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42                   Radiochemistry and Nuclear Chemistry

































                      FIG. 3.1. Chart of stable nuclides as a function of their proton (Z) and neutron (N) numbers.
                      The  numbers denoted  2,  8,  etc.,  are discussed  in Chapter  11.


               cadmium (Z  =  48) and tellurium (Z  =  52)  each have 8.  By contrast silver (Z  =  47)  and
               antimony (Z =  51) each have only 2 stable isotopes, and rhodium (Z =  45),  indium (Z  =
               49),  and  iodine  (Z  =  53)  have only  1 stable  isotope.  Many  other examples  of the  extra
               stabilization  of even  numbers  of nucleons  can  be  found  from  a  detailed  examination  of
               Figure 3.1,  or,  easier,  from nuclide charts,  e.g.  Appendix C.  The guide lines of N and Z
               equal  to  2,  8,  20,  etc.,  have  not  been  selected  arbitrarily.  These  proton  and  neutron
               numbers represent unusually stable proton and neutron configurations, as will be discusseA
               further in Chapter  11. The curved line through the experimental points is calculated based
               on the liquid drop model of the nucleus which is discussed later in this chapter.
                Elements of odd Z have none,  one or two stable isotopes, and their stable isotopes have
               an even number of neutrons,  except for the 5 odd-odd nuclei mentioned above.  This is in
               contrast to the range of stable isotopes of even Z, which includes nuclei  of both even and
               odd N,  although the former outnumber the latter.  Tin (Z =  50),  for example,  has 7 stable
               even-even isotopes and only 3 even-odd ones.
                The  greater  number  of  stable  nuclei  with  even  numbers  of  protons  and  neutrons  is
               explained  in  terms  of the  energy  stabilization gained by  combination of like nucleons  to
               form  pairs,  i.e.  protons  with  protons  and  neutrons  with  neutrons,  but  not  protons  with
              neutrons.  If a nucleus has,  for example,  an even number of protons,  all these protons can
               exist in pairs.  However,  if the nucleus has an odd number of protons, at least one of these
              protons must exist in an unpaired state.  The increase  in stability resulting  from complete
              pairing in elements of even Z is responsible for their ability to accommodate a greater range
               of neutron numbers as illustrated for the isotopes of germanium (32Ge, 5 stable isotopes),
   48   49   50   51   52   53   54   55   56   57   58