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The Schrödinger Wave Equation                                               247


                                       000                   –645
                                 +559        –559
                                                       –322        322
                                –559         +559      –322        322
                                       000                   645

                                       000                   –532
                                –461         461       –266        –266

                                –461         461
                                                        266         266
                                       000                   532
                                                  344
                                             344        344
                                             344        344

                                                  344
            FIGURE 11.5  The 2Pz coefficients of benzene multiplied by 1000, obtained from a STO-3G SCF-MO
            calculation using the program PCLOBE, see Chapter 17. Only the lowest five orbitals are shown. (From
            Trindle, C. and Shillady, D., Electronic Structure Modeling: Connections between Theory and Software, CRC
            Press, Boca Raton, FL, 2008. With permission.)

                                                                                8
                           2
                                                                 2
                         8p (9:10938215   10  31  kg)(2:22816   10  10  m) (2:99792458   10 m=s)
                                            5(6:62606896   10  J   s)
                 l p!p* ¼                                    34
                         l p!p* ¼ 3:231217   10  7  m ffi 3231:217   10  10  m ¼ 3231 A ˚ :
            Experimentally the leading edge of the ultraviolet spectrum of naphthalene occurs at about 3150 Å
            but electronic spectra of large molecules are broadened by vibrational interactions as we will see in a
            later chapter. Thus we will take the calculated p ! p* wavelength as qualitatively correct; quite
            good considering the simplicity of the model. Overall as the aromatic molecules become larger, the
            POR model is useful for qualitative reasoning. The POR model was first discussed by Platt [4] in
            1949, expanded by Moffit [5] in 1954 and used for interpretation of magnetic circular dichroism
            spectra by Michl [6] in 1978.

            COMPARISON OF PIB AND POR APPLICATIONS
            An instructive comparison of the PIB and POR models is given by the diagram in Figure 11.5. The main
            pointforstudentsistoknowwhethertousethedegeneratelevelsinthePORmodelorthenon-degenerate
            levels in the PIB model. The next important approximation is to estimate length or circumference using
            an average of the –C¼C– bond length as 1.4 Å. From then on we have to realize these models mainly
            apply to conjugated hydrocarbons. We should remember that the POR model provides understanding of
            aromaticity. We have used these simple, but solvable, model systems to illustrate the postulates of
            quantum mechanics and now we are ready to proceed to more realistic problems.


            ADDITIONAL THEOREMS IN QUANTUM MECHANICS
            We now have seen two problems with exact solutions in quantum mechanics. Actually there are
            only a few such exact solutions remaining such as the harmonic oscillator, the rigid rotor, the
            hydrogen atom, and the forced harmonic oscillator, and we need to know some general principles
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