Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

P5.1099 Integrated core-pedestal modeling with the AToM framework

Jul 6, 2018, 2:00 PM
2h
Mánes

Mánes

Speaker

Jeff Candy

Description

See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/P5.1099.pdf Integrated core-pedestal modeling with the AToM framework∗ J. Candy1 , E. Belli1 , D. Green3 , C. Holland2 , O. Meneghini1 , J.M. Park3 , S. Smith1 and the AToM team. 1 GeneralAtomics, San Diego, CA 2 Universityof California at San Diego, San Diego, CA 3 Oak Ridge National Laboratory, Oak Ridge, TN In this presentation we will report on two novel integrated simulation capabilities of the Ad- CORE TR PED vanced Tokamak Modeling (AToM) framework. The original AToM0 SciDAC-3 project was a 3- year effort that concluded in 2017. For the pe- riod 2017-2022, a new 5-year AToM SciDAC-4 project has begun. First, we give an overview of coupled core-pedestal integrated simulations, with application to DIII-D plasmas. These sim- ulations take into account the strong interplay between core turbulent-plus-collisional trans- port, pedestal structure, current profile and plasma equilibrium. Integrated modeling work- flows capable of calculating the steady-state self-consistent solution to this strongly-coupled problem have been developed and implemented Experimental data Successive workflow iterations in AToM via the OMFIT-TGYRO [1] and the Pedestal density input to the workflow IPS-FASTRAN [2] workflows. Here, kinetic plasma equilibrium is computed by EFIT using profile data from the transport solver and kinetic bootstrap current from the neoclassical module. Given an EFIT equilibrium, core profiles are evolved by the transport solver by combining col- lisional and turbulent fluxes to maintain balance with heating and fueling sources. The updated value of the global plasma pressure is passed to EPED to obtain the self-consistent pedestal structure. For the OMFIT-TGYRO-TGLF-NEO workflow (see plot), the scheme is iterated to convergence in a few iterations and is independent of initial profiles. By using only the elec- tron density at the top of the pedestal as an input, profiles are calculated from magnetic axis to separatrix – in good agreement with experiment (DIII-D 153523, 3745ms). Second, we will review a key subcomponent of these coupled core-pedestal simulations: the time-dependent (i.e, mulitple time-slice) kinetic EFIT reconstruction. Here, a self-consistent kinetic neoclas- sical bootstrap current calculation with NEO is coupled to the EFIT equilibrium solve. This ensures the highest-accuracy calculation of the bootstrap current and consistent plasma equilib- rium across the entire plasma profile. ∗ Work supported by US DOE under DE-SC0017992. References [1] O. Meneghini, S.P. Smith, P.B. Snyder, G.M. Staebler, J. Candy and E.A. Belli, Nucl. Fusion 57, 0866034 (2017) [2] J.M. Park, J.R. Ferron, C.T. Holcomb, et al, Phys. Plasmas 25, 012506 (2018)

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