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

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of 40%.) localized instabilities (tearing modes, edge localized modes) were mitigated or<br />

eliminated via lithium application, and record stability levels (normalized beta of 7.2)<br />

were reached. kinetic theory has provided understanding of the complex relationship<br />

between global instabilities and plasma rotation. The connection between observed fast<br />

particle loss and toroidal alfvén instabilities/theory was established.<br />

• control of high beta st plasmas: active control of resistive wall modes and maintenance<br />

of favorable plasma rotation profiles decreased the disruption probability <strong>for</strong> long-pulse<br />

plasmas while exceeding the stability limit <strong>for</strong> nonrotating plasmas by over 50%. Rotation<br />

is controlled by 3-d magnetic fields in plasmas with strong momentum input.<br />

• integration and sustainment at low aspect ratio: stability levels approaching that needed<br />

<strong>for</strong> a fusion component testing device were sustained <strong>for</strong> significant duration (3-4 resistive<br />

diffusion times) with a majority of the plasma current provided noninductively.<br />

Reversed Field Pinch<br />

The reversed field pinch (RFP) is an axisymmetric configuration in which electrical current in<br />

the plasma generates most of the magnetic field. The requirements on the external magnets are<br />

there<strong>for</strong>e greatly reduced. The RFP has a high ratio of plasma pressure to magnetic pressure. The<br />

ohmic heating from the plasma current could reduce or eliminate the need <strong>for</strong> complicated auxiliary<br />

heating systems. These features could yield a high power density fusion energy system with<br />

simple construction. highlights of RFP research include:<br />

• a 10-fold increase in energy confinement is obtained when fluctuations in the magnetic<br />

field are reduced using active control of the plasma current profile. This confinement is<br />

comparable to that in a tokamak of the same size and plasma current. high-temperature<br />

plasmas are produced without auxiliary (non-ohmic) heating, with electron temperature<br />

t e ~ 2 kev and ion temperature t i ~ 1 kev.<br />

• high-current plasmas (up to 1.5 ma in RFX-mod) spontaneously generate a helical<br />

magnetic field in the plasma core. The energy confinement time is improved in these sel<strong>for</strong>ganized,<br />

quasi-helical plasmas. The confinement time is increasing with plasma current.<br />

• Plasmas with thermal pressure exceeding theoretical limits <strong>for</strong> interchange and magnetic<br />

tearing stability are produced without exhibiting fast disruptive behavior.<br />

• active feedback stabilization is now routine when the plasma is contained in a thin-walled<br />

metal shell. discharge lengths up to 0.5 s are obtained, which is more than ten growth<br />

times <strong>for</strong> thin-shell instabilities that occur without feedback control.<br />

• Up to 10% of the plasma current has been sustained using low frequency ac induction<br />

(helicity injection), a promising approach <strong>for</strong> efficient steady-state operation of the RFP.<br />

• The physics of magnetic self-organization has been advanced by RFP (and compact<br />

torus) research, with strong connections to plasma astrophysics. areas include dynamo<br />

processes, momentum transport, collisionless ion heating, and magnetic reconnection<br />

and turbulence.<br />

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