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Fusion Science and Technology
Latest News
In transition: Commercializing fusion power
Commercial fusion power is closer than ever. There are now around 30 U.S. fusion companies, several of which claim to be on track to connect to the grid as early as the 2030s.
Tokamak and laser inertial confinement approaches benefit from decades of research at facilities such as the National Ignition Facility (NIF) at Lawrence Livermore National Laboratory and ITER, with alternative concepts including stellarator, magnetic mirror, and Z-pinch confinement also making notable progress as private and government funding for fusion increases.
Robert P. Rulko
Nuclear Science and Engineering | Volume 121 | Number 3 | December 1995 | Pages 371-392
Technical Paper | doi.org/10.13182/NSE95-A24141
Articles are hosted by Taylor and Francis Online.
Historically, the even-order PN equations have been considered a less accurate approximation to the transport equation than the odd-order PN-1 equations. This perception has stemmed from two apparent conceptual difficulties imposed by the even-order PN methods— the difficulty in prescribing rigorous boundary conditions for even-order PN equations that contain the odd number of angular flux moments and the discontinuous character of the even-order PN solutions at material interfaces. With the first one of the mentioned even-order PN conceptual problems, a presentation is made of a straightforward and physically-motivated variational procedure based on a new functional that leads from a multigroup planar geometry transport problem to a multigroup P2 problem with clearly and rigorously defined multigroup boundary conditions. These boundary conditions are new and allow neutron transfer between energy groups at the boundary. These boundary conditions are tested by comparing P2, P1, and SN calculations. Our results show that in the test problems considered, the multigroup P2 equations with variational boundary conditions are always more accurate than the P1 multigroup equations with Federighi-Pomraning or Marshak boundary conditions applied to each energy group.