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Division Spotlight
Fuel Cycle & Waste Management
Devoted to all aspects of the nuclear fuel cycle including waste management, worldwide. Division specific areas of interest and involvement include uranium conversion and enrichment; fuel fabrication, management (in-core and ex-core) and recycle; transportation; safeguards; high-level, low-level and mixed waste management and disposal; public policy and program management; decontamination and decommissioning environmental restoration; and excess weapons materials disposition.
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2025 ANS Annual Conference
June 15–18, 2025
Chicago, IL|Chicago Marriott Downtown
Standards Program
The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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BREAKING NEWS: Trump issues executive orders to overhaul nuclear industry
The Trump administration issued four executive orders today aimed at boosting domestic nuclear deployment ahead of significant growth in projected energy demand in the coming decades.
During a live signing in the Oval Office, President Donald Trump called nuclear “a hot industry,” adding, “It’s a brilliant industry. [But] you’ve got to do it right. It’s become very safe and environmental.”
D. Stöver, R. Hecker
Nuclear Technology | Volume 35 | Number 2 | September 1977 | Pages 465-474
Fission Product Release | Coated Particle Fuel / Fuel | doi.org/10.13182/NT77-A31906
Articles are hosted by Taylor and Francis Online.
Release data of cesium in Biso low-temperature isotropic (LTI) and high-temperature isotropic (HTI) coated particles are presented. Experimental and theoretical methods are briefly discussed. From the analysis of our experiments, kernel diffusion coefficients are calculated covering the kernel burnup range from 0.2 to 16% FIMA. At FIMA values ≥5%, cesium release is governed by the relatively low activation energy of ∼19 kcal/mole (79.6 kJ/mole), and even at temperatures as low as ∼900°C (1173 K), kernel retention remains low. The outer pyrocarbon layer acts as the release rate controlling barrier for both LTI and HTI coatings. Diffusion coefficients in the temperature range from 1000 to 1500°C (1273 to 1773 K) for LTI coatings and 1250 to 1600°C (1523 to 1873 K) for HTI coatings have been derived and lead to the following Arrhenius equations: On the basis of these data, releases for high-temperature-reactor cores can be calculated.