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Radiation Protection & Shielding
The Radiation Protection and Shielding Division is developing and promoting radiation protection and shielding aspects of nuclear science and technology — including interaction of nuclear radiation with materials and biological systems, instruments and techniques for the measurement of nuclear radiation fields, and radiation shield design and evaluation.
Meeting Spotlight
Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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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Latest News
Hinkley Point C gets over $6 billion in financing from Apollo
U.S.-based private capital group Apollo Global has committed £4.5 billion ($6.13 billion) in financing to EDF Energy, primarily to support the U.K.’s Hinkley Point C station. The move addresses funding needs left unmet since China General Nuclear Power Corporation—which originally planned to pay for one-third of the project—exited in 2023 amid U.K. government efforts to reduce Chinese involvement.
John T. Hogan
Nuclear Science and Engineering | Volume 64 | Number 1 | September 1977 | Pages 2-17
Technical Paper | doi.org/10.13182/NSE77-A27072
Articles are hosted by Taylor and Francis Online.
We describe the Oak Ridge Tokamak Transport Code. This code computes the number, momentum, and energy balance for particles and follows the evolution of tokamak poloidal and toroidal fields. The magnetic geometry is two dimensional, with solutions of the Grad-Shafranov equation providing flux surface topology. The velocity-space description of fast injected ions is also two dimensional, and the Fokker-Planck equation is solved for the injected species. Transport per se involves six coupled nonlinear partial differential equations, while the treatment of the plasma-wall interface requires the solution of 14 zero-dimensional rate equations. The XSDRN neutron and photon transport code has been adapted to serve as a neutral gas transport module. Some examples illustrating problems of present interest are presented.