Pitfalls in the interpretation of structural changes in mutant proteins from crystal structures

PpcA is a small protein with 71 residues that contains three covalently bound hemes. The structures of single mutants at residue 58 have shown larger deviations in another part of the protein molecule than at the site of the mutation. Closer examination of the crystal packing has revealed the origin of this unexpected structural change. The site of mutation is within Van der Waals distance from another protein molecule related by a crystallographic twofold axis within the crystal. The structural changes occurred at or near the mutation site have led to a slight adjustment of the surface residues in contact. The observed deviations between the native and the mutant molecular structures are derived from the new crystal packing even though the two crystals are essentially isomorphous. Without careful consideration of the crystal lattice a non-expert looking at only the coordinates deposited in the Protein Data Bank could draw erroneous conclusion that mutation in one part of the molecule affected the structure of the protein in a distant part of the molecule.     

Protein heat capacity reflects the dynamics of enthalpy exchange between the single macromolecule and the surroundings

Heat capacity has played a prominent role in relating macroscopic and microscopic properties of small molecules and crystals. However, its diagnostic power can also be used for macromolecules such as proteins. It is shown in the present study that the macroscopically observed protein heat capacity provides direct access to the thermodynamic state of the single protein molecule. The new model of the physical basis of protein heat capacity emphasizes the dynamic nature of protein molecules. It incorporates equilibrium fluctuations as an integral constituent and shows that the increase in the magnitude of equilibrium fluctuations is coupled to an increase in the enthalpy flux between the individual protein molecule and its surroundings. Proteins 2000;41:86–92. © 2000 Wiley‐Liss, Inc.     

Simulation of diffusion time of small molecules in protein crystals

A simple model for evaluation of diffusion times of small molecule into protein crystals has been developed, which takes into account the physical and chemical properties both of protein crystal and the diffusing molecules. The model also includes consideration of binding and the binding affinity of a ligand to the protein. The model has been validated by simulation of experimental set-ups of several examples found in the literature. These experiments cover a wide range of situations: from small to relatively large diffusing molecules, crystals having low, medium, or high protein density, and different size. The reproduced experiments include ligand exchange in protein crystals by soaking techniques. Despite the simplifying assumptions of the model, theoretical and experimental data are in agreement with available data, with experimental diffusion times ranging from a few seconds to several hours. The method has been used successfully for planning intermediate cryotrapping experiments in maltodextrin phosphorylase crystals.     

Use of a fusion protein to obtain crystals suitable for X-ray analysis: crystallization of a GST-fused protein containing the DNA-binding domain of DNA replication-related element-binding factor, DREF.

Crystals of glutathione-S-transferase (GST)-fused protein containing the DNA-binding domain of DNA replication-related element-binding factor, DREF, were obtained under crystallization conditions similar to those for GST. Preliminary X-ray crystallographic analysis revealed that crystals of the GST-fused protein belong to space group P6(1)22 or P6(5)22 with unit cell dimensions a = b = 140.4 A, c = 93.5 A and gamma = 120 degrees, having one molecule in the crystallographic asymmetric unit. The crystals diffract to 2.5 A resolution. The cell dimensions are related to those of GST crystals thus far reported. Crystallization of the DNA-binding domain that was cleaved from the fused protein by thrombin was also carried out using several methods under numerous conditions, but efforts to produce well-ordered large crystals were unsuccessful. A possible application of GST-fusion proteins for small target proteins or domains to obtain crystals suitable for X-ray structure determination is proposed.     

Crystallization of and preliminary X-ray data for the plasma retinol-binding protein

Crystals of the human and rabbit plasma retinol-binding proteins have been grown from solutions of polyethylene glycol 6000 and CdCl2. Two crystal forms have been observed for the human protein, while the rabbit protein has only crystallized in one form which is isomorphous with one of the human serum retinol-binding protein crystals. The crystals differ in their morphologies, but are both in space group P212121 and have similar unit cell sizes (a = 45.9, b = 53.3, c = 72.0 A and a = 45.7, b = 48.7, and c = 76.5 A). The crystals diffract to approximately 2.0 A resolution. In both cases there is 1 molecule/asymmetric unit.     

