ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Explore membership for yourself or for your organization.
Conference Spotlight
2026 Nuclear Energy Conference & Expo (NECX)
August 24–27, 2026
Dallas, TX|Hilton Anatole
Latest Magazine Issues
Aug 2026
Jan 2026
2026
Latest Journal Issues
Nuclear Science and Engineering
October 2026
Nuclear Technology
September 2026
Fusion Science and Technology
August 2026
Latest News
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.
Nancy Ma, John Walker, Tess Moon, Thanh Hua, Basil Picologlou
Fusion Science and Technology | Volume 25 | Number 4 | July 1994 | Pages 398-410
Technical Paper | Blanket Engineering | doi.org/10.13182/FST94-A30246
Articles are hosted by Taylor and Francis Online.
The three-dimensional magnetohydrodynamic (MHD) flow in a pair of finite-length, parallel, equal-area square ducts, connected to single rectangular ducts upstream and downstream is examined. Each duct has a different liner with a thin sheet of metal that is in contact with the coolant and that is electrically insulated from structural walls and from other duct liners, except at the junctions. The objective is to concentrate most of the flow in one of the two parallel ducts by making its metal wall much thinner than that of its neighbor, so that its MHD resistance to flow is smaller. Flow ratios approaching ten are obtained with typical values of the wall conductance ratios, which are proportional to the wall thicknesses. The flow at the entrance is complex, with some flow entering the low-velocity duct and then returning to the entrance, where it swirls around the upstream edge of the common wall to enter the high-velocity duct. The balance between three-dimensional and fully developed pressure drops is investigated as a function of the distance between the entrance and the exit of the parallel ducts.