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2.4 Diffraction by Randomly Oriented Molecules         27

             The beam has a wavelength determined by the momentum of a typical particle therein.
             This in turn is determined by the kinetic energy of the particle. The jet scatters the beam
             into a characteristic diffraction pattern.
                Consider the scheme in figure 2.1.  A potential between 30 and 70 kilovolts acceler-
             ates the electrons emitted by a hot filament. The electrons travel in a vacuum tube to a
             vapor stream containing the molecules to be studied. These diffract the beam. The result-
             ing pattern is recorded on a photographic plate. Pertinent measurements are then made.
                In analyzing these, we consider each atom in a target molecule to act as a scattering point.
             Since molecular distances are very small compared to the dimensions of the apparatus, we
             also consider the incident rays and the rays scattered at a certain angle by a molecule to be
             parallel. For simplicity, we also limit ourselves initially to diatomic molecules, those of type
             AB. A particular orientation of a scattering molecule then acts as shown in figure 2.2.
                A  reference Cartesian system is  erected on atom A as shown.  The corresponding
             spherical coordinates of atom B are (r, a ,[3). Line AC is drawn perpendicular to the inci-
             dent rays; line BD perpendicular to the scattered rays. Then points A and C would be at
             the same phase. Also points B and D. But the ray scattered by A travels the extra length
             (which may be either positive or negative)
                                              £5  =AD-CB.                            [2.19]
                From the figure and trigonometric definitions, we find that
                                    AD = rsin a cos r = rsin a sin(,B + e),          [2.20]


             so
                                            CB=rsinasin,B,                           [2.21]
                          £5  = r sin a[ Sin(,B + e) - Sin,B] = 2r sin ± sin a cos(,B + ± J   [2.22]
                                                           e
                                                                          e

                In the coherent approximation, the electron wave has the amplitude
                                                                                     [2.23]

             where N is a normalization constant, s the distance traveled, and t the time. Parameter
             k is the wavevector
                                                k =  27r                             [2.24]
                                                    ).,'

                           To Vacuum
                           I
                                                          Photographic Plate







                                                                   FIGORE:U  Setup tor
                                                                   studying' Ute diffraction of
                                                                   electrol1$ .Pv randomly
                                                                   orientedrnolecu1es·,
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