Volume 98, Issue 11, Pages (June 2010)

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Volume 98, Issue 11, Pages 2644-2652 (June 2010) Antimicrobial Protegrin-1 Forms Ion Channels: Molecular Dynamic Simulation, Atomic Force Microscopy, and Electrical Conductance Studies  Ricardo Capone, Mirela Mustata, Hyunbum Jang, Fernando Teran Arce, Ruth Nussinov, Ratnesh Lal  Biophysical Journal  Volume 98, Issue 11, Pages 2644-2652 (June 2010) DOI: 10.1016/j.bpj.2010.02.024 Copyright © 2010 Biophysical Society Terms and Conditions

Figure 1 MD simulation of channel structure. Channel structures averaged over the simulation in a ribbon representation (left column) for the (A) antiparallel and (B) parallel β-sheet channels of PG-1 are shown in the lateral view from the lipid bilayer. In the peptides, hydrophobic residues are shown in white, polar and Gly residues are shown in green, and positively charged residues are shown in blue. In each channel, the averaged water pore structure calculated by the HOLE program (77) is embedded. For the pore structures in the surface representation, green denotes pore diameter in the range, 0.8 nm <d < 1.4 nm and blue denotes pore diameter of d > 1.4 nm. The simulated PG-1 channel structures with highlighted subunits (right column) are viewed from the top leaflet of the lipid bilayer for the antiparallel (top right) and parallel (bottom right) β-sheet channels of PG-1. The channels are depicted in a cartoon representation with a transparent surface. Each subunit in the channels is colored in a different color. The discontinuous β-sheet network determines the boundary between the subunits in the channels. Antiparallel β-sheet channels of PG-1 contain four subunits. Parallel β-sheet channels contain five subunits. The shapes of the subunits vary, with β-hairpin monomers, and β-sheet dimer or trimer. Biophysical Journal 2010 98, 2644-2652DOI: (10.1016/j.bpj.2010.02.024) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 2 Probability distribution functions representing ionic permeation. Probability distribution functions for Mg2+ (green line), Na+ (orange line), Cl− (black line), and water (blue dashed line) as a function of the distance along the pore center axis for the (A) antiparallel and (B) parallel β-sheet channels of PG-1 are shown. The probability for water uses the scale on the right (blue labels). The high probability profile for Cl− in the pore indicates clearly that PG-1 forms an anionic conducting channel in the lipid bilayer. Biophysical Journal 2010 98, 2644-2652DOI: (10.1016/j.bpj.2010.02.024) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 3 PG-1 forms channel-like structures in DOPS/POPE lipid bilayers. (A and B) AFM height images of DOPS/POPE bilayer before and after addition of PG-1 (conc 150 μg/mL, scale bar = 1 μm). When PG-1 is added to a preformed DOPS/POPE bilayer, large globular oligomers are observed preferentially on the bilayer surface.(C) AFM image of a membrane patch with PG-1 oligomer-like structures. Scale bar in C is 100 nm. The inset represents the highlighted square area after flattening and low pass filtering (inset scale bar = 50 nm). (D) AFM image of the edge of a lipid bilayer with incorporated PG-1 peptides (scan size: 100 nm × 100 nm) with the insert representing a 75 nm × 75 nm area in the central region of a bilayer (scale bars = 50 nm). In C and D, green circles highlight PG-1 channel-like structures. Biophysical Journal 2010 98, 2644-2652DOI: (10.1016/j.bpj.2010.02.024) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 4 The structure of PG-1 ion channels incorporated in DOPS/POPE lipid bilayers from high resolution AFM imaging. (A–C) Examples of channel-like structures with different subunit organizations. (D and E) Inner and outer diameters of PG-1 channels that were measured from the cross-section profile of the channel height. The red arrows mark the outer diameter, and the green arrows mark the regions where the inner diameter was measured. The graphs shown in F–H represent pore (F) inner and (G) outer diameter distributions and (H) channel subunits distribution. Biophysical Journal 2010 98, 2644-2652DOI: (10.1016/j.bpj.2010.02.024) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 5 PG-1 channel activity is dependent on bilayer composition. (A) PG-1 activity in the anionic DOPS/DOPE 1:1 bilayer. Note the short lived and spiky behavior. (B) Membrane activity of PG-1 in DOPC/DOPE 1:1 bilayer. The activity shown here is well sustained with fast openings and closings. (C) Typical PG-1 activity in 1,2-diphytanoyl-sn-glycero-3-phosphatidylcholine or DOPC bilayers. Occasionally PC bilayers present short lived, low amplitude very sparse step like current jumps. Membranes were formed by the folded technique. Traces shown were recorded at 40 mV of applied potential. The electrolyte solution used was 100 mM KCl, 10 mM Hepes, and 1 mM MgCl2. PG-1 was added directly into one side of the recording chamber. Biophysical Journal 2010 98, 2644-2652DOI: (10.1016/j.bpj.2010.02.024) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 6 PG-1 membrane activities on zwitterionic DOPC/DOPE bilayers. (A) A 14-min trace presented in 5-min intervals. The top two 5-min fragments are at 40 mV. The calculated conductances for both steps shown are 100 pS and 190 pS. Using the lower current versus time trace shown in A, the conductance calculated as the slope of the linear fit for the current versus voltages 40, 0, −40, and −80 mV yields a conductance of ∼100 pS. The double arrow head under the traces show the current versus time fragments used to make B. The asterisk (∗) symbol marks a capacitance measurement to check membrane integrity during recording. The vertical arrow below the voltage versus time trace in A shows the trace fragment used to calculate the IV plot. Biophysical Journal 2010 98, 2644-2652DOI: (10.1016/j.bpj.2010.02.024) Copyright © 2010 Biophysical Society Terms and Conditions