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Molecular Orbital Theory   53

           Remember that there are N of these equations, one for each of the N possible
           values of i. If we regard the 6,'s  as unknowns, these equations constitute a set of N
           linear homogeneous equations in  N unknowns.  The set has solutions for those
           values of E for which the determinant







           is zero; in more compact notation,
                                       det JH,, - ES,,J  = 0                 (A2.15)
           This is the secular equation.
                Solution of the secular equation amounts to finding the roots of an Nth order
           equation in E. The N roots  are the energies of the  N molecular orbitals;  the
           forms of the orbitals in terms of the basis atomic orbitals gpj  are found by substi-
           tuting each value of E, in turn, back into Equations A2.13 and solving for the cys
           using the additional condition that each MO +, is to be normalized,





          Electrons  are  then  assigned,  two  to  each  molecular  orbital  starting from  the
          lowest energy.
               Standard  computer  methods  are  available  to  solve  Equation  A2.15  if
          numerical values can be found for Htj and St,. The St, can be determined easily
          with the aid of the computer, but the Hij, which represent the interactions be-
          tween the basis orbitals, are more difficult to obtain. A number of methods can
           be used to deal with this problem.







           The Hiickel method is the simplest of the quantitative MO techniques. It has the
           following characteristics :

               1.  Only .rr electrons are treated.
               2.  The basis consists of a p orbital on each carbon atom of the T system.
               3.  All  overlaps, Stj, i  # j,  are assumed  to be zero;  overlaps St, are unity
           because the basis orbitals are normalized.
               4.  Interactions Hi,, i # j, are assumed to be zero except for pairs of basis
           orbitals i and j that  are on carbons directly bonded  to each other.  All H,, for
           bonded pairs are assumed to have the same value, which is not calculated but is
           simply called /3.  (/3  represents an energy lowering and, therefore, is negative.)
               5.  Hi,, which represents the energy of an electron in the basis orbital i be-
           fore any interaction with its neighbors occurs, is the same for all i (because all
           basis orbitals are the same). It is called a.
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