2016
DOI: 10.1002/ctpp.201610056
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Modeling of ITER Edge Plasma in the Presence of Resonant Magnetic Perturbations

Abstract: The modeling of the ITER edge is performed with the use of the code B2SOLPS5.2 in the presence of the electron conductivity caused by RMPs as well as for the reference case with the same input parameters but without RMPs. The radial electric field close to the neoclassical one is obtained without RMPs. Even the modest level of RMPs changes the direction of the electric field and causes the toroidal spin-up of the edge plasma. At the same time the pump-out effect is small.

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Cited by 6 publications
(5 citation statements)
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“…In the confined region, the radial electric field, as shown in figure 4, is close to its neoclassical value computed analytically according to the expression in [3], which is typical for simulations with SOLPS5.2 for existing tokamaks [3] and for ITER [23]. For Case #1b at lower divertor pressure and lower separatrix density, the radial electric field in the pedestal region is stronger due to the larger neoclassical contribution associated with the density gradient, figure 5(a).…”
Section: Electrostatic Potentialsupporting
confidence: 73%
“…In the confined region, the radial electric field, as shown in figure 4, is close to its neoclassical value computed analytically according to the expression in [3], which is typical for simulations with SOLPS5.2 for existing tokamaks [3] and for ITER [23]. For Case #1b at lower divertor pressure and lower separatrix density, the radial electric field in the pedestal region is stronger due to the larger neoclassical contribution associated with the density gradient, figure 5(a).…”
Section: Electrostatic Potentialsupporting
confidence: 73%
“…Similar to results from simulations with SOLPS5.2 [17,27] and SOLPS-ITER [28] for present tokamaks [17] and for ITER [27,28], radial electric field (E r ) in the outer core is found to be close to its neoclassical value, as shown in figure 4. According to equation (42) in [17], neoclassical value of E r depends on the parallel velocity (  V ), radial density ( / ¶ ¶ n r) and temperature ( / ¶ ¶ T r) gradients.…”
Section: Electrostatic Potential and Fieldsupporting
confidence: 83%
“…The test calculation was made to confirm applicability of this code for beryllium transport. Earlier the SOLPS-ITER code was used for modeling of different tokamaks with different sorts of impurities (such as He, N, Ne, C) such as ITER [3], Globus-M [4], ASDEX Upgrade [5], JET [6], DIII-D [7], Alcator C-Mod [8] and others.…”
Section: Introductionmentioning
confidence: 99%