Factors Governing Intercalation of Fullerenes and Other Small Molecules Between the Side Chains of Semiconducting Polymers Used in Solar Cells

While recent reports have established significant miscibility in polymer:fullerene blends used in organic solar cells, little is actually known about why polymers and fullerenes mix and how their mixing can be controlled. Here, X‐ray diffraction (XRD), differential scanning calorimetry (DSC), and molecular simulations are used to study mixing in a variety of polymer:molecule blends by systematically varying the polymer and small‐molecule properties. It is found that a variety of polymer:fullerene blends mix by forming bimolecular crystals provided there is sufficient space between the polymer side chains to accommodate a fullerene. Polymer:tetrafluoro‐tetracyanoquinodimethane (F4‐TCNQ) bimolecular crystals were also observed, although bimolecular crystals did not form in the other studied polymer:non‐fullerene blends, including those with both conjugated and non‐conjugated small molecules. DSC and molecular simulations demonstrate that strong polymer–fullerene interactions can exist, and the calculations point to van der Waals interactions as a significant driving force for molecular mixing.     

Preliminary x-ray investigation of an orthorhombic crystal of hevein

Hevein, a small protein from the latex of Hevea brasiliensis, has been crystallized by the vapor diffusion method using 2-methyl-2,4-pentanediol and CaCl2 as the precipitant agents. The crystals are orthorhombic space group P21212 with a = 21.88, b = 31.90, and c = 51.24 A and one molecule in the asymmetric unit. The crystals are quite stable to x-rays and suitable for a high resolution three-dimensional structure determination.     

Deuterium NMR of water in immobilized protein systems.

Deuterium NMR spectra are reported for lysozyme crystals, powders, and frozen solutions. At high water contents the spectrum is a superposition of a narrow central component and a quadrupole doublet. The quadrupole splitting and the relaxation rates of both components, monitored as a function of water content and temperature, are discussed in terms of models for the water-protein interaction. The anisotropy of the water molecule motion is clearly demonstrated by the deuterium quadrupole splitting observed in the protein single crystal, but such splittings were not found in protein powders and frozen protein solutions. We therefore suggest that the most useful view of such data is to consider the water-protein interactions at the surface to be mixed rapidly and that a distribution of interactions be invoked rather than an oversimplified view often taken of a two or n-site mixing where n is small.     

Imaging of protein crystals with two-photon microscopy

Second-order nonlinear optical imaging of chiral crystals (SONICC), which portrays second-harmonic generation (SHG) by noncentrosymmetric crystals, is emerging as a powerful imaging technique for protein crystals in media opaque to visible light because of its high signal-to-noise ratio. Here we report the incorporation of both SONICC and two-photon excited fluorescence (TPEF) into one imaging system that allows visualization of crystals as small as ~10 μm in their longest dimension. Using this system, we then documented an inverse correlation between the level of symmetry in examined crystals and the intensity of their SHG. Moreover, because of blue-green TPEF exhibited by most tested protein crystals, we also could identify and image SHG-silent protein crystals. Our experimental data suggest that the TPEF in protein crystals is mainly caused by the oxidation of tryptophan residues. Additionally, we found that unspecific fluorescent dyes are able to bind to lysozyme crystals and enhance their detection by TPEF. We finally confirmed that the observed fluorescence was generated by a two-photon rather than a three-photon process. The capability for imaging small protein crystals in turbid or opaque media with nondamaging infrared light in a single system makes the combination of SHG and intrinsic visible TPEF a powerful tool for nondestructive protein crystal identification and characterization during crystallization trials.     

