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Overview of the JET results with the ITER-like wall

F Romanelli, I Abel, V Afanesyev, M Aftanas, G Agarici, KM Aggarwal, L Aho-Mantila, E Ahonen, M Aints, M Airila, et al. (2013) NUCLEAR FUSION. 53(10).
abstract
Following the completion in May 2011 of the shutdown for the installation of the beryllium wall and the tungsten divertor, the first set of JET campaigns have addressed the investigation of the retention properties and the development of operational scenarios with the new plasma-facing materials. The large reduction in the carbon content (more than a factor ten) led to a much lower Z(eff) (1.2-1.4) during L- and H-mode plasmas, and radiation during the burn-through phase of the plasma initiation with the consequence that breakdown failures are almost absent. Gas balance experiments have shown that the fuel retention rate with the new wall is substantially reduced with respect to the C wall. The re-establishment of the baseline H-mode and hybrid scenarios compatible with the new wall has required an optimization of the control of metallic impurity sources and heat loads. Stable type-I ELMy H-mode regimes with H-98,H-y2 close to 1 and beta(N) similar to 1.6 have been achieved using gas injection. ELM frequency is a key factor for the control of the metallic impurity accumulation. Pedestal temperatures tend to be lower with the new wall, leading to reduced confinement, but nitrogen seeding restores high pedestal temperatures and confinement. Compared with the carbon wall, major disruptions with the new wall show a lower radiated power and a slower current quench. The higher heat loads on Be wall plasma-facing components due to lower radiation made the routine use of massive gas injection for disruption mitigation essential.
Please use this url to cite or link to this publication:
author
organization
year
type
journalArticle (original)
publication status
published
subject
keyword
DIVERTOR, REGIME, TUNGSTEN, TOKAMAK PLASMAS, PLASMA-FACING COMPONENTS, PERFORMANCE
journal title
NUCLEAR FUSION
Nucl. Fusion
volume
53
issue
10
article number
104002
pages
19 pages
Web of Science type
Article
Web of Science id
000325005600003
JCR category
PHYSICS, FLUIDS & PLASMAS
JCR impact factor
3.243 (2013)
JCR rank
3/31 (2013)
JCR quartile
1 (2013)
ISSN
0029-5515
DOI
10.1088/0029-5515/53/10/104002
language
English
UGent publication?
yes
classification
A1
copyright statement
I have transferred the copyright for this publication to the publisher
id
5648201
handle
http://hdl.handle.net/1854/LU-5648201
date created
2014-07-10 21:01:00
date last changed
2016-12-21 15:41:20
@article{5648201,
  abstract     = {Following the completion in May 2011 of the shutdown for the installation of the beryllium wall and the tungsten divertor, the first set of JET campaigns have addressed the investigation of the retention properties and the development of operational scenarios with the new plasma-facing materials. The large reduction in the carbon content (more than a factor ten) led to a much lower Z(eff) (1.2-1.4) during L- and H-mode plasmas, and radiation during the burn-through phase of the plasma initiation with the consequence that breakdown failures are almost absent. Gas balance experiments have shown that the fuel retention rate with the new wall is substantially reduced with respect to the C wall. The re-establishment of the baseline H-mode and hybrid scenarios compatible with the new wall has required an optimization of the control of metallic impurity sources and heat loads. Stable type-I ELMy H-mode regimes with H-98,H-y2 close to 1 and beta(N) similar to 1.6 have been achieved using gas injection. ELM frequency is a key factor for the control of the metallic impurity accumulation. Pedestal temperatures tend to be lower with the new wall, leading to reduced confinement, but nitrogen seeding restores high pedestal temperatures and confinement. Compared with the carbon wall, major disruptions with the new wall show a lower radiated power and a slower current quench. The higher heat loads on Be wall plasma-facing components due to lower radiation made the routine use of massive gas injection for disruption mitigation essential.},
  articleno    = {104002},
