Page 35 - Radiochemistry and nuclear chemistry
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24                  Radiochemistry  and Nuclear  Chemistry

                (b) Rotational  energy.  Taking the simplest case,  a linear diatomic molecule with atomic
               masses m 1 and m 2 at a distance  r  apart,  the rotational  energy is given by

                                              Ero t  =  Iro t 60 2                 (2.28)

               where/rot is the rotational moment of inertia and w the angular velocity of rotation (radians
               s-l)"  [rot  is  calculated  from


                                              fro t  =  mre a r 2                  (2.29)

               where the reduced mass mred=(ml -  l +  m2-l)-t.  Equation (2.28),  derived from classical
               mechanics,  has  to  be  modified  to  take  into  account  that  only  certain  energy  states  are
               permitted

                                        Ero t  =  h2nr(nr +  1)/(87r2/rot)         (2.30)

               where n r is the rotational quantum number.  For transformation of energy in eV to the wave
               number  ~ or wavelength  ~, of the corresponding photon energy,  the relation

                                    AE (eV)  =  1.23980  x  10 -4  ~ (cm -l)       (2.31)


               is  used,  where  ~  =  1/~,. (For  blue  light  of  about  480  nm  the  following  relations  are
               obtained:  480 nm  =  4.8  •  10 -7 m  =  0.48 #m  =  20  833 era- 1 =  2.58 eV.) The rotational
               energies are normally in the range 0.001  -  0.1 eV, i.e. the wavelength region 10 -3  -  10 -5
               m.  The partition  function  for the rotational  energy is  obtained by introducing  (2.30)  into
               (2.19).  More complicated expressions are obtained for polyatomic and nonlinear molecules.
                (c)  Vibrational  energy.  For a diatomic  molecule the vibrational  energy is given by

                                           Evi b-  hewv(nv+ ~h)                    (2.32)

               where

                                          Wv=  V2(k' Imred) ~h /(vrc)              (2.33)

               is the zero point vibrational frequency (the molecule is still vibrating at absolute zero, when
               no other movements occur) and n v the vibrational quantum number,  k'  is the force  constant
               for  the particular  molecule.



               2.6.4.  The  isotopic  ratio

                It  is  seen  from  this  digression  that  the  mass  of  the  molecular  atoms  enters  into  the
               partition functions for all three modes of molecular movement.  The largest energy changes
               are  associated  with  the  vibrational  mode,  and  the  isotopic  differences  are  also  most
               pronounced  here.  Neglecting  quantization  of translational  and rotational  movements,  one
               can  show  that
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