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

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the high-n regime of iteR; the large collection of interacting alfvén modes will drive nonlinear<br />

cross-scale couplings from meso to micro-scale dynamics. This feature will become more dominant<br />

in iteR than in current experiments, which predominantly observe moderate-n versions of<br />

these instabilities. This regime requires a paradigm shift to nonlinear gyrokinetic models that include<br />

all relevant wave-particle resonances and finite larmor radius effects <strong>for</strong> both the thermal<br />

and energetic particle species. in addition, avalanche models need further development; the presence<br />

of many closely spaced modes could allow the energetic particle pressure gradient to progressively<br />

relax (flatten) from the center to the edge, implying rapid fast ion transport. to realistically<br />

model alpha transport in the edge plasma and divertor regions, improved equilibrium magnetic<br />

field models will be required that include the 3-d effects of toroidal field ripple, ferromagnetic<br />

materials, and coils to control resistive wall modes and edge localized modes; also, the effects<br />

of parasitic absorption of radiofrequency current drive power on alpha confinement will need to<br />

be assessed. The goals of such improved nonlinear models are to identify regimes that might be<br />

dangerous to the integrity of the plasma facing components, to predict the alpha heating profile<br />

evolution, and to evaluate the alpha particle influence on the driven current and its distribution.<br />

Ultimately, <strong>for</strong> iteR, with a fixed energy distribution (slowing-down, isotropic) <strong>for</strong> the alpha particles,<br />

it would also be expected that alpha transport scaling laws could be developed from simulations<br />

and experimental measurements. These could be useful <strong>for</strong> integrated modeling and <strong>for</strong><br />

operational scenario selection.<br />

The best simulation methods are in the process of being determined. Presently several approaches<br />

are in development. They include: (1) fully kinetic 3-d simulations that include the microinstability<br />

drive acting on the background plasma; (2) detailed 3-d hybrid mhd fluid simulations <strong>for</strong><br />

the energetic particles and core plasma with the effects from microinstability treated in viscous<br />

and heat transport terms; and (3) the development of quasi-linear codes that can couple results<br />

from large fluid-particle codes to determine the transport coefficients that apply in the reduced<br />

1-d profile evolution <strong>for</strong> the entire system. to achieve a deeper comprehension of the consequences<br />

of alfvénic activity driven by alpha particles, reduced nonlinear theory will be incorporated in<br />

quasi-linear codes and then compared with the results of the larger simulations. The development<br />

path and viability <strong>for</strong> any of the above approaches will depend on regular validation against experimental<br />

data provided by the new diagnostics discussed in the following section. While validation<br />

tests in fully consistent burning plasma regimes (low r/a, v a /v alfvén ≥ 1, central b a (0) ≈<br />

1 %) may have to wait <strong>for</strong> iteR, there are many other aspects that can be checked from ongoing<br />

experiments.<br />

advanced Diagnostics <strong>for</strong> alpha Physics<br />

For the above improvements in simulation to have realism, an aggressive program of advanced<br />

energetic particle diagnostic development is needed. The goal of this ef<strong>for</strong>t should be to provide<br />

validation at appropriately resolved spatial and temporal scales and to stimulate improvements<br />

in modeling as unexpected phenomena are uncovered. The requirements <strong>for</strong> such diagnostics is<br />

an area with important overlaps to Thrust 1 and that much of the underlying development activity<br />

may occur under Thrust 1.<br />

The first element of such a program is the measurement of the fluctuating electric and magnetic<br />

field instability mode structures. a number of techniques are now available <strong>for</strong> this task, such as<br />

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