Lei Yang, Guang Song, Robert L. Jernigan  Biophysical Journal 

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How Well Can We Understand Large-Scale Protein Motions Using Normal Modes of Elastic Network Models?  Lei Yang, Guang Song, Robert L. Jernigan  Biophysical Journal  Volume 93, Issue 3, Pages 920-929 (August 2007) DOI: 10.1529/biophysj.106.095927 Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 1 A simple illustration of the pathway difference for a global conformational change ΔX involving a rotation and the initial moving direction ΔX0 when translation is utilized to represent a rotation, as a rigid stick rotates counterclockwise 90° from position A to B. Biophysical Journal 2007 93, 920-929DOI: (10.1529/biophysj.106.095927) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 2 Characterization of the protein dataset: distributions of protein sizes, resolutions, and pairwise RMSDs. (a) Histogram of protein sizes. (b) Histogram of protein resolutions for x-ray structures. (c) Histogram of pairwise RMSDs. Biophysical Journal 2007 93, 920-929DOI: (10.1529/biophysj.106.095927) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 3 Histogram of the reduced degrees of freedom δreduced. There are some proteins that possess high degrees of freedom, and thus low collectivity, although most have <100 degrees of freedom. Biophysical Journal 2007 93, 920-929DOI: (10.1529/biophysj.106.095927) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 4 Concertedness of conformational transitions for 170 pairs of proteins. For category II.B (see Table 1) the domain hinge motions (with proteins indexed from 76 to 134, are marked by the black bar at the top of the figure), there typically exists a higher concertedness than for the other motion classes. Biophysical Journal 2007 93, 920-929DOI: (10.1529/biophysj.106.095927) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 5 Maximum overlaps using ENM. (a) Maximum overlap as a function of the transition scale, the RMSD between the open and closed structures. (b) Histogram of maximum overlaps. Biophysical Journal 2007 93, 920-929DOI: (10.1529/biophysj.106.095927) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 6 Comparison of the new model (domain-ENM) with the old (uniform ENM). (a) Scatter plot of the maximum overlaps. (b) Scatter plot of the CSO(20)s. The lines, along the direction of the arrow, indicate where the increasing scales of improvement are. Biophysical Journal 2007 93, 920-929DOI: (10.1529/biophysj.106.095927) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 7 Cumulative square overlaps (CSOs) for some proteins using different models: uniform ENM, ENM with rigid domains, ENM with the improved overlap definition (see Eq. 5), and ENM with both rigid domains and the improved overlap definition (i.e., domain-ENM). The first six modes account for the rigid body translation and rotation of the system. Biophysical Journal 2007 93, 920-929DOI: (10.1529/biophysj.106.095927) Copyright © 2007 The Biophysical Society Terms and Conditions

Figure 8 Relationship between the overlap (maximum overlap or CSO(20)) and δreduced (the inverse of collectivity) using the original overlap definition and ENM (a), the improved overlap definition and domain-ENM (b), and their dependence on protein size N (c). There is a strong correlation between overlap and collectivity (0.49 and 0.55 in a and 0.65 and 0.70 in b, from left to right), while there is almost no correlation between the overlap and the protein size (0.11 and 0.16 in c, from left to right). Biophysical Journal 2007 93, 920-929DOI: (10.1529/biophysj.106.095927) Copyright © 2007 The Biophysical Society Terms and Conditions