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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Work advances on X-energy’s TRISO fuel fabrication facility
Small modular reactor developer X-energy, together with its fuel-developing subsidiary TRISO-X, has selected Clark Construction Group to finish the building construction phase of its advanced nuclear fuel fabrication facility, known as TX-1, in Oak Ridge, Tenn. It will be the first of two Oak Ridge facilities built to manufacture the company’s TRISO fuel for use in its Xe-100 SMR. The initial deployment of the Xe-100 will be at Dow Chemical Company’s UCC Seadrift Operations manufacturing site on Texas’s Gulf Coast.
George I. Bell
Nuclear Science and Engineering | Volume 21 | Number 3 | March 1965 | Pages 390-401
Technical Paper | doi.org/10.13182/NSE65-1
Articles are hosted by Taylor and Francis Online.
We consider the probability, pn(R,t∫; ,,t), that in a multiplying system, a neutron with position velocity , at time t leads to exactly n neutrons in region R of , space at time t∫. By formulating pn in terms of first collision probabilities we derive a non-linear (Boltzmann-like) integro-differential equation for the probability generating function, G. The linearized equation for = 1 - G is shown to be adjoint to the usual Boltzmann equation for the average neutron flux. The behavior of for subcritical and supercritical systems is analyzed. For large t∫-t, it is shown that for subcritical systems approaches zero exponentially, while for supercritical systems → which is a solution of the time-independent non-linear equation for and equals the probability of getting a divergent chain reaction from the initial neutron. In section B, one-velocity theory with isotropic scattering is described in some detail while in section C are outlined the extensions to 1) energy-dependent problems with anisotropic scattering 2) multiple final states, 3) random sources, 4) counting problems, and 5) delayed neutron precursors. In section D methods for solution of equations for G are briefly discussed, and it is shown that the asymptotic behavior may be found from solutions of linear time-independent ‘adjoint α’ and ‘adjoint k’ calculations. Derivation of a point model independent of space and velocity is carried out by an expansion in adjoint α eigenfunctions and the model parameters are shown to differ from those usually assumed in point models.