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Unstable  Nuclei  and Radioactive Decay             79


                                 4.11.  Kinetics  of simple  radioactive  decay
                Most radioactive isotopes which are found in the elements on earth must have existed for
               at least as long  as the earth.  The nonexistence in nature of elements with atomic numbers
               greater than 92 is explained by the fact that all the isotopes of these elements have life-times
               considerably  shorter  than  the age of the earth.
                Radioactive decay is a random process.  Among the atoms in a sample undergoing decay
               it is not possible to identify which  specific  atom will be the next  to decay.  We denote the
               decay  rate  by A.  It is a  measure of the number of disintegrations per unit  time:

                                              A  =  -dN/dt                         (4.39)

                The decay rate is proportional to the number of radioactive atoms,  N, present: A  oc N.  If
               105 atoms  show a decay  rate of 5  atoms per  second then  106 atoms  show a decay  rate of
               50 atoms per second.  If the number of radioactive nuclei and the number of decays per unit
               time are  sufficiently  great  to permit a  statistical  treatment,  then


                                              -dN/dt  =  X N                       (4.40a)
               where  h  is  the  proportionality  constant  known  as  the  decay  constant.  If  the  time  of
               observation  At  during  which  AN atoms  decay  is  very  small  compared  to  tl,~ (usually  <
               1%),  one may  simply write

                                            A  =  AN~At  =  X N                   (4.40b)

               If the  number  of nuclei  present  at  some original  time t  =  0  is  designated  as  N 0,  (4.40a)
               upon  integration becomes  the general  equation  for simple radioactive decay:

                                              N  =  N O e -ht                      (4.41a)

                In Figure 4.8 the ratio of the number of nuclei at any time t to the original number at time
              t  =  0  (i.e.  N/No)  has been plotted on both a linear (left) and logarithmic (fight)  scale as a
               function of t.  The linearity of the decay curve in the semi-logarithmic graph illustrates the
              exponential  nature  of radioactive decay.  Since A  cx  N,  the equation can be  rewritten  as

                                              A  =  A 0 e -ht                     (4.41b)

                Commonly,  log  A  is  plotted  as  a  function  of  t  since  it  is  simpler  to  determine  the
              disintegration  rate  than  it  is  to  determine  the  number  of  radioactive  atoms  in  a  sample.
              Instead of the decay constant  X,  the average  lifetime  r  is  sometimes used:

                                                r  =  1/X                          (4.42)

                Even more common is the use of the half-life,  tt/~, which is the time needed to reduce the
              amount of radioactive  material  by a  factor of 2.  Thus
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