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Smarter waste strategies: Helping deliver on the promise of advanced nuclear
At COP28, held in Dubai in 2023, a clear consensus emerged: Nuclear energy must be a cornerstone of the global clean energy transition. With electricity demand projected to soar as we decarbonize not just power but also industry, transport, and heat, the case for new nuclear is compelling. More than 20 countries committed to tripling global nuclear capacity by 2050. In the United States alone, the Department of Energy forecasts that the country’s current nuclear capacity could more than triple, adding 200 GW of new nuclear to the existing 95 GW by mid-century.
Norman P. Goldstein, William H. Todt, Alex D. Service
Nuclear Technology | Volume 60 | Number 3 | March 1983 | Pages 430-438
Technical Paper | LWR Control Materials—I and II / Technique | doi.org/10.13182/NT83-A33129
Articles are hosted by Taylor and Francis Online.
Traditionally, air- and tissue-equivalent ion chambers have been used to determine the strength of radiation fields or the dose deposited in tissue, independent of the gamma-ray energy involved. Some applications, including those associated with U.S. Nuclear Regulatory Commission Regulatory Guide 1.97, call for the use of metallic-walled chambers with such an energy-independent response requirement. We examined by means of calculations and measurements the effect of three different gas fills on this characteristic of a stainless steel/aluminum Westinghouse ion chamber. Details of the gamma ray and electron interactions in these chambers have been examined and they have shown that both secondary interactions of scattered gamma rays and interactions of the incident gamma rays directly with the chamber gas are important current-producing mechanisms in ion chambers with large electrode structures. This information, along with results concerning the effect of gas pressure on the energy loss of traversing electrons, is used to explain the calculated flat energy response from a 1-atm 95% N—5% He gas fill, the less flat response for a 10-atm fill of the same gas, and the strong energy dependence of 7.5 atm of xenon.