Use of TLS parameters to model anisotropic displacements in macromolecular refinement.

An essential step in macromolecular refinement is the selection of model parameters which give as good a description of the experimental data as possible while retaining a realistic data-to-parameter ratio. This is particularly true of the choice of atomic displacement parameters, where the move from individual isotropic to individual anisotropic refinement involves a sixfold increase in the number of required displacement parameters. The number of refinement parameters can be reduced by using collective variables rather than independent atomic variables and one of the simplest examples of this is the TLS parameterization for describing the translation, libration and screw-rotation displacements of a pseudo-rigid body. This article describes the implementation of the TLS parameterization in the macromolecular refinement program REFMAC. Derivatives of the residual with respect to the TLS parameters are expanded in terms of the derivatives with respect to individual anisotropic U values, which in turn are calculated using a fast Fourier transform technique. TLS refinement is therefore fast and can be used routinely. Examples of TLS refinement are given for glyceraldehyde-3-phosphate dehydrogenase (GAPDH) and a transcription activator GerE, for both of which there is data to only 2.0 A, so that individual anisotropic refinement is not feasible. GAPDH has been refined with between one and four TLS groups in the asymmetric unit and GerE with six TLS groups. In both cases, inclusion of TLS parameters gives improved refinement statistics and in particular an improvement in R and free R values of several percent. Furthermore, GAPDH and GerE have two and six molecules in the asymmetric unit, respectively, and in each case the displacement parameters differ significantly between molecules. These differences are well accounted for by the TLS parameterization, leaving residual local displacements which are very similar between molecules and to which NCS restraints can be applied.

[1]  D. Phillips,et al.  Crystallographic studies of the dynamic properties of lysozyme , 1979, Nature.

[2]  A. Rich,et al.  Local mobility of nucleic acids as determined from crystallographic data. II. Z-form DNA. , 1984, Journal of molecular biology.

[3]  G. S. Pawley,et al.  Further refinements of some rigid boron compounds , 1966 .

[4]  E A Merritt,et al.  Raster3D: photorealistic molecular graphics. , 1997, Methods in enzymology.

[5]  J. Littlechild,et al.  Crystal structure of the glyceraldehyde-3-phosphate dehydrogenase from the hyperthermophilic archaeon Sulfolobus solfataricus. , 1999, Journal of molecular biology.

[6]  A. W. Pryor,et al.  Thermal vibrations in crystallography , 1975 .

[7]  D. S. Moss,et al.  RESTRAIN: restrained structure-factor least-squares refinement program for macromolecular structures , 1989 .

[8]  D S Moss,et al.  Segmented anisotropic refinement of bovine ribonuclease A by the application of the rigid-body TLS model. , 1989, Acta crystallographica. Section A, Foundations of crystallography.

[9]  D. S. Moss,et al.  TLSANL: TLS parameter-analysis program for segmented anisotropic refinement of macromolecular structures , 1993 .

[10]  R Diamond,et al.  On the use of normal modes in thermal parameter refinement: theory and application to the bovine pancreatic trypsin inhibitor. , 1990, Acta crystallographica. Section A, Foundations of crystallography.

[11]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[12]  M. Sternberg,et al.  Dynamic information from protein crystallography. An analysis of temperature factors from refinement of the hen egg-white lysozyme structure. , 1979, Journal of molecular biology.

[13]  W. Hendrickson,et al.  Description of Overall Anisotropy in Diffraction from Macromolecular Crystals , 1987 .

[14]  G. Sheldrick,et al.  SHELXL: high-resolution refinement. , 1997, Methods in enzymology.

[15]  N Go,et al.  Normal mode refinement: crystallographic refinement of protein dynamic structure. I. Theory and test by simulated diffraction data. , 1992, Journal of molecular biology.

[16]  M. A. Wilson,et al.  The 1.0 A crystal structure of Ca(2+)-bound calmodulin: an analysis of disorder and implications for functionally relevant plasticity. , 2000, Journal of molecular biology.

[17]  J. Dunitz,et al.  Non-rigid-body thermal-motion analysis , 1973 .

[18]  F. L. Hirshfeld Can X‐ray data distinguish bonding effects from vibrational smearing? , 1976 .

[19]  P. Kraulis A program to produce both detailed and schematic plots of protein structures , 1991 .

[20]  Jack D. Dunitz,et al.  A test for rigid‐body vibrations based on a generalization of Hirshfeld's `rigid‐bond' postulate , 1978 .

[21]  A lattice‐dynamical interpretation of molecular rigid‐body vibration tensors , 1973 .

[22]  K. Harata,et al.  Crystallographic evaluation of internal motion of human alpha-lactalbumin refined by full-matrix least-squares method. , 1999, Journal of molecular biology.

[23]  W. Schweizer,et al.  Internal molecular motion of triphenylphosphine oxide: analysis of atomic displacement parameters for orthorhombic and monoclinic crystal modifications at 100 and 150 K , 1985 .

[24]  Jack D. Dunitz,et al.  Atomic Dispacement Parameter Nomenclature. Report of a Subcommittee on Atomic Displacement Parameter Nomenclature , 1996 .

[25]  Jeremy C. Smith,et al.  X-ray diffuse scattering and rigid-body motion in crystalline lysozyme probed by molecular dynamics simulation. , 1998, Journal of molecular biology.