Page 107 - Bruno Linder Elementary Physical Chemistry
P. 107

August 18, 2010 11:36      9in x 6in     b985-ch08     Elementary Physical Chemistry





                               92                   Elementary Physical Chemistry

                               8.6. The Schr¨odinger Equation

                               Schr¨odinger’s treatment is mathematically the simplest, and is most often
                               used in calculations. Basically, it is a differential equation which has to be
                               solved to produce the properties of the system under consideration. For
                                              o
                               example, the Schr¨dinger equation of a particle moving in one dimension,
                               having a mass m,is
                                                   2
                                                       2
                                                                  2
                                                             2
                                                −(h /8π m)d ψ/dx + Vψ = Eψ                 (8.4)
                               where V is the potential energy, E is the energy of the particle and ψ is the
                               wave-function. Solving this equation produces two types of information:
                               (1) A set of energy levels: E 1 , E 2,etc.
                               (2) A set of wave-functions, ψ n (x), associated with each energy state.
                                  Originally, Schr¨dinger believed that the wave function described the
                                                o
                               position of the particle. However, Bohr, who invited him to Copenhagen,
                               quickly convinced him that that was not the case. The wave-function ψ
                               has no physical significance. Today’s accepted interpretation (due to Born)
                               is that ψ ψ represents a probability density,and that ψ ψδv denotes the
                                       ∗
                                                                                ∗
                               probability of finding the particle within the volume element δv.[Thewave-
                               function is in general complex and the ψ denotes the complex conjugate.
                                                                  ∗
                               The product of the wave-function and its complex conjugate is always real.]
                                                                 +
                               Example 8.1. The ground state of He is
                                                                          3
                                                            3 1/2
                                                  ψ =(8/πa )    exp (−2r/a )               (8.5)
                                                            0
                                                                          0
                               where r is the distance of the electron from the nucleus, and
                                                 a 0 =52.9 × 10 −12  m=(52.9pm)            (8.6)
                               (a) What is the probability of finding the electron within a volume of ∆v =
                                      3
                                  1pm around the nucleus?
                              (b) What is the probability of finding the electron within a volume of 1 pm 3
                                  at a distance a 0 from the nucleus?

                               Solution
                                  The probability expression is (ψ is real)
                                                         3           3  2
                                  Prob =   ψψdv = (8/πa ) {exp(−2r/a )} dv
                                                         0           0
                                                                                 3
                                  In this problem, the r’s are constant and  dv =1 pm .
   102   103   104   105   106   107   108   109   110   111   112