Transient forces between nanoscale objects on surfaces govern friction, viscous flow, and plastic deformation, occur during manipulation of matter, or mediate the local wetting behavior of thin films. To resolve transient forces on the (sub) microsecond time and nanometer length scale, dynamic atomic force microscopy (AFM) offers largely unexploited potential. Full spectral analysis of the AFM signal completes dynamic AFM. Inverting the signal formation process, we measure the time course of the force effective at the sensing tip. This approach yields rich insight into processes at the tip and dispenses with a priori assumptions about the interaction, as it relies solely on measured data. Force measurements on silicon under ambient conditions demonstrate the distinct signature of the interaction and reveal that peak forces exceeding 200 nN are applied to the sample in a typical imaging situation. These forces are 2 orders of magnitude higher than those in covalent bonds.T ime-dependent forces mediate adsorption, ordering phenomena, and visco-elasticity that are important in rheology and tribology, as well as in biology and catalysis. The importance of dynamic aspects becomes obvious when looking at the viscoelastic properties of polymers (1, 2). Even on the level of a single biomolecule under external stress, velocity dependence can be observed: the stability of the molecule increases with the applied force rate (3). However, dynamic forces occurring during processes at surfaces, in thin and confined lubrication films, or on the level of nanoscopic objects are experimentally not easily accessible.In this context, atomic force microscopy (AFM) offers a large potential to investigate and manipulate material at the (sub) microsecond time scales and nanometer length scale. AFM (4) and related techniques (5) have gained increasing importance in many fields of research and industrial applications. Raster scanning the sample with a sharp tip attached to the end of the microfabricated cantilever allows not only the visualization of objects in shape and size of single molecules, but also the ability to touch and squeeze, pull and push them (6). In dynamic force microscopy, the motion of the cantilever is externally modulated. In tapping-mode AFM, the most common dynamic mode, the cantilever is excited to oscillate at its fundamental resonant frequency. Once each oscillation cycle, the tip interacts with the surface, and information about the tip-sample interaction is transferred into the time course of the signal. The signal formation process is depicted in Fig. 1, and the inset shows schematically the setup of tapping-mode AFM.To obtain the acting forces from the dynamics of the oscillating cantilever, there are basically two routes. First, under ultra high vacuum conditions, the change of the resonant frequency of the force-coupled cantilever is used to estimate the interaction potential (7-9). These methods highly depend on the high quality factor of the oscillation under ultra high vacuum. Second, under ambient condi...