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234                                                  Essentials of Physical Chemistry






































            FIGURE 11.1  Erwin Rudolf Josef Alexander Schrödinger (1887–1961) was an Austrian theoretical physicist
            who is famous for his wave equation treatment of quantum mechanics. He was awarded the Nobel Prize in
            physics in 1933. He became a full professor at the University of Zurich in 1921 and in 1926 wrote four
            extremely important papers establishing wave mechanics. He left Germany in 1933, although his parents were
            Christian, and moved to various lecturing positions for several years until in 1940 he was invited to set up an
            Institute for Advanced Study in Dublin. There he continued to write many papers and a small book What is Life,
            with conjecture that genes are molecular, which inspired Francis Crick (of Watson and Crick) and Max
            Delbruck among others to study DNA.


            sophomore physics texts) and V as the conventional symbol for whatever potential energy there may
                                               mv 2  (mv) 2               2
                                                          ¼ (E tot   V) ) (mv) ¼ 2m(E tot   V) so
            be. With that understanding, we have T ¼  ¼
                                                2     2m
                          2                     2
                         d        2px       (mv)       2px      2m(E tot   V)     2px
            that  now        A sin      ¼         A sin     ¼               A sin        or
                         dx 2      l           h 2      l             h 2          l
               2
              d        2m(E tot   V)
                                   c. This is where it gets interesting in that Schrödinger identified the
                 c ¼
             dx 2            h 2
                                                    2     2
                                                   h
                                                        d
            energy with a mathematical operator! Thus       c ¼ (E tot   V)c and further we have
                                                  2m    dx 2
                2      2                           2     2
               h
                                                  h
                    d                                  d
                        c þ Vc ¼ E tot c and finally         þ V c ¼ E tot c or H op c ¼ E tot c.
              2m   dx 2                          2m    dx 2
              This has major implications in that there is a mathematical (calculus) operator H op , which
            represents the total energy of a particle (in only one dimension so far) and a function c, which
            incorporates the De Broglie condition and is an eigenfunction of the total energy operator. Note the
            left side of the equation must be in energy units since the right side is in terms of E tot .
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