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

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trol of the energy, impact angle, and species of bombarding ions onto well-controlled and characterized<br />

target surfaces. more sophisticated single-effect science ion-beam facilities equipped with<br />

in situ surface diagnosis can study more complex dynamic mechanisms such as surface mixing,<br />

morphology evolution and phase-dependent erosion, providing surface-response code validation.<br />

Facilities that per<strong>for</strong>m plasma bombardment of surfaces allow the study of synergistic effects<br />

that are limited using ion beam experiments. These plasma experiments allow macroscopic Pmi<br />

processes to be studied, such as erosion, redeposition, and hydrogenic retention, and can validate<br />

models of these processes, albeit not in the full demo plasma regime. a combination of ion-beam<br />

analysis in situ during plasma-material exposure provides direct measurement of plasma dynamics<br />

and surface evolution during exposure, and is essential to Psi basic science and development.<br />

as part of this research Thrust, resources <strong>for</strong> both existing ion beam and plasma bombardment<br />

facilities should be increased to enhance predictive capability and understanding on Psi issues.<br />

Further synergistic effects are expected to be important in the demo Psi environment that cannot<br />

be addressed in the experiments described, motivating a new class of facility. For example,<br />

the erosion and redeposition process will ultimately be determined by the properties of redeposited<br />

layers. to simulate this, experiments need to be per<strong>for</strong>med in the “strongly coupled” regime<br />

where eroded material is ionized in the plasma and returned to the surface. This requires a facility<br />

with characteristic dimensions larger than the neutral mean free path, which equates to a<br />

large plasma cross-section operating at very high density (>10 20 m -3 ). Furthermore, achievement<br />

of erosion conditions relevant to demo requires particle fluxes greater than 10 23 ions/m 2 /s and<br />

the ability to run <strong>for</strong> extremely long pulses, which further enhance the redeposited layers. very<br />

high density is also required <strong>for</strong> model validation in optically thick regimes to address the gap in<br />

radiation transport. assessment of retention of tritium and helium at demo-relevant parameters<br />

requires the ability to test materials at very high temperatures (> 600 o c). This can be readily<br />

achieved in the presence of very high plasma heat flux, which would also enable this device to<br />

per<strong>for</strong>m tests of materials <strong>for</strong> PFcs and internal components. an important capability would be<br />

the qualification to handle neutron-irradiated samples. The neutron damage that will be present<br />

in demo will have a profound impact on near-surface and bulk materials properties, affecting,<br />

<strong>for</strong> example, tritium retention as well as heat transfer and material joints in internal components.<br />

The ability to measure these effects with rapid turnaround of experiments is needed.<br />

The new class of facility described can be characterized by its ability to fully simulate the demo<br />

divertor. such a facility should have the following characteristics, which would fill many of the<br />

gaps requiring an integrated effects approach:<br />

• Particle flux > 10 23 m -2 s -1 , and target heat fluxes up to 20 mW/m 2 , delivered to target<br />

materials with inclined surfaces operating at elevated temperatures (> 600 o c).<br />

• large plasma area, ~100 cm 2 , to produce a strongly coupled plasma simulating detached<br />

conditions in a divertor. This will allow <strong>for</strong> the testing of small components and multilayered<br />

materials used, <strong>for</strong> instance, in antenna structures and microwave launchers.<br />

• ability to handle hazardous materials, such as beryllium, and neutron-irradiated material<br />

samples with significant displacement per atom.<br />

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