J. Günter Grossmann

The complete folding pathway of a protein from nanoseconds to microseconds

Combining experimental and simulation data to describe all of the structures and the pathways involved in folding a protein is problematical. Transition states can be mapped experimentally by φ values, but the denatured state is very difficult to analyse under conditions that favour folding. Also computer simulation at atomic resolution is currently limited to about a microsecond or less. Ultrafast-folding proteins fold and unfold on timescales accessible by both approaches, so here we study the folding pathway of the three-helix bundle protein Engrailed homeodomain. Experimentally, the protein collapses in a microsecond to give an intermediate with much native α-helical secondary structure, which is the major component of the denatured state under conditions that favour folding. A mutant protein shows this state to be compact and contain dynamic, native-like helices with unstructured side chains. In the transition state between this and the native state, the structure of the helices is nearly fully formed and their docking is in progress, approximating to a classical diffusion–collision model. Molecular dynamics simulations give rate constants and structural details highly consistent with experiment, thereby completing the description of folding at atomic resolution.

The structure of the C-terminal actin-binding domain of talin

Talin is a large dimeric protein that couples integrins to cytoskeletal actin. Here, we report the structure of the C‐terminal actin‐binding domain of talin, the core of which is a five‐helix bundle linked to a C‐terminal helix responsible for dimerisation. The NMR structure of the bundle reveals a conserved surface‐exposed hydrophobic patch surrounded by positively charged groups. We have mapped the actin‐binding site to this surface and shown that helix 1 on the opposite side of the bundle negatively regulates actin binding. The crystal structure of the dimerisation helix reveals an antiparallel coiled‐coil with conserved residues clustered on the solvent‐exposed face. Mutagenesis shows that dimerisation is essential for filamentous actin (F‐actin) binding and indicates that the dimerisation helix itself contributes to binding. We have used these structures together with small angle X‐ray scattering to derive a model of the entire domain. Electron microscopy provides direct evidence for binding of the dimer to F‐actin and indicates that it binds to three monomers along the long‐pitch helix of the actin filament.

X-ray solution scattering reveals conformational changes upon iron uptake in lactoferrin, serum and ovo-transferrins.

X-ray solution scattering has been used for studying the structural changes that take place upon uptake and release of iron from serum and chicken ovo-transferrin and human lactoferrin. In the case of chicken ovo-transferrin, data have been obtained for both the intact protein and the isolated N and C-lobes with and without iron. These studies reveal that both lobes undergo a change that is consistent with an opening of the inter-domain cleft when iron is removed from the protein. We suggest that the conformational change of the protein increases the specificity of receptor binding and that the closed configuration of the iron-loaded protein is one, or perhaps the, decisive step in the mechanism for receptor-mediated endocytosis.

The Structure of the Talin Head Reveals a Novel Extended Conformation of the FERM Domain

Summary FERM domains are found in a diverse superfamily of signaling and adaptor proteins at membrane interfaces. They typically consist of three separately folded domains (F1, F2, F3) in a compact cloverleaf structure. The crystal structure of the N-terminal head of the integrin-associated cytoskeletal protein talin reported here reveals a novel FERM domain with a linear domain arrangement, plus an additional domain F0 packed against F1. While F3 binds β-integrin tails, basic residues in F1 and F2 are required for membrane association and for integrin activation. We show that these same residues are also required for cell spreading and focal adhesion assembly in cells. We suggest that the extended conformation of the talin head allows simultaneous binding to integrins via F3 and to PtdIns(4,5)P2-enriched microdomains via basic residues distributed along one surface of the talin head, and that these multiple interactions are required to stabilize integrins in the activated state.

Structure of an Integrin-Ligand Complex Deduced from Solution X-ray Scattering and Site-directed Mutagenesis

The structural basis of the interaction of integrin heterodimers with their physiological ligands is poorly understood. We have used solution x-ray scattering to visualize the head region of integrin α5β1 in an inactive (Ca2+-occupied) state, and in complex with a fragment of fibronectin containing the RGD and synergy recognition sequences. Shape reconstructions of the data have been interpreted in terms of appropriate molecular models. The scattering data suggest that the head region undergoes no gross conformational changes upon ligand binding but do lend support to a proposed outward movement of the hybrid domain in the β subunit. Fibronectin is observed to bind across the top of the head region, which contains an α subunit β-propeller and a β subunit vWF type A domain. The model of the complex indicates that the synergy region binds on the side of the β-propeller domain. In support of this suggestion, mutagenesis of a prominent loop region on the side of the propeller identifies two residues (Tyr208 and Ile210) involved in recognition of the synergy region. Our data provide the first view of a complex between an integrin and a macromolecular ligand in solution, at a nominal resolution of ∼10 Å.

