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By Lewins J. (Ed)

ISBN-10: 0306470888

ISBN-13: 9780306470882

Due to the fact its initiation in 1962, this sequence has awarded authoritative stories of crucial advancements in nuclear technology and engineering, from either theoretical and utilized views. additionally, many unique contributions are integrated.

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J. , 1994, ‘Wartime evacuation and mortality from childhood leukaemia in England and Wales in 1945-9’, BMJ 309 pp 1197-2102. , 1995, ‘Epidemiological evidence for an infective basis in childhood leukaemia’, B. J. Cancer 71 pp 1-5. J. , 1995, ‘Childhood leukaemia and rural population movements: Greece, Italy, and other countries’, Cancer Causes and Control 6 pp 445-450. W. , 1997, ‘The excess of childhood leukaemia near Sellafield a commentary on the fourth COMARE report’, J. Radiol. Prot. 17 pp 63-71.

5(b). Therefore, we will adopt a new theoretical amplitude pdf: (129) where W 2 is the normalization constant. This amplitude pdf (129) provides a good fit to the experimental one as shown in the dash-dot line in Fig. 5(b). Also this amplitude pdf gives good fits in the other experimental ones for G2 and G1 as seen in Figs. 5(c) and (d). On the other hand, the phase pdf (128) is available for all the cases through G5 to G1 to get good fits to the experimental ones. (127) and (129), as was expected before analysis due to its strong intermittent oscillation.

5. Reactor-power dependence of neutronic variance The variance of neutron fluctuation σ NN becomes (71) where . This means that when k 0 > 1, C2 > 0; the stable steady state is realized under the constant reactivity insertion. The variance diverges as C2 → +O. Namely, C2 = 0 is the just critical point of the reactor. The divergence of variance known in linear theory is suppressed by the nonlinear negative feedback. Since C1 > 0 always hold even for k 0 > 1, the hard mode instability does not take place when the strength of the parametric noise of Gaussian white nature is small.

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Advances in Nuclear Science and Technology by Lewins J. (Ed)

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