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170                  Radiochemistry and Nuclear Chemistry


                                                     BREMSSTRAHLUNG
                                                                        8-TRACK OF SECONDARY
                                  BRANCHING TRACK                       ELECTRON OF > 100 eV
                                    < 8000  eV

                                                           TRACK > 6000 eV

                              COLUMN IONIZATION                     (~   SPUR < 100 eV
                            ALONG PRIMARY TRACK
                                                                                IONIZING
               ca. 2nm  I                   _      _    .  .  .  .              PROJECTILE

                                           "4       ca. 30 eV        HOT ATOM
                          SPUR FROM SECONDARY ELECTRON
                          OF 10 - 100 eV (CA. 1-3 ION PAIRS AND
                          :1-10 EXCITED ATOMS PER 600 nmTRACK
                          LENGTH).  ALSO CALLED A BLOB
                      FIG.  7.1.  Track  formed  by  energetic  ionizing  particle  in  condensed  matter.  Distances
                      between  ion  pairs  along  track  are:  -- 1000  nm  3',  500-100  nm  fast electron,  -- 1 run  slow
                      electron  and  c~.


               columns  of  excited  and  ionizeA  species.  Differences  in  chemical  and  biological  effects
               caused by different  radiations  reflects  the varying track structures.
                The tracks of X-ray and ~,-radiation results in tracks of fast electrons.  The energy of these
               fast electron is consumed by the formation of spurs (6 -  100 eV), blobs (100 -  500 eV) and
               short tracks (500 -  5000 eV), see Figure 7.1. For a primary electron in the range 104 -  107
               eV the distribution of energy of secondary electrons is approximately 40 %  <  3.4 eV, 20 %
               3.4  -6.8  eV,  18%  6.8  -  13.5 eV and  12%  13.5 -  27.1  eV.  The radius of the core at low
               electron  velocities  is of the order of  1 nm.
                The  energy  transferred  to  the  electrons  by  an  energetic  ion  depends  on  the  mass,  the
               charge  (Z)  and  velocity  (v)  of  the  ion,  of.  (6.13):  the  probability  of  interaction  is
               proportional  to the ratio Z 2/mv 2.  Heavy ions produce track structures  similar to  those of
               fast  electrons.  However,  the  spurs  are  quite  close  to  each  other  and,  for  the  case  of
               c~-particles,  the original  distance between them is of the order of fractions of a nanometer.
               Immediately at their formation they comprise a continuous cylindrical column. The column
               consists  of  a  dense  core  surrounded  by  a  more  diffuse  shell  of  tracks  of  high  energy
               6-electrons.



                                   7.3.  Radiation dose and radiation yield

                The oldest radiation unit still in use is the roentgen (R).  It applies only to photons and is
               defined  as  the  exposure.  The  exposure  is  the  energy  flux  of  the  unperturbed  photon
               radiation hitting matter.  1 R is the exposure that in air produces ion pairs with total charge
               per unit mass of 2.58  x  10 -4 C/kg.  This corresponds to  1.61  x  1015 ion pairs per kg air or
               8.8  •  10 -3  J/kg  absorbed  energy  at  an  average  ion pair  formation  energy  of  34  eV.  The
               roentgen has been in use for more than 60 years and is still not uncommon in  the medical
              profession.
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