The hydration shell of myoglobin

The space in the unit cell of a metmyoglobin crystal not occupied by myoglobin atoms was filled with water using Monte Carlo calculations. Independent calculations with different amounts of water have been performed. Structure factors were calculated using the water coordinates thus obtained and the known coordinates of the myoglobin atoms. A comparison with experimental structure factors showed that both the low and the high resolution regime could be well reproduced with 814 Monte Carlo water molecules per unit cell with a B-value of 50 Ų. The Monte Carlo water molecules yield a smaller standard R-value (0.166) than using a homogeneous electron density for the simulation of the crystal water (R = 0.212). A reciprocal space refinement of the water and the protein coordinates has been performed. Monte Carlo calculations can be used to obtain information for crystallographically invisible parts of the unit cell and yield better coordinates for the visible part in the refinement. Correspondence to: F. Parak     

X-Ray Analysis of the Magnesium-containing Endonuclease from Serratia marcescens

The three-dimensional crystal structure of the DNA/RNA nonspecific endonuclease from Serratia marcescenswas refined at the resolution of 1.07 Å to Rfactor of 12.4% and R _freefactor of 15.3% using the anisotropic approximation. The structure includes 3924 non-hydrogen atoms, 715 protein-bound water molecules, and a Mg²⁺ion in each binding site of each subunit of the nuclease homodimeric globular molecule. The 3D topological model of the enzyme was revealed, the inner symmetry of the monomers in its N-and C-termini was found, and the local environment of the magnesium cofactor in the nuclease active site was defined. Mg²⁺ion was found to be bound to the Asn119 residue and surrounded by five associated water molecules that form an octahedral configuration. The coordination distances for the water molecules and the O¹atom of Asn119 were shown to be within the range of 2.01–2.11 Å. The thermal factors for the magnesium ion in subunits are 7.08 and 4.60 Ų, and the average thermal factors for the surrounding water molecules are 11.14 and 10.30 Ų, respectively. The region of the nuclease subunit interactions was localized, and the alternative side chain conformations were defined for 51 amino acid residues of the nuclease dimer.     

Crystal structures of a type-1 ribosome inactivating protein from Momordica balsamina in the bound and unbound states

The ribosome inactivating proteins (RIPs) of type 1 are plant toxins that eliminate adenine base selectively from the single stranded loop of rRNA. We report six crystal structures, type 1 RIP from Momordica balsamina (A), three in complexed states with ribose (B), guanine (C) and adenine (D) and two structures of MbRIP-1 when crystallized with adenosine triphosphate (ATP) (E) and 2′-deoxyadenosine triphosphate (2′-dATP) (F). These were determined at 1.67 Å, 1.60 Å, 2.20 Å, 1.70 Å, 2.07 Å and 1.90 Å resolutions respectively. The structures contained, (A) unbound protein molecule, (B) one protein molecule and one ribose sugar, (C) one protein molecule and one guanine base, (D) one protein molecule and one adenine base, (E) one protein molecule and one ATP-product adenine molecule and (F) one protein molecule and one 2′-dATP-product adenine molecule. Three distinct conformations of the side chain of Tyr70 were observed with (i) χ¹ = − 66°and χ² = 165° in structures (A) and (B); (ii) χ¹ = − 95° and χ² = 70° in structures (C), (D) and (E); and (iii) χ¹ = − 163° and χ² = 87° in structure (F). The conformation of Tyr70 in (F) corresponds to the structure of a conformational intermediate. This is the first structure which demonstrates that the slow conversion of DNA substrates by RIPs can be trapped during crystallization.     

Side-chain dynamics are critical for water permeation through aquaporin-1

Molecular dynamics simulations of aquaporin-1 embedded in a solvated lipid bilayer were carried out to investigate the mechanism of water permeation. The 2.2 Å resolution crystal structure of the bovine protein was used for five independent trajectories. During the equilibration and preparatory steps in which the protein was held fixed, water molecules inside the water channel adopted the same positions as observed in the crystal structure but they did not pass through the channel, suggesting that the dynamic motion of the protein is critical for water permeation. When the protein atoms were allowed to move, the side chains of the two asparagines in the two conserved Asn-Pro-Ala motifs near the center of the channel formed hydrogen bonds with water and helped water molecules move through the channel by actively aligning them for transport. The main-chain oxygen atoms, which were exposed to the pore surface in the crystal structure, also contributed to water transfer. Besides the constriction region observed in the crystal structure (Arg¹⁹⁷, Phe⁵⁸, His¹⁸², and Cys¹⁹¹), we found that His⁷⁶ and Val¹⁵⁵ act as a valve by dynamically blocking water permeation and helping control flow.     

