z-logo
Premium
TLSANL : TLS parameter‐analysis program for segmented anisotropic refinement of macromolecular structures
Author(s) -
Howlin B.,
Butler S. A.,
Moss D. S.,
Harris G. W.,
Driessen H. P. C.
Publication year - 1993
Publication title -
journal of applied crystallography
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.429
H-Index - 162
ISSN - 1600-5767
DOI - 10.1107/s0021889893002729
Subject(s) - macromolecule , anisotropy , rigid body , planar , displacement (psychology) , principal axis theorem , group (periodic table) , crystallography , materials science , physics , chemistry , geometry , classical mechanics , mathematics , computer science , optics , quantum mechanics , psychology , biochemistry , computer graphics (images) , psychotherapist
The atomic displacements of many of the atoms in a macromolecular structure can be modelled in terms of group motions described in the harmonic approximation by T , L and S tensors. Relevant groups may be planar side groups of protein chains, units of secondary structure such as α ‐helices or whole protein domains. For the TLS parameters to be interpreted, they must be related to the axes of inertia of the rigid groups and, in the case of the T and S tensors, must be calculated with respect to the centre of reaction of the rigid group. A program ( TLSANL ) is described that analyses these 21 TLS rigid‐body displacement parameters and their relation with the principal axes of the rigid body, from the output of the segmented anisotropic refinement of a macromolecular structure, as produced by a program such as RESTRAIN [Haneef, Moss, Stanford & Borkakoti (1985). Acta Cryst. A 41 , 426–433; Driessen, Haneef, Harris, Howlin, Khan & Moss (1989). J. Appl. Cryst. 22 , 510–516].

This content is not available in your region!

Continue researching here.

Having issues? You can contact us here