Membrane curvature sensing and symmetry breaking of the M2 proton channel from Influenza A

  1. James Lincoff
  2. Cole VM Helsell
  3. Frank V Marcoline
  4. Andrew M Natale
  5. Michael Grabe  Is a corresponding author
  1. Cardiovascular Research Institute, Department of Pharmaceutical Chemistry, University of California, San Francisco, United States
  2. Graduate Group in Biophysics, University of California, San Francisco, United States
18 figures, 3 tables and 1 additional file

Figures

M2 channels and influenza egress.

(A) Structural organization of the nascent viral bud. M2 first accumulates in the host plasma membrane (PM), which is approximately flat and therefore has zero Gaussian curvature. M2 then diffuses …

Unrestrained simulations reveal dynamic amphipathic helix (AH) domains.

(A) RMSDs of Ca backbones over time. Yellow indicates the transmembrane (TM) domain only, red the AH domain only, and blue the full protein. Snapshots from unrestrained molecular dynamics (MD) are …

Figure 2—source data 1

Raw double electron–electron resonance (DEER) data from Figure 7 of Kim et al., 2015 (green curves in panel B).

https://cdn.elifesciences.org/articles/81571/elife-81571-fig2-data1-v2.xlsx
Influence of lipid packing on bilayer tension and shape.

Comparison of tension and structural features of simulated membranes with the initial packing (left, panels A, C) versus the rebalanced leaflets (right, panels B, D). (A) Lateral pressure profile of …

M2 membrane deformation patterns from simulation.

(A) Structures for restrained-protein simulations. Extracellular loops in green, transmembrane (TM) domain in yellow, amphipathic helix (AH) domain in blue (polar/charged) and white (hydrophobic). …

Figure 4—source data 1

Structure of the parallel amphipathic helix (pAH) model.

https://cdn.elifesciences.org/articles/81571/elife-81571-fig4-data1-v2.zip
Surface height and thickness heatmaps for three different channel configurations.

Compressive deflections are negative/shown in bright colors. Expansive deflections are positive/dark colors. The same scale is used for the upper and lower leaflets to highlight the greater amount …

Leaflet thicknesses and position of the bilayer midplane.

Upper and lower leaflet thicknesses are plotted as time-averaged surface values in the top and middle rows, with lighter shades of blue denoting regions of leaflet thinning. The height of the …

Lipid tilt around different M2 conformations.

The top row shows representative all-atom snapshots extracted from the protein-restrained, equilibrium simulations of 2L0J, parallel amphipathic helix (AH) domain model, and 2N70 (2, 3, and 4 in Tabl…

Figure 7—source data 1

Full size image of lipids around 2L0J.

https://cdn.elifesciences.org/articles/81571/elife-81571-fig7-data1-v2.pdf
Figure 7—source data 2

Full size image of lipids around the parallel amphipathic helix (AH) domain model.

https://cdn.elifesciences.org/articles/81571/elife-81571-fig7-data2-v2.pdf
Figure 7—source data 3

Full size image of lipids around 2N70.

https://cdn.elifesciences.org/articles/81571/elife-81571-fig7-data3-v2.pdf
Mean deflection and tilt as a function of distance from the protein center.

Mean deflection (A) and tilt (B) as a function of radial distance from the protein center for restrained simulations. Points are colored by local density, such that bright spots reflect highly …

Boundary conditions extracted from molecular dynamics (MD) simulations.

(A) Parallel amphipathic helix (AH) domain M2 protein in a lipid bilayer. The molecular surface is shown with hydrophobic residues in white and charged and polar residues in blue. The mean …

Continuum model membrane deformations compared to molecular dynamics (MD) surfaces.

Left column: MD upper and lower leaflet mean positions. Right column: continuum model minimum energy upper and lower leaflet surfaces for a flat membrane (200 Å by 200 Å membrane with zero …

C2 symmetry broken conformations are stabilized in membranes with negative Gaussian curvature.

(A) Transfer free energy ΔΔG(K) for moving M2 from a flat region to a region with Gaussian curvature K = ±1/Rc2, where Rc is the radius of curvature (top X-axis). Solid lines at negative K show ΔΔG

Appendix 1—figure 1
Leaflet surfaces (left and middle columns) and bilayer thicknesses (right column) for the original restrained 2L0J simulation and restrained Repack simulations 1–4.

The upper leaflet has 200 lipids, and the lower leaflet lipid count is indicated in parentheses.

Appendix 1—figure 2
Leaflet tilt surfaces for the original restrained 2L0J simulation and restrained Repack simulations 1–4.

