New PDF release: 40.Nuclear Science

By John G. Webster (Editor)

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The neutron population grows in response to the slow removal of the control mechanisms until a self-sustaining neutron chain reaction is achieved. The second regime is that in which the power is raised from whatever level existed when criticality was attained to the point-of-adding-heat, which is usually 1% to 3% of full power. The point-of-adding-heat is defined as the power level above which a change in power is reflected as a change in temperature. At lower powers, the plant heat capacity is such that power changes do not affect temperature.

After n generations, that population will be If the core multiplication factor K is less than unity, then the series 1 + K + K2 + ··· Kn will converge to 1/(1 − K) as Kn approaches 0. Thus, the total neutron population is S0 /(1 − K). This relation may be used to calculate the equilibrium neutron level in a subcritical reactor. To do this, recognize that the count rate (CR) obtained over a designated time interval is proportional to the neutron population. Thus, Several caveats apply.

Sci. , 68: 728–731, 1997. 16. D. , TFTR Thomson scattering system, Rev. Sci. , 56: 1015–1017, 1985. 17. H. , The LIDAR Thomson scattering diagnostic on JET, Rev. Sci. , 59: 1451–1456, 1988. 18. D. V. Bartlett, Physics Issues of ECE and ECA for ITER, in P. E. Stott, G. Gorini, and E. ), Diagnostics for Experimental Thermonuclear Fusion Reactors, New York: Plenum, 1996, pp. 183–192. 19. K. W. Hill, M. Bitter, and S. von Goeler, Concepts and Requirements of ITER X-Ray Diagnostics, in P. E. Stott, G.

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40.Nuclear Science by John G. Webster (Editor)

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