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

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to demonstrate that steady and transient heat flux control and other PFc solutions will be compatible<br />

with optimal core plasmas, the facility to support this Thrust must have the ability to obtain<br />

a robust edge pedestal. an important parameter <strong>for</strong> obtaining demo-like pedestal behavior<br />

is the edge bootstrap current profile that strongly affects edge stability and elm dynamics. to approach<br />

demo conditions the edge collisionality must be low. study of pedestal issues, as well as<br />

radiative mantle solutions, will add an additional requirement on the input power to be a significant<br />

multiple of the power required to obtain high confinement mode (h-mode). taken together<br />

these capabilities will produce a robust pedestal with demo-like elm characteristics as a test bed<br />

<strong>for</strong> the most promising techniques and technologies <strong>for</strong> controlling both steady-state and transient<br />

heat flux.<br />

Plasma sustainment is also an important characteristic of the facility to support this Thrust in<br />

achieving very long pulses. The facility should be designed to allow <strong>for</strong> testing a variety of heating<br />

and current drive issues and options. design of heating and current drive systems employing ion<br />

cyclotron resonance heating and lower-hybrid must include an examination of coupling efficiency<br />

through the expected dense boundary plasma and the strong pressure gradients in the pedestal<br />

into the core plasma. The launching structures must endure long periods of interaction with the<br />

boundary plasma. The design of neutral beam, electron cyclotron current drive and electron cyclotron<br />

heating systems will generally be less sensitive to edge issues, but here the focus will be<br />

on their capabilities <strong>for</strong> controlling the core over a sufficient range of densities, due to accessibility<br />

physics.<br />

another demo characteristic that will not be addressed by current or planned facilities is that<br />

of high temperatures <strong>for</strong> all components; this will be required in demo because higher operating<br />

temperatures lead to higher thermal conversion efficiency to electricity. The capability to attain<br />

such high temperatures (in the range 500 o c to 1000 o c), as well as explore their effects on<br />

core and boundary characteristics, is central to the goals of this Thrust. he coolant technology<br />

options are currently the most strongly considered <strong>for</strong> demo, but liquid metal coolants should<br />

also be considered. tungsten PFcs will likely have an operational temperature window above the<br />

ductile to brittle transition temperature, but below the limit due to recrystallization. liquid-surface<br />

PFcs are likely to have a lower maximum operating temperature due to their higher evaporation<br />

and sputtering rates at high temperature. techniques to monitor and control dust production<br />

from solid PFc surfaces and evaporated material from liquid PFc surfaces will need to be qualified.<br />

Fuel retention and permeation into PFcs will also have a strong temperature dependence,<br />

and thus control of temperature will be needed to allow exploration of the effect on retention in<br />

PFcs and on the overall fuel cycle. Given the history of tokamaks showing a strong dependence<br />

of core energy and particle confinement on recycling and surface conditions, active control of surface<br />

temperatures could also be important <strong>for</strong> maximizing the per<strong>for</strong>mance of the core plasma.<br />

While the ultimate goal <strong>for</strong> a steady-state demo is pulse lengths of order 10 7 sec with >80%<br />

duty factor, design and science trade-offs (e.g., costs of pulse length vs. gains in physics explored)<br />

should be considered in determining the appropriate specifications <strong>for</strong> a facility to support Thrust<br />

12. in general, the requirement is that the cumulative particle and energy fluence to the plasma<br />

boundary and materials reach a level where the long-term evolution of the PFcs, due to erosion,<br />

fuel recycling, macroscopic PFc thickness changes (positive and negative) and the fuel residing<br />

328

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