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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.”
Robert R. Peterson
Fusion Science and Technology | Volume 13 | Number 2 | February 1988 | Pages 279-289
Technical Paper | Heavy-Ion Fusion | doi.org/10.13182/FST88-A25105
Articles are hosted by Taylor and Francis Online.
The limits on the cavity gas density required for beam propagation and condensation times for material vaporized by target explosions can determine the maximum repetition rate of heavy-ion fusion (HIF) driven reactors. If the ions are ballistically focused onto the target, the cavity gas must have a density below roughly 3 × 1012cm-3 at the time of propagation; other propagation schemes may allow densities as high as 1 Torr or more. In some reactor designs, several kilograms of material may be vaporized from the target chamber walls by target-generated X rays, raising the average density in the cavity to 3 × 1018 cm-3 or more. A one-dimensional combined radiation hydrodynamics and vaporization and condensation computer code has been used to simulate the vaporization and condensation of material in the target chambers of HIF reactors. Repetition rates in excess of 1 Hz are possible in the three types of target chambers studied. Means of increasing allowable repetition rates are discussed.