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
Jun 2026
Jan 2026
2026
Latest Journal Issues
Nuclear Science and Engineering
July 2026
Nuclear Technology
June 2026
Fusion Science and Technology
May 2026
Latest News
North American construction is back—smaller and faster—at OPG’s Darlington
“The nuclear renaissance is real here,” said Ontario Power Generation’s Subo Sinnathamby on May 8, one year to the day after OPG secured a final investment decision to build the first of four planned BWRX-300 reactors at its Darlington nuclear power plant, and shortly after the new reactor’s foundation was lifted into place. “We got our license to construct in April and our [final investment decision] in May, and we’ve been off to the races since.”
Keiji Miyazaki, Shoji Inoue, Nobuo Yamaoka, Tomomitsu Horiba, Kazushige Yokomizo
Fusion Science and Technology | Volume 10 | Number 3 | November 1986 | Pages 830-836
Liquid-Metal Blankets and Magnetohydrodynamic Effects | Proceedings of the Seveth Topical Meeting on the Technology of Fusion Energy (Reno, Nevada, June 15–19, 1986) | doi.org/10.13182/FST10-830
Articles are hosted by Taylor and Francis Online.
The MHD pressure drop was measured by providing a lithium circulation loop of 40 lit/min and 0.3MPa head with a square test section of 2a=15.7mm × 2b=15.7mm or a rectangular one of 2a=26.8mm × 2b=ll.lmm inner cross-section made of tw=2.1mm thick 304-SS walls. The experiment covered ranges of B=0.2–1.5T (Ha=200–2100), U=0.2–4.0m/sec (Re=500–38000), and TLi=309–380°C. Theoretical prediction was made on an assumption of a uniform electric current density, neglecting the friction with walls. The MHD pressure gradient -dP/dz is given by -dP/dz = KpσfUB2 where Kp= C/(l+a/3b+C) and C=σwtw/σfa. The theory agreed well with the experimental data for both the square and rectangular test sections. Under the ununiform magnetic field of the exit, the pressure drop data agreed with an approximated prediction of Δ P= ∫KpσfUB2(z)dz.