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The science program of the TCV tokamak: exploring fusion reactor and power plant concepts
- Source :
- Nuclear fusion 55 (2015). doi:10.1088/0029-5515/55/10/104004, info:cnr-pdr/source/autori:Coda, S. for the TVC Team (R. Albanese (a; S. Alberti (v; R. Ambrosino (a; H. Anand (v; Y. Andrebe (v; M. Ariola (a; J.E. Barton (b; R. Behn (v; P. Blanchard (v; J.A. Boedo (c; A. Bortolon (d; F.H. Braunm¨uller (v; S. Br´emond (e; S. Brunner (v; Y. Camenen (f ; G.P. Canal (v; S. Coda (v; W.A. Cooper (v; N. Cruz (g; M. de Baar (h,i); J. Decker (v; C.A. de Meijere (v; B.P. Duval (v; A. Fasoli (v; L. Federspiel (v; F. Felicih,M. Fontana (v; I. Furno (v; C. Galperti (v, I. Garrido (j; J. Genoud (v; T.P. Goodman (v; J.P. Graves (v; P. Hennequink, J.-Ph. Hoggev, G. Hommenh,i, Z. Huangv, B. Joye (v; J. Kamleitner (v; A. Karpushov (v; D. Kim (v; N. Kirneva (l,m); A. Kr¨amer-Flecken (n; B. Labit (v; E. Lazzaro (o; H.B. Le (v; L. Lefevre (p; F. Li (v; B. Lipschultz (q; J.B. Lister (v; X. Llobet (v; T. Lunt (r ; A. Malygin (v; E. Maljaars (h; C. Marini (v; Y. Martin (v; M. Mattei (a; A. Merle (v; P.A. Molina Cabrera (v; D. Moreau (e; J.-M. Moret (v; T. Morgan (i; N.A. Mustafin (l; F. Nespoli (v; R. Nouailletas (e; S. Nowak (o; Y. Peysson (e; A. Pironti (a; A. Pochelon (v; L. Porte (v; H. Reimerdes (v; O. Sauter (v; Ch. Schlatter (v; E. Schuster (b; M. Silva (v; J. Sinha (v; T. Stoltzfus-Dueck (s, B. T´al (t ; A.A. Teplukhina (v; D. Testa (v; C. Theiler (v; G. Tonetti (v; M.Q. Tran (v; C. Tsui (c; L. Vermare (k; T. Vernay (v; W.A.J. Vijvers (q; N.M.T. Vu (p; V. Vuille (v; H. Weisen (v; R. Wenninger (r ; E. Witrant (u.)/titolo:The science program of the TCV tokamak: exploring fusion reactor and power plant concepts/doi:10.1088%2F0029-5515%2F55%2F10%2F104004/rivista:Nuclear fusion/anno:2015/pagina_da:/pagina_a:/intervallo_pagine:/volume:55, Nuclear Fusion, Nuclear Fusion, IOP Publishing, 2015, 55 (10), pp.104004. ⟨10.1088/0029-5515/55/10/104004⟩, Nuclear Fusion, 2015, 55 (10), pp.104004. ⟨10.1088/0029-5515/55/10/104004⟩
- Publication Year :
- 2015
- Publisher :
- IOP Publishing, 2015.
-
Abstract
- International audience; TCV is acquiring a new 1 MW neutral beam and 2 MW additional third-harmonic electron cyclotron resonance heating (ECRH) to expand its operational range. Its existing shaping and ECRH launching versatility was amply exploited in an eclectic 2013 campaign. A new sub-ms real-time equilibrium reconstruction code was used in ECRH control of NTMs and in a prototype shape controller. The detection of visible light from the plasma boundary was also successfully used in a position-control algorithm. A new bang-bang controller improved stability against vertical displacements. The RAPTOR real-time transport simulator was employed to control the current density profile using electron cyclotron current drive. Shot-by-shot internal inductance optimization was demonstrated by iterative learning control of the current reference trace. Systematic studies of suprathermal electrons and ions in the presence of ECRH were performed. The L?H threshold power was measured to be ?50?75% higher in both H and He than D, to increase with the length of the outer separatrix, and to be independent of the current ramp rate. Core turbulence was found to decrease from positive to negative edge triangularity deep into the core. The geodesic acoustic mode was studied with multiple diagnostics, and its axisymmetry was confirmed by a full toroidal mapping of its magnetic component. A new theory predicting a toroidal rotation component at the plasma edge, driven by inhomogeneous transport and geodesic curvature, was tested successfully. A new high-confinement mode (IN-mode) was found with an edge barrier in density but not in temperature. The edge gradients were found to govern the scaling of confinement with current, power, density and triangularity. The dynamical interplay of confinement and magnetohydrodynamic modes leading to the density limit in TCV was documented. The heat flux profile decay lengths and heat load profile on the wall were documented in limited plasmas. In the snowflake (SF) divertor configuration the heat flux profiles were documented on all four strike points. SF simulations with the EMC3-EIRENE code, including the physics of the secondary separatrix, underestimate the flux to the secondary strike points, possibly resulting from steady-state E × B drifts. With neon injection, radiation in a SF was 15% higher than in a conventional divertor. The novel triple-null and X-divertor configurations were also achieved in TCV.
- Subjects :
- Nuclear and High Energy Physics
Tokamak
DEMO
ITER
nuclear fusion
plasma
TCV
tokamak
Condensed Matter Physics
Cyclotron
Condensed Matter Physic
7. Clean energy
Electron cyclotron resonance
law.invention
[PHYS.PHYS.PHYS-PLASM-PH]Physics [physics]/Physics [physics]/Plasma Physics [physics.plasm-ph]
Physics::Plasma Physics
law
Physics
Toroid
Divertor
Plasma
Fusion power
Computational physics
Heat flux
Atomic physics
Subjects
Details
- ISSN :
- 17414326, 00295515, 07413335, 00030503, 00189499, 17426596, and 00223115
- Volume :
- 55
- Database :
- OpenAIRE
- Journal :
- Nuclear Fusion
- Accession number :
- edsair.doi.dedup.....7941dc90fb86c440ba76a8531c33becf
- Full Text :
- https://doi.org/10.1088/0029-5515/55/10/104004