Page 95 - Mechanism and Theory in Organic Chemistry
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of all the rotational  degeneracies of the molecule. For  example,  in  acetone  the
                molecule as a whole has a  twofold axis of symmetry  (this is called the external
                axis). Each  of the two  methyl groups has a  threefold axis of symmetry  (called
                internal axes). Thus for acetone u is 2  x  3  x  3 and So is calculated :


                                                \   ,-
                                  -Rho=  -Rln18=       -5.74
                                       So (acetone)  = + 70.09 cal mole-'   OK- '
                The experimental value is  70.5 cal mole-l  OK-l.
                     If a molecule is optically active, R In n must be added to its entropy estim-
                ate, where n is the total number of stereoisomers of equal energy.

                Guide to the Use of the Group Tables (Tables 2.6-2.10)
                     1.  AH;  and So are the  heat  of formation  and  entropy,  respectively, of a
                group when that group is in a molecule in its standard state of hypothetical ideal
                gas at 1 atm pressure and 25°C. All values of AH;  are in kilocalories per  mole,
                and all values of So are in calories per mole per degree (K) . For a simple method
                of converting So and AH;  to other temperatures, see Benson et al., Chem. Rev., 69
                (1969), p. 313.
                     2.  In order  to  assign  values  to  all groups,  some groups  have  had  to  be
                assigned  arbitrary  values.  Groups  in  brackets  in  Tables  2.G2.10  are  those
                groups. Estimated values obtained from a single compound are in parentheses.


                2.4  SOLUTIONS 27
                The thermochemical additivity scheme outlined in the previous section is based on
                gas-phase data. Since most organic reactions are carried out in solution, it would
                be most useful to be able to understand and predict the thermochemical changes
                that  molecules,  ions,  and  transition  states  undergo  when  dissolved in  various
                solvents. Our knowledge of the structure of liquids and of their interactions on the
                molecular  level with  solutes is still too incomplete  to permit  more  than a  very
                rough qualitative answer to this problem. We shall proceed by discussing briefly
                the influence on solvent properties of the most important parameters characteriz-
                ing liquids.
                Dielectric Constant
                The first property of solvents to be  considered is the dielectric constant,  E.  The
                dielectric constant of a  substance measures the reduction of the strength of the
                electric  field  surrounding  a  charged  particle  immersed  in  the substance,  com-
                pared to the field strength around the same particle in a vacuum. The dielectric
                constant  is  a  macroscopic  property;  that  is,  its  definition  and  measurement


                  The following discussions of solvent effects will provide further information: (a) T. C. Waddington,
                Non-Aqueous  Solvents,  ThomasNelson, London,  1969;  (b) E.  M.  Kosower,  An  Introduction  to Physical
                Organic Chemistry, Wiley,  New  York,  1968, p.  259;  (c) T. C.  Waddington, Ed.,  Non-Aqueous  Solvent
                System, Academic,  London,  1965; (d) E. S. Amis and J. F.  Hinton, Solvent  Effects  on Chemical Phcno-
                menu, Academic, New York,  1973; (e) J. F. Coetzee and C. D. Ritchie, Eds., Solute-Solvent  Interactions,
                Marcel Dekker,  New York,  1969; (f) A. J. Parker, Chem. Rev.,  69,  1  (1969).
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