VII-2 383 radius. In a
Page 411:
IAEA-CN-50/A-VH-2 385 [11] Goldston
Page 414 and 415:
388 NAGAYAMA et al. of the magnetic
Page 416 and 417:
390 NAGAYAMA et al. RECONNECTION RE
Page 418 and 419:
392 NAGAYAMA et al. m/n=2/1 island
Page 421 and 422:
STABILITY OF TFTR PLASMAS IAEA-CN-5
Page 423 and 424:
IAEA-CN-50/A-VII-4 397 the electron
Page 425 and 426:
9 8 — 7 6 5 4 - 3 2 X • * • i
Page 427 and 428:
0.5 ' 0.4 0.3 - 3 0.2 0.1 - 0 —r"
Page 429 and 430:
0.4 0.3 0.2 0.1 n IAEA-CN-50/A-VH-4
Page 431 and 432:
Ip(MA) 0.85 0.89 0.9 0.9 1.4 IAEA-C
Page 433:
IAEA-CN-50/A-VH-4 407 ACKNOWLEDGMEN
Page 436 and 437:
410 AGIM et al. , , , , I , , , .,
Page 438 and 439:
412 AGIM et al. to diminish and the
Page 440 and 441:
414 AGIM et al. Hence, the preventi
Page 442 and 443:
416 MAUELetal. Small tokamak plasma
Page 444 and 445:
418 MAUELetal. 3. Mode structure of
Page 446 and 447:
420 100- 350 MAUEL et al. RAOIUS (c
Page 449 and 450:
STUDY OF PLASMA MHD STABILITY IN T-
Page 451 and 452:
1.5 _ 1.0 >
Page 453 and 454:
20 £ 15 - " 10 II 5 5 — ECH IAEA
Page 455 and 456:
200 - IAEA-CN-S0/A-Vn-7 429 I I I I
Page 457 and 458:
60 40 20 n / l IAEA-CN-S0/A-VII-7 4
Page 459 and 460:
LU 30 - 20 - 10 - IAEA-CN-50/A-V1I-
Page 461 and 462:
as if 200 - 100 -- 20 - I 10 - 15
Page 463 and 464:
RELAXATION OF q PROFILE IN A HIGH B
Page 465 and 466:
0 0.5 1.0 IAEA-CN-50/A-VII-8 439 .
Page 467 and 468:
0 6 12 (Wall) r(cm) IAEA-CN-50/A-VH
Page 469:
5. CONCLUSIONS IAEA-CN-50/A-VH-8 44
Page 472 and 473:
446 HENDERetal. An alternative meth
Page 474 and 475:
448 HENDER et al. and Jdriven(max)
Page 476 and 477:
450 HENDER et al. TJ :? Island V 6
Page 479 and 480:
IAEA-CN-50/A-VII-10 PARTICLE REMOVA
Page 481 and 482:
IAEA-CN-50/A-VH-10 455 3. POLOIDAL
Page 483 and 484:
X > o S 6 U- 2- 0 160 • 80 0 1 0.
Page 485 and 486:
IAEA-CN-S0/A-VH-10 459 between scoo
Page 487 and 488:
THE ROLE OF LIMITERS AND WALLS IN I
Page 489 and 490:
Shine through IAEA-CN-50/A-VH-ll 46
Page 491 and 492:
3 01 £ "c t=! o E c 12 10 8 6 4 2
Page 493 and 494:
THE PLASMA BOUNDARY IN JET IAEA-CN-
Page 495 and 496:
o x CO o 3.0 2.0 .2-0.5 'in c 0.3 1
Page 497 and 498:
1 10" IAEA-CN-50/A-VI1-12 LCFS LCFS
Page 499 and 500:
o •£ 0.15 'o = 0.05 C O J3 o 0.0
Page 501:
IAEA-CN-50/A-VIM2 475 densities, bu
Page 504 and 505:
478 LEONOV et al. 2. INSTALLATION A
Page 506 and 507:
480 LEONOV et al. &r (cm) 0.2 -0.2
Page 508 and 509:
482 LEONOV et al. Uo, at constant p
Page 510 and 511:
484 CHEETHAM et al. We present simu
Page 512 and 513:
486 CHEETHAM et al. 0 20 40 60 30 1
Page 514 and 515:
488 CHEETHAM et al. o LU 3.0 2.8
Page 516 and 517:
490 CHEETHAM et al. sior CO 111 c o
Page 518 and 519:
492 CHEETHAM et al. reported from o
Page 521 and 522:
IAEA-CN-S0/A-Vn-15 EXPERIMENTAL RES
Page 523 and 524:
IAEA-CN-50/A-VII-15 497 800 (a) _ -
Page 525 and 526:
IAEA-CN-50/A-VII-15 499 formation.
