Volume 99, Issue 5, Pages (September 2010)

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Volume 99, Issue 5, Pages 1529-1538 (September 2010) Chemical versus Mechanical Perturbations on the Protonation State of Arginine in Complex Lipid Membranes: Insights from Microscopic pKa Calculations  Jejoong Yoo, Qiang Cui  Biophysical Journal  Volume 99, Issue 5, Pages 1529-1538 (September 2010) DOI: 10.1016/j.bpj.2010.06.048 Copyright © 2010 Biophysical Society Terms and Conditions

Figure 1 Chemical structures of lipids and the Arginine analog considered in this work. (A) 1,2-di-palmitoyl-sn-glycero-3-phosphatidylcholine (DPPC). (B) 1-stearoyl-2-docosahexaenoyl-sn-glycero-3-phosphatidylcholine (SDPC) and 1-stearoyl-2-docosahexaenoyl-sn-glycero-3-phosphatidylethanolamine (SDPE). (C) Cholesterol. (D) Arginine analog. Biophysical Journal 2010 99, 1529-1538DOI: (10.1016/j.bpj.2010.06.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 2 Cumulative radial distribution functions for (A) lipid oxygen, (B) water oxygen, and (C) total oxygen with respect to the guanidinium Cζ in three systems without cholesterol. Note that more water molecules are in contact with Arg+ in DPPC, while a smaller number of lipid headgroups are in contact with Arg+ in the bilayer with saturated hydrocarbon tails (DPPC) than in bilayers with polyunsaturated tails (SDPC and SDPC/E). In all figures in the main text, for the SDPC-containing systems, the results shown are from low surface-tension simulations; the corresponding data at high surface-tension are included in the Supporting Material. Biophysical Journal 2010 99, 1529-1538DOI: (10.1016/j.bpj.2010.06.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 3 (A–C) Energy gap (in color, ΔU =U0 –U+ in Eq. 1) and the number of oxygen (in black) in the vicinity (≤8 Å) of Arg Cζ at three charge-states as a function of time in the SDPC system under low surface-tension. Note that the energy gap is positively correlated to the number of oxygen at charged states (λ = 0.0, 0.5), while it is negatively correlated at the neutral state (λ = 1.0). Biophysical Journal 2010 99, 1529-1538DOI: (10.1016/j.bpj.2010.06.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 4 (Color online) Number density maps (in the unit of nm−3) of phosphorus/hydrocarbon (left) and water oxygen (right) in three cholesterol-free bilayers (A) DPPC, (B) SDPC, and (C) SDPC/E with a fully charged Arg at the origin. Note that both head- and tailgroups of unsaturated lipids have higher affinity to Arg+ than those of DPPC. Consequently, there are smaller numbers of water molecules in the water defect in SDPC and SDPC/E bilayers than in a DPPC bilayer, which is consistent with the radial distribution plots in Fig. 2. (D) Typical configuration of SDPC with its DHA wrapping around Arg+. (Green) Lipids in contact with Arg+ (hydrogen not included for clarity). (Orange spheres) Phosphorus in the headgroup. Biophysical Journal 2010 99, 1529-1538DOI: (10.1016/j.bpj.2010.06.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 5 (A–C) Histograms of the energy gap, ∂U/∂λ =U0 –U+, at the charged and neutral Arg states in SDPC/E systems (dotted and solid lines, respectively). Histograms at the neutral state, which deviate significantly from the Gaussian distribution, are further decomposed into contributions from substates by the number of oxygen atoms in contact with the guanidinium group; the population and the average ∂U/∂λ of each substate are given in the corresponding color. Note that the population for the substate in which the guanidinium group has no contact with oxygen decreases significantly as the cholesterol concentration increases while the average ∂U/∂λ for the substates is largely independent of cholesterol concentration. Biophysical Journal 2010 99, 1529-1538DOI: (10.1016/j.bpj.2010.06.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 6 Cumulative radial distribution functions of (A) phosphate oxygen, (B) water oxygen, (C) cholesterol oxygen, and (D) total oxygen near Arg in SDPC/E simulations with different cholesterol concentrations. Note that the total number of oxygen in contact with the neutral guanidinium group is highly correlated with the significant drop of Δ < ∂U/∂λ(λ = 1.0) > in Table 1. Biophysical Journal 2010 99, 1529-1538DOI: (10.1016/j.bpj.2010.06.048) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 7 (Color online) Number densities (in nm−3) of lipid phosphorus (rainbow color in the left panel), cholesterol hydroxyl oxygen (gray scale in the left panel), and water oxygen (rainbow color in the right panel) around the neutral Arg at the origin in SDPC/E systems with (A) 20% and (B) 40% (CHOL). Biophysical Journal 2010 99, 1529-1538DOI: (10.1016/j.bpj.2010.06.048) Copyright © 2010 Biophysical Society Terms and Conditions