Kremer, K.

Lipowsky, R.

Richter, D.

Rädler, Joachim O.

Sackmann, E.

English

Open Access LMU

R. Lipowsky • D. Richter • K. Kremer (Eds.) The Structure and Conformation of Amphiphilic Membranes Proceedings of the International Workshop on Amphiphilic Membranes, Jülich, Germany, September 16-18, 1991 With 150Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Barcelona Budapest Contents The Structure and Conformation of Amphiphilic Membranes: Overview By R. Lipowsky, D. Richter, and K. Kremer (With 1 Figure) 1 Part I Molecular St ructure of Membranes Monolayers of Amphiphilic Molecules By H. Möhwald, R.M. Kenn, K. Kjaer, and J. Als-Nielscn (With 4 Figures) 9 The Determination of the Structure of a Mixed Surfactant Monolayer by Specular Neutron Rcflection By J. Pcnfold, R.K. Thomas, E.M. Lee, E.A. Simister, J.R. Lu, and A.R. Rennie (With 3 Figures) 19 Docs the Scanning Force Microsopc Resolve Individual Lipid Molecules? By M. Radmacher, R.M. Zimmermann, and H.E. Gaub (With 5 Figures) 24 Domain Formation in a Lipid Monolayer By A. Gliozzi, A.C. Levi, M. Menessini, and E. Scalas (With 2 Figures) 30 Structure and Dynamics of Planar and Spherical Supported Phospholipid Bilayers By C. Dolainsky, T. Köchy, C. Naumann, T. Brumm, S.J. Johnson, and T M . Bayerl (With 5 Figures) 34 Translational Diffusion and Fluid Phase Connectivity in Multi-Component, Multi-Phase Lipid Bilayer Membranes By W.L.C. Vaz, T.E. Thompson, P.F. Almeida, T. Bultmann, and E.C.C. Melo 40 Estimation of Gel and Fluid Domain Sizes in Two-Component Lipid Bilayers By M.B. Sankaram, D. Marsh, and T.E. Thompson (With 1 Figure) 45 VII Phosphatidyl-Glycerol in Mixtures with Positively Charged Amphiphiles: A 2H- and 31P-NMR Study of the Phase Behaviour and Headgroup Structure By R.G.K. Habiger and J. Seelig (With 3 Figures) 49 Diffusion Controlled Reactions in Two-Dimensional Space. The Pyrene Excimer Example By J.M. Martins and E.C.C. Melo (With 1 Figure) 53 Ripple Phase in Mixed Model Membrane By C. Cametti, F. De Luca, A. D'Ilario, G. Briganti, M.A. Macri, and B. Maraviglia (With 2 Figures) 57 Microscopic Theory for the Ripple Phase By R.R. Netz (With 1 Figure) 61 The Influence of Local Anaesthetics on the Temperature and Pressure Dependent Phase Behaviour of Model Biomembranes By M. Böttner, M.-H. Christmann, and R. Winter (With 7 Figures) . . . . 65 Bilayer Elasticity and Its Effects on Channel-Forming Peptides By H.W. Huang (With 5 Figures) 70 Interaction of Charged and Uncharged Calcium Channel Antagonists with Phospholipid Membranes. Binding Equilibrium, Binding Enthalpy, and Membrane Location By H.-D. Bäuerle and J. Seelig (With 2 Figures) 76 Melittin-Induced Reversible Micelle Bilayer Transition By B. Sternberg and C.E. Dempsey (With 2 Figures) 80 Theory of Hydration Forces By A.A. Kornyshev and S. Leikin 83 Force Equilibria Between Charged Surfaces with Confined Polyelectrolyte Chains By R. Podgornik (With 1 Figure) 87 Part II Conformation of Membranes Büdding Transition for Bilayer Fluid Vesicles with Area-Difference Elasticity By U. Seifert, L. Miao, H.-G. Döbereiner, and M. Wortis (With 1 Figure) 93 Some Remarks on the Shape of Toroidal Vesicles By R. Mosseri, J.F. Sadoc, and J. Charvolin (With 2 Figures) 97 The Effect of Membrane Elasticity on Shapes of Nearly Spherical Phospholipid Vesicles By F. Sevsek, S. Svetina, and B. £eks (With 1 Figure) 101 VIII Electron Microscopy of Biological Model Membranes By B. Klösgen and W. Helfrich (With 6 Figures) 105 Erythrocytes Membranes: Tethered Shells with Fluid-Like Deformation Regime By A. Zilker, H. Strey, and E. Sackmann (With 9 Figures) 113 The Isolated Human Red Blood Cell Skeleton: An Example of a Flexible Tethered Membrane By C.F. Schmidt, K. Svoboda, N. Lei, C R . Safinya, S.M. Block, and D. Branton (With 3 Figures) 128 Dynamics of Fiat Membranes and Flickering in Red Blood Cells By E. Frey and D.R. Nelson 133 A New Cell Model - Actin