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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.
J. F. Lyon, B. A. Carreras, K. K. Chipley, M. J. Cole, J. H. Harris, T. C. Jernigan, R. L. Johnson, V. E. Lynch, B. E. Nelson, J. A. Rome, J. Sheffield, P. B. Thompson
Fusion Science and Technology | Volume 10 | Number 2 | September 1986 | Pages 179-226
Technical Paper | Experimental Devices | doi.org/10.13182/FST86-A24973
Articles are hosted by Taylor and Francis Online.
The Advanced Toroidal Facility (ATF), now under construction at Oak Ridge National Laboratory, will be the world's largest stellarator experiment when it begins operation in early 1987. It will have a 2.1-m major radius and a 0.3-m average plasma radius, a magnetic field capability of up to 2 T for a 5-s pulse and up to 1 T steady state, and up to 5 MW of plasma heating. The ATF is designed to study a wide range of toroidal confinement issues, including confinement and stability of high-beta plasmas, low-collisionality transport, impurity behavior, magnetic configuration optimization, and steady-state operation. The ATF is the result of a study of a large number of possible coil configurations. It is an 1 = 2, 12-field-period torsatron with rotational transform between 0.3 and 1 and a plasma aspect ratio of R/ā = 7. This optimized helical field coil configuration permits direct access to a high-beta, second stability region in a flux-conserving manner, and volume-average beta values >8% may be achieved. The poloidal coil system allows study of a large variety of stellarator configurations, including those with a helical magnetic axis, and external control of the fundamental magnetic configuration parameters, including rotational transform, shear, magnetic well, and plasma shape. The ATF consists of two segmented, jointed helical field coils; three sets of poloidal field coils; a thin, helically contoured vacuum vessel; and a thick, segmented, toroidal shell support structure. Its important design features include extensive access for plasma heating and diagnostics, a high degree of construction accuracy, and parallel construction techniques. A description of the ATF torsatron, the physics and engineering reasons for the different design choices, and the expected capabilities of the device are presented.