Material Science for Nuclear Fusion
Tritium, Lithium-6, Beryllium, Tungsten. Most fusion power plants run deuterium and tritium in a loop — injecting it, burning it in the plasma, recovering unused gas and newly bred tritium, reprocessing it, and injecting it again. Cluster 3 maps every stage of that cycle to the specialized Swiss industry that makes it possible.
01 — The Cycle
Deuterium and tritium fuse in the plasma at over 100 million °C. Almost none of it burns on the first pass — the rest has to be recovered, cleaned, and re-injected, while new tritium is continuously bred to replace what's consumed.
Simplified fusion fuel cycle — injection, storage, management, and exhaust/impurity processing, in continuous loop.
02 — The Materials
Each one is either scarce, hazardous to handle, or both — which is exactly where specialized industrial know-how matters more than raw material access.
Doesn't occur naturally in usable quantities — must be bred in the reactor itself via lithium breeder blankets (breeding ratio > 1 required). ~USD 35,000/g.
The feedstock for tritium breeding. Isotopically pure Li-6 is limited and requires extensive isotope separation — the limiting factor for many breeding-blanket concepts.
Neutron multiplier in breeder blankets — needed as FLiBe (fluorine-lithium-beryllium) breeder and coolant. Handling requires dedicated equipment and engineering.
The plasma-facing material of choice — highest melting point of any metal, used for divertor components that face the reactor's most extreme heat loads.
03 — Why Tritium Is Hard
Tritium's 12.32-year half-life means it can't simply be stockpiled — a fusion power plant has to breed its own supply continuously, in the reactor, faster than it decays.
Every stage of this cycle — breeding, injection, recovery, storage, analysis — maps to specialized Swiss suppliers, engineers, and research labs already working the problem.
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