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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.”
Thomas Hladschik, Klaus Schoepf
Fusion Science and Technology | Volume 26 | Number 3 | November 1994 | Pages 588-592
Plasma Heating and Current Drive, Plasma Engineering | Proceedings of the Eleventh Topical Meeting on the Technology of Fusion Energy New Orleans, Louisiana June 19-23, 1994 | doi.org/10.13182/FST94-A40221
Articles are hosted by Taylor and Francis Online.
In ITER the main loss mechanism of fast fusion alpha particles is expected to be due to toroidal field (TF) ripples caused by the finite number of TF coils. The associated radial diffusion of fast alphas is specified by an energy and space dependent diffusion coefficient which can be extended to account also for toroidal Alfven eigenmode (TAE) diffusion. Energy transfer from the fast alphas to the thermal background plasma is considered to occur due to Coulomb collisions and nuclear elastic scattering (NES). The α-transport is described here by a reduced slowing down kinetic equation of which the numerical solution provides for the energy-, space- and time-dependent alpha particle distribution in the tokamak plasma. This alpha distribution then constitutes the basis for a determinative calculation of the actual fusion power allocation to each distinct background species. Though TAE diffusion alone is not a significant fusion power loss mechanism, our recent calculations indicate that the coaction of TF-ripple (TFR) and TAE transport processes synergisticly results in a substantial reduction of fusion alpha power deposition.