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How do molecules interact with each other? What happens if a neurotransmitter binds to a ligand‐operated ion channel? How do antibodies recognize their antigens? Molecular recognition events play a pivotal role in nature: in enzymatic catalysis and during the replication and transcription of the genome; it is also important for the cohesion of cellular structures and in numerous metabolic reactions that molecules interact with each other in a specific manner. Conventional methods such as calorimetry provide very precise values of binding enthalpies; these are, however, average values obtained from a large ensemble of molecules without knowledge of the dynamics of the molecular recognition event. Which forces occur when a single molecular couple meets and forms a bond? Since the development of the scanning force microscope and force spectroscopy a couple of years ago, tools have now become available for measuring the forces between interfaces with high precision—starting from colloidal forces to the interaction of single molecules. The manipulation of individual molecules using force spectroscopy is also possible. In this way, the mechanical properties on a molecular scale are measurable. The study of single molecules is not an exclusive domain of force spectroscopy; it can also be performed with a surface force apparatus, laser tweezers, or the micropipette technique. Regardless of these techniques, force spectroscopy has been proven as an extraordinary versatile tool. The intention of this review article is to present a critical evaluation of the actual development of static force spectroscopy. The article mainly focuses on experiments dealing with inter‐ and intramolecular forces—starting with “simple” electrostatic forces, then ligand–receptor systems, and finally the stretching of individual molecules.

This study focuses on the structural organization of surfactant protein B (SP-B) containing lipid monolayers. The artificial system is composed of the saturated phospholipids dipalmitoylphosphatidylcholine (DPPC) and dipalmitoylphosphatidylglycerol (DPPG) in a molar ratio of 4:1 with 0.2 mol% SP-B. The different "squeeze-out" structures of SP-B were visualized by scanning probe microscopy and compared with structures formed by SP-C. Particularly, the morphology and material properties of mixed monolayers containing 0.2 mol% SP-B in a wide pressure range of 10 to 54 mN/m were investigated revealing that filamentous domain boundaries occur at intermediate surface pressure (15-30 mN/m), while disc-like protrusions prevail at elevated pressure (50-54 mN/m). In contrast, SP-C containing lipid monolayers exhibit large flat protrusions composed of stacked bilayers in the plateau region (app. 52 mN/m) of the pressure-area isotherm. By using different scanning probe techniques (lateral force microscopy, force modulation, phase imaging) it was shown that SP-B is dissolved in the liquid expanded rather than in the liquid condensed phase of the monolayer. Although artificial, the investigation of this system contributes to further understanding of the function of lung surfactant in the alveolus.

The suitability of the quartz crystal microbalance (QCM) technique for monitoring the attachment and spreading of mammalian cells has recently been established. Different cell species were shown to generate an individual response of the QCM when they make contact with the resonator surface. Little is known, however, about the underlying mechanisms that determine the QCM signal for a particular cell type. Here we describe our results for different experimental approaches designed to probe the particular contributions of various subcellular compartments to the overall QCM signal. Using AC impedance analysis in a frequency range that closely embraces the resonators' fundamental frequency, we have explored the signal contribution of the extracellular matrix, the actin cytoskeleton, the medium that overlays the cell layer, as well as the liquid compartment that is known to exist between the basal plasma membrane and the culture substrate. Results indicate that the QCM technique is only sensitive to those parts of the cellular body that are involved in cell substrate adhesion and are therefore close to the resonator surface. Because of its noninvasive nature, sensitivity, and time resolution, the QCM is a powerful means of quantitatively studying various aspects of cell-substrate interactions.

The specific adhesion of unilamellar vesicles with an average diameter of 100 nm on functionalized surfaces mediated by molecular recognition was investigated in detail. Two complementary techniques, scanning force microscopy (SFM) and quartz crystal microbalance (QCM) were used to study adhesion of liposomes consisting of 1, 2-dipalmitoyl-sn-glycero-3-phosphocholine and varying concentrations of N-((6-biotinoyl)amino)hexanoyl)-1, 2-dihexadecanoyl-sn-glycero-3-phosphoethanolamine (biotin-X-DHPE). Monitoring the adhesion of the receptor-doped vesicles to avidin-coated gold surfaces by QCM (f(0) = 5 MHz) revealed an increased shift in resonance frequency with increasing biotin concentration up to 10 mol% biotin-X-DHPE. To address the question of how the morphology of the liposomes changes upon adhesion and how that contributes to the resonator's frequency response, we performed a detailed analysis of the liposome morphology by SFM. We found that, with increasing biotin-concentration, the height of the liposomes decreases considerably up to the point where vesicle rupture occurs. Thus, we conclude that the unexpected high frequency shifts of the quartz crystal (>500 Hz) can be attributed to a firm attachment of the spread bilayers, in which the number of contacts is responsible for the signal. These findings are compared with one of our recent studies on cell adhesion monitored by QCM.