Crystal structure of low humidity tetragonal lysozyme at 2.1-A resolution. Variability in hydration shell and its structural consequences

Tetragonal crystals of hen egg white lysozyme undergo a reversible transformation, accompanied by loss of water, when the relative humidity of the environment is reduced to about 90%. The structure of the low humidity form has been analyzed, using x-ray data collected at 88% relative humidity, in order to explore the variability in protein hydration caused by a change in the amount of water surrounding the protein molecule and the consequent conformational perturbations in the molecule. The structure has been refined by the restrained least-squares method to an R value of 0.162 for 6269 observed reflections in the 10-2.1-A resolution shell. The refined structure provides interesting examples for the variability in helical parameters, the role of interactions involving side chains and water in the stabilization of secondary structural features, and favorable specific hydration sites. The protein molecule as a whole moves slightly in the low humidity form from its position in the native crystals. The hydration shell tends to move along with the protein. Significant changes, however, occur in the hydration shell. These changes cause structural perturbations in the enzyme molecule, which are most pronounced in regions involved in substrate binding.     

Evidence for ligandable sites in structured RNA throughout the Protein Data Bank

RNA has attracted considerable attention as a target for small molecules. However, methods to identify, study, and characterize suitable RNA targets have lagged behind strategies for protein targets. One approach that has received considerable attention for protein targets has been to utilize computational analysis to investigate ligandable “pockets” on proteins that are amenable to small molecule binding. These studies have shown that selected physical properties of pockets are important parameters that govern the ability of a structure to bind to small molecules. This work describes a similar analysis to study pockets on all RNAs in the Protein Data Bank (PDB). Using parameters such as buriedness, hydrophobicity, volume, and other properties, the set of all RNAs is analyzed and compared to all proteins. Considerable overlap is observed between the properties of pockets on RNAs and proteins. Thus, many RNAs are capable of populating conformations with pockets that are likely suitable for small molecule binding. Further, principal moment of inertia (PMI) calculations reveal that liganded RNAs exist in diverse structural space, much of which overlaps with protein structural space. Taken together, these results suggest that complex folded RNAs adopt unique structures with pockets that may represent viable opportunities for small molecule targeting.     

SuperStar: comparison of CSD and PDB-based interaction fields as a basis for the prediction of protein-ligand interactions.

SuperStar is an empirical method for identifying interaction sites in proteins, based entirely on the experimental information about non-bonded interactions, present in the IsoStar database. The interaction information in IsoStar is contained in scatterplots, which show the distribution of a chosen probe around structure fragments. SuperStar breaks a template molecule (e.g. a protein binding site) into structural fragments which correspond to those in the scatterplots. The scatterplots are then superimposed on the corresponding parts of the template and converted into a composite propensity map.The original version of SuperStar was based entirely on scatterplots from the CSD. Here, scatterplots based on protein-ligand interactions are implemented in SuperStar, and validated on a test set of 122 X-ray structures of protein-ligand complexes. In this validation, propensity maps are compared with the experimentally observed positions of ligand atoms of comparable types. Although non-bonded interaction geometries in small molecule structures are similar to those found in protein-ligand complexes, their relative frequencies of occurrence are different. Polar interactions are more common in the first class of structures, while interactions between hydrophobic groups are more common in protein crystals. In general, PDB and CSD-based SuperStar maps appear equally successful in the prediction of protein-ligand interactions. PDB-based maps are more suitable to identify hydrophobic pockets, and inherently take into account the experimental uncertainties of protein atomic positions. If the protonation state of a histidine, aspartate or glutamate protein side-chain is known, specific CSD-based maps for that protonation state are preferred over PDB-based maps which represent an ensemble of protonation states.     

X-Ray-Radiation-Induced Cooperative Atomic Movements in Protein

X-rays interact with biological matter and cause damage. Proteins and other macromolecules are damaged primarily by ionizing X-ray photons and secondarily by reactive radiolytic chemical species. In particular, protein molecules are damaged during X-ray diffraction experiments with protein crystals, which is, in many cases, a serious hindrance to structure solution. The local X-ray-induced structural changes of the protein molecule have been studied using a number of model systems. However, it is still not well understood whether these local chemical changes lead to global structural changes in protein and what the mechanism is.We present experimental evidence at atomic resolution indicating the movement of large parts of the protein globule together with bound water molecules in the early stages of radiation damage to the protein crystal. The data were obtained from a crystal cryocooled to ~ 100 K and diffracting to 1 ?. The movement of the protein structural elements occurs simultaneously with the decarboxylation of several glutamate and aspartate residues that mediate contacts between moving protein structural elements and with the rearrangement of the water network. The analysis of the anisotropy of atomic displacement parameters reveals that the observed atomic movements occur at different rates in different unit cells of the crystal. Thus, the examination of the cooperative atomic movement enables us to better understand how radiation-induced local chemical and structural changes of the protein molecule eventually lead to disorder in protein crystals.     

