1958
DOI: 10.2172/4333126
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Analyses of Experimental Power-Reactivity Feedback Transfer Functions for a Natural Circulation Boiling Water Reactor

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Cited by 11 publications
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“…This function satisfies the same boundary condition as the temperature, so that, for every r' in the core and for all t > 0, we have #(r f l ,r';*) =0 (17) where r s is a point on the surface. In order to solve (12), we may substitute n^r\t)=A(r't)Ur) (18) and obtain…”
Section: B* = (Vs U --£»()/A)mentioning
confidence: 99%
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“…This function satisfies the same boundary condition as the temperature, so that, for every r' in the core and for all t > 0, we have #(r f l ,r';*) =0 (17) where r s is a point on the surface. In order to solve (12), we may substitute n^r\t)=A(r't)Ur) (18) and obtain…”
Section: B* = (Vs U --£»()/A)mentioning
confidence: 99%
“…32). The shift of the average power level is calculated by SP 0 = P 0 \im[so 7 k ext (s)L(s)] (18) which is obtained from (4.4, Eq. 32) by replacing Z(s) by L(s).…”
Section: K { (Oo) = P(oo)h(0)mentioning
confidence: 99%
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