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

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will dominate the external sources of heating and current drive, and the plasma will self-organize<br />

to a state consistent with its underlying physics. The power from alpha particles (P alpha ), in<br />

the demo regime, will be larger than the externally injected power (P input ) by a factor of 4-9, i.e.,<br />

the ratio Q=P fus /P input = 20-45. in addition, the ratio of plasma self-driven current (i bootstrap ) to<br />

the total plasma current (i plasma ) is expected to reach values of 0.65-0.90, or perhaps even higher.<br />

although we have concentrated on the plasma transport and current drive couplings, shown schematically<br />

in Figure 3, it is recognized that there are also couplings in the mhd area, among fast<br />

alpha particles, global instabilities, and the pedestal.<br />

trans<strong>for</strong>mer source<br />

of poloidal flux<br />

V loop<br />

J ohm<br />

J cd<br />

J bs<br />

magnetic flux<br />

diffusion<br />

B pol<br />

bootstrap<br />

current<br />

conductivity<br />

profile<br />

auxiliary<br />

current drive<br />

α-particle<br />

heating<br />

p, T, n, V<br />

profiles<br />

Figure 3: Some of the many feedback loops important in plasma scenarios with strong self-heating and selfdriven<br />

currents. From P. Politzer et al, Nucl. <strong>Fusion</strong> 45 (2005) 417-424.<br />

This regime will generate dominant heating of the electron channel, where our understanding is<br />

limited, as opposed to the ion channel, where experimental evidence and theoretical understanding<br />

have made significant progress. operation at high density, near the empirical Greenwald density<br />

limit, which is traditionally avoided, will become the norm as the requirement to generate fusion<br />

power <strong>for</strong>ces the plasma density higher than in deuterium (d-d) experiments. There is limited<br />

understanding of the processes determining this empirical limit. The impact of driven and<br />

intrinsic rotation on transport and stability, which is only now being explored in detail on existing<br />

tokamaks, is difficult to project to future devices, particularly with a dominant alpha heating<br />

source. it is recognized that the plasma rotation present on existing tokamaks has a fundamental<br />

82<br />

auxiliary<br />

heating<br />

Σ<br />

heat, particle, &<br />

momentum fluxes Σ<br />

transport coefficients<br />

turbulent & neoclassical<br />

auxiliary angular<br />

momentum<br />

fueling<br />

& pumping<br />

external<br />

internal<br />

wall sources<br />

and sinks

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