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

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primarily electrostatic, in the case where the ion gyroradius is relatively large, and the direction of<br />

the magnetic field lines changes rapidly within the plasma, (2) control of multiple instabilities in a<br />

plasma surrounded by a metal vessel of finite electrical conductivity, (3) understanding high-pressure<br />

plasmas exceeding stability limits locally or globally, (4) dynamics of magnetic self-organization<br />

in which magnetic reconnection, dynamo, momentum transport, and ion heating occur simultaneously,<br />

and (5) the generic linkage of these phenomena to plasma astrophysics.<br />

Summary of Existing RFP Experimental Facilities and Other available Means<br />

There are four RFP experiments operating in the world. (1) The mst facility at the University of<br />

Wisconsin-madison is the centerpiece of the Us proof-of-principle RFP program. it is physically<br />

large in the RFP context (toroidal minor radius, a=0.5 m, and major radius, R=1.5 m), but has medium<br />

plasma current capability (ip ~ 0.5 ma). The mst program emphasizes the study of plasmas<br />

with high confinement at high pressure made possible by control of the radial profile of the<br />

plasma current density and by auxiliary plasma heating. it also includes investigation of current<br />

sustainment by oscillating Field current drive (oFcd), a low frequency <strong>for</strong>m of magnetic induction.<br />

(2) The world’s largest and highest power RFP facility is RFX-mod in italy (a=0.46 m, R=2.0<br />

m), with an achieved current of 1.5 ma and a design current of 2.0 ma. The RFX program emphasizes<br />

RFP per<strong>for</strong>mance at high current and active feedback control of resistive-wall instabilities<br />

with the most sophisticated sensing and feedback system in the world fusion program. a primary<br />

research goal is also optimization of magnetic self-organization to improve fusion per<strong>for</strong>mance.<br />

(3) a second, smaller european RFP experiment is extrap-t2R in sweden (a=0.18 m, R=1.24 m). it<br />

also has a sophisticated sensing and feedback system, and this program is focused mainly on advanced<br />

control techniques using this system. (4) a new, small aspect ratio RFP has recently commenced<br />

operation in Japan. The aspect ratio is the major radius divided by the minor radius. The<br />

RelaX device (a=0.25 m, R=0.51 m) aims to understand possible benefits of the low aspect ratio<br />

RFP, including the possibility <strong>for</strong> substantial pressure-driven “bootstrap” current.<br />

a number of computational tools are available <strong>for</strong> RFP research. owing to the importance of magnetohydrodynamics<br />

in RFP physics, state-of-the-art nonlinear resistive mhd computation has<br />

long been employed, e.g., the debs code. nonlinear two-fluid (electron and ion fluids) studies are<br />

beginning to use new tools such as nimRod. Gyrokinetic calculations have recently been initiated,<br />

adapting codes developed <strong>for</strong> tokamak research. similarly, simulation tools developed <strong>for</strong><br />

astrophysics studies are being adapted <strong>for</strong> RFP applications. The last major fusion power system<br />

study (titan) was completed around 1990. The titan codes are still available, but they are outdated<br />

and difficult to use.<br />

Scientific issues and <strong>Research</strong> Requirements<br />

eight scientific and technical issues <strong>for</strong> the RFP were identified by taP. The research requirements<br />

<strong>for</strong> each of these are described below. table 2 at the end of this section summarizes the issues and<br />

connections to theory and modeling, and facility capabilities.<br />

tRanSPORt MECHaniSMS anD COnFinEMEnt SCaLing<br />

key dimensionless parameters <strong>for</strong> transport mechanisms in the RFP are the lundquist number,<br />

S = tR /ta ~ ipt 3/2<br />

e /ni 1/2 , and normalized ion gyroradius, r* = ri /a. in these expressions, tR is the<br />

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