Benchmark analysis of in-vacuum vessel LOCA scenarios for code-to-code comparison

2021 ◽  
pp. 112938
Author(s):  
Matteo D'Onorio ◽  
Salvatore D'Amico ◽  
Antonio Froio ◽  
Maria Teresa Porfiri ◽  
Gandolfo Alessandro Spagnuolo ◽  
...  
2015 ◽  
Vol 3 (5) ◽  
pp. 371-375
Author(s):  
Pielah Kim ◽  
◽  
Songyee Hur ◽  
Boram Park ◽  
Leslie Stoel

2020 ◽  
Vol 86 (5) ◽  
Author(s):  
Y. Lin ◽  
J. C. Wright ◽  
S. J. Wukitch

Ion cyclotron range of frequencies (ICRF) heating will be the sole auxiliary heating method on SPARC for both full-field (Bt0 ~ 12 T) D–T operation and reduced field (Bt0 ~ 8 T) D–D operation. Using the fast wave at ~120 MHz, good wave penetration and strong single-pass absorption is expected for D–T(3He), D(3He), D(H) and 4He(H) heating scenarios. The dependences of wave absorption on ${k_\parallel }$ , 3He concentration, resonance location, antenna poloidal location and losses on alpha particles and ash have been studied. The antenna loading has been assessed by comparison with the Alcator C-Mod antennae. An antenna spectrum of ${k_\parallel }\sim 15\text{--}18\,{\textrm{m}^{ - 1}}$ is shown to be good for both core absorption and edge coupling. For the control of impurity sources, the antenna straps are rotated ~10° to be perpendicular to the B field and the straps can run with different power levels in order to optimize the antenna spectrum and to minimize the image current on the antenna frame. Combining the physics constraints with the SPARC port design, maintenance requirement and contingency against antenna failure during D–T operation, we plan to mount on the inner wall of the vacuum vessel a total of 12 4-strap antennae in 6 ports while keeping 3-strap antennae that are insertable and removable on port plugs as the backup option.


2021 ◽  
Vol 171 ◽  
pp. 112568
Author(s):  
Nisarg Patel ◽  
Jakub Hromadka ◽  
Josef Havlicek ◽  
Vojtech Balner ◽  
David Sestak ◽  
...  
Keyword(s):  

2019 ◽  
Vol 485 (3) ◽  
pp. 3370-3377 ◽  
Author(s):  
Lehman H Garrison ◽  
Daniel J Eisenstein ◽  
Philip A Pinto

Abstract We present a high-fidelity realization of the cosmological N-body simulation from the Schneider et al. code comparison project. The simulation was performed with our AbacusN-body code, which offers high-force accuracy, high performance, and minimal particle integration errors. The simulation consists of 20483 particles in a $500\ h^{-1}\, \mathrm{Mpc}$ box for a particle mass of $1.2\times 10^9\ h^{-1}\, \mathrm{M}_\odot$ with $10\ h^{-1}\, \mathrm{kpc}$ spline softening. Abacus executed 1052 global time-steps to z = 0 in 107 h on one dual-Xeon, dual-GPU node, for a mean rate of 23 million particles per second per step. We find Abacus is in good agreement with Ramses and Pkdgrav3 and less so with Gadget3. We validate our choice of time-step by halving the step size and find sub-percent differences in the power spectrum and 2PCF at nearly all measured scales, with ${\lt }0.3{{\ \rm per\ cent}}$ errors at $k\lt 10\ \mathrm{Mpc}^{-1}\, h$. On large scales, Abacus reproduces linear theory better than 0.01 per cent. Simulation snapshots are available at http://nbody.rc.fas.harvard.edu/public/S2016.


2014 ◽  
Vol 89 (7-8) ◽  
pp. 1826-1831 ◽  
Author(s):  
Vladimir Rozov ◽  
J.-M. Martinez ◽  
C. Portafaix ◽  
G. Sannazzaro

2007 ◽  
Vol 82 (15-24) ◽  
pp. 2081-2088 ◽  
Author(s):  
Katsusuke Shimizu ◽  
Masanori Onozuka ◽  
Yukinori Usui ◽  
Kazuhiro Urata ◽  
Yoshihiro Tsujita ◽  
...  
Keyword(s):  

2007 ◽  
Vol 82 (15-24) ◽  
pp. 1866-1870 ◽  
Author(s):  
V. Komarov ◽  
H. Heidl ◽  
R. Tivey ◽  
J. Palmer
Keyword(s):  

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