Honolulu, Hawaii
June 24, 2007
June 24, 2007
June 27, 2007
2153-5965
Curriculum Development and Delivery Modes in Nuclear Engineering
Nuclear and Radiological
17
12.1358.1 - 12.1358.17
https://peer.asee.org/3042
76
James Paul Holloway is Arthur F. Thurnau Professor and Professor of Nuclear Engineering and Radiological Sciences at the University of Michigan. He teaches classes in engineering, from first year computing through design and gradaute courses in nuclear engineering. His research interests are in mathematics and computation applied to radiation transport and nuclear reactor analysis. He is also the incoming Associate Dean for Undergraduate Education of the College of Engineering at Michigan, effective July 1 2007.
Teaching Flux in the Age of Desktop Monte Carlo
1. Introduction
Asked to deﬁne the scalar ﬂux, too many students reach for an explanation involving surfaces and areas. Something along the lines of “scalar ﬂux is the rate at which particles cross the surface into a sphere . . .” This inadequate response is not surprising. Students are often introduced to ﬂux in various special monodirectional cases in which the rate at which particles cross a surface can be evaluated using even scalar ﬂux (along with the implicit knowledge of the directional dependance of the ﬁeld). That the units of ﬂux involve something per unit area further compounds students’ belief that ﬂux has something to do with particles crossing a surface. The misappropriation in radiation transport theory of the word “ﬂux” for what is truly a volumetric concept does not help. My assertion is that no understanding of scalar ﬂux in terms of surface crossing is adequate for our students. They must come to understand scalar ﬂux in terms of path-length rate density.
2. Competing interpretations of scalar ﬂux
Scalar ﬂux, or ﬂuence rate, is a central concept for nuclear engineering analysis. It is deﬁned in several related ways, one of which is under the control of an international standards body. The International Commission on Radiation Units deﬁnes1 ﬂuence as dN number of particles incident on a sphere Φ= = (1) da cross sectional area of sphere with the (unstated) understanding that the cross sectional area da is very small compared to macro- scopic spatial variations in the particle population and that the period of observation is ﬁnite. The ﬂuence rate, called scalar ﬂux in most nuclear engineering literature, is then simply the rate of change of the ﬂuence. This deﬁnition centers on the rate at which particles enter a sphere, and it is often asserted that the deﬁnition is founded on some idealized measurement with a spherical detector. This is peculiar, because detectors do not count particles that enter them; all detectors measure reaction rates within a detector volume.
The deﬁnition of scalar ﬂux as the rate at which particles enter a sphere, divided by the cross sectional area of the sphere, is useless as a concept for computation of the ﬂux, and it makes no obvious connection to the reaction rate density. In nuclear reactor analysis, in shielding analysis, indeed in all applications of radiation, the scalar ﬂux is required as a means to describe the particle population in a manner suited to the computation of reaction rate densities. But reaction rate density is a volumetric concept, while the ICRU deﬁnition of ﬂux emphasizes surfaces (of a sphere) and areas (cross section of a sphere). In the development of radiation transport theory, and its approximate cousins like diffusion theory, the ﬂux is introduced in yet another way. Most careful developments move from the particle number density—a concept easily understood—to the ﬂux as particle speed times the number density. This approach is followed because this product naturally arises in computing reaction rate density.
Holloway, J. (2007, June), Teaching Flux In The Age Of Desktop Monte Carlo Paper presented at 2007 Annual Conference & Exposition, Honolulu, Hawaii. https://peer.asee.org/3042
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