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

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introduction<br />

Thrust 11 addresses the fundamental engineering science and the technology required to develop<br />

components that can handle the higher heat fluxes in a power-producing fusion reactor. much of<br />

this technology is useful in alternate concepts as well as conventional toroidal devices. Plasma facing<br />

components such as those in the first wall and divertor, and internal components (ics) such as<br />

radiofrequency launchers, Faraday shields and electron cyclotron resonance heating (ecRh) mirrors,<br />

will need to operate at higher temperatures and handle particle and heat loads much higher<br />

than iteR. First wall and blanket components may consist of refractory alloys, vanadium alloys,<br />

reduced activation ferritic martinsitic steel (RaFms), oxide dispersion strengthened ferritic steel,<br />

and silicon carbide composite. Power conversion systems <strong>for</strong> demo will require heat sinks <strong>for</strong> plasma<br />

facing components that can operate at high temperatures as part of a highly efficient closed<br />

brayton cycle. Plasma facing components could endure peak heat fluxes in excess of 10 mW/m 2<br />

at the divertor and localized peak heat fluxes as high as 0.5-2 mW/m 2 on the first wall and internal<br />

components. since these components are an integral part of the power conversion system, this<br />

work must connect closely to Thrust 13 to ensure careful integration with blanket requirements.<br />

The technologies and components developed in this Thrust feed directly into Thrust 12, and likewise<br />

benefit from the integrated testing in Thrust 12’s toroidal confinement facility. in addition,<br />

the activities in Thrust 11 focus on the bulk PFc properties and complement the basic plasma-surface<br />

interaction research of the first few micrometers described in Thrust 10.<br />

a close coupling must exist between the PFc materials research focused on the development of<br />

more ductile refractories and improved joining techniques in Thrust 14 with PFc development in<br />

Thrust 11. both free-surface liquid metal PFcs and ducted liquid metal and gas coolants in solid<br />

PFcs are under consideration. currently, the technology Readiness level (tRl) (mankins, 1995)<br />

<strong>for</strong> helium-cooled components is approximately 3 and that <strong>for</strong> liquid metal PFcs is about 4. more<br />

fundamental research is required to assess the temperature limits of free-surface liquid metal PFcs<br />

and devise efficient power conversion systems that address this limitation. certainly, further development<br />

is required to reach the technology readiness level required <strong>for</strong> demo (9-10). Progress is<br />

stymied by a lack of investment in high-temperature materials and liquid metal research, and the<br />

limited capabilities of our present test loops and equipment to operate at the required high temperatures<br />

and pressures. Unless the community addresses this need in a timely manner, we will<br />

not have the actively cooled components required <strong>for</strong> high-temperature applications like demo, or<br />

even the intermediate facilities needed to fulfill the goals described in Thrusts 12 and 13.<br />

advanced Cooling technologies <strong>for</strong> Solid PFCs<br />

helium cooling has many advantages in a nuclear system due to its inherently safe, inert chemical<br />

properties; lack of corrosion; vacuum compatibility; single-phase heat transfer without the possibility<br />

of a critical heat flux (chF) excursion; lack of neutron activation; and easy separation from<br />

tritium. most importantly <strong>for</strong> demo, helium is the fluid of choice <strong>for</strong> a highly efficient, high-temperature<br />

brayton cycle exhibiting minimal wear and corrosion of gas turbines, and the closed cycle<br />

helps contain any tritium reaching the coolant.<br />

one key disadvantage of helium is its low thermal mass, rc p , that is less than 1% of water. This<br />

necessitates the use of high mass flow rates and greatly enhanced heat transfer area and turbulence<br />

promoters <strong>for</strong> efficient heat transfer. tremendous progress occurred in this regard during<br />

320

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