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

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• study FRc stability at small ion gyroradius in a new or upgraded facility with energetic ion<br />

sources. success will enable integrated tests of stability, confinement, and sustainment.<br />

• develop improved current sustainment methods <strong>for</strong> the spheromak. small experiments<br />

will feed trans<strong>for</strong>mational ideas to a larger facility to test integrated confinement and<br />

sustainment.<br />

• extend confinement scaling and demonstrate current sustainment at high temperature in<br />

a new large-current RFP. a staged, upgradeable facility would eventually demonstrate nearburning<br />

plasma conditions with integrated plasma-boundary and magnetohydrodynamic<br />

(mhd) stability control.<br />

• Quantify the benefits of low external field and ct geometry in system studies with<br />

updated physics and engineering in<strong>for</strong>mation. evaluate pulsed vs. steady-state reactor<br />

operation.<br />

Scientific and technical <strong>Research</strong><br />

minimizing the external magnetization required to confine fusion plasma would be a major advance<br />

toward making fusion power an economical reality. This goal guides research ef<strong>for</strong>ts <strong>for</strong><br />

the RFP, spheromak, and FRc magnetic configurations and motivates research that answers important<br />

scientific questions. magnetic fluctuations arise more easily without a large externally<br />

imposed stabilizing field, and this affects both plasma stability and confinement quality. Understanding<br />

the scaling of fluctuations is crucial to predict reactor-grade per<strong>for</strong>mance. efficient<br />

plasma current drive is vital, and many of the techniques are distinct from methods used <strong>for</strong> tokamaks.<br />

control of the plasma boundary is essential <strong>for</strong> any fusion system, and optimized solutions<br />

will depend to some degree on magnetic geometry. While the integration of stability, confinement,<br />

and boundary control and other scientific challenges are particular <strong>for</strong> any magnetic<br />

configuration, the underlying physics has a large degree of commonality.<br />

The similarities of the scientific issues <strong>for</strong> low external-field configurations help define a unified<br />

thrust; nevertheless, the configurations described in this Thrust are distinct and offer unique approaches<br />

to achieving a fusion power source. each of them requires separate experimental work<br />

but contributes to a common physics understanding. The magnetic profile of the RFP is characteristically<br />

paramagnetic with the magnetic field orientation changing from toroidal in the core to<br />

purely poloidal near the edge. The profile there<strong>for</strong>e has large negative shear, which enhances mhd<br />

stability to interchange distortion at moderately high plasma-b (the ratio of plasma pressure to<br />

magnetic energy density). also, many robustly damped helical modes resonate within the plasma,<br />

enhancing nonlinear stability. The toroidal geometry facilitates external control of the magnetic<br />

field at the surface of the plasma. This control has been used to achieve high confinement, and it<br />

underlies the RFP scheme <strong>for</strong> ac current drive.<br />

engineering requirements are further simplified <strong>for</strong> the two ct configurations. The plasma-containment<br />

volumes are basically cylindrical with no components placed along the geometric axis.<br />

access to all plasma facing components is there<strong>for</strong>e relatively simple. The absence of external toroidal<br />

field coils allows more flexibility <strong>for</strong> designing the divertor systems that strongly influence<br />

edge plasma conditions while channeling hot plasma exhaust. however, qualitative differences<br />

380

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