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

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esearch requirements<br />

installation of neutral beams at larger energies, currents, and time duration are required to study<br />

the effects of significant populations of super-alfvénic particles. The energy content and momentum<br />

of the beams must be comparable to or higher than that of the background plasma. The beam<br />

duration must be longer than both the plasma confinement time and the fast ion confinement<br />

time. Theoretical and numerical tools, such as tRansP, nova, and oRbit, require adaptation<br />

<strong>for</strong> the RFP configuration.<br />

DEtERMining bEta LiMiting MECHaniSMS<br />

The required value ~20% of poloidal beta (ratio of plasma pressure to poloidal magnetic field pressure)<br />

<strong>for</strong> an attractive RFP reactor has already been experimentally achieved, but complete theoretical<br />

understanding is lacking. it is there<strong>for</strong>e not yet possible to project beta limits in a burning<br />

plasma. optimization and control of the plasma pressure profile, possibly as a function of plasma<br />

cross section and aspect ratio, may become important to avoid instability and maintain the high<br />

beta necessary to achieve the iteR-era goals.<br />

research requirements<br />

by upgrading the existing facilities, especially the neutral beam injection system in terms of power<br />

and fueling rate, it is possible that the beta limit could be identified at moderate S <strong>for</strong> both axisymmetric<br />

and helical RFP equilibrium. however, the plasma parameters (energy confinement<br />

time, fast ion slowing down time, and plasma duration) make fast ion thermalization difficult,<br />

most likely limited to higher density operation provided by pellet injection. dependence of beta<br />

limits on cross section and aspect ratio cannot be studied on the existing facilities, requiring new<br />

facilities to explore geometric optimization.<br />

testing beta limits at the larger S available in an advanced, long-pulse proof-of-principle facility<br />

and a subsequent per<strong>for</strong>mance extension facility with full heating and fueling capabilities is essential<br />

in achieving the RFP goal.<br />

comprehensive theoretical analyses are required beyond the standard suydam criteria (critical<br />

pressure gradient), which have been surpassed by experimentally achieved values. extended capability<br />

<strong>for</strong> computational tools at larger S and with two-fluid physics is also required, in conjunction<br />

with theory, to confirm and quantitatively predict the beta limits.<br />

aCtiVE COntROL OF MHD inStabiLitiES<br />

both resonant and nonresonant mhd instabilities play an important role in the RFP. The control<br />

of these instabilities and their consequences by means of non-axisymmetric coils (both saddle<br />

and flux loops) is an important area of investigation, since this may be essential in any major<br />

next-step RFP device and a future reactor. The t2R and RFX-mod facilities in europe have significant<br />

active control experimental capability used to completely stabilize resistive wall modes. This<br />

establishes the critical physics requirement that RFP plasmas be maintained beyond the time<br />

scale of passive stabilization by an electrically conducting wall. in addition, saddle loops located<br />

at cuts or breaks in the conducting vessels surrounding the plasma have been used to mitigate lo-<br />

209

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