SiC 4 units. The integral ratios were reproducible, with varying pulse delay times between 3 and 30 s, indicating that the 29 Si nuclei were sufficiently relaxed to give accurate integrals. Nitrogen isotherms demonstrated the ordered mesoporous nature of both PMD-2 and PMD-3 by showing typical type-IV isotherms. The BET surface areas were 775 m 2 g j1 (PMD-2) and 767 m 2 g j1 (PMD-3). The BJH analysis revealed a narrow pore size distribution with average pore sizes of 9.1 nm (PMD-2) and 8.2 nm (PMD-3), which is consistent with the TEM data. The circumrotation of a submolecular fragment in either direction in a synthetic molecular structure is described. The movement of a small ring around a larger one occurs through positional displacements arising from biased Brownian motion that are kinetically captured and then directionally released. The sense of rotation is governed solely by the order in which a series of orthogonal chemical transformations is performed. The minimalist nature of the [2]catenane flashing ratchet design permits certain mechanistic comparisons with the Smoluchowski-Feynman ratchet and pawl. Even when no work has to be done against an opposing force and no net energy is used to power the motion, a finite conversion of energy is intrinsically required for the molecular motor to undergo directional rotation. Nondirectional rotation has no such requirement.Molecular-level motors differ from their macroscopic counterparts not only in scale but in how environmental factors influence their operation. Macroscopic machines are generally unaffected by ambient thermal energy, and a directional force must be applied to cause movement of each component. For molecular-sized motors, however, inertia is negligible and the parts are subject to random and incessant Brownian motion (1). Rather than fight this effect, biological motors use these random fluctuations in their mechanisms (2). For example, in F 1 F 0 -adenosine triphosphatase (ATPase), which spins the g shaft counterclockwise (viewing F 1 from above) as proton-motive force powers ATP production and clockwise if ATP is consumed to drive proton flow against a concentration gradient (3), Brownian motion drives both the power and exhaust strokes (2). Inspired by such biological motors and by Feynman_s celebrated discussion (4) of the miniature ratchet and pawl first introduced (5) by Smoluchowski, efforts have been made to design molecules that exhibit directional control over submolecular rotary motion (6-10). Unidirectional rotation about single (11, 12), double (13-16), and mechanical (17) bonds has been achieved, but unlike F 1 F 0 -ATPase, these artificial motor molecules are only able to rotate in one direction but not the other. We now report on a molecular structure in which a fragment can be circumrotated in either direction, and we probe features of the underlying mechanism. During the past decade, a number of remarkable theoretical formalisms have been developed using nonequilibrium statistical physics that explain how various types of fluctu...