Page 527 and 528:
300 4X10' 3 - IAEA-CN-50/A-VII-15 5
Page 529:
CONCLUSION IAEA-CN-50/A-VU-1S 503 W
Page 532 and 533:
506 KIKUCH1 et al. 1. INTRODUCTION
Page 534 and 535:
508 KIKUCHI et al. 1.0 o.s 1 — -
Page 536 and 537:
510 KIKUCHIetal. REFERENCES [1] ZAR
Page 539 and 540:
STUDY OF DENSITY LIMIT AND LOW q(aL
Page 541 and 542:
IAEA-CN-50/E-I-l-l 515 1 2 3 4 5 ne
Page 543 and 544:
/ / IAEA-CN-50/E-I-l-l 517 / / / /
Page 545 and 546:
(J n 3 o ? 2 i o ' 1 IAEA-CN-50/E-M
Page 547 and 548:
0.03 - 0.02 - 0.01 - IAEA-CN-50/E-I
Page 549 and 550:
CO u CO "o IC 7 - 6 — 5 - 4 - 3 1
Page 551:
IAEA-CN-50/E-I-l-l REFERENCES 52 5
Page 554 and 555:
528 PRATER et al. 1. INTRODUCTION E
Page 556 and 557:
530 PRATER et al. 0.8 0.6 0.4 0.2 n
Page 558 and 559:
532 PRATER et al. 1.5 x 10 19 m~ 3
Page 560 and 561:
534 PRATER et al. 10 1 0.75 0.25 0.
Page 562 and 563:
536 PRATER et al. added to 1.25 MW
Page 564 and 565:
538 PRATER et al. 2.0 1.5 1.0 0.5 /
Page 567 and 568:
INSIDE LAUNCH ELECTRON CYCLOTRON HE
Page 569 and 570:
0-20 0-15 a CO. 0-10 0-05 0-0 5S g.
Page 571 and 572:
IAEA-CN-50/E-I-3 545 0.25 • (a) 1
Page 573 and 574:
IAEA-CN-50/E-I-3 547 A/3 deduced fr
Page 575:
IAEA-CN-50/E-I-3 549 ECRH phases as
Page 578 and 579:
552 MOTOJIMA et al. ICRF and plasma
Page 580 and 581:
554 MOTOJIMA et al. (a) 0.6SneS0.9x
Page 582 and 583:
556 MOTOJIMA et al. 0 20 W 60 80 10
Page 584 and 585:
558 5 4 3 2 1 0 60 40 20 0 la) cuto
Page 586 and 587:
560 MOTOJIMA et al. 3 0.005 0 0.2 0
Page 589 and 590:
RF CURRENT DRIVE AND MHD INSTABILIT
Page 591 and 592:
IAEA-CN-50/E-I-5 565 80 PEC
Page 593 and 594:
of x o o i L_ t IAEA-CN-50/E-I-5 56
Page 595 and 596:
IAEA-CN-50/E-I-5 569 FIG. 5. Contou
Page 597 and 598:
HEATING AND CONFINEMENT STUDIES WIT
Page 599 and 600:
R 6 IAEA-CN-50/E-IM 0.5 10 1.5 Ne(r
Page 601 and 602:
IAEA-CN-50/E-II-l FIG. 3. Total rad
Page 603 and 604:
IAEA-CN-50/E-II-l 577 1.0 2.0 Time
Page 605 and 606:
IAEA-CN-50/E-II-l 579 TABLE I. SUMM
Page 607 and 608:
6. SAWTOOTH BEHAVIOUR IAEA-CN-50/E-
Page 609 and 610:
IAEA-CN-50/E-II-2 LONG PULSE HIGH P
Page 611 and 612:
IAEA-CN-50/E-II-2 585 23996 2 3 0 U
Page 613 and 614:
IAEA-CN-50/E-II-2 587 TABLE I. a) C
