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The Radiation Protection and Shielding Division is developing and promoting radiation protection and shielding aspects of nuclear science and technology — including interaction of nuclear radiation with materials and biological systems, instruments and techniques for the measurement of nuclear radiation fields, and radiation shield design and evaluation.
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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.
Dong H. Nguyen
Nuclear Science and Engineering | Volume 55 | Number 3 | November 1974 | Pages 307-319
Technical Paper | doi.org/10.13182/NSE74-A23457
Articles are hosted by Taylor and Francis Online.
Transient solutions of a nonlinear nuclear reactor with various temperature-dependent feedbacks are obtained by the modified Newton-Raphson-Kantorovich’s iterative technique. The difference between the first and higher iterates is shown explicitly to be negligible at all times, so that the first iterate represents well the entire solution. It is also shown that the spatial distribution of the neutron flux during transience is dominated by the fundamental mode and that the negligible difference between the second and the first iterates is composed of higher harmonics.—, The maximum flux, the time at which it occurs, and the rate of flux increase are all readily obtained from the solutions. For an increase in reactor buckling and for a positive initial flux disturbance, the neutron flux in a reactor with Newtonian or prompt feedback reaches a finite asymptotic value, whereas that of an adiabatic reactor first rises, then drops off. However, for the same initial conditions, the maximum flux attained in an adiabatic reactor is several fold higher than that of a reactor with Newtonian or prompt feedback.