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Methods for Structural and Chemical Characterization of Nanomaterials  135

        2000 g/mol (i.e., n~ 28) in 1 L. The density of the resulting solution is
                 3
        1.06 g/cm . First, the solution is mounted in a variable light path X-ray
        cell for measuring its transmission as a function of its thickness. The
        transmission T of a monochromatic X-ray beam obeys the following
        relationship:

                                    I    2m*>re
                                      5 e                             (22)
                                    I o
                                                           ~
                                                   2
        where 
   is the mass absorption coefficient (cm /g), e   d  d is the thick-
        ness, and   the density. The mass absorption coefficient is tabulated for
        each atom at all X-ray incident energies. (The mass absorption coeffi-
        cient can be found on the NIST website http://www.nist.gov). For a mix
        of compounds, the average mass attenuation coefficient is obtained with
        the following formulation:

                                  m*
                                         x sm/rd
                                  r  5    i    i                      (23)
        where x is the mass fraction of compound i. For the cerium solution, we have
               i
                                                            2
                                  2
        x powder   38/1060   3.58 10 ; x PAA   30/1060   2.83 10 ; and x water
        1 x powder   0.9242. The mass attenuation coefficient of the powder and
                                               2
        water are respectively 179.88 and 9.83 cm /g. Thus, according to Eq.17,
                                                            2
        the solution has a mass attenuation coefficient of 15.9 cm /g. Figure 4.16
        shows the comparison between the experimental measurement of the


























        Figure 4.16 Experimental and theoretical transmission through a 38 g/l CeO 2 nanopar-
        ticle suspension.
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