Page 615 and 616:
t a ce> 03 E cs o. otal 100 90 80 7
Page 617 and 618:
IAEA-CN-50/E-H-2 591 and confinemen
Page 619 and 620:
IAEA-CN-50/E-n-3 EXPERIMENTAL AND T
Page 621 and 622:
§ 1PUTUDE ( $ #•14613 200 (a) 18
Page 623 and 624:
IAEA-CN-50/E-II-3 597 The results o
Page 625 and 626:
to V. (a)' • \ \ \ \ \ \ w \'\ \\
Page 627 and 628:
IAEA-CN-50/E-II-3 601 cccurs progre
Page 629:
IAEA-CN-50/E-II-3 603 [5] CAMPBELL,
Page 632 and 633:
606 FUJII et al. 1. INTRODUCTION Se
Page 634 and 635:
608 140 " (0,0) PIC= l~ 3 MW 120 '
Page 636 and 637:
610 FUJII et al. ACKNOWLEDGEMENTS T
Page 638 and 639:
612 BATCHELOR et al. resolves this
Page 640 and 641:
614 BATCHELOR et al. •J5 1
Page 642 and 643:
616 BATCHELOR et al. to match asymp
Page 644 and 645:
618 BATCHELOR et al. of T, R, and C
Page 646 and 647:
620 BATCHELOR et al. [3] SMITHE, D.
Page 648 and 649:
622 USHIGUSA et al. 1. INTRODUCTION
Page 650 and 651:
624 USHIGUSA et al. at f = 1.74 GHz
Page 652 and 653:
626 USHIGUSA et al. BT (T) (ms) ao
Page 654 and 655:
628 USHIGUSA et al. [2] JT-60 TEAM,
Page 656 and 657:
630 ITOH et al. , Breakdown 20 40 6
Page 658 and 659:
632 ITOH et al. 1.0 20 30 40 50 60
Page 660 and 661:
634 ITOH et al. 30 |20 a "" 10 n H=
Page 662 and 663:
636 ITOH et al. REFERENCES [1] ITOH
Page 664 and 665:
638 ALLADIO et al. generation of hi
Page 666 and 667:
640 ALLADIO et al. 4 T (keV) 3 2 -
Page 668 and 669:
642 ALLADIO et al. 3 ID 10 2 10' 10
Page 671 and 672:
IAEA-CN-50/E-ID-4 LOWER HYBRID WAVE
Page 673 and 674:
1000 - 500 1001— o — 2 35 IAEA-
Page 675 and 676:
10 10* 10 10 IAEA-CN-50/E-HI-4 649
Page 677 and 678:
IAEA-CN-50/E-III-4 651 density of t
Page 679 and 680:
IAEA-CN-50/E-IU-4 653 I I I I I I F
Page 681 and 682:
CURRENT DRIVE AND CONFINEMENT OF AN
Page 683 and 684:
1.0 -0.5 o - - 4.0 IAEA-CN-50/E-III
Page 685 and 686:
IAEA-CN-50/E-III-5 659 TABLE I. SUM
Page 687 and 688:
IAEA-CN-SO/E-in-S 661 0.4 RADIUS (m
Page 689 and 690:
10' Convection Dominates IAEA-CN-50
Page 691 and 692:
IAEA-CN-50/E-III-5 665 versus unbal
Page 693:
IAEA-CN-50/E-III-5 667 [11] ZARNSTO
Page 696 and 697:
670 SIMONEN et al. Neutral beam cur
Page 698 and 699:
