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2025 ANS Winter Conference & Expo
November 9–12, 2025
Washington, DC|Washington Hilton
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A webinar, and a new opportunity to take ANS’s CNP Exam
Applications are now open for the fall 2025 testing period for the American Nuclear Society’s Certified Nuclear Professional (CNP) exam. Applications are being accepted through October 14, and only three testing sessions are offered per year, so it is important to apply soon. The test will be administered from November 12 through December 16. To check eligibility and schedule your exam, click here.
In addition, taking place tomorrow (September 19) from 12:00 noon to 1:00 p.m. (CDT), ANS will host a new webinar, “How to Become a Certified Nuclear Professional.” More information is available below in this article.
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.