TCV is well suited for electron transport studies due to its well developed ECRH system. Ion heating is achieved by thermal equilibration at high density in combination with strong third harmonic X-mode (X3) ECRH heating. In TCV shot 29892, X3 heating was applied to an ohmic ELMy H-mode, either at full or modulated power. This shot covers four stationary H-mode phases, one ohmic followed by three ELMy or ELM-free X3 heated. The final two are akin to improved H-modes. Previous analysis with the GLF model implied the discharge to be ITG dominated, in accordance with a preliminary Weiland stability analysis. As the applied heating only affects the electrons it is important to analyze this discharge regarding ETG and/or TEM modes. The ETG turbulence calculated with the IFS-ETG model will be presented. This model has already successfully calculated electron transport in dominantly electron-heated NSTX and Tore Supra.
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Authors
Elina Asp
Ecole Polytechnique Federale de Lausanne, Centre de Recherches en Physique des Plasmas, Association Euratom Confederation Suisse, CH-1015 Lausanne
Ecole Polytechnique Federale de Lausanne (EPFL), Centre de Recherches en Physique de Plasmas, Association EURATOM Conf\'ed\'eration Suisse
Juhyung Kim
Institute for Fusion Studies, University of Texas Austin, Austin, Texas 78712, US
Wendell Horton
UT Austin
Institute for Fusion Studies, University of Texas at Austin
The University of Texas at Austin
Institute for Fusion Studies, University of Texas Austin, Austin, Texas 78712, US
Laurie Porte
Ecole Polytechnique Federale de Lausanne (EPFL), Centre de Recherches en Physique de Plasmas, Association EURATOM Confederation Suisse, 1015 Lausanne
Ecole Polytechnique Federale de Lausanne (EPFL), Centre de Recherches en Physique de Plasmas, Association EURATOM Conf\'ed\'eration Suisse
Ecole Polytechnique Federale de Lausanne, Centre de Recherches en Physique des Plasmas, Association Euratom Confederation Suisse, CH-1015 Lausanne
Stefano Alberti
Ecole Polytechnique Federale de Lausanne (EPFL), Centre de Recherches en Physique de Plasmas, Association EURATOM Conf\'ed\'eration Suisse
Ecole Polytechnique Federale de Lausanne, Centre de Recherches en Physique des Plasmas, Association Euratom Confederation Suisse, CH-1015 Lausanne
Emiliano Fable
Ecole Polytechnique Federale de Lausanne, Centre de Recherches en Physique des Plasmas, Association Euratom Confederation Suisse, CH-1015 Lausanne
Yves Martin
Ecole Polytechnique Federale de Lausanne (EPFL), Centre de Recherches en Physique de Plasmas, Association EURATOM Conf\'ed\'eration Suisse
Ecole Polytechnique Federale de Lausanne, Centre de Recherches en Physique des Plasmas, Association Euratom Confederation Suisse, CH-1015 Lausanne
\'Ecole Polytechnique F\'ed\'erale de Lausanne (EPFL), Centre de Recherches en Physique des Plasmas, Association Euratom, CH-1015 Lausanne Suisse
Olivier Sauter
Ecole Polytechnique Federale de Lausanne, Centre de Recherches en Physique des Plasmas, Association Euratom Confederation Suisse, CH-1015 Lausanne
Ecole Polytechnique Federale de Lausanne (EPFL), Centre de Recherches en Physique de Plasmas, Association EURATOM Conf\'ed\'eration Suisse
\'Ecole Polytechnique F\'ed\'erale de Lausanne (EPFL), Centre de Recherches en Physique des Plasmas, Association Euratom, CH-1015 Lausanne Suisse
Gianpaolo Turri
Ecole Polytechnique Federale de Lausanne, Centre de Recherches en Physique des Plasmas, Association Euratom Confederation Suisse, CH-1015 Lausanne
\'Ecole Polytechnique F\'ed\'erale de Lausanne (EPFL), Centre de Recherches en Physique des Plasmas, Association Euratom, CH-1015 Lausanne Suisse