The upper leaflet has 200 lipids, and the lower leaflet lipid count is indicated in parentheses.

Appendix 1—figure 3
Leaflet thicknesses for the original restrained 2L0J simulation and restrained Repack simulations 1–4.

The upper leaflet has 200 lipids, and the lower leaflet lipid count is indicated in parentheses.

Appendix 1—figure 4
Amphipathic helix (AH) domain mobility in Repack 4, unrestrained 2L0J simulations.

(A) Trajectory RMSDs for the AH domain. Independent replicates are color coded. (B) Trajectory RMSDs for the transmembrane (TM) domain. (C) I51–I51 distance distributions from unrestrained …

Appendix 1—figure 5
Boundary conditions extracted from molecular dynamics (MD) simulations.

(A, B) Membrane–protein boundary information for the fourfold 2L0J structure. (C, D) Membrane–protein boundary information for the twofold 2N70 structure. Upper and lower bounds of the mean …

Appendix 1—figure 6
Influence of cholesterol enrichment on membrane curvature sensing by different M2 channel conformations.

Membrane parameters from Table 2 were used to calculate the membrane bending energy for moving from a flat membrane region to regions of differing curvature. (A) A 0% cholesterol membrane with 28.5 …

Appendix 1—figure 7
Membrane shapes which approximate an ideal spherical cap or saddle.

(A) Dash–dotted red: circle of radius R = 200 Å. Dashed blue: quadratic approximation of circle, valid for rR. Solid black: the m = 0 analytic biharmonic solution finite at the origin behaves …

Tables

Table 1
List of simulations.
IDLabelGromacsLength (ns)PDBIDBilayer # lipidsRestraints
1Unrestrained 12020.628292L0J200 upper; 150 lowerNo
22L0J 12020.638082L0J200 upper; 150 lowerYes
3pAH 12020.63760Parallel AH200 upper; 150 lowerYes
42N70 12020.617272N70200 upper; 150 lowerYes
52L0J Repack 12020.627402L0J200 upper; 158 lowerYes
62L0J Repack 22020.625002L0J200 upper; 166 lowerYes
72L0J Repack 32020.628902L0J200 upper; 174 lowerYes
82L0J Repack 4 – Final2020.650002L0J200 upper; 183 lowerYes
9Unrestrained 22020.626502L0J200 upper; 183 lowerNo
10Unrestrained 32020.630002L0J200 upper; 183 lowerNo
11Unrestrained 42020.630002L0J200 upper; 183 lowerNo
12Unrestrained 52020.630002L0J200 upper; 183 lowerNo
13pAH Repack Final2020.63000Parallel AH200 upper; 183 lowerYes
142N70 Repack Final2020.630002N70200 upper; 183 lowerYes
Table 2
Default elastic membrane material properties.
Parameters% cholesterolValuesReference
Membrane thickness (LC)028.5 ÅArgudo et al., 2017
3035 ÅThis manuscript
5037 ÅScaling from Ferreira et al., 2013
Surface tension (α)03.0 × 10−13 N/ÅLatorraca et al., 2014
303.0 × 10−13 N/Å“ ”
503.0 × 10−13 N/Å“ ”
Bending modulus (KC)029 kBTAverage value described in Methods
3065 kBTScaling from Henriksen et al., 2006
5068 kBTScaling from Pan et al., 2009
Gaussian modulus (KG)0−26 kBTRelation from Hu et al., 2012
30−56 kBT“ ”
50−61 kBT“ ”
Areal compression modulus (Ka)02.13 × 10−11 N/ÅHenriksen et al., 2006
303.55 × 10−11 N/Å“ ”
503.73 × 10−11 N/ÅScaling described in Methods
Appendix 1—table 1
Leaflet properties for restrained 2L0J simulations with varying lipid numbers.
SimulationArea per lipid (Å2)Thickness at box edges (Å)Tension (mN/m)
(lower lipid #)Upper leafletLower leafletUpper leafletLower leafletUpper leafletLower leaflet
Original (150)*42.549.918.516.3−10.824.6
Repack 1 (158)43.849.018.215.8−13.120.2
Repack 2 (166)44.447.417.916.4−11.813.2
Repack 3 (174)45.246.117.817.0−9.67.6
Repack 4 (183)46.445.117.417.2−3.88.0
  1. *

    The original restrained 2L0J simulation used a semi-isotropic Berendsen barostat for pressure coupling. All repacked simulations, and extension simulations for Gromacs-LS calculations, use a Parrinello–Rahman barostat. Other simulation parameters were identical for all simulations.

  2. Lipid ratio used for all subsequent 2L0J analysis.

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