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Second round of Launch Pad selections includes eight newcomers
The National Reactor Innovation Center at Idaho National Laboratory has announced 13 project selections across 12 companies for the Nuclear Energy Launch Pad, a Department of Energy–led program that integrates reactor and fuel facility authorization, testing, and deployment support for private nuclear developers.
The Launch Pad emerged from the Reactor Pilot Program and Fuel Line Pilot Program.
According to INL, projects selected include reactor development and nuclear fuel cycle advancements, including fabrication, enrichment, and conversion technologies.
Glenn T. Sager, George H. Miley, Keith H. Burrell
Fusion Science and Technology | Volume 18 | Number 3 | November 1990 | Pages 389-396
Alpha Particles in Fusion Research | Technical Paper | doi.org/10.13182/FST90-A29272
Articles are hosted by Taylor and Francis Online.
Neoclassical transport of minority suprathernial alpha particles is investigated. This work departs from previous investigations in that (a) the banana-width ordering parameter ρθ/L is not formally restricted to be a small parameter and (b) a linearized collision operator that retains the effects of pitch-angle scattering, electron and ion drag, and speed diffusion is used. A step model approximation for the large-aspect-ratio, circular-cross-section tokamak magnetic field is adopted to simplify the orbit-averaging procedure. Assuming that the suprathermal alphas are in the banana regime, an asymptotic expansion in τB/τs ≪ 1 is carried out. The lowest order distribution is independent of poloidal angle on a drift surface and is completely determined by solving an orbit-averaged drift kinetic equation, A variational problem is derived that is equivalent to this three-dimensional, inhomogeneous differential equation. A similar procedure yields an expression for the first-order component f1. Knowledge of f1 is sufficient to obtain expressions for particle and heat fluxes directly from the definitions or from alternate expressions. Extension of this model to account for loss regions in phase space is outlined.