1H and 15N NMR assignment and solution structure of the SH3 domain of spectrin: Comparison of unrefined and refined structure sets with the crystal structure

The assignment of the ¹H and ¹⁵Nnuclear magnetic resonance spectra of the Src-homology region 3 domain ofchicken brain -spectrin has been obtained. A set of solutionstructures has been determined from distance and dihedral angle restraints,which provide a reasonable representation of the protein structure insolution, as evaluated by a principal component analysis of the globalpairwise root-mean-square deviation (rmsd) in a large set of structuresconsisting of the refined and unrefined solution structures and the crystalstructure. The solution structure is well defined, with a lower degree ofconvergence between the structures in the loop regions than in the secondarystructure elements. The average pairwise rmsd between the 15 refinedsolution structures is 0.71 ± 0.13 Å for the backbone atoms and1.43 ± 0.14 Å for all heavy atoms. The solution structure isbasically the same as the crystal structure. The average rmsd between the 15refined solution structures and the crystal structure is 0.76 Å forthe backbone atoms and 1.45 ± 0.09 Å for all heavy atoms. Thereare, however, small differences probably caused by intermolecular contactsin the crystal structure.     

Crystal structure and microstructure of cholesteryl oleyl carbonate

The crystal structure as well as the microstructure, i.e., size and strain, of crystallites of cholesteryl oleyl carbonate was determined from X-ray powder diffraction data. The X-ray line broadening was analyzed through the refinement of TCH-pseudo-Voigt function parameters (isotropic effects) and the refinement of multipolar functions, i.e., symmetrized cubic harmonics (anisotropic effects). The crystal structure turns out to be primitive monoclinic, space group Pc, type I monolayer having two molecules per unit cell with parameters: a = 18.921 ± 0.006 Å, b = 12.952 ± 0.003 Å, c = 9.276 ± 0.002 Å and β = 91.32 ± 0.03°. The average size of a well ground specimen of crystallites was 60 nm. The average micro-strain, e.g., 45 × 10⁻⁴ has been tentatively attributed to fatty chain conformational disorder. The unit cell parameters, including the lamellar thickness, of COC crystal is very closely similar to those of another, structurally similar cholesterol ester, e.g., cholesteryl oleate (CO) crystal, space group P2₁, type II monolayer. Type I monolayer structure has been established for COC on the basis of the intensity calculations of the XRD profiles of both CO and COC. The dipolar and structural disorder in a 4:1 molar, binary mixture of CO and COC can be accommodated in an induced smectic phase with a lamellar thickness, which is nearly equal to that of pure CO or pure COC.     

Engineering protein allostery: 1.05 A resolution structure and enzymatic properties of a Na+-activated trypsin

Some trypsin-like proteases are endowed with Na⁺-dependent allosteric enhancement of catalytic activity, but this important mechanism has been difficult to engineer in other members of the family. Replacement of 19 amino acids in Streptomyces griseus trypsin targeting the active site and the Na⁺-binding site were found necessary to generate efficient Na⁺ activation. Remarkably, this property was linked to the acquisition of a new substrate selectivity profile similar to that of factor Xa, a Na⁺-activated protease involved in blood coagulation. The X-ray crystal structure of the mutant trypsin solved to 1.05 Å resolution defines the engineered Na⁺ site and active site loops in unprecedented detail. The results demonstrate that trypsin can be engineered into an efficient allosteric protease, and that Na⁺ activation is interwoven with substrate selectivity in the trypsin scaffold.     

