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Research Needs for Magnetic Fusion Energy Sciences - US Burning ...

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Heating and fueling. during the ramp-up and flattop phases in iteR, heating and fueling must<br />

be carefully programmed to reach the high-gain state where alpha particle heating becomes dominant.<br />

iteR will be heated by a combination of neutral beam injection and various radiofrequency<br />

heating methods (ion cyclotron, electron cyclotron and possibly lower hybrid waves). The heating<br />

physics of these methods is well understood, and the full injected power is expected to be effectively<br />

absorbed by the plasma; however, there are plasma interface or technological issues associated<br />

with each of the methods. of particular interest in the Us is the interaction of the ion cyclotron<br />

antenna with the edge plasma. The questions are: What will be the nature of the radiofrequency<br />

sheaths <strong>for</strong>med by the ion cyclotron antenna? What will be its effect on impurity production and the effect<br />

of impurities on antenna operation? What will be the antenna impedance and will the required antenna<br />

voltage be acceptable?<br />

The specific Thrust element is a program focused on the interaction of ion cyclotron antennas<br />

with the edge plasma, including development, verification, and validation of models <strong>for</strong> radiofrequency<br />

sheaths and their effects. closely coordinated work using experimental, theoretical, and<br />

computational tools is required. it is expected that this activity will point toward the need <strong>for</strong> advanced<br />

antenna designs, and these should be implemented and their per<strong>for</strong>mance validated in<br />

existing machines. it is also expected that methods of reducing the antenna voltage below breakdown<br />

levels will be developed and validated within the frame of this Thrust element.<br />

control of the density and impurities and, to the extent possible, their spatial profiles is important<br />

<strong>for</strong> the transient and steady discharge phases. The limits of gas fueling at high neutral opacity<br />

and the role of transport in setting the density profile need to be explored. The fact that the<br />

particle transport differs among species could be leveraged to isolate control of particular fueling<br />

and impurity species. Questions to be resolved in this domain are: What is the particle transport,<br />

including impurity transport, <strong>for</strong> the various ITER operating scenarios, and what pellet ablation and fuel<br />

deposition models are appropriate? Can diagnostics be developed to determine the core deuterium and tritium<br />

ratio to aid burn control and as an adjunct to determining tritium retention? The specific activity<br />

in this Thrust element involves measuring and characterizing transport in transient phases and<br />

validating models of fueling via (inside launch) pellet injection. existing tokamaks properly outfitted<br />

with inside launch pellet fueling and an appropriate diagnostic set should suffice <strong>for</strong> carrying<br />

out this mission. in addition, advanced fueling techniques, e.g., compact tori injection, should<br />

be pursued.<br />

H-mode pedestals. The ability of the iteR device to achieve its high fusion gain (Q=10) mission<br />

depends on having an edge pedestal sufficient to maintain high core confinement. typical profiles<br />

<strong>for</strong> the density and temperature edge pedestals are shown in Figure 2. The questions are: What is<br />

the physics of the edge pressure pedestal in H-mode plasmas, and how does the pedestal interact with core<br />

heat and momentum transport? Recent modeling has reproduced the height of the h-mode pressure<br />

pedestal in several tokamaks by combining a prediction of edge mhd stability limits from<br />

peeling-ballooning mode theory with an empirical scaling <strong>for</strong> the pedestal width. transport can<br />

play a role when elms are mitigated or suppressed so that the pressure gradient is held below the<br />

threshold <strong>for</strong> peeling-ballooning instability. models of the h-mode pedestal structure and of the<br />

complete elm cycle need to be further developed and thoroughly tested against experiment. This<br />

includes the effect of pellet fueling and low flow/torque. in addition, models of the h-mode ped-<br />

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