Nanocars are artificial molecular machines with chassis, axles, and wheels designed for nanoscale transport at materials' surfaces. Understanding the dependence of surface dynamics of nanocars on the substrate's physicochemical properties is critical to the design of the transport properties of such man-made nanoscale devices. Among the multitude of potential substrates for the nanotransporters, graphene exhibits intrinsic ripples on its surface, which may affect the surface dynamics of nanocars. In this work, we report our molecular dynamics study of motion of C 60 , a popular nanocar wheel, on the graphitic substrates with systematically controllable surface ripples. We find that surface ripples increase the amplitude of fullerene fluctuation in the direction normal to surface, which leads to decrease of the desorption temperature from 650 K on a double-layer graphite system with less ripples to 550 K on single-layer graphene with more ripples. The surface diffusion of C 60 follows the rare hops mechanism for temperatures up to 30 K. It switches to continuous semiballistic motion at 150 K. The surface ripples do not significantly affect the diffusion coefficients, but change the anomaly parameter, especially at low temperatures. The ripples exhibit no major effect on the rotational dynamics of C 60 , which is attributed to very small energy barriers for C 60 rotation on graphitic surfaces.

We provide a comprehensive computational characterization of surface motion of two types of nanomachines with four C60 “wheels”: a flexible chassis Nanocar and a rigid chassis Nanotruck. We study the nanocars’ lateral and rotational diffusion as well as the wheels’ rolling motion on two kinds of graphene substrates—flexible single-layer graphene which may form surface ripples and an ideally flat graphene monolayer. We find that the graphene surface ripples facilitate the translational diffusion of Nanocar and Nanotruck, but have little effect on their surface rotation or the rolling of their wheels. The latter two types of motion are strongly affected by the structure of the nanomachines instead. Surface diffusion of both nanomachines occurs preferentially via a sliding mechanism whereas the rolling of the “wheels” contributes little. The axial rotation of all “wheels” is uncorrelated.

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