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

By John G. Webster (Editor)

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N. J. , Spectroscopy for Impurity Control in ITER, in P. E. Stott, G. Gorini, and E. ), Diagnostics for Experimental Thermonuclear Fusion Reactors, New York: Plenum, 1996, pp. 291–306. 27. A. T. , Radiation effects on heated optical fibers, Rev. Sci. , 68: 632–635, 1997. 28. A. T. Ramsey and S. L. Turner, HAIFA: A modular fiber-optic coupled, spectroscopic diagnostic for plasmas, Rev. Sci. , 58: 1211–1220, 1987. 8. ITER Physics Basis Document, Nucl. Fusion, to be published 1998. 29. R. Reichle, M.

S. Marmar, Active Spectroscopy Diagnostics for ITER Utilizing Neutral Beams, in P. E. Stott, G. Gorini, and E. ), Diagnostics for Experimental Thermonuclear Fusion Reactors, New York: Plenum Press, 1996, pp. 281–290. 22. H. A. , Progress toward a microsecond duration, repetitively pulsed, intense-ion beam for active spectroscopic measurements on ITER, Rev. Sci. , 68: 332–335, 1997. 23. H. Soltwisch, Current distribution in a tokamak by FIR, Rev. Sci. , 57: 1939–1950, 1986. 24. F. M. , Magnetic field pitch angle diagnostic using the motional Stark effect, Rev.

The slowing-down process is called neutron moderation. Moderation is optimized by causing the fast neutrons to collide with something of similar mass. A head-on collision between two objects of the same mass will result in a complete transfer of energy. Thus, for nuclear reactors, the moderators of choice are hydrogen-rich substances such as light water. It is important to recognize that the slowing down occurs in discrete steps. Neutrons do not lose energy continuously. Rather they lose it every time they undergo a collision.

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

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