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Conference on Nuclear Training and Education: A Biennial International Forum (CONTE 2025)
February 3–6, 2025
Amelia Island, FL|Omni Amelia Island Resort
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How to talk about nuclear
In your career as a professional in the nuclear community, chances are you will, at some point, be asked (or volunteer) to talk to at least one layperson about the technology you know and love. You might even be asked to present to a whole group of nonnuclear folks, perhaps as a pitch to some company tangential to your company’s business. So, without further ado, let me give you some pointers on the best way to approach this important and surprisingly complicated task.
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).