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

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ent drive alone cannot account <strong>for</strong> the observed broad current profile. similarly, simulations <strong>for</strong><br />

iteR indicate that the day-one mix of heating and current drive capability is insufficient to robustly<br />

maintain the requisite flat shear <strong>for</strong> an extended duration. The mechanism leading to the<br />

low shear with q(0) ≥ 1 in present-day devices is correlated with the appearance of benign mhd<br />

instabilities, <strong>for</strong> example, the appearance of fishbone activity in asdeX-Upgrade and a low-level<br />

3/2 neoclassical tearing mode in diii-d. These instabilities prevent the central safety factor from<br />

dropping below unity, which results in stabilization of the sawtooth instability normally found in<br />

h-mode discharges. more research is required to determine if this “natural” current profile broadening<br />

can be expected in iteR.<br />

experimental results also suggest that per<strong>for</strong>mance in the hybrid regime is adversely affected by<br />

operating characteristics expected to be encountered in iteR, such as low rotation and t e /t i =1.<br />

improvements in the ability to simulate these changes using theory-based transport models is<br />

needed to confirm whether improved per<strong>for</strong>mance can be realized in iteR.<br />

Steady-state Operation: steady-state operation of iteR is highly desirable, not only to carry<br />

out the nuclear testing part of the iteR mission, but also to demonstrate the tokamak’s potential<br />

to <strong>for</strong>m the core of a practical fusion reactor. in general, steady-state operation of a tokamak is<br />

based on replacing the current normally generated by induction with current generated by other<br />

means. although toroidal current can and will be produced in iteR by neutral beam injection and<br />

the various <strong>for</strong>ms of radiofrequency current drive, the efficiency of these systems is too low to<br />

generate a substantial fraction of the total current, i.e., the power required to replace the normal<br />

inductive current would be comparable to the total power derived from the fusion reactions. Thus,<br />

the approach to steady state <strong>for</strong> iteR, and indeed <strong>for</strong> a tokamak reactor, is to maximally exploit<br />

the “bootstrap current,” which is naturally produced in a toroidal plasma by the plasma’s temperature<br />

and density gradients. achieving this “self-organized” state requires operation at relatively<br />

high beta, which means that steady-state tokamak operating regimes represent a delicate balance<br />

between generating sufficient bootstrap current and respecting mhd stability limits.<br />

Good progress in achieving practical, near-steady-state tokamak operating regimes has been<br />

made in the worldwide tokamak research ef<strong>for</strong>t, in particular, in the diii-d tokamak in the Us.<br />

as in the case of hybrid modes, the magnetic shear appears to play a key role in <strong>for</strong>ming highbootstrap-fraction<br />

discharges. in diii-d, fully noninductive discharges have been obtained with<br />

a bootstrap fraction of ~ 60% in regimes with flat shear and q min ~ 1.5. another example of nearsteady-state<br />

operation in low-shear regimes is provided by the so-called high poloidal beta regimes<br />

obtained in Jt-60U. in these discharges, the central safety factor remains in the range 1 <<br />

q(0)

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