ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Explore membership for yourself or for your organization.
Conference Spotlight
2026 Nuclear Energy Conference & Expo (NECX)
August 24–27, 2026
Dallas, TX|Hilton Anatole
Latest Magazine Issues
Jun 2026
Jan 2026
2026
Latest Journal Issues
Nuclear Science and Engineering
July 2026
Nuclear Technology
June 2026
Fusion Science and Technology
May 2026
Latest News
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.”
Glenn Gerdin, Donald Mueller, Bernard W. Wehring
Fusion Science and Technology | Volume 7 | Number 2 | March 1985 | Pages 180-196
Technical Paper | Experimental Device | doi.org/10.13182/FST85-A24533
Articles are hosted by Taylor and Francis Online.
A method is proposed to measure the properties of the alphas escaping a deuterium-tritium-fueled magnetically confined fusion reactor. This method is called the charge neutralization approach; it involves the slowing down of alphas in carbon foils of known thickness so that a significant percentage of the alphas are neutralized. These alphas can be detected by methods similar to those developed for charge-exchange neutral analysis. The foils would be placed in a recessed slot in the foil holder that would, in turn, be placed in the shadow of the limiter to reduce the heat and particle flux to the foils. Considerable energy selection can be achieved by varying the foil thickness; the lower limit on detectable alpha energy is ∼200 keV. The ratio of alpha signal to nuclear noise was estimated for a ZnS scintillator 15 μm thick being operated in the current mode in a borated limestone shield. Experimental values were used for the response to neutrons, and linear absorption coefficients were used for the response to gammas. The alpha wall flux was that calculated for a Tokamak Fusion Test Reactor (TFTR) with Q = 1, a plasma current of 2.5 MA, and a minor radius of 85 cm; the radiation fluxes were scaled from the one-dimensional calculations of L-P. Kufor TFTR at Q = 1. For this example, the signal to nuclear noise ratio becomes greater than unity at ∼75 cm into the shield indicating the amount of shielding material required.