Measurement of Ligand-Receptor Interactions (Biomembrane Interactions/Adhesion/Biotin/Streptavidin) CHRISTIANE A
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Proc. Natl. Acad. Sci. USA Vol. 88, pp. 8169-8173, September 1991 Biochemistry Measurement of ligand-receptor interactions (biomembrane interactions/adhesion/biotin/streptavidin) CHRISTIANE A. HELM*t, WOLFGANG KNOLL*§, AND JACOB N. ISRAELACHVILI* *Department of Chemical and Nuclear Engineering, and Materials Department, University of California, Santa Barbara, CA 93106; and tMax-Planck-Institut for Polymerforschung, Postfach 3148, D-6500 Mainz, Federal Republic of Germany Communicated by Charles P. Bean, June 10, 1991 ABSTRACT One distinguishing feature of "life" is that deposition of a layer of L-a-dilauroylphosphatidylethanol- the physical forces between biological molecules and membrane amine (DLPE; Sigma) of area 0.55 nm2 per molecule (con- surfaces are often highly specific, in contrast to nonspecific taining 5% DPPE-biotin) (Molecular Probes), thereby expos- interactions such as van der Waals, hydrophobic, and electro- ing one biotin ligand group per 11 nm2. This deposition was static (Coulombic) forces. We have used the surface-forces- done at 30TC from a 1 mM NaCl solution at a pressure ofabout apparatus technique to study the specific "lock and key" or 38 mN/m. "ligand-receptor" interaction between two model biomem- An avidin surface was prepared from a biotin surface by brane surfaces in aqueous solution. The membranes were lipid adsorbing soluble streptavidin molecules (kindly provided by bilayers supported on mica surfaces; one carrying streptavidin Boehringer Mannheim) from an aqueous solution, thereby receptors, the other exposing biotin ligand groups. We found yielding a surface with the same density ofunsaturated avidin that, although no unusual or specific interaction occurs be- (receptor) sites as biotin (ligand) groups. Avidin surfaces tween two avidin or two biotin surfaces, an avidin and a biotin could be prepared either before they were installed in the surface exhibit a very strong, very short-range (<1 nm) surface forces apparatus or after installation inside the cham- attraction and that the binding mechanism involves equally ber. specific molecular rearrangements. The results also show that After the biotin and/or avidin surfaces were prepared, they highly specific biological interactions such as are involved in were transferred (under water) into the surface forces appa- immunological recognition and cell-cell contacts may be stud- ratus chamber previously filled with a 1 mM NaCl solution ied at the molecular level and in real time by the surface-forces- saturated with DLPE at the critical micelle concentration. apparatus technique. This was to ensure that no DLPE desorbed during the course of an experiment (10-12). To ensure also that the second During the past 20 years the fundamental forces between monolayer remained in the fluid state, all measurements were surfaces in liquids have been systematically studied both done at 33 + 1TC, which is well above the phase transition experimentally and theoretically (1). These forces-e.g., van temperature of DLPE bilayers (30.50C). The force laws, der Waals, electrostatic, hydrophobic-are not system- adhesion energies, and surface deformations were measured specific in the sense that the interaction potential is a known as previously described (8-13) between the following sur- function of distance, such as a power law or an exponential faces shown in Fig. 2: biotin-biotin, avidin-avidin, and function. Less studied is a specific binding mechanism be- avidin-biotin. tween certain molecules that have a perfect geometrical fit. Such "lock and key" or "ligand-receptor" interactions (2, 3) give rise to very strong physical-as opposed to chemical, RESULTS AND DISCUSSION covalent or metal chelating-bonds with minimal expendi- The force law between two biotin surfaces in 1 mM NaCl ture of energy. Such noncovalent bonds are central to a solution at pH -5.8 is shown in Fig. 3 Inset. The force was molecular understanding of biological recognition and mo- purely repulsive, and no adhesion was measured at any lecular engineering applications (4-7). We have studied the separation, including contact. The measured repulsion of interactions between biotin ligands and streptavidin recep- exponential decay length of -9 nm is that characteristic ofan tors (5, 7). This is one of the most-thoroughly studied electrostatic "double-layer" interaction between two sur- ligand-receptor systems, with a binding constant of 88 kJ/ faces in 1 mM monovalent electrolyte solution (1), where mol (-35 kT per bond) that is one of the highest known. each surface has a surface potential of 37 + 4 mV, corre- sponding to a surface charge density of 1 unit charge per 55 MATERIALS AND METHODS nm2. Since pure DLPE is uncharged and exhibits no double- layer repulsion (10-12), the negative surface charge must A surface-forces apparatus (8, 9) was used to measure reside on the anionic directly the forces between mica surfaces coated with lipid