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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.
Om Prakash Joneja, Vijay R. Nargundkar, Tejen Kumar Basu
Fusion Science and Technology | Volume 12 | Number 1 | July 1987 | Pages 114-118
Technical Paper | Blanket Engineering | doi.org/10.13182/FST87-A25055
Articles are hosted by Taylor and Francis Online.
The experimentally measured value of 14-MeV neutron multiplication for 10-cm-thick lead in rectangular geometry agrees within 1% of the corresponding calculated value using the MORSE-E code with the Los Alamos National Laboratory 30-group cross-section set CLAW-IV, in P3 scattering approximation. This result is in direct contrast with Takahashi's measurements with lead spheres of 3-, 6-, 9-, and 12-cm radii, where the measured multiplication values are found to be ˜15% higher than the corresponding transport calculations performed using the ANISN and NITRAN codes with the ENDF/B-IV library. However, Monte Carlo calculations using the MORSE-E code with the CLAW-IV library, as well as those of Cheng et al, using the MCNP code with the ENDF/B-V library, agree very well with Takahashi's measurements. Thus, the real difference of leakage neutron multiplication in lead is not between the measurements and the calculations, as reported by Takahashi, but between Takahashi's and other calculations. It is found that by using lead as a neutron multiplier in practical fusion blankets, a 5 to 10% higher neutron multiplication can be obtained than with beryllium for identical configurations of the multiplier.
