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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Deep Space: The new frontier of radiation controls
In commercial nuclear power, there has always been a deliberate tension between the regulator and the utility owner. The regulator fundamentally exists to protect the worker, and the utility, to make a profit. It is a win-win balance.
From the U.S. nuclear industry has emerged a brilliantly successful occupational nuclear safety record—largely the result of an ALARA (as low as reasonably achievable) process that has driven exposure rates down to what only a decade ago would have been considered unthinkable. In the U.S. nuclear industry, the system has accomplished an excellent, nearly seamless process that succeeds to the benefit of both employee and utility owner.
A. J. Buslik
Nuclear Science and Engineering | Volume 35 | Number 3 | March 1969 | Pages 303-318
Technical Paper | doi.org/10.13182/NSE69-A20009
Articles are hosted by Taylor and Francis Online.
A self-adjoint positive-definite variational principle is presented which leads to upper and lower bounds for < S*, ϕ >, where < S*, ϕ > is an integral over position and angular direction of the product of the one-velocity neutron transport flux, ϕ and an arbitrary adjoint source, S*. The Euler equation of the functional is a new form of the one-velocity Boltzmann neutron transport equation in which the dependent variable is one-half the sum of ϕ and ϕ*, where ϕ* is the adjoint flux. When a trial function consisting of an expansion in spherical harmonics is used, one obtains as a lower bound for < S*, ϕ > the quantity < US1, ϕ(P−N′; S1) > − < US2, ϕ(P−N″; S2) >, where S1(r, Ω) = [S(r, Ω) + S*(r, −Ω)]/2, S2(r, Ω) = [S(r, Ω) − S*(r, −Ω)]/2, ϕ(P-N′; S1) is an odd P−N approximation to a problem with the same cross sections as the original problem, but with source S1; ϕ(P−N″; S2) is an even P−N approximation to a problem with source S2, and U is the operator that takes a function f(r, Ω) into f(r, −Ω).