Page 81 - Advanced Organic Chemistry Part A - Structure and Mechanisms, 5th ed (2007) - Carey _ Sundberg
P. 81

60                    Qualitative VB theory uses resonance structures and bond polarity relationships
                       to arrive at an indication of relative charge distribution. For example, in propenal
     CHAPTER 1         the combination of a preferred resonance structure and the higher electronegativity of
     Chemical Bonding  oxygen relative to carbon leads to the expectation that there will be a net negative
     and Molecular Structure
                       charge on oxygen and compensating positive charges on C(1) and C(3) (see p. 21).
                       How much the hydrogen atoms might be affected is not clear. As a first approximation,
                       they are unaffected, since they lie in the nodal plane of the conjugated   system, but
                       because the electronegativity of the individual carbons is affected, there are second-
                       order adjustments.
                                                            δ–
                                                            O
                                                      δ+   δ+

                           Numerical expression of atomic charge density in qualitative VB terminology
                       can be obtained by use of the electronegativity equalization schemes discussed in
                       Section 1.1.4. The results depend on assumptions made about relative electronegativity
                       of the atoms and groups. The results are normally in agreement with chemical intuition,
                       but not much use is made of such analyses at the present time. MO calculations
                       give the total electron density distribution as the sum of the electrons in all the filled
                       molecular orbitals. The charge distribution for individual atoms must be extracted
                       from the numerical data. Several approaches to the goal of numerical representation
                       of electron distribution have been developed. 79


                       1.4.1. Mulliken Population Analysis
                           In MO calculations, the total electron density is represented as the sum of all
                       populated MOs. The electron density at any atom can be obtained by summing the
                       electron density associated with the basis set orbitals for each atom. Electron density
                       shared by two or more atoms, as indicated by the overlap integral, is partitioned equally
                       among them. This is called a Mulliken population analysis. 80

                                                  N occ

                                             P = 2   c c X X                            (1.21)
                                                           $
                                                      #$ #
                                                   #=1
                                                   $

                                            P =     c c X X for %   on A                (1.22)
                                              A      #$ #   $     #
                           The Mulliken population analysis, and all other schemes, depend on the definition
                       used to assign charges to atoms. For example, the   orbital in formaldehyde has two
                       electrons, and according to HF/3-21G calculations they are assigned as shown at the left
                       below. When all the basis set orbitals are considered, the charge distribution is as shown
                                81
                       ontheright. OutputfromtypicalMOcalculationscanprovidethiskindofatomiccharge
                       distribution. No great significance can be attached to the specific numbers, since they are
                       dependent on the particular basis set that is used. The qualitative trends in redistribution
                        79
                          S. M. Bachrach, Rev. Comput. Chem., 5, 171 (1994).
                        80   R. S. Mulliken, J. Chem. Phys., 36, 3428 (1962).
                        81
                          W. J. Hehre, L. Radom, P. v. R. Schleyer, and J. A. Pople, Ab Initio Molecular Orbital Theory, Wiley-
                          Interscience, New York, 1986, pp. 118–121; A. Szabo and N. S. Ostlund, Modern Quantum Chemistry:
                          Introduction to Advanced Electronic Structure Theory, Macmillan, New York, 1982.
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