  author       = {Romanelli, F and Abel, I and Afanesyev, V and Aftanas, M and Agarici, G and Aggarwal, KM and Aho-Mantila, L and Ahonen, E and Aints, M and Airila, M and Akers, R and Alarcon, T and Albanese, R and Alexeev, A and Alfier, A and Allan, P and Almaviva, S and Alonso, A and Alper, B and Altmann, H and Alves, D and Ambrosino, G and Amosov, V and Andersson, F and Sunden, EA and Andreev, V and Andrew, Y and Angelone, M and Anghel, M and Anghel, A and Angioni, C and Apruzzese, G and Arcis, N and Arena, P and Argouarch, A and Ariola, M and Armitano, A and Arnoux, G and Arshad, S and Artaserse, G and Artaud, JF and Ash, A and Asp, E and Asunta, O and Atanasiu, CV and Atkins, G and Avotina, L and Axton, MD and Ayres, C and Baciero, A and Bailescu, V and Baiocchi, B and Baker, RA and Balboa, I and Balden, M and Balorin, C and Balshaw, N and Banks, JW and Baranov, YF and Barbier, D and Barlow, IL and Barnard, MA and Barnsley, R and Barrena, L and Barrera, L and Baruzzo, M and 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and Mironov, M and Mitteau, R and Mlynar, J and Mollard, P and Monakhov, I and Monier-Garbet, P and Mooney, R and Moreau, D and Moreau, P and Moreira, L and Morgan, A and Morgan, PD and Morlock, C and Morris, AW and Mort, GL and Murakami, M and Murari, A and Mustata, I and Nabais, F and Nakano, T and Nardon, E and Nash, G and Naulin, V and Nave, MFF and Nazikian, R and Nedzelski, I and Negus, CR and Neilson, JD and Nemtsev, G and Neto, A and Neu, R and Neubauer, O and Newbert, GJ and Newman, M and Nicholls, KJ and Nicolai, A and Nicolas, L and Nieckchen, P and Nielsen, AH and Nielsen, SK and Nielsen, P and Nielsen, G and Nieto, J and Nightingale, MPS and Nishijima, D and Noble, C and Nocente, M and Nordman, H and Norman, M and Nowak, S and Nunes, I and Oberkofler, M and Odstrcil, M and O'Gorman, T and Ohsako, T and Okabayashi, M and Olariu, S and Oleynikov, A and O'Mullane, M and Ongena, J and Orsitto, F and Oswuigwe, OI and Ottaviani, M and Oyama, N and Pacella, D and Paget, K and Pajuste, E and Palazzo, S and Palenic, J and Pamela, J and Pamela, S and Pangione, L and Panin, A and Panja, S and Pankin, A and Pantea, A and Parail, V and Paris, P and Parisot, T and Park, M and Parkin, A and Parsloe, A and Parsons, BT and Pasqualotto, R and Pastor, P and Paterson, R and Paul, MK and Peach, D and Pearce, RJH and Pearson, BJ and Pearson, IJ and Pedrick, LC and Pedrosa, MA and Pegourie, B and Pereira, R and Pereslavtsev, P and Perevezentsev, A and von Thun, CP and Pericoli-Ridolfini, V and Perona, A and Perrot, Y and Peruzzo, S and Peschanyy, S and Petravich, G and Petrizzi, L and Petrov, V and Petrzilka, V and Philipps, V and Piccolo, F and Pietropaolo, A and Pillon, M and Pinches, SD and Pinna, T and Pintsuk, G and Piovesan, P and Pironti, A and Pisano, F and Pitts, R and Plaum, B and Plyusnin, V and Polasik, M and Poli, FM and Pomaro, N and Pompilian, O and Poncet, L and Pool, PJ and Popovichev, S and Porcelli, F and Porfiri, MT and Portafaix, C and Pospieszczyk, A 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and Theis, JM and Thomas, JD and Thomas, PD and Thomas, PR and Thompson, VK and Thomser, C and Thyagaraja, A and Tigwell, PA and Tiseanu, I and Tivey, R and Todd, JM and Todd, TN and Tokar, MZ and Tosti, S and Trabuc, P and Travere, JM and Trimble, P and Trkov, A and Trukhina, E and Tsalas, M and Tsitrone, E and Jun, DT and Tudisco, O and Tugarinov, S and Turner, MM and Tyrrell, SGJ and Umeda, N and Unterberg, B and Urano, H and Urquhart, AJ and Uytdenhouwen, I and Vaccaro, A and Vadgama, AP and Vagliasindi, G and Valcarcel, D and Valisa, M and Vallory, J and Valovic, M and Van Eester, D and van Milligen, B and van Rooij, GJ and Varandas, CAF and Vartanian, S and Vasava, K and Vdovin, V and Vega, J and Verdoolaege, Geert and Verger, JM and Vermare, L and Verona, C and Versloot, T and Vervier, M and Vicente, J and Villari, S and Villedieu, E and Villone, F and Vince, JE and Vine, GJ and Vinyar, I and Viola, B and Vitale, E and Vitelli, R and Vitins, A and Vlad, M and Voitsekhovitch, I 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  issn         = {0029-5515},
  journal      = {NUCLEAR FUSION},
  keyword      = {DIVERTOR,REGIME,TUNGSTEN,TOKAMAK PLASMAS,PLASMA-FACING COMPONENTS,PERFORMANCE},
  language     = {eng},
  number       = {10},
  pages        = {19},
  title        = {Overview of the JET results with the ITER-like wall},
  url          = {http://dx.doi.org/10.1088/0029-5515/53/10/104002},
  volume       = {53},
  year         = {2013},
}

Chicago
Romanelli, F, I Abel, V Afanesyev, M Aftanas, G Agarici, KM Aggarwal, L Aho-Mantila, et al. 2013. “Overview of the JET Results with the ITER-like Wall.” Nuclear Fusion 53 (10).
APA
Romanelli, F., Abel, I., Afanesyev, V., Aftanas, M., Agarici, G., Aggarwal, K., Aho-Mantila, L., et al. (2013). Overview of the JET results with the ITER-like wall. NUCLEAR FUSION, 53(10).
Vancouver
1.
Romanelli F, Abel I, Afanesyev V, Aftanas M, Agarici G, Aggarwal K, et al. Overview of the JET results with the ITER-like wall. NUCLEAR FUSION. 2013;53(10).
MLA
Romanelli, F, I Abel, V Afanesyev, et al. “Overview of the JET Results with the ITER-like Wall.” NUCLEAR FUSION 53.10 (2013): n. pag. Print.