Networks Encaged by Giant Vesicles By M. Bärmann, J. Käs, H. Kurzmeier, and E. Sackmann (With 4 Figures) 137 Numerical Simulations of Vesicular and Red Blood Cell Shapes in Three Dimensions By J. Hektor, W. Form, R. Grebe, and M.J. Zuckermann (With 1 Figure) 144 Dynamic Coupling and Nonlocal Curvature Elasticity in Bilayer Membranes By E. Evans, A. Yeung, R. Waugh, and J. Song (With 3 Figures) 148 Phospholipid Membrane Local and Non-Local Bending Moduli Determined by Tether Formation from Aspirated Vesicles By S. Svetina, B. Boziö, J. Song, R.E. Waugh, and B. Zeks (With 2 Figures) 154 Vesicle-Substrate Interaction Studied by Reflection Interference Contrast Microscopy By J. Rädler and E. Sackmann (With 5 Figures) 158 Surface Induced Fusion of Vesicles into Planar Bilayers By G. Cevc, W. Fenzl, and L. Sigl (With 2 Figures) 162 The Shape of an Adhered Membrane Cylinder By M.M. Kozlov 166 Deformation of Giant Lipid Vesicles in an Electric Field By M. Kummrow and W. Helfrich 170 The Effect of the Electric Field on the Shapes of Phospholipid Vesicles By B. Zekä and S. Svetina (With 2 Figures) 174 AC Field Controlled Formation of Giant Fluctuating Vesicles and Bending Elasticity Measurements By M.I. Angelova, S. Soleau, P. Meieard, J.F. Faucon, and P. Bothorel (With 3 Figures) 178 IX Part III M e m b r a n e s in Complex Fluids Micelles and Vesicles of Gangliosides By L. Cantü, M. Corti, and M. Musolino (With 1 Figure) 185 Self-Assembly of Bipolar Lipids By A. Relini, F. Cavagnetto, and A. Gliozzi (With 1 Figure) 189 Determination of Size and Structure of Lipid I V A Vesicles by Quasi-Elastic Light Scattering and Small-Angle X-Ray Scattering By N. Maurer and O. Glatter (With 7 Figures) 193 Multicomponent Vesicular Aggregates (MCVA): Spontaneous Vesiculation of Perfluorinated Single-Chain Surfactant Mixtures By S. Szönyi, A. Cambon, H J . Watzke, P. Schurtenberger, and E. Wehrli (With 3 Figures) 198 Formation of Colloid and Liquid Crystal Phases of Magnesium Dodecylbenzenesulfonate: Interpretation by Fractals By D. Tezak, I. Fischer-Palkovic, S. Heimer, and F. Strajnar (With 3 Figures) 202 Ginzburg-Landau Theory of Bulk and Interfacial Properties of Amphiphilic Systems By G. Gompper and S. Zschocke (With 4 Figures) 206 Shape and Size Fluctuation of Microemulsion Droplets By B. Farago (With 5 Figures) 212 Microemulsions in Technical Processes By K. Stickdorn and M.J. Schwuger 218 The Effect of Additives on Surfactant Sheets in Microemulsions By M.A. Lopez-Quintela, W. Korneta, and L. Liz 222 Membrane Curvature and Structural Transitions for Charged/Uncharged Phospholipid Mixtures By D. Lerche, N.L. Füller, and R.P. Rand (With 4 Figures) 226 Epitaxial Relationships Between Adjacent Phases in Hydrated Monoolein By R.H. Templer, N.A. Warrender, R. Meadows, and J.M. Seddon (With 2 Figures) 230 Films of Amphiphiles and Minimal Surfaces By J. Charvolin and J.F. Sadoc (With 7 Figures) 234 Phase Transitions in Cubic Amphiphilic Crystals By M. Clerc and J.F. Sadoc (With 4 Figures) 244 Elasticity and Excitations of Minimal Crystals By R. Bruinsma (With 3 Figures) 250 x Inverse Micellar Cubic Phases of Lipids By J.M. Seddon and E.A. Bartie (With 1 Figure) 257 Swollen Lyotropic Cubic Phases in Fully Hydrated Mixtures of Monoolein, Dioleoylphosphatidylcholinc, and Dioleoylphosphatidylethanolamine By R.H. Templer, K.H. Madan, N.A. Warrender, and J.M. Seddon (With 1 Figure) 262 Surfactant Phases with Bilayer Structures and Their Rheological Properties By C. Thunig, G. Platz, and H. Hoffmann (With 7 Figures) 266 Sponge Phases By M.E. Cates 275 Structural Inversion Processes in Three-Component Ionic Microemulsion Studied by Small Angle Neutron Scattering By S.H. Chen, S.L. Chang, R. Strey, and P. Thiyagarajan (With 3 Figures) 281 The L3 Phase Microstructure in the AOT-Brine System has a Low Average Coordination Number By U. Olsson, B. Balinov, and O. Söderman (With 2 Figures) 287 Hydrodynamic