Page 73 - Radiochemistry and nuclear chemistry
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62                   Radiochemistry and Nuclear Chemistry

               disappearance of mass, cf.  eqns.  (3.2) and (3.5).  This energy is also called the Q-value of
               the reaction

                                        Q (MeV)  =  -931.5AM  (u)                  (4.12)

               For a-decay  we can define the Q-value as

                                    Qo~ =  -931"5(Mz-2  +  MHe  -  MZ)             (4.13)

               We always write the products minus the reactants within the parenthesis. A decrease in total
               mass  in a-decay  means a release of energy.  The  minus sign before  the constant 931.5  is
               necessary  to  make Q positive for spontaneous decay.
                An example will show the use of this equation.  For the decay reaction 238U --) 234Th +
               4He,  the mass values for 238U and 4He are in Table 3.1;  for 234Th it is 234.043  594.  Thus
               we obtain  Qa  =  -931.5 (234.043 594 +  4.002 603  -  238.050 7785)  =  4.274  MeV.
                If the products are formed in their ground states, which is common for a-decay,  the total
               decay energy is partitioned into the kinetic energies of the daughter nucleus (E z_ 2) and the
               helium nucleus  (Ea):

                                            Qot =  EZ- 2  + Eo~                    (4.14)

               Because of conservation of energy (4.2)  and momentum (4.4)

                                           EZ_ 2  =  Qa Ma /M z                    (4.15)

               and

                                           Et~ =  Qa MZ_ 2/M Z                     (4.16)

               From these equations we can calculate the kinetic energy of the 234Th daughter to be 0.072
               MeV,  while  that  of  the  a-particle  is  4.202  MeV.  Because  of  the  large  mass  difference
               between  the a-emitting  nucleus and  the helium atom,  almost  all  of the energy  is  carried
               away with  the a-particle.
                Although the kinetic energy of the daughter nucleus is small in comparison with that of
               the a-particle,  it is large (72 000 eV) in comparison with chemical binding energies (<  5
               eV).  Thus the recoiling daughter easily breaks all chemical bonds by which it is bound to
               other atoms.
                In  1904 it was observed by H.  Brooks that measurements on 218po (RaA), obtained from
               radon,  led to a contamination of the detection chamber by 214pb (RaB) and 214Bi (RaC).
               This was explained by Rutherford as being due to daughter recoil m  the a-decay of 218po
               in  the sequence (written symbolically):

                    222Rn(c~, 3.8  d) 218po(a,  3.05  min) 214pb(~-,  27 min) 214Bi(~J-, 20 rain)...
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