A crystal form of ribulose-1,5-bisphosphate carboxylase/oxygenase from Nicotiana tabacum in the activated state

A new crystal form of ribulose-1,5-bisphosphate carboxylase/oxygenase (EC 4.1.1.39) from Nicotiana tabacum has been obtained at alkaline pH with polyethylene glycol 8000 in the presence of a non-ionic detergent, beta-octyl glucoside. The crystals are grown at room temperature by the hanging-drop vapor diffusion technique from a protein solution containing enzyme complexed with CO2, Mg2+, and the transition state analog 2-C-carboxy-D-arabinitol-1,5-bisphosphate. The crystals belong to the the space group P3(1)21 (or P3(2)21) with the cell parameters a = 204.6 A, and c = 117.4 A (1 A = 0.1 nm). The asymmetric unit contains half (L4S4: L, large subunit, 53,000 Mr; S, small subunit, 15,000 Mr) of a hexadecameric molecule (L8S8, 540,000 Mr). The crystals diffract to at least 2.6 A Bragg spacing and are suitable for X-ray structure determination.     

A nuclear magnetic resonance study of the hydrogen-exchange behaviour of lysozyme in crystals and solution

Amide hydrogen/deuterium exchange behaviour has been studied for all of the peptide amides of hen lysozyme by means of two-dimensional n.m.r. spectroscopy. The amides have been grouped into four categories on the basis of their rates of exchange in solution at pH 4.2 and 7.5. The distribution of the amides into the different categories has been examined in the light of the crystallographic structural information, considering the type of secondary structure, the nature of hydrogen bonding and the distance from the protein surface. None of these features was found to determine uniquely the pattern of hydrogen exchange rates within the protein. The exchange behaviour of the individual amides could, however, in general be rationalized by a combination of these features. Hydrogen exchange was also monitored in both tetragonal and triclinic crystals of lysozyme, by allowing exchange to take place in the crystals prior to dissolution and recording of n.m.r. spectra under conditions where further exchange was minimized. This enabled direct comparison to be made of the exchange behaviour in the crystals and solution. A reduction in exchange rate was observed in the crystalline state relative to solution for a substantial number of amides and distinct differences between exchange in the different crystals could be observed. These differences between the solution and the different crystal states do not, however, correlate in a simple manner with proximity to intermolecular contacts in the crystals. However, the existence of these contacts, which are on the surface of the protein molecule, have a profound effect on the exchange of amides in the interior of the protein. The results indicate that the spectrum of fluctuations giving rise to hydrogen exchange may be significantly altered by the intermolecular interactions present within the crystalline state.     

Influence of the crystalline state on photoinduced dynamics of photoactive yellow protein studied by ultraviolet-visible transient absorption spectroscopy

Time-resolved ultraviolet-visible spectroscopy was used to characterize the photocycle transitions in single crystals of wild-type and the E-46Q mutant of photoactive yellow protein (PYP) with microsecond time resolution. The results were compared with the results of similar measurements on aqueous solutions of these two variants of PYP, with and without the components present in the mother liquor of crystals. The experimental data were analyzed with global and target analysis. Distinct differences in the reaction path of a PYP molecule are observed between these conditions when it progresses through its photocycle. In the crystalline state i), much faster relaxation of the late blue-shifted photocycle intermediate back to the ground state is observed; ii), this intermediate in crystalline PYP absorbs at 380 nm, rather than at 350-360 nm in solution; and iii), for various intermediates of this photocycle the forward reaction through the photocycle directly competes with a branching reaction that leads directly to the ground state. Significantly, with these altered characteristics, the spectroscopic data on PYP are fully consistent with the structural data obtained for this photoreceptor protein with time-resolved x-ray diffraction analysis, particularly for wild-type PYP.     

