Global motions of the nuclear pore complex: Insights from elastic network models

30Citations
Citations of this article
74Readers
Mendeley users who have this article in their library.

Abstract

The nuclear pore complex (NPC) is the gate to the nucleus. Recent determination of the configuration of proteins in the yeast NPC at ,5 nm resolution permits us to study the NPC global dynamics using coarse-grained structural models. We investigate these large-scale motions by using an extended elastic network model (ENM) formalism applied to several coarse-grained representations of the NPC. Two types of collective motions (global modes) are predicted by the ENMs to be intrinsically favored by the NPC architecture: global bending and extension/contraction from circular to elliptical shapes. These motions are shown to be robust against tested variations in the representation of the NPC, and are largely captured by a simple model of a toroid with axially varying mass density. We demonstrate that spoke multiplicity significantly affects the accessible number of symmetric low-energy modes of motion; the NPC-like toroidal structures composed of 8 spokes have access to highly cooperative symmetric motions that are inaccessible to toroids composed of 7 or 9 spokes. The analysis reveals modes of motion that may facilitate macromolecular transport through the NPC, consistent with previous experimental observations. © 2009 Lezon et al.

Figures

  • Figure 1. Schematic view of model adopted for the NPC/NE system. The yeast NPC consists of 456 proteins (nucleoporins), shown here as spheres, that form eight identical spokes. The cytoplasmic face of the NPC (facing the viewer) is colored pink, and the nuclear face is colored light blue. A single spoke is highlighted in red/blue. The lumenal ring, consisting of sixteen POM152 nucleoporins is colored orange. Half of the NE fragment is shown in silver, and the border of the NE fragment is colored black. doi:10.1371/journal.pcbi.1000496.g001
  • Figure 2. Slow modes of a uniform-density toroid. (A) The first mode is a two-fold degenerate bending of the toroid. The centroids are colored blue to red to indicate increasing mobility. (B) The second mode is a two-fold degenerate stretching of the toroid. (C) The third mode is a nondegenerate rolling mode. The centroids here are colored from blue to red as a function of initial distance from the center of the toroid. The mass centroids on the top (visible) surface move along the toroid surface toward the central channel, and the centroids on the opposite side move away from the central channel toward the toroid perimeter. (D) Mode 6 is a non-degenerate dilation. doi:10.1371/journal.pcbi.1000496.g002
  • Figure 3. Differences in the mobilities of toroid models induced by mass redistribution. (A) Three views are shown for the second mode of a toroid with axially varying mass density. In each view, the z-axis is shown (by the dot or arrow). The uneven mass distribution causes increased mobility on the lighter side of the toroid (compare to Figure 2B). (B) The fraction change in mobility, DB/B, from the uniform-density toroid is plotted against axial coordinate for three toroid models with non-uniform mass distributions: mass distributions linearly dependent on radial coordinate (red squares), distance from minor axis (black circles), and axial coordinate (blue triangles). The solid lines and filled symbols refer to the first mode, which is only slightly altered in the first two cases, as indicated by all points falling close to zero on the ordinate. When the mass is distributed such that the cytoplasmic (z.0) side is more massive than the nuclear (z,0) side, there is an increase in mobility in the cytoplasmic side and a decrease in mobility in the nuclear side relative to the first mode. The opposite effect is observed for the second mode, shown in dashed lines. doi:10.1371/journal.pcbi.1000496.g003
  • Figure 4. Overlap of global modes for spoke-based models with those of uniform toroid. The three panels show the correlation cosines between the slowest modes of toroids composed of 7 (panel A), 8 (panel B) and 9 (panel C) uniform-density spokes with those of a uniform toroid. Perfect agreement between the modes of two models would be indicated by the unit matrix. For clarity, the blocks corresponding to different modes are separated by thin lines. The 262 blocks refer to 2-fold degenerate modes, and the smaller squares within each of these capture the mode overlap as well as an arbitrary phase separation. Here it can be seen that increasing the number of spokes reduces the number of off-diagonal elements in the matrix, indicating a higher overlap between the two sets. doi:10.1371/journal.pcbi.1000496.g004
  • Figure 5. First two modes of yeast NPC. Three views of the two slowest modes of the NPC without (A and D) and with (B and E) the NE fragment are shown. The z-axis is shown in panel A, and orientations are the same in panels B, D and E. Mode 1 is a ‘‘stretching/elongation’’ mode that mobilizes the nuclear face (z,0) more than the cytoplasmic face, whether or not the NE fragment is included in the model. Mode 2 is a ‘‘bending’’ mode that elongates the NPC in the absence of the NE (D), but not when the NE is included (E). For a clearer visualization of the motion, the lower half of the structure is shown in translucid colors in panel E. Scaled mobilities are plotted against axial position in panels C and F for the NPC alone (blue) and the NPC/NE (red). The addition of the NE decreases mobility of the POM rings in the first mode, as shown by the absence of a peak near z = 0 in panel C. In the second mode, the NE creates a more even distribution of motion in the cytoplasmic and nuclear faces, as shown by the peaks near z = +/212 for the red curve in panel F. doi:10.1371/journal.pcbi.1000496.g005

References Powered by Scopus

Anisotropy of fluctuation dynamics of proteins with an elastic network model

1404Citations
N/AReaders
Get full text

Simple allosteric model for membrane pumps [27]

966Citations
N/AReaders
Get full text

A hierarchy of timescales in protein dynamics is linked to enzyme catalysis

918Citations
N/AReaders
Get full text

Cited by Powered by Scopus

Global dynamics of proteins: Bridging between structure and function

497Citations
N/AReaders
Get full text

Normal mode analysis as a routine part of a structural investigation

59Citations
N/AReaders
Get full text

Mechanosensing at the nuclear envelope by nuclear pore complex stretch activation and its effect in physiology and pathology

49Citations
N/AReaders
Get full text

Register to see more suggestions

Mendeley helps you to discover research relevant for your work.

Already have an account?

Cite

CITATION STYLE

APA

Lezon, T. R., Sali, A., & Bahar, I. (2009). Global motions of the nuclear pore complex: Insights from elastic network models. PLoS Computational Biology, 5(9). https://doi.org/10.1371/journal.pcbi.1000496

Readers over time

‘09‘10‘11‘12‘13‘14‘15‘16‘17‘18‘19‘20‘21‘22‘230481216

Readers' Seniority

Tooltip

PhD / Post grad / Masters / Doc 29

45%

Researcher 26

40%

Professor / Associate Prof. 8

12%

Lecturer / Post doc 2

3%

Readers' Discipline

Tooltip

Agricultural and Biological Sciences 27

47%

Biochemistry, Genetics and Molecular Bi... 12

21%

Chemistry 10

17%

Physics and Astronomy 9

16%

Save time finding and organizing research with Mendeley

Sign up for free
0