Modes of a Viscoelastic Membrane or Interface By H. Pleiner and J.L. Harden 291 The Undulation Mode of Freely Suspended Liquid Films By H. Pleiner and H.R. Brand 295 Index of Contributors 297 XI Vesicle-Substrate Interaction Studied by Reflection Interference Contrast Microscopy J . Rädler and E . Setckmann Physik Department, Biophysics Group E22, Technische Universität München, James Franck-Str., W-8046 Garching, Fed. Rep. of Germany Abstract . Giant DMPC-Ves ic les interacting with a supported D M P C -bilayer are investigated by Reflection Interference Contrast Microscopy ( R I C M ) . Spherical vesicles whose shape fluctnations are suppressed by osmotic pressure can be observed to fluctuate like Brownian parti-cles above the Substrate. The interaction potential can be determined from the measured distribution function of distances. In the case of adhesion, the contact contour of deflated vesicles can be calculated. Contact roundings for of weak adhesion as well as contact angles for strong adhesion have been measured. 1 Introduct ion The adhesion of vesicles to a wall has recently become of interest in the context of the variety of shape transformations that free vesicles exhibit [1]. Clearly, in the case of adhering vesicles the equilibrium shape and the dynamics of the fluid membrane is strongly dependent on the strength of the vesicle wall interaction [2]. We investigated repulsive vesicle wall interaction as well as vesicle adhesion. 2 Experimental setup and methods The experimental setup is depicted in Fig. l . The vesicles are studied by reflec-tion interference contrast microscopy. By this technique interference is observed between the object beam reflected at the membrane and the reference beam reflected at the glass-biifTer interface. In the case of an osmotically swollen, spherical vesicle the interference pattern are known as Newton rings and the absolute sphere-substrate distance can be measured from the position of the fringes. Consequently, fast image processing allows monitoring distance fluctu-ations in real time [3]. Furthermore, the interference fringes at the edge of the contact zone of ad-hering vesicles of arbitrary shape can be used to calculate the vesicle contour close to the surface. Thus the nature of the equilibrium shape of adhering vesicles in the contact zone can be studied; i.e. the contact angle for strongly adhering vesicles or smooth contact curvatures in the case of weak adhesion. Special thought must be given to the preparation of the surface of the Sub-strate. Since optica! techniques require glass as the underlying Substrate, surface 158 Springer Procccdings in Physics, Vol. 66 The Structure and Conformation of Amphiphilic Membranes Editors: R. Lipowsky • D. Richter • K. Krcmcr (5) Springer-Verlag Berlin Heidelberg 1992 Figure 1: Principle of the reflection in-terference contrast microscopy. The in-terference between the object beam 7o3 and the reference beam I \ n is observed. roughness and unspecific electrostatic effects are considerable shortcomings in vesicle adhesion experiments. Most glass effects, however, are suppressed by silanizing the glass surface, i.e. chemically attaching C\s hydrocarbon chains to the surface and depositing a lecithin monolayer on top. Using this kind of Substrate supported monolayer has the advantage of studying the Symmetrie lecithin-lecithin interaction that has already been measured by other techniques. 3 Repulsive interaction Prieve et al. [4] showed recently that the interaction of a sphere which by Brownian motion fluetuates above a repulsive surface can be measured by sam-pling the distance distribution funetion of the ranclom motion. The distribution funetion of distances contains the interaction potential simply by the Boltz-mann relation. Giant DMPC vesicles are observed not to adhere to DMPC supported monolayers at low ionic strength (< 20mA/) and osmotically swollen vesicles shovv distance fluctuations. The negative logarithm of the measured distance distribution is shown in Fig. 2. The solid line indicates a best fit to the theoretical mteraction potential including electrostatic, Van der Waals and gravitational forces. The figure also shows that under the same conditions but increased ionic strength the theoretical interaction becomes attractive as experimentally observed (dashed line). 