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Additional resources for 40.Nuclear Science
After the possible radiation exposure the voltage is read on an electrometer. The reduction of voltage is proportional to the number of ion pairs created in the gas volume by the well-known equation for a capacitor, Vi Ϫ Vf ϭ Q/C, where Q is the total charge collected from the ionization and C is the capacitance of the chamber. For a given type of radiation the collected charge is proportional to the radiation dose, and the device can be readily calibrated by exposure to standard radiation sources.
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.
D. S. Darrow, S. J. Zweben, and H. W. Herrmann, Alpha particle loss diagnostics in TFTR and tokamak reactors, Fusion Eng. , 34–35: 53–58, 1997. 39. E. R. Hodgson, Radiation Problems and Testing of ITER Diagnostic Components, in P. E. Stott, G. Gorini, and E. ), Diagnostics for Experimental Thermonuclear Fusion Reactors, New York: Plenum, 1998, pp. 261–268. 40. V. S. , Imitation of Fusion Reactor Environment Effects on the Inner Elements of Spectroscopical, mm and Submm Diagnostics, in P. E. Stott, G.