The concept of a folding funnel with kinetic traps describes folding of individual proteins. Using in situ Atomic Force Microscopy to investigate S-layer assembly on mica, we show this concept is equally valid during self-assembly of proteins into extended matrices. We find the S-layer-on-mica system possesses a kinetic trap associated with conformational differences between a long-lived transient state and the final stable state. Both ordered tetrameric states emerge from clusters of the monomer phase, however, they then track along two different pathways. One leads directly to the final low-energy state and the other to the kinetic trap. Over time, the trapped state transforms into the stable state. By analyzing the time and temperature dependencies of formation and transformation we find that the energy barriers to formation of the two states differ by only 0.7 kT, but once the high-energy state forms, the barrier to transformation to the low-energy state is 25 kT. Thus the transient state exhibits the characteristics of a kinetic trap in a folding funnel.biological assembly | protein crystal growth | two-step crystallization | protein folding funnel P roteins that naturally self-assemble into extended ordered structures often adopt conformations that are distinct from those of the individual monomeric proteins (1-4). For example, collagen matrices, which constitute the organic scaffolds of bones and teeth in all higher organisms, are constructed from triple helices of the individual collagen monomers (4). These helices further assemble into highly organized twisted fibrils exhibiting a pseudohexagonal symmetry. In some cases, assembly is inexorably linked to folding transformations, as in the case of prion or amyloid fibrils, where misfolding of the monomers triggers assembly, which in turn drives misfolding of new monomers (1).When individual proteins transform from an unstructured state to the final equilibrium state, the concept of a folding funnel characterized by a large number of potential initial states higher in energy than the final state is often invoked (5, 6). The walls of the funnel are presumed not to be smooth and the resulting bumps and valleys define kinetic traps where the protein exhibits nonequilibrium structures for extended periods of time. These transient structures can be disordered "molten globules" or partially ordered intermediates (7). This physical picture of folding in which one fraction of a protein population promptly reaches the folded state while the remaining fraction gets trapped in metastable states has been referred as the kinetic partitioning mechanism (8). The energy landscape that defines the funnel as well as the pathways through it have been explored in some detail at the single molecule level for a number of small proteins and protein subdomains through both simulations (8-10) and experiments (11-13). However, despite the fact that conformational transformations are part and parcel of protein self-assembly into extended architectures, this concept of the folding fu...