The linac coherent light source single particle imaging road map.

Intense femtosecond x-ray pulses from free-electron laser sources allow the imaging of individual particles in a single shot. Early experiments at the Linac Coherent Light Source (LCLS) have led to rapid progress in the field and, so far, coherent diffractive images have been recorded from biological specimens, aerosols, and quantum systems with a few-tens-of-nanometers resolution. In March 2014, LCLS held a workshop to discuss the scientific and technical challenges for reaching the ultimate goal of atomic resolution with single-shot coherent diffractive imaging. This paper summarizes the workshop findings and presents the roadmap toward reaching atomic resolution, 3D imaging at free-electron laser sources.

High apparent dielectric constants in the interior of a protein reflect water penetration.

A glutamic acid was buried in the hydrophobic core of staphylococcal nuclease by replacement of Val-66. Its pK(a) was measured with equilibrium thermodynamic methods. It was 4.3 units higher than the pK(a) of Glu in water. This increase was comparable to the DeltapK(a) of 4.9 units measured previously for a lysine buried at the same location. According to the Born formalism these DeltapK(a) are energetically equivalent to the transfer of a charged group from water to a medium of dielectric constant of 12. In contrast, the static dielectric constants of dry protein powders range from 2 to 4. In the crystallographic structure of the V66E mutant, a chain of water molecules was seen that hydrates the buried Glu-66 and links it with bulk solvent. The buried water molecules have never previously been detected in >20 structures of nuclease. The structure and the measured energetics constitute compelling and unprecedented experimental evidence that solvent penetration can contribute significantly to the high apparent polarizability inside proteins. To improve structure-based calculations of electrostatic effects with continuum methods, it will be necessary to learn to account quantitatively for the contributions by solvent penetration to dielectric effects in the protein interior.

The duplication of an eight-residue helical stretch in Staphylococcal nuclease is not helical: a model for evolutionary change.

A common method of evolutionary change is gene duplication, followed by other events that lead to new function, decoration of folds, oligomerization, or other changes. As part of a study on the potential for evolutionary change created by duplicated sequences, we have carried out a crystallographic study on a mutant of Staphylococcal nuclease in which residues 55-62 have been duplicated in a wild-type variant termed PHS. In the parental protein (PHS) these residues form the first two turns of a helix running from residue 54 to 68 (hereafter designated as helix I). The crystal structure of the mutant is very similar to that of the parental, with helix I being unaltered. The duplicated residues are accommodated by expanding an existing loop N-terminal to helix I. In addition, circular dichroism (CD) studies have been carried out on a parental peptide containing helix I with six flanking residues at each terminus (residues 48-74) and on the same peptide expanded by the duplication, as a function of 2,2,2-trifluoroethanol (TFE) concentration. Each peptide possesses only modest helical propensity in solution. Our data, which is different from what was observed in T4 lysozyme, show that the conformation of the duplicated sequence is determined by a balance of sequential and longer-range effects. Thus duplicating sequence need not mean duplicating structure. Proteins 2000;40:465-472.

Crystal structure of a conserved ribosomal protein-RNA complex.

The structure of a highly conserved complex between a 58-nucleotide domain of large subunit ribosomal RNA and the RNA-binding domain of ribosomal protein L11 has been solved at 2.8 angstrom resolution. It reveals a precisely folded RNA structure that is stabilized by extensive tertiary contacts and contains an unusually large core of stacked bases. A bulge loop base from one hairpin of the RNA is intercalated into the distorted major groove of another helix; the protein locks this tertiary interaction into place by binding to the intercalated base from the minor groove side. This direct interaction with a key ribosomal RNA tertiary interaction suggests that part of the role of L11 is to stabilize an unusual RNA fold within the ribosome.

Crystal packing induces a conformational change in profilin-I from Acanthamoeba castellanii.

Profilin-I from Acanthamoeba castellanii is a 13-kDa protein that binds actin and poly-l-proline. The native protein has been crystallized in two different but closely related forms. The second form proved more amenable to three-dimensional structural determination using heavy-atom isomorphous methods to obtain crystallographic phase information. We used the second crystal structure as a test molecule in the molecular replacement procedure to determine the structure of the first crystal form of profilin-I. More residues participate in crystal lattice contacts in the first crystal form than in the second. The two crystal forms differ significantly in the C-terminal helix that interacts with actin and in the loop preceding this helix. Coordinates of some main chain atoms here differ by about 1.0 A, and side chain atoms differ by more than 2.0 A.

Crystal structure of the actin-binding protein actophorin from Acanthamoeba.

Actophorin is a member of the actin-depolymerizing factor/cofilin family. It severs actin filaments and sequesters actin monomers. The crystal structure of actophorin will help to elucidate actin-ADF/cofilin interactions.

Experimental measurement of the effective dielectric in the hydrophobic core of a protein.

