Probing the Lipid Membrane Dipole Potential by Atomic Force Microscopy

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Probing the Lipid Membrane Dipole Potential by Atomic Force Microscopy Yi Yang, Kathryn M. Mayer, Nissanka S. Wickremasinghe, Jason H. Hafner  Biophysical Journal  Volume 95, Issue 11, Pages 5193-5199 (December 2008) DOI: 10.1529/biophysj.108.136507 Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 1 AFM analysis of the membrane dipole potential. (A) A schematic of the tip-sample region (not to scale), along with a plot that illustrates the three membrane potentials. (B) The observed repulsive force interaction between the negatively charged silicon nitride tip and DOPC membrane. Biophysical Journal 2008 95, 5193-5199DOI: (10.1529/biophysj.108.136507) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 2 Repulsive force data measured between a silicon nitride tip and supported DOPC membranes were analyzed by a numerical model to yield an effective membrane surface charge density (circles). The measurements are taken from many experiments and multiple tips. GCS models of lipid membranes are shown for Cl− binding constants of K=0.9M−1 (solid line) and K=10M−1 (dashed line). Biophysical Journal 2008 95, 5193-5199DOI: (10.1529/biophysj.108.136507) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 3 Numerical simulation of the tip-dipole interaction. (A) A schematic of the tip-sample region, illustrating the planes of charge used to model the molecular membrane dipoles and the hydrophobic region of the lipid bilayer (shaded). (B) A portion of a mesh from the numerical simulations of the tip-dipole interaction. Biophysical Journal 2008 95, 5193-5199DOI: (10.1529/biophysj.108.136507) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 4 The dipole density (A) and dipole potential (B) of a supported DOPC membrane as determined by analysis of electrostatic interactions measured with the AFM. The results are plotted for analysis with two different charge plane separations according to the schematic in Fig. 3 A. Biophysical Journal 2008 95, 5193-5199DOI: (10.1529/biophysj.108.136507) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 5 The topography (A) and surface charge map (B) of a DOPC/SM/cholesterol supported membrane exhibiting lipid rafts recorded with the AFM. Each image is 5×5μm. Biophysical Journal 2008 95, 5193-5199DOI: (10.1529/biophysj.108.136507) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 6 The effect of mica surface charge on the dipole simulations. Force data (circles) are plotted with results from the dipole model (lines) with an optimized dipole density of 1.5 Debye/lipid and mica surface charge of −0.01 C/m2 (i), 1.5 Debye/lipid and 0.0 C/m2 (ii), and 1.5 Debye/lipid and +0.01 C/m2 (iii). The results of these three simulations are very similar. A fourth simulation is displayed for 0.0 Debye/lipid and −0.01 C/m2 (iv). Biophysical Journal 2008 95, 5193-5199DOI: (10.1529/biophysj.108.136507) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 7 Ratiometric fluorescence imaging of a supported DOPC lipid membrane with Di-8-ANEPPS. Fluorescence images were bandpass-filtered at 675nm with excitation wavelengths of 510nm (A) and 425nm (B). The ratio of the images (425 nm/510nm) is displayed in panel C. The average ratio value is 0.62. Biophysical Journal 2008 95, 5193-5199DOI: (10.1529/biophysj.108.136507) Copyright © 2008 The Biophysical Society Terms and Conditions