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

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gap: Current understanding of strength-ductility/fracture toughness relationships is inadequate to simultaneously<br />

achieve high-strength and high-ductility and fracture toughness.<br />

The lower operating temperature limit <strong>for</strong> most fusion structural materials is determined by radiation<br />

hardening and embrittlement. at irradiation temperatures less than about 30% of the<br />

absolute melting point the defect structures produced by neutron damage significantly increase<br />

tensile strength, and decrease ductility and fracture toughness. although the experimental parameters<br />

that cause radiation hardening and embrittlement are well known, the fundamental<br />

mechanisms responsible <strong>for</strong> loss of ductility are not fully understood. improved multi-scale models<br />

coupled with appropriate experiments are needed to determine the causes of ductility loss in<br />

irradiated metals and suggest possible metallurgical solutions to ameliorate this effect.<br />

standard measurement methods of fracture toughness are not adequate <strong>for</strong> fusion power systems<br />

because the underlying principles of elastic-plastic fracture mechanics are violated <strong>for</strong> small<br />

specimens or in thin-walled structures with shallow cracks. a new method has been developed to<br />

provide a highly efficient means of acquiring and applying fracture toughness in<strong>for</strong>mation, but<br />

further work is needed to verify its technical basis and account <strong>for</strong> embrittlement effects due to<br />

synergistic hardening and non-hardening mechanisms including helium and hydrogen.<br />

gap: Predictive, physics-based, multi-scale models of materials behavior in the fusion environment are<br />

needed <strong>for</strong> development of advanced materials.<br />

The cost and time required to design, per<strong>for</strong>m and examine materials from reactor irradiation<br />

experiments is high. Further, there is a combinatorial problem in that the broad range of materials,<br />

phenomena, irradiation variables and variable combinations makes a purely experimental<br />

approach intractable <strong>for</strong> fusion materials development. Robust computational models provide a<br />

means to reevaluate existing data, optimize the design and execution of new experiments, and<br />

interpret the results from those experiments. Physically based multi-scale models describing irradiation<br />

and mechanical damage processes <strong>for</strong> fusion applications are being developed, but numerous<br />

fundamental details remain to be fully resolved. models of key properties that simultaneously<br />

span spatial and temporal scales ranging from the atomistic to the continuum and from<br />

sub-picosecond to years are urgently needed.<br />

gap: Fundamental understanding of high-temperature de<strong>for</strong>mation mechanisms is lacking.<br />

For fusion to be an economically attractive power source it must possess high thermodynamic<br />

efficiency. This increases the demand <strong>for</strong> structural materials capable of operation at high temperatures<br />

where materials can plastically de<strong>for</strong>m at stresses well below the elastic limit. This phenomenon<br />

is known as thermal creep and is typically a concern <strong>for</strong> materials operating at temperatures<br />

greater than about half the absolute melting point. While considerable research has been<br />

per<strong>for</strong>med on the mechanisms of thermal creep, only an elementary knowledge of the rate controlling<br />

processes is currently available. Present models tend to be semi-empirical in nature, do<br />

not fully capture the relevant physics associated with the de<strong>for</strong>mation mechanisms operating at<br />

these temperatures, and generally have limited predictive capability, even <strong>for</strong> relatively simple<br />

metals and alloys.<br />

154

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