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However, full CFD modeling and simulation toward the whole blanket flow channels is computationally expensive.
The analysis indicates that as low as 2 MPa of pressure difference over the blanket modules will ensure substantial evacuation of the water in blankets with just a few percent remaining in the blanket flow channels.
The blanket flow scheme enables operating Pb-17Li at a high outlet temperature (about 1100 °C) for high power cycle efficiency while maintaining SiCf/SiC at a substantially lower temperature consistent with allowable limits.
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As an illustration, two blanket flows have been considered: Pb 17Li flow in a channel with a silicon carbide flow channel insert, and Li flow in a channel with insulating coating.
Liquid metal HCLL blanket flows are expected to be mainly driven by buoyancy forces caused by non-isothermal operating conditions due to neutron volumetric heating, since only a weak forced flow is required for tritium extraction.
Leave the rest of the blanket flowing.
In the DCLL blanket, the flow channel insert (FCI) is a critical component.
The power core uses an advanced 'dual-cooled' breeding blanket with flowing PbLi breeder and He-cooled ferritic steel structures.
The result is an advanced helium-cooled ferritic steel blanket with flowing PbLi breeder and tungsten plasma-interactive components.
Although also relevant to the design of fusion reactor blankets, the flow entering the fringing field of a magnet remains unexplored because its high intricacy precludes any simplification of the governing equations.
The power core uses an advanced 'dual-cooled' breeding blanket with flowing PbLi breeder and He-cooled ferritic steel structures that can achieve a thermal conversion efficiency of ∼45%.
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