Page 97 - Mechanism and Theory in Organic Chemistry
P. 97

solute particle  that itself has a dipole moment or a  net  charge. The solvent di-
                poles will  tend  to orient themselves around the solute in the manner  indicated
                in Figure 2.5.  The first solvent layer will be the most highly ordered, with ran-
                domness increasing as the influence of the solute particle decreases with increasing
                distance. A smaller solute ion will generate a more intense electric field than will
                a large one, and so will have a stronger and more far-ranging capacity to orient
                solvent dipoles around it. In the solvent molecule itself, one end of the dipole may
                be  exposed while  the  other  end  is  buried  inside the  bulk  of  the  molecule.  In
                dimethylsulfoxide, for instance, the negative oxygen end of the dipole is exposed
                (27), whereas the positive end is not; this solvent interacts  much more strongly










                with the cations of an ionic solute than with the anions. Formation of solvation
                layers around the solute particles will be accompanied by heat evolution  (nega-
                tive AH) and an increase in order (negative AS).



               Table 2.11  DIELECTRIC CONSTANT, DIPOLE MOMENT, AND  MOLECULAR
                         POLARIZAB~LITY SELECTED SOLVENTS'
                                      FOR
                                                              P        PolarizabilityC
                Solvent                              eb     (debyes)   (cm3 x  loz4)
               Nonpolar Proticd
                     0
                     11                             6.15@    1.68          5.16
               CH3-C-OH
                (CH3)3C-OH                          12.47    1.66          8.82
               CH3-(CH2)6-OH                        13.3     1.55         12.46









               Nonpolar Aprotic
                CCl,
   92   93   94   95   96   97   98   99   100   101   102