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Hence, the adoption of Cermet fuel concept shows a core lifetime decrease of about 3.1 EFPY.
During the core lifetime, the burn-up swings slightly due to the perfect breeding capability.
The extension of the core lifetime by battery type module shuffling and refueling is shown.
The presented analysis is focused on the TRU-impact on the single-batch mode (no-refueling) VHTR core lifetime.
A fast flux greater than 5.6E15 n/cm2-s is maintained over the core lifetime in the central irradiation position.
The reactivity swing during the core lifetime is less than $1 without burnable poison rods to minimize excess reactivity.
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The results suggest that the core fuel lifetime beyond 12 equivalent full power years (EFPYs) is possible.
The core emission lifetime and peak position/spectral width as a function of the applied potential are presented in Fig. 4a and c, respectively.
This allows comparison of different graphite grades and a qualitative assessment of their appropriateness for HTR applications, as a basis of selection, design and core component lifetime.
We can obtain such characteristics as high operational temperature of the reactor (between 550 °C and 1200 °C) and elongation of the core operational lifetime by the inherent fission product separation in the liquid fuel by using these alloys.
Furthermore, our XES spectra and maps give information about ultra-fast dissociation on the timescale of the O 1s core hole lifetime, which is strongly affected by the initial state hydrogen bonding configuration.
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