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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.”
Yasuhiro Suzuki
Fusion Science and Technology | Volume 59 | Number 3 | April 2011 | Page 626
Appendix A | Fourth ITER International Summer School (IISS2010) / Extended Abstracts | doi.org/10.13182/FST11-A11707
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The stellarator and heliotron are alternate candidates for magnetically confined fusion devices. A major difference is the source of the rotational transform [iota] = 1/q. In tokamaks, the rotational transform [iota] is produced by coupling the symmetric toroidal field and the poloidal field produced by the plasma current along the toroidal direction. Strictly speaking, the tokamak configuration can be assumed to be a two-dimensional (2-D) system. Note that the rotational transform does not exist for the vacuum. For stellarator and heliotron configurations, the rotational transform is produced by the shaping of flux surfaces. To shape flux surfaces, the vacuum magnetic field is produced by external coils with helical-winding laws. This means the vacuum magnetic field produced for the vacuum is intrinsically three dimensional (3-D). Thus, the plasma current is not required to make flux surfaces. This characteristic is an advantage. Since the plasma current is not necessary, disruptions do not appear and steady-state operation is possible. However, because of the 3-D plasma responses, experimental and theoretical studies become more complex.