Troponin is essential in Ca(2+) regulation of skeletal and cardiac muscle contraction. It consists of three subunits (TnT, TnC and TnI) and, together with tropomyosin, is located on the actin filament. Here we present crystal structures of the core domains (relative molecular mass of 46,000 and 52,000) of human cardiac troponin in the Ca(2+)-saturated form. Analysis of the four-molecule structures reveals that the core domain is further divided into structurally distinct subdomains that are connected by flexible linkers, making the entire molecule highly flexible. The alpha-helical coiled-coil formed between TnT and TnI is integrated in a rigid and asymmetric structure (about 80 angstrom long), the IT arm, which bridges putative tropomyosin-anchoring regions. The structures of the troponin ternary complex imply that Ca(2+) binding to the regulatory site of TnC removes the carboxy-terminal portion of TnI from actin, thereby altering the mobility and/or flexibility of troponin and tropomyosin on the actin filament.

Actin plays crucial parts in cell motility through a dynamic process driven by polymerization and depolymerization, that is, the globular (G) to fibrous (F) actin transition. Although our knowledge about the actin-based cellular functions and the molecules that regulate the G- to F-actin transition is growing, the structural aspects of the transition remain enigmatic. We created a model of F-actin using X-ray fibre diffraction intensities obtained from well oriented sols of rabbit skeletal muscle F-actin to 3.3 A in the radial direction and 5.6 A along the equator. Here we show that the G- to F-actin conformational transition is a simple relative rotation of the two major domains by about 20 degrees. As a result of the domain rotation, the actin molecule in the filament is flat. The flat form is essential for the formation of stable, helical F-actin. Our F-actin structure model provides the basis for understanding actin polymerization as well as its molecular interactions with actin-binding proteins.

Troponin (Tn), the complex of three subunits (TnC, TnI, and TnT), plays a key role in Ca 2؉ -dependent regulation of muscle contraction. To elucidate the interactions between the Tn subunits and the conformation of TnC in the Tn complex, we have determined the crystal structure of TnC (two Ca 2؉ bound state) in complex with the N-terminal fragment of TnI (TnI 1-47 ). The structure was solved by the single isomorphous replacement method in combination with multiple wavelength anomalous dispersion data. The refinement converged to a crystallographic R factor of 22.2% (R free ‫؍‬ 32.6%). The central, connecting ␣-helix observed in the structure of uncomplexed TnC (TnC free ) is unwound at the center (residues Ala-87, Lys-88, Gly-89, Lys-90, and Ser-91) and bent by 90°. As a result, TnC in the complex has a compact globular shape with direct interactions between the N-and C-terminal lobes, in contrast to the elongated dumb-bell shaped molecule of uncomplexed TnC. The 31-residue long TnI 1-47 ␣-helix stretches on the surface of TnC and stabilizes its compact conformation by multiple contacts with both TnC lobes. The amphiphilic C-end of the TnI 1-47 ␣-helix is bound in the hydrophobic pocket of the TnC C-lobe through 38 van der Waals interactions. The results indicate the major difference between Ca 2؉ receptors integrated with the other proteins (TnC in Tn) and isolated in the cytosol (calmodulin). The TnC͞TnI 1-47 structure implies a mechanism of how Tn regulates the muscle contraction and suggests a unique ␣-helical regulatory TnI segment, which binds to the N-lobe of TnC in its Ca 2؉ bound conformation.

Cytoskeletal filaments are often capped at one end, regulating assembly and cellular location. The actin filament is a right-handed, two-strand long-pitch helix. The ends of the two protofilaments are staggered in relation to each other, suggesting that capping could result from one protein binding simultaneously to the ends of both protofilaments. Capping protein (CP), a ubiquitous alpha/beta heterodimer in eukaryotes, tightly caps (K(d) approximately 0.1-1 nM) the barbed end of the actin filament (the end favored for polymerization), preventing actin subunit addition and loss. CP is critical for actin assembly and actin-based motility in vivo and is an essential component of the dendritic nucleation model for actin polymerization at the leading edge of cells. However, the mechanism by which CP caps actin filaments is not well understood. The X-ray crystal structure of CP has inspired a model where the C termini ( approximately 30 amino acids) of the alpha and beta subunits of CP are mobile extensions ("tentacles"), and these regions are responsible for high-affinity binding to, and functional capping of, the barbed end. We tested the tentacle model in vitro with recombinant mutant CPs. Loss of both tentacles causes a complete loss of capping activity. The alpha tentacle contributes more to capping affinity and kinetics; its removal reduces capping affinity by 5000-fold and the on-rate of capping by 20-fold. In contrast, removal of the beta tentacle reduced the affinity by only 300-fold and did not affect the on-rate. These two regions are not close to each other in the three-dimensional structure, suggesting CP uses two independent actin binding tentacles to cap the barbed end. CP with either tentacle alone can cap, as can the isolated beta tentacle alone, suggesting that the individual tentacles interact with more than one actin subunit at a subunit interface at the barbed end.

A crystallographic study reveals the structural basis for regulation by two different inhibitors of the actin capping protein, a critical factor controlling actin-driven cell motility.

Actin depolymerizing factor (ADF) and cofilin accelerate actin dynamics by severing and disassembling actin filaments. Here, we present the 3.8 Å resolution cryo-EM structure of cofilactin (cofilin-decorated actin filament). The actin subunit structure of cofilactin (C-form) is distinct from those of F-actin (F-form) and monomeric actin (G-form). During the transition between these three conformations, the inner domain of actin (subdomains 3 and 4) and the majority of subdomain 1 move as two separate rigid bodies. The cofilin–actin interface consists of three distinct parts. Based on the rigid body movements of actin and the three cofilin–actin interfaces, we propose models for the cooperative binding of cofilin to actin, preferential binding of cofilin to ADP-bound actin filaments and cofilin-mediated severing of actin filaments.

SummaryUsing correlated live-cell imaging and electron tomography we found that actin branch junctions in protruding and treadmilling lamellipodia are not concentrated at the front as previously supposed, but link actin filament subsets in which there is a continuum of distances from a junction to the filament plus ends, for up to at least 1 mm. When branch sites were observed closely spaced on the same filament their separation was commonly a multiple of the actin helical repeat of 36 nm. Image averaging of branch junctions in the tomograms yielded a model for the in vivo branch at 2.9 nm resolution, which was comparable with that derived for the in vitro actinArp2/3 complex. Lamellipodium initiation was monitored in an intracellular wound-healing model and was found to involve branching from the sides of actin filaments oriented parallel to the plasmalemma. Many filament plus ends, presumably capped, terminated behind the lamellipodium tip and localized on the dorsal and ventral surfaces of the actin network. These findings reveal how branching events initiate and maintain a network of actin filaments of variable length, and provide the first structural model of the branch junction in vivo. A possible role of filament capping in generating the lamellipodium leaflet is discussed and a mathematical model of protrusion is also presented.

The intracellular distribution and migration of many protein complexes and organelles is regulated by the dynamics of the actin filament. Many actin filament endbinding proteins play crucial roles in actin dynamics, since polymerization and depolymerization of actin protomers occur only at the filament ends. We present here an EM structure of the complex of the actin filament and hetero-dimeric capping protein (CP) bound to the barbedend at 23 Å resolution, by applying a newly developed methods of image analysis to cryo-electron micrographs. This structure was fitted by the crystal structure of CP and the proposed actin filament structure, allowing us to construct a model that depicts two major binding regions between CP and the barbed-end. This binding scheme accounted for the results of newly performed and previously published mutation experiments, and led us to propose a two-step binding model. This is the first determination of an actin filament end structure.