Ultrahigh (0.93 Å) resolution structure of manganese peroxidase from Phanerochaete chrysosporium: Implications for the catalytic mechanism

Manganese peroxidase (MnP) is an extracellular heme enzyme produced by the lignin-degrading white-rot fungus Phanerochaete chrysosporium. MnP catalyzes the peroxide-dependent oxidation of Mn^II to Mn^III. The Mn^III is released from the enzyme in complex with oxalate, enabling the oxalate-Mn^III complex to serve as a diffusible redox mediator capable of oxidizing lignin, especially under the mediation of unsaturated fatty acids. One heme propionate and the side chains of Glu35, Glu39 and Asp179 have been identified as Mn^II ligands in our previous crystal structures of native MnP. In our current work, new 0.93 Å and 1.05 Å crystal structures of MnP with and without bound Mn^II, respectively, have been solved. This represents only the sixth structure of a protein of this size at 0.93 Å resolution. In addition, this is the first structure of a heme peroxidase from a eukaryotic organism at sub-Ångstrom resolution. These new structures reveal an ordering/disordering of the C-terminal loop, which is likely required for Mn binding and release. In addition, the catalytic Arg42 residue at the active site, normally thought to function only in the peroxide activation process, also undergoes ordering/disordering that is coupled to a transient H-bond with the Mn ligand, Glu39. Finally, these high-resolution structures also reveal the exact H atoms in several parts of the structure that are relevant to the catalytic mechanism.     

Crystal structure of the complex of concanavalin A and tripeptide

The X-ray structure analysis of a cross-linked crystal of concanavalin A soaked with the tripeptide molecule as the probe molecule showed electron density corresponding to full occupation in the binding pocket. The site lies on the surface of concanavalin A and is surrounded by three symmetry-related molecules. The crystal structure of the tripeptide complex was refined at 2.4-Å resolution to an R-factor of 17.5%, (R_free factor of 23.7%), with an RMS deviation in bond distances of 0.01 Å. The model includes all 237 residue of concanavalin A, 1 manganese ion, 1 calcium ion, 161 water molecules, 1 glutaraldehyde molecule, and 1 tripeptide molecule. This X-ray structure analysis also provides an approach to mapping the binding surface of crystalline protein with a probe molecule that is dissolved in a mixture of organic solvent with water or in neat organic solvent but is hardly dissolved in aqueous solution.     

[Cu4(H2O)4(dmapox)2(btc)]n · 10nH2O: The first two-dimensional polymeric copper(II) complex with bridging μ-trans-oxamidate and μ4-1,2,4,5-benzentetracarboxylato ligands: Synthesis, crystal structure and DNA binding studies

A two-dimensional copper(II) polymer with formula of [Cu₄(H₂O)₄(dmapox)₂(btc)]_n · 10nH₂O, where dmapox is the dianion of N,N′-bis[3-(dimethylamino)propyl]oxamide and btc is the tetra-anion of 1,2,4,5-benzenetetracarboxylic acid, was synthesized and characterized by elemental analysis, conductivity measurement, IR and electronic spectral studies. The crystal structure of the complex has been determined by X-ray single-crystal diffraction. The structure consists of crystallized water molecules and neutral two-dimensional copper(II) coordination polymeric networks constructed both by the bis-tridentate μ-trans-dmapox and tetra-monodentate μ₄-btc bridging ligands. Each btc ligand links four trans-dmapox-bridged binuclear copper(II) building blocks [Cu₂(H₂O)₂(trans-dmapox)]²⁺ and each binuclear copper(II) building block attaches to two btc ligands forming an infinite 2D layer which consists of 4+4 grids with dimensions of 13.563(5) × 15.616(5) Å. The environment around the copper(II) atom can be described as a distorted square-pyramid and the Cu?Cu separations through μ-trans-dmapox and μ₄-btc bridging ligands are 5.225 Å (Cu1-Cu1ⁱ), 5.270 Å (Cu2-Cu2ⁱⁱ), 6.115 Å (Cu1-Cu2), 9.047 Å (Cu1-Cu2ⁱⁱⁱ) and 10.968 Å (Cu1-Cu1ⁱⁱⁱ), respectively. Abundant hydrogen bonds among the crystallized, the coordinated water molecules, and the uncoordinated carboxyl oxygen atoms cross-link the two-dimensional layers into an overall three-dimensional channel-like framework. The interaction of the copper(II) polymer with calf thymus DNA (CT-DNA) has been investigated by using absorption, emission spectral and electrochemical techniques. The results indicate that the copper(II) polymer interacts with DNA strongly (K_b = 4.8 × 10⁵ M⁻¹ and K_sv = 1.1 × 10⁴) and the interaction mode between the copper(II) polymer and DNA may be the groove binding. To the best of our knowledge, this is the first report about the crystal structure and DNA-binding studies of a two-dimensional copper(II) polymer bridged both by the trans-oxamidate and btc ligands.     

