Surface properties such as adhesion are influenced by the surface topography. This dependency complicates any quantitative investigation of the material constants. A simple and efficient model is used to calculate the influence of the topography on the pull of force determined by a scanning force microscope (SFM). In the model the SFM tip is represented by a sphere. The sample surface is modeled by two geometries: a step on a plane and a blister (spherical cap) on a plane. The atomic interaction between the tip and the surface is of the Lennard-Jones type. The theoretical results are compared with SFM-measurements on highly oriented pyrolytic graphite (HOPG) in electrolytic environment. The calculations are in good agreement with the measured images.The SFM has become an indispensable tool for surface investigations on the nanometer scale. With the SFM it is possible to image the sample topography and properties such as friction [1-3], local stiffness [4], the adhesive force [5-8], and magnetic [9] and electrical forces [9]. In order to investigate these properties, specialized measurement modes are used. One main interest in SFM investigations is to determine macroscopic material constants, such as the friction coefficient, on a microscopic scale. It has been shown that this is very difficult. To determine the influence of material parameters on the measured signals the interaction between the tip and the sample has to be examined. Because material properties are often not directly accessible and the measured signal depends nonlinearly on various parameters, it is necessary to compare simulations and measurements.When formulating a theory, one can have two sometimes contradicting aims: either one focuses on the behavior of the interaction between the tip and the sample or one is interested in explaining the results of a specific experimental setup. The first concept is represented by the theories of Hertz [10], Johnson et al. [11], Derjaguin et al. [12], and Maugis [13]. * Corresponding author These theories describe the interactions necessary to the understanding of the tip-sample system. The second concept is exemplified by the works of Burnham [14] and Rabe [15].Their goal is to compare computer simulations with a real experiment. The model for the SFM typically consists of a sphere or point mass representing the tip and a plane representing the sample. However, these simplifications often make a comparison between the theoretical and the measured results impossible. For example, the representation of the surface by a plane is not sufficient if the calculations should describe the dependence on topographical changes. Investigating surface properties, e.g. the adhesive force, on a corrugated sample, one notices that SFM images show a change in the properties correlated with topographical features. The adhesive force often decreases strongly at slopes even if the height differences at the surface are rather small (see SFM images in Fig. 1).It is interesting to explore whether these variations in the adhesive fo...