2020
DOI: 10.1088/1741-4326/ab8c64
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Burning fraction, radial transport, and steady state profiles of multi-species particles in CFETR burning plasmas

Abstract: The burning fraction of fuel particles is a crucial issue for future fusion reactors. In order to achieve the high tritium burning fraction required by China Fusion Engineering Test Reactor (CFETR) engineering design, fueling depths and quantities should be estimated by particle control analysis for different scenarios. Thus, in this paper, a multi-species fluid model of deuterium-tritium (D-T) fusion plasmas is applied to study radial transport and profile evolution with CFETR parameters under different fueli… Show more

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Cited by 3 publications
(3 citation statements)
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“…The prescribed concentration of helium ash in both ITER and CFETR should be less than 10% [7,8], and successive progress on CFETR further requires 5% as the upper operational limit due to the decrease of fusion power and T burnup fraction by helium ash [9]. α particles from the D-T reaction, acting as the source of helium ash [10], would affect the density profile of helium ash [11,12]. The experiments on TFTR tokamak show that except the very central region, the transport level of helium ash in D-T plasmas is much higher than the prediction from neoclassical theory [13].…”
Section: Introductionmentioning
confidence: 99%
“…The prescribed concentration of helium ash in both ITER and CFETR should be less than 10% [7,8], and successive progress on CFETR further requires 5% as the upper operational limit due to the decrease of fusion power and T burnup fraction by helium ash [9]. α particles from the D-T reaction, acting as the source of helium ash [10], would affect the density profile of helium ash [11,12]. The experiments on TFTR tokamak show that except the very central region, the transport level of helium ash in D-T plasmas is much higher than the prediction from neoclassical theory [13].…”
Section: Introductionmentioning
confidence: 99%
“…While the kinetic simulation is computational-time-consuming [13] and the momentum of the fueling source term is hardly estimated both in theory and experiment, the reduced Braginskii [14] equations are used in our model with source and sink terms due to fueling and fusion reaction. As introduced previously [12] and taking the thermal transport into account, the set of model equations is thus written: where the term S D,T is the PI source term, as described in section 4.2. To explore the possibility of satisfying the burn fraction criterion, certain assumptions are made including 100% fueling efficiency and 50:50 deuterium to tritium ratio.…”
Section: Basic Equationsmentioning
confidence: 99%
“…In section 2, we first start from a zero-dimensional (0D) burning fraction model to make a magnitude estimation of the requirement for future reactor design. Then, a 1D radial transport model introduced in our previous work [12] is modified to take the temperature profile evolution into account and with the pellet deposition described by the neutral gas (NGS) and magnetohydrodynamic (MHD) drift model. This extended transport model with boundary conditions and CFETR parameters applied is described in section 3.…”
Section: Introductionmentioning
confidence: 99%