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MODEL BUILDING, REFINEMENT, AND VALIDATION  161

        goal of maximizing the agreement between the mea-  experimental diffraction data extending to at least
        sured experimental diffraction data and predicted  atomic resolution (about 1.2 Å) are necessary to pro-
        structure factors from the model. At the same time,  vide a sufficient number of reflections and thus
        they optimize the agreement to a variety of a priori  a high enough observation-to-parameter ratio to
        available information, most commonly the stereo-  justify an atomic model. The dependence of the
        chemistry of the model. The objective function for  observation-to-parameter ratio is exemplified in
        the refinement is a high-dimensional function. Its  Fig. 11.3. The number of diffracted X-ray reflections
        dimensionality is equal to the number of refined  for a complete data in P1 lattice can be computed as
        independent parameters and thus typically is in
                                                             2π
        the order of many thousands. The reader may be  N refl  =  3  V
        referred to Tronrud (2004) for a discussion on crys-  3d
        tallographic model parametrization. The landscape  where V is the volume of the asymmetric unit and
        of this objective function in its multidimensional  d is the resolution. Assuming the asymmetric unit
        space depends primarily on the atomic coordinates  to contain only one ‘average’ atom, nitrogen, with
        of the model and is characterized by many minima.  a molecular mass of 14 and the xyzB refinement
        An additional complexity arises from the crystallo-  (four parameters per atom) it is straightforward to
        graphic phase problem and the often initially poor  compute the observation-to-parameter ratio for a
        phase quality, which affect the completeness of the  given value of the solvent content. From Fig. 11.3
        model, where even challenging techniques, such as  it becomes evident that at atomic resolution the
        conjugate-gradient, do not necessarily lead to the  optimization problem is well overdetermined and
        global minimum.                              one can easily afford even anisotropic treatment of
          Macromolecular diffraction data are rarely of  atomic displacement parameters, while at a resolu-
        sufficient quality and quantity to allow construc-  tion lower than about 2.7 Å the number of observed
        tion of atomic models that would obey basic  data becomes smaller than the number of parame-
        stereochemistry just based on this optimization of  ters. This problem of lack of data is (to an extent)
        parameters to data. The observation-to-parameter  overcome by restraining (or less usually constrain-
        ratio is a key factor in optimization procedures.  ing) the model parameters to values determined
        For the optimization of a crystallographic model,  from small molecule structure solutions. Most of the


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                       Reflections per parameter  13 9 8
                         15
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                         12
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                          4 7 6 5
                          3
                          2
                          1
                          0
                           0.0     0.5     1.0    1.5     2.0     2.5     3.0
                                             Resolution of the data (Å)
        Figure 11.3 The ratio of the number of reflections to the number of parameters in the XYZB crystallographic refinement of a protein
        model as a function of the resolution of the data. The data are assumed to be complete and the solvent content to be 50%.
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