Progress on the small modular stellarator SCR-1: new diagnostics and heating scenarios. (August 2020)

• Record Type: Journal Article
• Authors: Coto-Vílchez, F.; Vargas, V. I.; Solano-Piedra, R.; Rojas-Quesada, M. A.; Araya-Solano, L. A.; Ramírez, A. A.; Hernández-Cisneros, M.; Pérez-Hidalgo, J. E.; Köhn-Seemann, A.; Cerdas, F.; Vílchez-Coto, F.; Jiménez, D.; Campos-Duarte, L.; Meneses, E.; González-Vega, M.; Arias, S.
• Is Part Of: Journal of plasma physics. Volume 86:Number 4(2020)
• Publication Date: 2020-08
• Subjects: plasma diagnostics, -- fusion plasma, -- plasma heating; Plasma (Ionized gases) -- Periodicals; 530.4405
• DOI: 10.1017/S0022377820000677
• Languages: English
• ISSNs: 0022-3778

Abstract

Abstract : This work presents updates in the diagnostics systems, magnetohydrodynamics (MHD) calculations and simulations of microwave heating scenarios of the small modular Stellarator of Costa Rica 1 (SCR-1). Similarly, the design of a flexible bolometer and magnetic diagnostics (a set of Mirnov coils, Rogowski coils and two diamagnetic loops) are introduced. Furthermore, new MHD equilibrium calculations for the plasma of the SCR-1 device were performed using the VMEC code including the poloidal cross-section of the magnetic flux surfaces at different toroidal positions, profiles of the rotational transform, magnetic well, magnetic shear and total magnetic field norm. Charged particle orbits in vacuum magnetic field were computed by the magnetic field solver BS-SOLCTRA (Vargas et al. In 27th IAEA Fusion Energy Conference (FEC 2018), 2018. IAEA). A visualization framework was implemented using Paraview (Solano-Piedra et al. In 23rd IAEA Technical Meeting on the Research Using Small Fusion Devices (23rd TM RUSFD), 2017) and compared with magnetic mapping results (Coto-Vílchez et al. In 16th Latin American Workshop on Plasma Physics (LAWPP), 2017, pp. 43–46). Additionally, simulations of microwave heating scenarios were performed by the IPF-FDMC full-wave code. These simulations calculate the conversion of the ordinary waves to extraordinary waves and allow us to identify the location where the conversion takes place. Finally, the microwave heating scenarios for the $330^{\circ }$ toroidal position are presented. The microwave heating scenarios showed that the O–X–B mode conversion is around 12–14 %. It was possible to identify the spatial zone where the conversion takes place (upper hybrid frequency).