672 SIMONEN et al. 1.6 2.0 FIG. 3.
Page 700 and 701:
674 SIMONEN et al. MHD modes, obser
Page 702 and 703:
676 SIMONEN et al. toroidal drift o
Page 704 and 705:
678 SIMONEN et al. occurs near the
Page 707 and 708:
NEW CURRENT DRIVE AND CONFINEMENT T
Page 709 and 710:
IAEA-CN-50/E-III-7 683 is typically
Page 711 and 712:
IAEA-CN-S0/E-III-7 685 plasma beta
Page 713 and 714:
IAEA-CN-50/E-III-7 687 The equilibr
Page 715:
IAEA-CN-50/E-III-7 689 [8] McGUIRE,
Page 718 and 719:
692 100 a 10- 0.1 WILSON et al. •
Page 720 and 721:
694 WILSON et al. 3. Plasma Heating
Page 722 and 723:
696 WILSON et al. I 3 i - • / Tim
Page 725 and 726:
INVESTIGATION OF ICRH ON THE TUMAN-
Page 727 and 728:
~x o X •9to 12 1 11 10 180 s - 12
Page 729 and 730:
400 - 300 - 200 - I 100 - 35 / 1 ,
Page 731 and 732:
5 - IAEA-CN-50/E-IV-2 r (cm) FIG. 7
Page 733 and 734:
IAEA-CN-50/E-IV-3 CONVERSION AND CY
Page 735 and 736:
IAEA-CN-50/E-IV-3 709 bution, e(j,
Page 737 and 738:
IAEA-CN-S0/E-IV-3 711 FIG. 3. kxPd
Page 739 and 740:
IAEA-CN-50/E-IV-3 713 3. NON-LOCAL
Page 741 and 742:
x exp | ds" ' u ' x -oosgn u d fiV2
Page 743 and 744:
IAEA-CN-50/E-IV-3 717 x If {sin i [
Page 745:
IAEA-CN-5O/E-IV-3 719 2. A non-loca
Page 748 and 749:
722 MOREAU et al. =t _» Here, K is
Page 750 and 751:
724 MOREAU et al. FIG. 1. Modulus o
Page 752 and 753:
726 MOREAU et al. REFERENCES [1] MA
Page 754 and 755:
728 YASAKA et al. 2. EFFICIENT PLAS
Page 756 and 757:
730 YASAKA et al. '£ 1 0.5 0 4 Pne
Page 758 and 759:
732 YASAKA et al. WT-3 1 2 Q,f C 10
Page 760 and 761:
734 invi p o p p •^ CJ -^ o IO o
Page 762 and 763:
736 YAMAMOTO et al. (A) OJ — o (A
Page 764 and 765:
738 YAMAMOTO et al. of Tsx =1.5 keV
Page 766 and 767:
740 PEREVERZEV current drive produc
Page 768 and 769:
742 PEREVERZEV 300 - - 150 ne (10 1
Page 770 and 771:
744 PEREVERZEV 0.2- -0.2- 0.1X10 19
Page 772 and 773:
746 PEREVERZEV The dependences of l
Page 774 and 775:
748 PORKOLAB et al. ASPECT RATIO FI
Page 776 and 777:
750 PORKOLAB et al. 1.0 _, 0.8 1 0.
Page 778 and 779:
752 PORKOLAB et al. X D E o Q_ 1.8
Page 780 and 781:
754 LUO et al. - o £ 3 §. II Ml "
Page 782 and 783:
756 LUO et al. 20 10 ATe ( 1 m11 1
Page 785 and 786:
IAEA-CN-50/E-IV-10 MICROWAVE HEATIN
Page 787 and 788:
n MCPAT _ Analysis IAEA-CN-50/E-IV-
Page 789 and 790:
IAEA-CN-50/E-IV-10 763 3. QUASI-LIN
Page 791 and 792:
IAEA-CN-50/E-IV-10 765 In the limit
Page 793 and 794:
IAEA-CN-50/E-IV-ll SECOND ELECTRON
Page 795 and 796:
IAEA-CN-50/E-IV-ll 769 FIG. ]. Real
Page 797 and 798:
-0.2 IAEA-CN-50/E-IV-ll 771 FIG. 3.
Page 799:
IAEA-CN-50/E-IV-ll 773 gests that i
Page 802:
HOW TO ORDER IAEA PUBLICATIONS An e
show all

1 - Nuclear Sciences and Applications - IAEA

Create successful ePaper yourself

Delete template?

Save as template?