The dielectric inside a protein is a key physical determinant of the magnitude of electrostatic interactions in proteins. We have measured this dielectric phenomenologically, in terms of the dielectric that needs to be used with the Born equation in order to reproduce the observed pKa shifts induced by burial of an ionizable group in the hydrophobic core of a protein. Mutants of staphylococcal nuclease with a buried lysine residue at position 66 were engineered for this purpose. The pKa values of buried lysines were measured by difference potentiometry. The extent of coupling between the pKa and the global stability of the protein was evaluated by measuring pKa values in hyperstable forms of nuclease engineered to be 3.3 or 6.5 kcal mol-1 more stable than the wild type. The crystallographic structure of one mutant was determined to describe the environment of the buried lysine. The dielectrics that were measured range from 10 to 12. Published pKa values of buried ionizable residues in other proteins were analyzed in a similar fashion and the dielectrics obtained from these values are consistent with the ones measured in nuclease. These results argue strongly against the prevalent use of dielectrics of 4 or lower to describe the dielectric effect inside a protein in structure-based calculations of electrostatic energies with continuum dielectric models.

Crystal structure of the haemopexin-like C-terminal domain of gelatinase A.

The crystal structure of the haemopexin-like C-terminal domain of gelatinase A reveals that it is a four-bladed beta-propeller protein. The four blades are arranged around a channel-like opening in which Ca2+ and a Na-Cl+ ion pair are bound.

One-step evolution of a dimer from a monomeric protein.

Deletion of six amino acids in a surface loop transforms staphylococcal nuclease from a monomeric protein into a very stable dimer (Kd < 1 x 10(-8)M). A 2 A X-ray crystal structure of the dimer (R = 0.176) shows that the carboxy-terminal alpha-helix has been stripped from its normal position in one monomer and is now incorporated into the equivalent position on the adjoining monomer. This swapping creates an association interface of 2900 A 2. A second, smaller interface of 460 A 2 is also formed. The spontaneous exchange or swapping of secondary structural elements provides a simple pathway for the formation of large, stable protein/protein interfaces and may play an important role in the evolution of oligomeric proteins.

X-ray crystal structures of staphylococcal nuclease complexed with the competitive inhibitor cobalt(II) and nucleotide.

Two crystal structures of ternary complexes of staphylococcal nuclease, cobalt(II), and the mononucleotide pdTp are reported. The first has been refined at 1.7 A to a crystallographic R value of 0.198; the second, determined from a crystal soaked for 9 months in a slightly different mother liquor than the first crystal, has been refined at 1.85 A to an R value of 0.174. In the first structure, the cobalt ion is displaced 1.94 A from the normal calcium position, and the active site is dominated by a salt bridge between Asp-21 and Lys-70 from a symmetry-related molecule in the crystal lattice. The Co2+ ion appears unable to displace this lysine; consequently, the metal is bound in a vestibular site adjacent to the calcium site. The metal-binding pocket in the second structure adopts a configuration similar to that of the calcium complex, with the cobalt ion binding only 0.36 A from the calcium position. However, an inner sphere water seen in the calcium structure is missing from this structure. The cobalt ion in the second structure appears to be loosely or transiently coordinated within the calcium binding pocket, as evidenced by the high value of its refined thermal factor. Loss of catalytic activity for cobalt(II)-substituted nuclease is perhaps due to its inability to bind this inner sphere water.

Residual structure in a staphylococcal nuclease fragment. Is it a molten globule and is its unfolding a first-order phase transition?

Temperature-induced unfolding of staphylococcal nuclease and its large fragment, which lacks 13 C-terminal amino acid residues, was studied calorimetrically, and by CD and fluorescence spectroscopy. It was shown that, in contrast to the full length protein which includes two domains and unfolds in two distinct stages under some conditions, the fragment unfolds in one stage. Unfolding of the fragment proceeds in the same temperature range in which the N-terminal beta-barrel domain unfolds in the full length staphylococcal nuclease. Therefore, the fragment is initially partly unfolded. It retains a stable N-terminal domain which unfolds co-operatively with significant heat absorption. Unfolding of the fragment can be regarded as a first-order phase transition, but its initial state certainly does not represent a molten globule, as it was believed.

X-ray structures of isoforms of the actin-binding protein profilin that differ in their affinity for phosphatidylinositol phosphates.

We determined the structures of Acanthamoeba profilin I and profilin II by x-ray crystallography at resolutions of 2.0 and 2.8 A, respectively. The polypeptide folds and the actin-binding surfaces of the amoeba profilins are very similar to those of bovine and human profilins. The electrostatic potential surfaces of the two Acanthamoeba isoforms differ. Two areas of high positive potential on the surface of profilin II are candidate binding sites for phosphatidylinositol phosphates. The proximity of these sites to the actin binding site provides an explanation for the competition between actin and lipids for binding profilin.