Page 23 - Mechanism and Theory in Organic Chemistry
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surfaces
                                                                                are
                                                                           they
                  of all ad.jacent poin~~hickaLnct~-zerazera~~eec~~d~o~es;
                  in three-dimensional space, and most of the important ones for our purposes are
                  planes, like those shown in Figure 1 .I  for the P and d orbitals illustrated.  (Nodes
                  can also be spherical, and of other shapes, but these are of less concern to us.)
                  The Physical Significance of Atomic Orbital Functions
                  The fact that an orbital function p is of different algebraic sign in different regions
                  has no particular  physical significance for the behavior  of an electron that finds
                  itself in the state defincd by the orbital. (We shall scc shortly that the significance
                  of the signs comes from  the way in which  orbitals can be  combined  with  each
                  other.) The quantity that has physical meaning is  the value at each point of the
                  function qP, which is positive  everywhere, since the square of a negative number
                  is positive.  T_he ssquared functionLP2, gives the probability of findingthe electron
                  at various  points  in  space.  Diagrams  like  that  in  Figure  1.2,  with  shading of
                  <arying  density showing the relative probabilityoffinding the electron in various
                  regions or, more succinctly, the electron dzrtrzbuLzon or electron denrzty,  are ~tually
                            w2. not of o, itself. The genemlshpeaf~ will be similaa~heshape
                  pi-res_of
                  of2.  The orbitals and their squares have no edges, even though definite outlines
                  are usually  drawn in diagrams; the values merely  approach closer and closcr  to
                  zero as one goes farther and farther from the nucleus.
                  Extension to Other Atoms
                  The hydrogen  atomic orbitals would  not do us a great deal of good if orbitals of
                  other  atoms were radically  different, since in that case different pictures would
                  be required for each atom. But the feature of the hydrogen  atom problem  that
                  determines the most  important characteristics of the hydrogen  atom orbitals is
                  the spherical symmetry. Since all the atoms are spherically symmetric, the atomic
                  orbitals of all atoms are similar, the main difference being in their radial depen-
                  dence,  that is,  in how rapidly they approach zero as one moves away from the
                  nucleus. Because the radial dependence is of minimal importance in qualitative
                  Figure 1.2  Electron  density, v2, for  1s and  2p  atomic orbitals.  The density  of  shading is
                           roughly proportional  to v2.
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