Structural heterogeneity in protein crystals

Extensive conformational heterogeneity is reported in highly refined crystallographic models for the proteins crambin, erabutoxin, myohemerythrin, and lamprey hemoglobin. From 6% to 13% of the amino acid side chains of these four proteins are seen in multiple, discrete conformations. Most common are flexible side chains on the molecular surface, but structural heterogeneity occasionally extends to buried side chains or to the polypeptide backbone. A few instances of sequence heterogeneity are also very clear. Numerous solvent sites are multiplets, and at high resolution, multiple, mutually exclusive solvent networks are observed. The proteins have been studied with X-ray diffraction data extending to spacings of from 0.945 to 2.0 A. The extensive heterogeneity observed here provides detailed, accurate structures for conformational substates of these molecules and sets a lower bound on the number of substates accessible to each protein molecule in solution. Electron density is missing or very weak for only a few side chains in these protein crystals, revealing a strong preference for discrete over continuous conformational perturbations. The results at very high resolution further suggest that even rather small conformational fluctuations produce discrete substates and that unresolved conformers are accommodated in increased atomic thermal parameters.     

Water structure in vitamin B12 coenzyme crystals. II. Structural characteristics of the solvent networks.

The geometrical details of the solvent structure in vitamin B12 coenzyme crystals with respect to hydrogen bonding and nonbonded contacts, are described. The individual H-bond geometries varied over wide ranges, similar to those observed in small molecule structures. Large deviations from tetrahedral coordination were found around a majority of the waters. The mutual positions and orientations of the water molecules could not be adequately explained in terms of the H-bonding relationships present in the structure. However, additional investigations, which focused on the short range nonbonded contacts around water positions in a variety of crystal hydrates, revealed several structural regularities (Savage, 1986b). These features relate to the nonbonded O...O, H...O, and H...H interactions, and give rise to a set of repulsive restrictions that are seen to be very much stronger stereochemical restraints than those associated with H-bonding. The short-range restrictions appear largely to govern the local orientational correlations and packing arrangements of the water structure within the coenzyme (and other hydrate) crystals. In more general terms, the inclusion of the nonbonding relationships as well as the attractive H-bonding interactions, leads to a significant increase in our understanding of water structure(s). The repulsive restrictions can be used as stereochemical restraints in the interpretation and refinement of solvent structures within larger hydrate systems, such as protein crystals. They may also be included in potential functions used to simulate solvent structures in aqueous solutions and hydrate systems.     

Crystallization and preliminary X-ray analysis of a 1:1 complex between a designed monomeric interferon-gamma and its soluble receptor.

A variant of human interferon-gamma (IFN-gamma) has been created in which the two chains of the homodimeric cytokine were linked N- to C-terminus by an eight residue polypeptide linker. The sequence of this linker was derived from a loop in bira bifunctional protein, and was determined from a structural database search. This "single-chain" variant was used to create an IFN-gamma molecule that binds only a single copy of the alpha-chain receptor, rather than the 2 alpha-chain receptor: 1 IFN-gamma binding stoichiometry observed for the native hormone. Crystals have been grown of a 1:1 complex between this single-chain molecule and the extracellular domain of its alpha-chain receptor. These crystals diffract beyond 2.0 A, significantly better than the 2.9 A observed for the native 2:1 complex. Density calculations suggest these crystals contain two complexes in the asymmetric unit; a self-rotation function confirms this conclusion.     

Highly ordered crystals of the plant seed protein crambin.

Crystals of crambin, a plant seed protein of molecular weight 5000, diffract X-rays strongly to the interplanar spacing limit of 0.88 Å. These diffraction data should allow a definition of atomic structure that is on a par with that typically obtained from crystals of small organic molecules. The crystals are in space group P2₁ and have unit cell dimensions $\text{a = 41.1}\text{A}\text{?}\text{, b = 18.7}\text{A}\text{?}\text{, c = 22·7}\text{A}\text{?}\text{,}\text{and}\text{β = 90.6 °}$. The asymmetric unit contains one protein molecule.