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Applied vibrational spectroscopy     329





                                 Polyatomic normal modes

        A diatomic molecule possesses only  one  mode of vibration, the stretching and
        compression of the bond between the two atoms. The number  of  distinct  modes  of
        vibration in a non-linear polyatomic molecule containing N>2 atoms is 3N−6. (To specify
        the displacement of each of  N atoms in three dimensions requires a  total  of  3N
        coordinates. Three of these coordinates specify the position of the center of mass of the
        molecule, and therefore correspond to the translational modes of the molecule, and three
        coordinates specify the orientation in space of the molecule, and therefore correspond to
        the rotational modes of the molecule.) A linear molecule of  N atoms possesses  3N−5
        vibrational modes since only two angles are required to specify the orientation in space of
        a linear molecule.
           The number of vibrational modes increases rapidly with the size of the molecule. For
        example, H 2O is a non-linear triatomic molecule and has three modes of vibration, CO 2 is
        a linear triatomic molecule and has four modes of vibration, whereas benzene, C 6H 6, has
        30 modes of vibration.
           It is easier to visualize the vibrational modes of a polyatomic molecule when particular
        combinations  of  bond  stretches  or bends are considered together. These collective
        vibrational displacements, in which the atoms all move in phase and with the same
        frequency, are called normal modes. Exactly 3N−6, or 3N−5, independent normal modes
        of molecular vibration can be derived for non-linear,  or  linear,  polyatomic  molecules,
        respectively. Each normal mode behaves like a harmonic oscillator with a reduced mass,
        µ, and force constant,  k,  that  depend  on  which atoms and bonds contribute to the
        vibration (Table 2).
           Figure 1  illustrates  the normal modes of vibration of H 2O and CO 2. The bending
        vibration of CO 2 is doubly  degenerate since the bending motion can also be drawn
        perpendicular to the plane of the paper in  Fig. 1b. The degeneracy accounts  for  the
        required additional vibrational mode of linear
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