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

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3-d shaping, and beta control to significantly reduce disruption probability and variations<br />

in fusion reactivity.<br />

• demonstrate sustained operation at normalized beta values beyond st-ctF, approaching<br />

demo levels, to reduce per<strong>for</strong>mance risk, and rapidly achieve neutron fluence goals.<br />

• develop validated computational tools <strong>for</strong> the experimental research actions.<br />

Links to other thrusts: Thrust 2 (transient/disruption control), Thrust 5 (continuous,<br />

high-per<strong>for</strong>mance operations), Thrust 6 (predictive modeling), Thrust 17 (3-D fields <strong>for</strong><br />

stability), Thrust 18 (low field)<br />

5. employ energetic particle beams, plasma waves, particle control, and core fueling techniques to<br />

maintain the current, and control the plasma profiles.<br />

The sustainment of high-per<strong>for</strong>mance integrated st scenarios requires full noninductive current<br />

drive and sufficient control of the plasma profiles. Future st applications are expected to rely on<br />

a combination of current drive sources, including the neoclassical bootstrap current, nbi current<br />

drive, and plasma wave current drive (fast-wave, electron bernstein, and/or electron cyclotron).<br />

spherical torus operation at high plasma current (4-10 ma) will require access to a new st parameter<br />

regime of sustained low collisionality, high thermal confinement, and high beta to provide<br />

high current drive efficiency and high bootstrap fraction. This regime must be self-consistently<br />

accessible with the heating and current-drive techniques proposed <strong>for</strong> st applications — including<br />

during plasma current startup and ramp-up. control of the nbi and wave current drive can in<br />

principle be achieved by varying injection parameters to vary the power deposition profile. however,<br />

the bootstrap current profile is largely determined by the plasma thermal and particle transport.<br />

Thus, new control techniques must be developed to optimize and ultimately control the plasma<br />

pressure profile to control the current profile.<br />

actions:<br />

• access one to two orders of magnitude lower collisionality by increasing plasma temperature<br />

with a two to four-fold increase in magnetic field, plasma current, and heating power.<br />

• implement particle pumping to achieve factor of two to four reduction in normalized<br />

density to support access to very low collisionality values. Pumping techniques <strong>for</strong> access<br />

to very low recycling regimes should also be investigated.<br />

• assess and optimize the impact of reduced collisionality on core and edge transport — in<br />

particular, the impact of transport on the bootstrap current density profiles.<br />

• test the ability of improved pumping and low recycling, combined with the development<br />

of deep core fueling, to enable modification and control of the core transport and pressure<br />

profile (and there<strong>for</strong>e the bootstrap current profile) <strong>for</strong> plasma sustainment and optimal<br />

stability.<br />

365

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