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Vibration coordinate
                Figure 2.12  The zero-point energy is proportional  to v  and thus to dm the C-D   bond
                          therefore has a  lower zero-point energy than the C-H   bond.


                The quantum mechanical treatment of the same model leads to energy levels


                and thus to energy-level separations Ae  = hv, where v is the classical frequency
                given  by  Equation  2.67.  Energies are measured  from  the lowest point  on the
                potential energy curve.
                     An important feature of the vibrational  energy levels is that the energy of
                the lowest possible level lies 3hv above the minimum of the potential curve. This
                zero-point energy, is by Equation 2.67,  inversely proportional to the square root
                of the mass.

                Primary Isotope Effects
                Figure 2.12 illustrates the zero-point energy level for a C-H   stretching vibration
                and compares it with the zero-point energy of the same stretch for a C-D   bond.
                In a reaction in which the GH (GD) bond breaks, there will be a primary
                isotope  effect. The stretching vibration  of the reactants is converted to the trans-
                lational motion over the barrier,  and the zero-point energy disappears for that   -
                particular  degree of freedom.  Since the  C-H   molecule starts out  at a  higher
                energy, its activation energy is lower, and k,/k,   will be greater than  1.
                     We can easily calculate the isotope effect to be expected were this loss of
                zero-point energy the sole contributor.  The C-D   frequency should be smaller :
                than the  GH frequency by  a factor of roughly  1/d2 = 111.41  according to
                Equation  2.67 ; the observed ratio is  closer to  1/1.35.50 The zero-point energy

                reduced  mass,


                When one of the masses is much larger than the other, as would be the case for a hydrogen attached
                to a large molecule p is approximately equal to the smaller mass.
                60 A.  Streitwieser, Jr.,  R. H. Jagow,  R. C. Fahey, and S. Suzuki, J. Amer.  Chem. Soc., 80, 2326 (1958).
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