0 -•I -2 -- 4 --l2mM NaCI 25mM NaCI 20 4 0 60 distance / nm 80 100 Figure 2: The interaction potential obtained from the distance fluctuations of a spherical DMPC vesicle above a DMPC supported monolayer in lOOmM inositol plus 12mM NaCI. The solid line depicts the theoretical interaction potential for = \.%mV. Increasing the ionic strength to 25mM leads to adhesion due to Van der Waals forces as indicated bv the dashed line. 159 4 Weak adhesion Adhesion is observed, if the ionic strength in a system of DMPC vesicles on a DMPC supported monolayer surface is increased to 20mM. However, the ad-hesion is weak vvhich is obvious from visible surface undulations on the vesicle. Fig. 3 depicts the contour of the vesicle in the contact zone. The shape exhibits a contact rounding that is fitted by a circle of contact radius R r (dashed line). The contact curvature has been predicted to depend on the ratio of bending to adhesion energy [6, 2] : RK = y/2Kc~h (1) Taking Kc to be 10~ 1 9J the adhesion energy turns out to be on the order of 1.2 • 10~8J/??72. This value is small compared to 10~5J/???2 measured by micropipette [6] and surface force technique [7]. However, in those cases tension is applied to the membranes, while in contrast at very low tension 7 is reduced due to steric repulsion of the undulating membrane [8]. E 0.25-0.00 - L ~i 1 r 4 5 6 x/p.m Figure 3: Calculated con-tour from the interference fringes of a DM PC-vesicle on a DMPC supported mono-layer. The contour rounding gives an estimate for the ad-hesion energy. The dashed line depicts a circle of contact radius R k (distorted scale !). 5 Strong adhesion Strong interaction is achieved by incorporating negative charges into the sup-ported monolayer and positve charges into the vesicle. Fig. 4 shows an exam-ple of a vesicle (SOPC:Chol:DODAB) (49:49:2 mol%) adhered to a supported monolayer (DMPCrPS) (98:2 mol%). It depicts the reconstructed profile of the vesicle. The vesicle is only slightly deflated and the contour is close to the spherical shape (dashed line). However, the contact zone exhibits sharp con-tact angles. The equilibrium shape of adhering vesicles has been calculated by Seifert and Lipowsky [2]. In agreement with their predictions we also found the following shapes schematically depicted in figure 5. E 0 . 8 -0 . 4 -0.0 x / Mm Figure 4: Reconstructed contour of a strongly ad-hering vesicle. The con-tact zone shows a contact angle. 160 Figure 5: Schematic rep-resentation of experimen-tally found sliapes. Acknowledgments We like to thank A. Zilker for support with the image processing System. We also gratefully acknowledge the financial support by the D F G SA 2 4 6 / 2 0 and by the Fond der chemischen Industrie. References [1] Kaes .J . and Sackmann, E.. Bio. Phys L 6 0 (1991) 1 [2] Seifert ,U. and Lipowsky,R., Phys .Rev A 4 2 (1990) 4768 [3] Raedler, .Land Sackmann,E . submit ted [4] P r i e v e . D . C . and Frey.N.A., Laiigimiir G (1990) 396 [5] Evans .E .A . and Parseg ian .V.A. . in Surface P h e n o m e n a in Hemorheology : Cop-ley .A.L. and S e a m a n , G . V . F . , E d s . . N .Y . Acad. Sei. (1983) 13 [6] Evans ,E .A . and Metcalf .M., Biophys . J. 4 6 (1984) 423 [7] Maria , . ] , and Israelachvil i .L. Biochemistry 2 4 (1985) 4608 [8] Servuss .R .M. and Reif l ich .W. J .Phys . France 5 0 (1989) 809 161 

Vesicle-Substrate Interaction

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Vesicle-Substrate Interaction

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