phosphate groups (pK 3) of the bilayers whose outer fluid monolayers contained either the biotinylated lipid molecules (see Fig. 1). Assuming that none ligand L-a-dipalmitoylphosphatidylethanolamine-biotin of the charged DPPE-biotin had gone into solution, the (DPPE-biotin) or streptavidin (the protein receptor) as measured surface charge density indicates that 20% (or more) shown in Fig. 1. For convenience and simplicity we shall call ofthe biotin groups are dissociated-a value that is typical for these surfaces the "biotin" surface and the "avidin" surface. surfactant head groups in electrolyte solutions (14). We The Langmuir-Blodgett deposition technique (10-12) was therefore conclude that the interaction between two biotin used to prepare these surfaces. First, a primary close-packed surfaces exhibits no unusual or "specific" features. monolayer of DPPE (Sigma) of area 0.42 nm2 per molecule was deposited on a mica surface. This was followed by the Abbreviations: DPPE, L-a-dipalmitoylphosphatidylethanolamine; DLPE, L-a-dilauroylphosphatidylethanolamine. tPresent address: Institut fur Physikalische Chemie, Johannes The publication costs of this article were defrayed in part by page charge Gutenberg Universitit, Jakob-Welder-Weg 11, D-6500 Mainz, Fed- payment. This article must therefore be hereby marked "advertisement" eral Republic of Germany. in accordance with 18 U.S.C. §1734 solely to indicate this fact. §To whom reprint requests should be addressed. 8169 Downloaded by guest on October 1, 2021 8170 Biochemistry: Helm et al. Proc. Natl. Acad. Sci. USA 88 (1991) Biotin surface r v. Mica substrate 2.7 nm n m SolutionSoltin ... ._..--------------------------- ----.-- -.- - - --. Streptavidin- 4.5 n FIG. 1. Schematic illustration .~~~~~~~~~~~~~~~~~~~~~~~~~~~. ofthe two types ofsurfaces used in r-- NH the experiments. The biotin sur- face exposes a fluid DLPE mono- layer containing DPPE-biotin lig- DLPE and molecules (5, 7) at a surface DPPE-- F w Ho A6d 9uL % a %-# W coverage of -5%. The avidin sur- biotin KNI face exposes the 4.5-nm-thick molecule 1 streptavidin receptor proteins, Ii-P-iliA each of which has four binding l11 sites for biotin-two on either side I _ _ F' of the molecule (6). The thick- .. ... nesses shown are estimates only; K . t1 I L _- __ in particular, the 4.5-nm-thick Avidin surface streptavidin molecule can easily be compressed to 3.5 nm (see Fig. 3). The force law between two avidin surfaces is shown in Fig. required a wait of about 10-20 min between force runs to 3. These surfaces were prepared..............by first .............................installing two . .... reach equilibrium (dashed line in Fig. 3). Since these maxima identical biotin surfaces in the apparatusF.... ........... ............and then, .. ..after ... ....the . represent the force needed to separate and intercalate the forces between them were measured, injecting a small quan- avidin-biotin complexes over an area of roughly irr2 10-11 tity (100 1l) of 0.6 ,uM streptavidin_solution between them. m2 (as measured optically¶), we estimate that the lateral Assuming the same adsorption kinetics as previously mea- diffusion constant for the biotin-avidin complex within the sured for a similar system (15), this procedure should have outer supported monolayer is Ddff = r2/t 10-10 cm2/s, produced an equilibrated streptavidin-saturated avidin sur- which is close to typical values previously measured for face after about 30 min. Identical force curves were measured proteins in membranes (17, 18). 2 and 5 hr after injection. If the measured adhesion force of FIR = -0.4 mN/m When the two avidin surfaces were brought together (Fig. between two contacting surfaces of close-packed avidin 3), they first experienced a weakly attractive van der Waals molecules separated by an aqueous film of thickness AD = force, resulting in an instability that caused them to "jump 1.2 nm (Fig. 3 and the left schematic of Fig. 2B) is due to van in" from D = 14 nm to the outermost weakly adhesive force der Waals forces, the Hamaker constant A, given by the minimum at D = 9 nm (cf. the left schematic in Fig. 2B). On equation lFIR = -A/6AD2, would be A 4 x 10-21 J. This further approach the two surfaces then experienced a repul- can be compared with previously measured values of A sion reflecting the unfavorable work needed to compress the (1.5-7.0) x 10-21 J for uncharged bilayers (10, 11, 21, 22) and system (aqueous gap, compressible protein, and fluid mono- A 10-20 J for adsorbed proteins (23) interacting across layers). The activation barrier needed to laterally part the aqueous solutions. We conclude that-as in the case of two proteins was finally overcome at D = 7 nm when a second instability occurred and another jump in to a more-adhesive 1From the shapes of the optical interference fringes used to "ob- minimum was found (cf. the right schematic in Fig. 2B). serve" the interacting surfaces, one can directly measure not only When the surfaces were separated from either force mini- the distance between the two surfaces (to +1A) but also the mum, they "jumped out".