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Unformatted text preview: was captured ±rom the lowest shell (where the absolute value o± the energy, E K , is quite large ±or large Z – see Eq. 4125). To a very good approximation, the energy o± the Kshell electron in Vanadium is equal to that in Titanium (where there is now a “vacancy” that must be flled by a readjustment o± the whole electron cloud), and we write Q = − ∆ mc 2 − E K so that Eq. 4327 still holds. Thus, Q = ( m V − m Ti ) c 2 − E K ....
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This note was uploaded on 11/12/2011 for the course PHYS 2001 taught by Professor Sprunger during the Fall '08 term at LSU.
 Fall '08
 SPRUNGER
 Physics, Mass

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