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284                               NUCLEAR REACTIONS                              [CHAP. 19


               19.5. NUCLEAR FISSION AND FUSION
                   Nuclear fission refers to splitting a (large) nucleus into two smaller ones, plus one or more tiny particles
               listed in Table 19-3. Nuclear fusion refers to the combination of small nuclei to make a larger one. Both types of
               processes are included in the term artificial transmutation.


                                         Table 19-3 Nuclear Projectiles and Products ∗

                                                                         Nuclear Rest Mass
                                Name      Symbol        Identity               (amu)


                               Proton     1 Horp   Hydrogen nucleus         1.00728
                               Deuteron   2 Hord   Heavy hydrogen nucleus   2.0135
                               Tritium    3 H      Tritium nucleus          3.01550
                               Helium-3   3 He     Light helium nucleus     3.01493
                               Neutron    1 norn   Free neutron             1.008665
                               Alpha      α        Helium nucleus           4.001503
                               Beta       β        High-energy electron     0.00054858
                               Gamma      γ        High-energy light particle  0.0
                               Positron   + β      Positive electron        0.00054858

                             ∗                                                12
                              Larger projectiles are identified by their regular isotopic symbols, such as  C.
                                                                              6
                   Transmutation means converting one element to another (by changing the nucleus). The first artificial
               transmutation was the bombardment of  14 N by alpha particles in 1919 by Lord Rutherford.
                                                7
                                                 14   4       17   1
                                                                   1
                                                      2
                                                  7  N + He −→  8 O + H
               The alpha particles could be obtained from a natural decay process. At present, a variety of particles can be used
               to bombard nuclei (Table 19-3), some of which are raised to high energies in “atom smashing” machines. Again,
               nuclear equations are written in which the net charge and the total of the mass numbers on one side must be the
               same as their counterparts on the other side.

               EXAMPLE 19.8. What small particle(s) must be produced with the other products of the reaction of a neutron with a  235 U
                                                                                                     92
               nucleus by the following reaction?
                                               235   1     90    143 Xe + ?
                                                92  U + n −→  38  Sr +  54
                                                     0
               Ans.  In order to get the subscripts and the superscripts in the equation to balance, the reaction must produce three neutrons:
                                                  235  1     90   143 Xe + 3 n
                                                                         1
                                                       0
                                                             38
                                                  92 U + n −→ Sr +  54   0
                   This reaction is an example of a nuclear chain reaction, in which the products of the reaction cause more
               of the same reaction to proceed. The three neutrons can, if they do not escape from the sample first, cause three
               more such reactions. The nine neutrons produced from these reactions can cause nine more such reactions, and
               so forth. Soon, a huge number of nuclei are converted, and simultaneously a small amount of matter is converted
               to a great deal of energy. Atomic bombs and nuclear energy plants both run on this principle.

               EXAMPLE 19.9. If each neutron in a certain nuclear reaction can produce three new neutrons, and each reaction takes
               1 s, how many neutrons can be produced theoretically in the 15th second?
               Ans.  Assuming that no neutrons escaped, the number of neutrons produced during the 15th second is
                                                         15
                                                        3 = 14 348 907
                                                            28
                     The number produced in the 60th second is 4.24 × 10 .
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