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NN Asks: What hurdles stand in the way of nuclear power’s global expansion?
Jake Jurewicz
Nuclear technology is mature. It provides firm power at scale with minimal externalities and has done so for decades. The core problem isn’t about the technology—it is how the plants are built. Nuclear construction has a well-documented history of cost and schedule overruns. Previous nuclear plants often spent more than twice what was first budgeted, making nuclear among the power technologies with the largest average cost overruns worldwide.
Recent projects illustrate how severe the problem can be. In South Carolina, the V.C. Summer nuclear expansion saw projected costs rise from roughly $10 billion to more than $25 billion before the project was abandoned in 2017, by which time more than $9 billion had already been spent and customers were stuck paying for a site they have yet to benefit from.
Edward J. Waller
Nuclear Technology | Volume 175 | Number 1 | July 2011 | Pages 89-92
Technical Note | Special Issue on the 16th Biennial Topical Meeting of the Radiation Protection and Shielding Division / Radiation Measurements and General Instrumentation | doi.org/10.13182/NT11-A12275
Articles are hosted by Taylor and Francis Online.
Recent nuclear weapons testing in the limit of low-yield detonations has underscored the need to ensure that radiation detection and monitoring equipment can adequately respond to these events. Testing and validating equipment in appropriate reference fields have become difficult since the closing of the NATO primary fission spectra reference at the Aberdeen Proving Ground Fast Burst Reactor facility post-9/11. A simple and low-cost device was designed to perform testing of commercial off-the-shelf neutron detection equipment to the expected spectral shape from a low-yield nuclear weapon. By enclosing an 241AmBe (,n) neutron source within a heavy water-moderated sphere, the general shape of a 1-kiloton standard fission weapon was generated at 1 m, valid between 100 and 2000 keV. The 1-m dose rate expected from this configuration is [approximately]2.16 × 10-10 Svh-1Bq-1 , which is less than one-half of the unshielded dose rate.