Structure of Isoprene Synthase Illuminates the Chemical Mechanism of Teragram Atmospheric Carbon Emission

The X-ray crystal structure of recombinant PcISPS (isoprene synthase from gray poplar hybrid Populus × canescens) has been determined at 2.7 Å resolution, and the structure of its complex with three Mg²⁺ and the unreactive substrate analogue dimethylallyl-S-thiolodiphosphate has been determined at 2.8 Å resolution. Analysis of these structures suggests that the generation of isoprene from substrate dimethylallyl diphosphate occurs via a syn-periplanar elimination mechanism in which the diphosphate-leaving group serves as a general base. This chemical mechanism is responsible for the annual atmospheric emission of 100 Tg of isoprene by terrestrial plant life. Importantly, the PcISPS structure promises to guide future protein engineering studies, potentially leading to hydrocarbon fuels and products that do not rely on traditional petrochemical sources.     

Synthesis and crystal structure of the low-spin iron(II) complex [Fe(bpz)3](ClO4)2 · H2O (bpz=2,2-bipyrazine)

The crystal structure of the title compound [Fe(bpz)₃](ClO₄)₂ · H₂O (bpz=2,2^′-bipyrazine) has been determined by a single crystal X-ray diffraction study at 293(2) K. The complex is monoclinic, P2₁/c, a=17.263(3), b=9.983(2), c=17.921(4) Å, β=107.94(3)°, V=2938.3(10) ų, Z=4, R=0.073 and R_w=0.118. The structure is made up of tris-chelated [Fe(bpz)₃]²⁺ cations, uncoordinated perchlorate anions and crystallization water molecules. The iron atom exhibits a FeN₆ distorted octahedral geometry with average Fe-N bond length and N-Fe-N bidentate angle of 1.962(5) Å and 81.6(2)°. The value of the Fe-N bond distance and that of the room temperature magnetic moment are in agreement with a singlet ¹A₁ ground state. The structure of 1 is compared to those of other tris-chelated iron(II) complexes with bidentate nitrogen heterocycles.     

Crystal structure of Tk-subtilisin folded without propeptide: requirement of propeptide for acceleration of folding

Tk-subtilisin (a subtilisin homologue from Thermococcus kodakaraensis) is matured from Pro-Tk-subtilisin upon autoprocessing and degradation of Tk-propeptide. To analyze the folding mechanism of Tk-subtilisin, the crystal structure of the active site mutant of Tk-subtilisin (S324A-subtilisin^∗), which was refolded in the presence of Ca²⁺ and absence of Tk-propeptide, was determined at 2.16 Å resolution. This structure is essentially the same as that of Tk-subtilisin matured from Pro-Tk-subtilisin. S324A-subtilisin^∗ was refolded with a rate constant of 0.17 and 1.8 min⁻¹ at 30 °C in the absence and presence of Tk-propeptide, respectively, indicating that Tk-subtilisin does not require Tk-propeptide for folding but requires it for acceleration of folding.     

Halogenated Benzenes Bound within a Non-polar Cavity in T4 Lysozyme Provide Examples of I?S and I?Se Halogen-bonding

We showed earlier that the mutation of Leu99 to alanine in bacteriophage T4 lysozyme creates an internal cavity of volume ∼ 150 Å³ that binds benzene and a variety of other ligands. As such, this cavity provides an excellent target to study protein-ligand interaction. Here, we use low-temperature crystallography and related techniques to analyze the binding of halogen-incorporated benzenes typified by C₆F₅X, where X = H, F, Cl, Br or I, and C₆H₅X, where X = H or I was also studied. Because of the increased electron density of fluorine relative to hydrogen, the geometry of binding of the fluoro compounds can often be determined more precisely than their hydrogen-containing analogs. All of the ligands bind in essentially the same plane but the center of the phenyl ring can translate by up to 1.2 Å. In no case does the ligand rotate freely within the cavity. The walls of the cavity consist predominantly of hydrocarbon atoms, and in several cases it appears that van der Waals interactions define the geometry of binding. In comparing the smallest with the largest ligand, the cavity volume increases from 181 Å³ to 245 Å³. This shows that the protein is flexible and adapts to the size and shape of the ligand. There is a remarkably close contact of 3.0 Å between the iodine atom on C₆F₅I and the sulfur or selenium atom of Met or SeMet102. This interaction is 1.0 Å less than the sum of the van der Waals radii and is a clear example of a so-called halogen bond. Notwithstanding this close approach, the increase in binding energy for the halogen bond relative to a van der Waals contact is estimated to be only about 0.5-0.7 kcal/mol.     

