Fusion Physics

Aneutronic Fuel Cycle

A fusion fuel cycle that produces few or no neutrons, avoiding the radiation damage and activation problems of D-T fusion. The most studied aneutronic reaction is p-B11 (proton + boron-11 → 3 alpha particles), which requires temperatures of ~500 keV — far higher than D-T. Aneutronic fusion would simplify reactor design by eliminating neutron shielding and tritium breeding requirements.

Frequently Asked Questions

What is Aneutronic Fuel Cycle?
A fusion fuel cycle that produces few or no neutrons, avoiding the radiation damage and activation problems of D-T fusion. The most studied aneutronic reaction is p-B11 (proton + boron-11 → 3 alpha particles), which requires temperatures of ~500 keV — far higher than D-T. Aneutronic fusion would simplify reactor design by eliminating neutron shielding and tritium breeding requirements.
How does Aneutronic Fuel Cycle relate to other concepts?
Aneutronic Fuel Cycle is closely related to Neutron Flux, Neutron Degradation. These relationships are documented in the research glossary and cross-referenced with primary source documents.
When did Aneutronic Fuel Cycle appear in the research timeline?
Aneutronic Fuel Cycle is referenced in 3 timeline events, including "MARAUDER program begins — AFRL fires compact toroid plasmoids as weapons" (1990). The timeline provides chronological context for the development and application of this concept.