Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session UP11: Poster Session VIII: MST; DIII-D Tokamak; SPARC, C-Mod, and High Field Tokamaks; HBT-EP; Transport and LPI in ICF Plasmas, Hydrodynamic Instability; HEDP Posters; Space and Astrophysical Plasmas (2:00pm-5:00pm)
Thursday, November 8, 2018
OCC
Room: Exhibit Hall A1&A
Abstract ID: BAPS.2018.DPP.UP11.116
Abstract: UP11.00116 : Modeling of LPI and non-local electron transport for radiation hydrodynamic simulation*
Presenter:
Hideo Nagatomo
(ILE Osaka Univ)
Authors:
Hideo Nagatomo
(ILE Osaka Univ)
Takashi Asahina
(ILE Osaka Univ)
Tomoyuki Johzaki
(Hiroshima Univ)
Yasuhiko Sentoku
(ILE Osaka Univ)
In the last phase of the shock ignition scheme, an intense spike laser pulse drives a strong shock in order to ignite the compressed fuel. The generation of strong shock is in a laser-plasma interaction regime where laser-plasma instabilities are expected. For example, generation of hot electron and its non-local transport cannot be ignored. The kinetic simulations are effective to evaluate these dynamics. However, spatial domain of the implosion simulation is very huge for kinetic simulations, and it is unrealistic. The effect of the LPI, generation of hot electron and laser absorption rate is modeled using PIC simulation and reflected into radiation hydrodynamic simulation [1] where non-local electron conduction model [2] is installed. A typical SI simulation is conducted to evaluate the performance of the implosion using the simulation models. We also consider the effect of external magnetic field for magnetized fast ignition.
[1] H. Nagatomo et al., Nucl. Fusion 57, 086009 (2017)
[2] Ph. D. Nicolai et al, Phys. Plasmas 13, 032701 (2006)
*This study was supported by JSPS KAKENHI Grant No. 17K05728
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.UP11.116
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