Hydrothermal synthesis, structure characterization and catalytic property of a new 1-D chain built on bi-capped Keggin type mix-valence molybdenum compound: (NH4)[Mo6Mo6O36(AsO4)Mo(MoO)]

The synthesis and structure of a new 1-D molybdenum-arsenic compound based on the bi-capped Keggin anion [Mo^VI₆Mo^V₆O₃₆(AsO₄)(Mo^VO)₂]⁻ have been reported, and its catalytic property has been examined. The title compound was characterized by IR, TG and X-ray diffraction analysis. Single crystal X-ray diffraction shows that it crystallizes in cubic crystal system, space group Pn-3m with cell dimension: a = 11.749(2) Å, V = 1622.0(5) Å³, Z = 2. Its structure has a 1-D infinite chain, in which the bi-capped Keggin anions are connected by sharing one terminal oxygen atom from the caps. The compound shows a moderate styrene conversion (48%), the major product for the oxidation of styrene is benzaldehyde (85.2%).     

Structure of duplex DNA containing the cisplatin 1,2-{Pt(NH3)2}-d(GpG) cross-link at 1.77 Å resolution

We report the 1.77-Å resolution X-ray crystal structure of a dodecamer DNA duplex with the sequence 5′-CCTCTGGTCTCC-3′ that has been modified to contain a single engineered 1,2-cis-{Pt(NH₃)₂}²⁺-d(GpG) cross-link, the major DNA adduct of cisplatin. These data represent a significant improvement in resolution over the previously published 2.6-Å structure. The ammine ligands in this structure are clearly resolved, leading to improved visualization of the cross-link geometry with respect to both the platinum center and to the nucleobases, which adopt a higher energy conformation. Also better resolved are the deoxyribose sugar puckers, which allow us to re-examine the global structure of platinum-modified DNA. Another new feature of this model is the location of four octahedral [Mg(H₂O)₆]²⁺ ions associated with bases in the DNA major groove and the identification of 124 ordered water molecules that participate in hydrogen-bonding interactions with either the nucleic acid or the diammineplatinum(II) moiety.     

Analysis of Flavivirus NS5 Methyltransferase Cap Binding

The flavivirus 2′-O-nucleoside N-terminal RNA methyltransferase (MTase) enzyme is responsible for methylating the viral RNA cap structure. To increase our understanding of the mechanism of viral RNA cap binding we performed a detailed structural and biochemical characterization of the guanosine cap-binding pocket of the dengue (DEN) and yellow fever (YF) virus MTase enzymes. We solved an improved 2.1 Å resolution crystal structure of DEN2 Mtase, new 1.5 Å resolution crystal structures of the YF virus MTase domain in apo form, and a new 1.45 Å structure in complex with guanosine triphosphate and RNA cap analog. Our structures clarify the previously reported DEN MTase structure, suggest novel protein-cap interactions, and provide a detailed view of guanine specificity. Furthermore, the structures of the DEN and YF proteins are essentially identical, indicating a large degree of structural conservation amongst the flavivirus MTases. Guanosine triphosphate analog competition assays and mutagenesis analysis, performed to analyze the biochemical characteristics of cap binding, determined that the major interaction points are (i) guanine ring via π−π stacking with Phe24, N1 hydrogen interaction with the Leu19 backbone carbonyl via a water bridge, and C2 amine interaction with Leu16 and Leu19 backbone carbonyls; (ii) ribose 2′ hydroxyl interaction with Lys13 and Asn17; and (iii) α-phosphate interactions with Lys28 and Ser215. Based on our mutational and analog studies, the guanine ring and α-phosphate interactions provide most of the energy for cap binding, while the combination of the water bridge between the guanine N1 and Leu19 carbonyl and the hydrogen bonds between the C2 amine and Leu16/Leu19 carbonyl groups provide for specific guanine recognition. A detailed model of how the flavivirus MTase protein binds RNA cap structures is presented.     

