Page 92 - Radiochemistry and nuclear chemistry
P. 92

Unstable  Nuclei  and  Radioactive  Decay          81

               radioactive decay,  ff commonly has a value between 0.01  and 0.5.  Equation (4.45)  is only
               valid provided At  ,r  tt h (in which case AN ,~ N), where At is the time of measurement; this
               is  the normal  situation;  cf.  (4.40b).
                Figure 4.9  shows the radioactivity of a 32p sample measured every third day with a GM
               counter.  It is  seen that  the activity decreases  from about  8400 cpm at t  =  0  to 4200  cpm
               in  14.3  days,  and  to  about  2100  cpm  in  2  •  14.3  days.  The  uncertainty  in  the
               measurements  is about the size of the circles,  i.e.  about  +  110 cpm at t  =  0  and about  +
               65  cpm  at  30  days.  In  plots  of this  kind,  the  count  rate  measured  in  the  absence  of the
               sample (the background)  must be subtracted from that obtained with the sample present  to
               yield  the  correct  radioactivity  for  the  sample  alone.  In  Figure  4.9  the  background  is  so
               small  (i.e.  about  20 cpm)  that  it has very little  influence  on the decay curve.
                The half-life  is such a definitive characteristic of a radioactive species that knowledge of
               it plus the decay energy is often sufficient to allow identification of a nuclide.  A radioactive
               sample,  which exhibits a half-life of 4.5  •  109 y with a-decay energies of 4.8 MeV (77 %)
               and 4.3  MeV  (23 %),  is almost certainly 238U as there is no other nuclide known with this
               exact  set of properties.
                With  (4.39),  (4.43),  and  (4.45)  one obtains

                                            R  =  ~, N  ln(2)/t~/=                 (4.46)

               Knowing  the  counting  efficiency  ~  and  the  number  of  atoms  N,  the  half-life  can  be
               calculated  from  measurement  of R.  For  example,  in  a  counting  arrangement  with  ~  =
               0.515  for  a-particles,  159  cpm  are  observed  from  a  232Th  deposit  of  1.27  mg  (sample
              weight a).  Thus A  -  R/~k  --  309 dpm,  N  -  a  N/M  -  1.27  x  10 -3  x  6.02  x  1023/232.0
               =  3.295  x  1018 232Th atoms,  and t~ h  =  0.693  x  3.295  x  1018/309  =  7.40  x  1015 min  =
               1.41  •  101~ y.



                         .=
                         A
                          r
                          9 8000                   Ao 8410
                          E
                          c
                          =  6(xx)
                         o  o
                         >-
                                                   i
                                P
                         (J
                         <C
                         o3oo0

                                --  2103
                         uj  2(X)0
                         n,
                                                  14.3 d              28.5  d
                                    "   "   !   I   I   II   I   I   I   I
                         uJ            6        12      18      24      30
                         =E
                                               DECAY  TIME  (days)
                     FIG. 4.9. Semilogarithmic plot of the measured decay of 32p using a GM counter with a
                     background of 20 cpm.
   87   88   89   90   91   92   93   94   95   96   97