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Conference Spotlight
Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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NECX debut: Shaping the next era of energy
The sold-out inaugural Nuclear Energy Conference & Expo (NECX) got off to a bumping start in Atlanta, Ga., Tuesday morning with an opening plenary that felt like part dance party and part highlight reel showing off the latest industry achievements.
That intro left the audience pumped up for Entergy’s CEO and NEI chair Drew Marsh, who welcomed everyone to the event, hosted jointly by the American Nuclear Society and the Nuclear Energy Institute. He spoke to a full house of more than 1,300 attendees, promising a blend of science, technology, policy, and advocacy centered around the future of nuclear energy.
Michael J. Zavisca, J. Michael Doster
Nuclear Technology | Volume 109 | Number 1 | January 1995 | Pages 76-86
Technical Paper | Heat Transfer and Fluid Flow | doi.org/10.13182/NT95-A35069
Articles are hosted by Taylor and Francis Online.
Finite difference schemes currently applied to the modeling of two-phase flows in flow networks exhibit difficulties in properly simulating certain spatial and temporal discontinuities. These discontinuities include points along the one-dimensional flow axis where density and other thermophysical properties become discontinuous or experience rapid state domain changes. A methodology for treating spatial and temporal discontinuities is presented. This methodology consists of three main features: (a) subnode time-averaged do-noring of thermodynamic properties, (b) a variable pressure-at-discontinuity staggered mesh discretization, and (c) a variable point state equation linearization. The proposed scheme is similar in form to standard semi-implicit, staggered mesh discretizations, requires little extra overhead, and results in substantially improved accuracy and code execution times. Comparisons are made with standard time and spatial discretizations, as well as with two simpler alternate methods for recognizing and tracking discontinuities. The first of these attempts is to adjust the time-step size such that the fluid discontinuity arrives at a node boundary, or a change in fluid state occurs precisely at the end of a time advancement. The second attempts to redistribute mass and energy to correct for improperly donored values when a discontinuity crosses a node boundary during a time step. Neither of these alternatives proved adequate.