Page 147 - Radiochemistry and nuclear chemistry
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132                  Radiochemistry  and  Nuclear  Chemistry

                      TABLE 6.2. Range in water, and average linear energy transfer (LET) values for different
                      radiation

                     Upper half refers to monoenergetic (accelerated) particles. For B-decay E.b .  =  1/3 Ems x

                                                 Maximum   range           Average LET
                                                                           value in water
                 Radiation      Energy (MeV)   cm air       mm water        0ceV/~,m)
                 Electron         1            405           4.1              0.24
                                  3            1400          15               0.20
                                 10            4200          52               0.19
                 Proton           1              2.3         0.023           43
                                  3             14           0.014           21
                                 10            115           1.2              8.3
                 Deuteron         1              1.7          -                -
                                  3              8.8         0.088           34
                                 10             68           0.72            14
                 Helium           1              0.57        0.0053          190
                                  3              1.7         0.017           180
                                 10             10.5         0.11            92
                 Fiss.  fragment   100           2.5         0.025          3300
                 Z2~a (cx)      E, 4.80          3.3         0.033           145
                 21~  (o0       E,~ 5.30         3.8         0.039           136
                 222Rn (r       E, 5.49          4.0         0.041           134
                 3H (/3)        Ema x 0.018      0.65        0.0055           1.1
                 35S (t3)       Ema x 0.167     31           0.32             0.17
                 ~176 (/3)      Ema x 0.544     185          1.8              0.10
                 32p (13)       Ema x 1.71      770          7.9              0.07
                 ~/'  (~        Ema x 2.25     1020          11               0.07
                 137Cs (3')     E v 0.66       x,/i =  8.1 cm H20             0.39
                 ~~  (3')       E,  1.20-1.30   x u  =  11.1 cm H20           0.27


               where  A z  is  the  atomic  weight  of  the  absorber.  Figure  6.6  shows  the  range  of  various
               charged  particles  in  an  aluminum  absorber.  The  range  of a  5  MeV  c~ is  6  nag  cm-2;  thus
               ~m  =  6  x  10-3/OAl  cm  =  0.002  ram.  Alpha-particles  from  radioactive  decay  are  easily
               stopped  even  by  the  thickness  of a  sheet  of paper.
                When  the  absorber  consists  of a  composite  material,  containing  the weight  fractions  w 1,
               w 2,  w 3,  etc  of  elements  1,  2,  3,  etc  with  ranges  ~l,/~2,/~3,  etc,  the  range  Rcomp  in  the
               absorber  is  obtained  from  the  relation


                                  1/~comp  =  Wl/~ 1  +  w2/~ 2  +  w3/~ 3  +  ...   (6.12)

                The  number  of  ion  pairs  formed  per  millimeter  of  range  for  c~-particles,  protons,  and
               electrons  are  shown  in  Figure  6.7a.  The  larger  specific  ionization  of  the  a-particles
               compared  to the protons is related to the fact that the former are doubly  charged.  In general
               the  specific  ionization  increases  with  the  ionic  charge  of the  particle  for  the  same  kinetic
               energy.  Fission  fragments  that  initially  have  very  large energies  also have very  large  ionic
               charges  leading  to  quite  high  specific  ionization  in  their  absorption  in  matter;  their  range
               is  2-3  cm  in  air  and  2-3  mg  cm -2  in  aluminum.
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