Residues 262-274 form a loop between subdomains 3 and 4 of actin. This loop may play an important role in actin filament formation and stabilization. To assess directly the behavior of this loop, we mutated Ser 265 of yeast actin to cysteine (S265C) and created another mutant (S265C/C374A) by changing Cys 374 of S265C actin to alanine. These changes allowed us to attach a pyrene maleimide stoichiometrically to either Cys 374 or Cys 265 . These mutations had no detectable effects on the protease susceptibility, intrinsic ATPase activity, and thermal stability of labeled or unlabeled G-actin. The presence of the loop cysteine, either labeled or unlabeled, did not affect the actin-activated S1 ATPase activity or the in vitro motility of the actin. Both mutant actins, either labeled or unlabeled, nucleated filament formation considerably faster than wild-type (WT) actin, although the critical concentration was not affected. Whereas the fluorescence of the C-terminal (WT) probe increased during polymerization, that of the loop (S265C/C374A) probe decreased, and the fluorescence of the doubly labeled actin (S265C) was ϳ50% less than the sum of the fluorescence of the individual fluorophores. Quenching was also observed in copolymers of labeled WT and S265C/C374A actins. An excimer peak was present in the emission spectrum of labeled S265C F-actin and in the labeled S265C/C374A-WT actin copolymers. These results show that in the filaments, the C-terminal pyrene of a substantial fraction of monomers directly interacts with the loop pyrene of neighboring monomers, bringing the two cysteine sulfurs to within 18 Å of one another. Finally, when bound to labeled S265C/ C374A F-actin, myosin S1, but not tropomyosin, caused an increase in fluorescence of the loop probe. Both proteins had no effect on excimer fluorescence. These results help establish the orientation of monomers in Factin and show that the binding of S1 to actin subdomains 1 and 2 affects the environment of the loop between subdomains 3 and 4.The crystal structure of the actin monomer has been elucidated as part of a 1:1 complex with three actin-binding proteins (1-3). However, the structure of the two-stranded actin filament at atomic resolution has not been determined due to the inability to date to crystallize F-actin. One F-actin model, proposed by Schutt et al. (2,4), is based on the profilin/-actin ribbon structure in which actin monomers contact each other in a continuous fashion, with profilin molecules bridging between the actins on the outside of the structure. In this structure, actin subdomains 1 and 2 are near the center of the ribbon, whereas the subdomain 3/4 interface is near its exterior. Schutt et al. have proposed that the ribbon can be transformed into a classical ADP-containing helical filament by a compression and a twist. However, coordinates of this filament model have not yet been published.Holmes et al. (5) have generated an alternative model based on fitting the coordinates of the monomer into a density map generated from low angle x...