By Ziya Akcasu

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**Additional resources for Mathematical Methods in Nuclear Reactor Dynamics**

**Sample text**

W e do not consider n e u t r o n s escaping t h e reactor in t h e positive z direction a n d r e t u r n i n g back u n d e r t h e influence of gravity. 1). , (ijjn | 0 m > ^+ Snm . H o w e v e r , by c o m p a r i n g (21a) to (3a), we can guess that t h e set ^n(z)y defined as 2 12 i/j +(z) n = (2/a) I e+»*/ sin[(« + l>rs/5] (22) is o r t h o n o r m a l to i/*n(z) in t h e sense that + + <

Any vector e x p a n d e d into {| n>} as l<£> = |

Mathematical Preliminaries + w h e r e s is t h e outer surface of t h e reactor. Since