Measurement of chemical exchange between RNA conformers by F NMR

Many noncoding RNA molecules adopt alternative secondary and tertiary conformations that are critical for their roles in gene expression. Although many of these rearrangements are mediated by other biomolecular components, it is important to evaluate the equilibrium relationship of the conformers. To measure the spontaneous interconversion in a bi-stable RNA stem loop sequence into which a single ¹⁹F-uridine label was incorporated, a ¹⁹F–¹⁹F EXSY experiment was employed. The kinetic exchange rate measured from EXSY experiments for this system was 37.3 ± 2.8 s⁻¹. The advantage of this approach is that exchange kinetics can be monitored in any RNA sequence into which a single ¹⁹F nucleotide is incorporated by commercial synthesis. This method is therefore suitable for application to biologically significant systems in which dynamic conformational rearrangement is important for function and may therefore facilitate studies of RNA structure–function relationships.     

Solution structure of porcine pancreatic phospholipase A2 complexed with micelles and a competitive inhibitor

Summary The three-dimensional structure of porcine pancreatic PLA₂ (PLA₂), present in a 40 kDa ternary complex with micelles and a competitive inhibitor, has been determined using multidimensional heteronuclear NMR spectroscopy. The structure of the protein (124 residues) is based on 1854 constraints, comprising 1792 distance and 62 torsion angle constraints. A total of 18 structures was calculated using a combined approach of distance geometry and restrained molecular dynamics. The atomic rms distribution about the mean coordinate positions for residues 1–62 and 72–124 is 0.75±0.09 Å for the backbone atoms and 1.14±0.10 Å for all atoms. The rms difference between the averaged minimized NMR structures of the free PLA₂ and PLA₂ in the ternary complex is 3.5 Å for the backbone atoms and 4.0 Å for all atoms. Large differences occur for the calcium-binding loop and the surface loop from residues 62 through 72. The most important difference is found for the first three residues of the N-terminal -helix. Whereas free in solution Ala¹, Leu² and Trp³ are disordered, with the -amino group of Ala¹ pointing out into the solvent, in the ternary complex these residues have an -helical conformation with the -amino group buried inside the protein. As a consequence, the important conserved hydrogen bonding network which is also seen in the crystal structures is present only in the ternary complex, but not in free PLA₂. Thus, the NMR structure of the N-terminal region (as well as the calcium-binding loop and the surface loop) of PLA₂ in the ternary complex resembles that of the crystal structure. Comparison of the NMR structures of the free enzyme and the enzyme in the ternary complex indicates that conformational changes play a role in the interfacial activation of PLA₂.     

Structural refinement of membrane proteins by restrained molecular dynamics and solvent accessibility data

We present an approach for incorporating solvent accessibility data from electron paramagnetic resonance experiments in the structural refinement of membrane proteins through restrained molecular dynamics simulations. The restraints have been parameterized from oxygen (ΠO₂) and nickel-ethylenediaminediacetic acid (ΠNiEdda) collision frequencies, as indicators of lipid or aqueous exposed spin-label sites. These are enforced through interactions between a pseudoatom representation of the covalently attached Nitroxide spin-label and virtual “solvent” particles corresponding to O₂ and NiEdda in the surrounding environment. Interactions were computed using an empirical potential function, where the parameters have been optimized to account for the different accessibilities of the spin-label pseudoatoms to the surrounding environment. This approach, “pseudoatom-driven solvent accessibility refinement”, was validated by refolding distorted conformations of the Streptomyces lividans potassium channel (KcsA), corresponding to a range of 2-30 Å root mean-square deviations away from the native structure. Molecular dynamics simulations based on up to 58 electron paramagnetic resonance restraints derived from spin-label mutants were able to converge toward the native structure within 1-3 Å root mean-square deviations with minimal computational cost. The use of energy-based ranking and structure similarity clustering as selection criteria helped in the convergence and identification of correctly folded structures from a large number of simulations. This approach can be applied to a variety of integral membrane protein systems, regardless of oligomeric state, and should be particularly useful in calculating conformational changes from a known reference crystal structure.