Search Results - "JARDIN, S"

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  1. 1

    Self-Organized Stationary States of Tokamaks by Jardin, S C, Ferraro, N, Krebs, I

    Published in Physical review letters (20-11-2015)
    “…We demonstrate that in a 3D resistive magnetohydrodynamic simulation, for some parameters it is possible to form a stationary state in a tokamak where a…”
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  2. 2

    Ideal MHD Limited Electron Temperature in Spherical Tokamaks by Jardin, S. C., Ferraro, N. M., Guttenfelder, W., Kaye, S. M., Munaretto, S.

    Published in Physical review letters (17-06-2022)
    “…It is well documented that the central electron temperature in the national spherical torus experiment (NSTX) remains largely unchanged as the external heating…”
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  3. 3

    Review of implicit methods for the magnetohydrodynamic description of magnetically confined plasmas by Jardin, S.C.

    Published in Journal of computational physics (01-02-2012)
    “…Implicit algorithms are essential for predicting the slow growth and saturation of global instabilities in today’s magnetically confined fusion plasma…”
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  4. 4

    Calculations of two-fluid magnetohydrodynamic axisymmetric steady-states by Ferraro, N.M., Jardin, S.C.

    Published in Journal of computational physics (01-11-2009)
    “…M3D- C 1 is an implicit, high-order finite element code for the solution of the time-dependent nonlinear two-fluid magnetohydrodynamic equations [S.C. Jardin,…”
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  5. 5

    A high-order implicit finite element method for integrating the two-fluid magnetohydrodynamic equations in two dimensions by Jardin, S.C., Breslau, J., Ferraro, N.

    Published in Journal of computational physics (01-10-2007)
    “…We describe a new method for solving the time-dependent two-fluid magnetohydrodynamic (2F-MHD) equations in two dimensions that has significant advantages over…”
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  6. 6

    A triangular finite element with first-derivative continuity applied to fusion MHD applications by Jardin, S.C.

    Published in Journal of computational physics (10-10-2004)
    “…We describe properties of the reduced quintic triangular finite element. The expansion used in the element will represent a complete quartic polynomial in two…”
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  7. 7

    Design Details of the Transient CHI Plasma Start-up System on NSTX-U by Raman, Roger, Jarboe, T. R., Nelson, B. A., Mueller, D., Jardin, S. C., Neumeyer, C., Ono, M., Menard, J. E.

    Published in IEEE transactions on plasma science (01-08-2014)
    “…Elimination of the central solenoid would simplify the engineering design of a fusion nuclear science facility and tokamak based devices. The method of…”
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  8. 8

    Modeling of lithium granule injection in NSTX with M3D-C1 by Fil, A., Kolemen, E., Bortolon, A., Ferraro, N., Jardin, S., Parks, P.B., Lunsford, R., Maingi, R.

    Published in Nuclear materials and energy (01-08-2017)
    “…•A new ablation model for Li granules is implemented in the MHD code M3D-C1.•2D simulations of Li granule injections in NSTX realistic H-mode plasmas are…”
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  9. 9
  10. 10

    3D adaptive mesh refinement simulations of pellet injection in tokamaks by Samtaney, R., Jardin, S.C., Colella, P., Martin, D.F.

    Published in Computer physics communications (01-12-2004)
    “…We present results of Adaptive Mesh Refinement (AMR) simulations of the pellet injection process, a proven method of refueling tokamaks. AMR is a…”
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  11. 11

    Plasma profile and shape optimization for the advanced tokamak power plant, ARIES-AT by Kessel, C.E., Mau, T.K., Jardin, S.C., Najmabadi, F.

    Published in Fusion engineering and design (2006)
    “…An advanced tokamak plasma configuration is developed based on equilibrium, ideal MHD stability, bootstrap current analysis, vertical stability and control,…”
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  12. 12

    Physics basis for the advanced tokamak fusion power plant, ARIES-AT by Jardin, S.C., Kessel, C.E., Mau, T.K., Miller, R.L., Najmabadi, F., Chan, V.S., Chu, M.S., LaHaye, R., Lao, L.L., Petrie, T.W., Politzer, P., St.John, H.E., Snyder, P., Staebler, G.M., Turnbull, A.D., West, W.P.

    Published in Fusion engineering and design (2006)
    “…The advanced tokamak is considered as the basis for a fusion power plant. The ARIES-AT design has an aspect ratio of A ≡ R / a = 4.0 , an elongation and…”
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  13. 13

    A flux-limited numerical method for solving the MHD equations to simulate propulsive plasma flows by Sankaran, K., Martinelli, L., Jardin, S. C., Choueiri, E. Y.

    “…For numerical simulations to be effective tools in plasma propulsion research, a high‐order accurate solver that captures MHD shocks monotonically and works…”
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  14. 14

    ITER cold VDEs in the limit of a perfectly conducting first wall by Clauser, C. F, Jardin, S. C

    Published 11-11-2020
    “…Physics of Plasmas 28, 012511 (2021) Recently, it has been shown that a vertical displacement event (VDE) can occur in ITER even when the walls are perfect…”
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  15. 15

    Approach to nonlinear magnetohydrodynamic simulations in stellarator geometry by Zhou, Yao, Ferraro, N. M, Jardin, S. C, Strauss, H. R

    Published 10-07-2021
    “…Nucl. Fusion 61, 086015 (2021) The capability to model the nonlinear magnetohydrodynamic (MHD) evolution of stellarator plasmas is developed by extending the…”
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  16. 16

    MHD simulations with resistive wall and magnetic separatrix by Strauss, H.R., Pletzer, A., Park, W., Jardin, S., Breslau, J., Sugiyama, L.

    Published in Computer physics communications (01-12-2004)
    “…A number of problems in resistive MHD magnetic fusion simulations describe plasmas with three regions: the core, the halo region, and the resistive boundary…”
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  17. 17

    Symmetric solution in M3D by Chen, J., Breslau, J., Fu, G., Jardin, S., Park, W.

    Published in Computer physics communications (01-12-2004)
    “…The coefficient matrices in M3D are reformed here to have symmetric structures. They are further categorized into 3 types: weak diagonally-dominant matrix,…”
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  18. 18

    A parallel algorithm for global magnetic reconnection studies by Breslau, J.A., Jardin, S.C.

    Published in Computer physics communications (01-03-2003)
    “…A new algorithm is presented for the computation of two-dimensional magnetic reconnection in plasmas. Both resistive magnetohydrodynamic (MHD) and two-fluid…”
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  19. 19

    Modeling of carbon pellets disruption mitigation in an NSTX-U plasma by Clauser, C. F, Jardin, S. C, Raman, R, Lyons, B. C, Ferraro, N. M

    Published 28-06-2021
    “…Single carbon pellet disruption mitigation simulations using M3D-C1 were conducted in an NSTX-U-like plasma to support the electromagnetic pellet injection…”
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  20. 20

    Linear and nonlinear benchmarks between the CLT code and the M3D-C1 code for the 2/1 resistive tearing mode and the 1/1 resistive kink mode by Zhang, W., Jardin, S.C., Ma, Z.W., Kleiner, A., Zhang, H.W.

    Published in Computer physics communications (01-12-2021)
    “…The linear and nonlinear benchmarks between the CLT code and the M3D-C1 code for the 2/1 resistive tearing mode and the 1/1 resistive kink mode are presented…”
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