Structure of a double ubiquitin-like domain in the talin head: a role in integrin activation

Talin is a 270‐kDa protein that activates integrins and couples them to cytoskeletal actin. Talin contains an N‐terminal FERM domain comprised of F1, F2 and F3 domains, but it is atypical in that F1 contains a large insert and is preceded by an extra domain F0. Although F3 contains the binding site for β‐integrin tails, F0 and F1 are also required for activation of β1‐integrins. Here, we report the solution structures of F0, F1 and of the F0F1 double domain. Both F0 and F1 have ubiquitin‐like folds joined in a novel fixed orientation by an extensive charged interface. The F1 insert forms a loop with helical propensity, and basic residues predicted to reside on one surface of the helix are required for binding to acidic phospholipids and for talin‐mediated activation of β1‐integrins. This and the fact that basic residues on F2 and F3 are also essential for integrin activation suggest that extensive interactions between the talin FERM domain and acidic membrane phospholipids are required to orientate the FERM domain such that it can activate integrins.

Structural Determinants of Integrin Binding to the Talin Rod

The adaptor protein talin serves both to activate the integrin family of cell adhesion molecules and to couple integrins to the actin cytoskeleton. Integrin activation has been shown to involve binding of the talin FERM domain to membrane proximal sequences in the cytoplasmic domain of the integrin β-subunit. However, a second integrin-binding site (IBS2) has been identified near the C-terminal end of the talin rod. Here we report the crystal structure of IBS2 (residues 1974-2293), which comprises two five-helix bundles, “IBS2-A” (1974-2139) and “IBS2-B” (2140-2293), connected by a continuous helix with a distinct kink at its center that is stabilized by side-chain H-bonding. Solution studies using small angle x-ray scattering and NMR point to a fairly flexible quaternary organization. Using pull-down and enzyme-linked immunosorbent assays, we demonstrate that integrin binding requires both IBS2 domains, as does binding to acidic phospholipids and robust targeting to focal adhesions. We have defined the membrane proximal region of the integrin cytoplasmic domain as the major binding region, although more membrane distal regions are also required for strong binding. Alanine-scanning mutagenesis points to an important electrostatic component to binding. Thermal unfolding experiments show that integrin binding induces conformational changes in the IBS2 module, which we speculate are linked to vinculin and membrane binding.

Biological role and structural mechanism of twinfilin-capping protein interaction.

Twinfilin and capping protein (CP) are highly conserved actin‐binding proteins that regulate cytoskeletal dynamics in organisms from yeast to mammals. Twinfilin binds actin monomer, while CP binds the barbed end of the actin filament. Remarkably, twinfilin and CP also bind directly to each other, but the mechanism and role of this interaction in actin dynamics are not defined. Here, we found that the binding of twinfilin to CP does not affect the binding of either protein to actin. Furthermore, site‐directed mutagenesis studies revealed that the CP‐binding site resides in the conserved C‐terminal tail region of twinfilin. The solution structure of the twinfilin–CP complex supports these conclusions. In vivo, twinfilins binding to both CP and actin monomer was found to be necessary for twinfilins role in actin assembly dynamics, based on genetic studies with mutants that have defined biochemical functions. Our results support a novel model for how sequential interactions between actin monomers, twinfilin, CP, and actin filaments promote cytoskeletal dynamics.

Knotted Fusion Proteins Reveal Unexpected Possibilities in Protein Folding

Proteins that contain a distinct knot in their native structure are impressive examples of biological self-organization. Although this topological complexity does not appear to cause a folding problem, the mechanisms by which such knotted proteins form are unknown. We found that the fusion of an additional protein domain to either the amino terminus, the carboxy terminus, or to both termini of two small knotted proteins did not affect their ability to knot. The multidomain constructs remained able to fold to structures previously thought unfeasible, some representing the deepest protein knots known. By examining the folding kinetics of these fusion proteins, we found evidence to suggest that knotting is not rate limiting during folding, but instead occurs in a denatured-like state. These studies offer experimental insights into when knot formation occurs in natural proteins and demonstrate that early folding events can lead to diverse and sometimes unexpected protein topologies.

Assembly of Oligomeric Death Domain Complexes during Toll Receptor Signaling

The Drosophila Toll receptor is activated by the endogenous protein ligand Spätzle in response to microbial stimuli in immunity and spatial cues during embryonic development. Downstream signaling is mediated by the adaptor proteins Tube, the kinase Pelle, and the Drosophila homologue of myeloid differentiation primary response protein (dMyD88). Here we have characterized heterodimeric (dMyD88-Tube) and heterotrimeric (dMyD88-Tube-Pelle) death domain complexes. We show that both the heterodimeric and heterotrimeric complexes form kidney-shaped structures and that Tube is bivalent and has separate high affinity binding sites for dMyD88 and Pelle. Additionally we found no interaction between the isolated death domains of Pelle and dMyD88. These results indicate that the mode of assembly of the heterotrimeric dMyD88-Tube-Pelle complex downstream of the activated Toll receptor is unique. The measured dissociation constants for the interaction between the death domains of dMyD88 and Tube and of Pelle and a preformed dMyD88-Tube complex are used to propose a model of the early postreceptor events in Drosophila Toll receptor signaling.