Crystal structures of A-DNA duplexes

All crystal structures of A-DNA duplexes exhibit a typical crystal packing, with the termini of one molecule abutting the shallow grooves of symmetry related neighbors, while all other forms (B, Z, and RNA) tend to form infinitely stacked helices. The A-DNA arrangement leads to the formation of shallow groove base multiples that have implications for the structure of DNA in compacted states. The characteristic packing leaves big solvent channels, which can be sometimes occupied by B-DNA duplexes. Comparisons of the structures of the same oligomer crystallizing in two different space groups and of different sequences crystallizing in the same space group show that the lattice forces dominate the A-DNA conformation in the crystals, complicating the effort to elucidate the influence of the base sequence on the structures. Nevertheless, in both alternating and nonalternating fragments some sequence effects can still be uncovered. Furthermore, several studies have started to define the minimal sequence changes or chemical modifications that can interconvert the oligomers between different double-helical conformers (A-, B-, and Z-form). Overall, it is seen that the rigid nucleotide principle applies to the oligomeric fragments. Besides the structures of the naked DNAs, their interactions with water, polyamines, and metal ions have attracted considerable attention. There are conserved patterns in the hydration, involving both the grooves and the backbone, which are different from those of B-DNA or Z-DNA. Overall, A-DNA seems to be more economically hydrated than B-DNA, particularly around the sugar-phosphate backbone. Spermine was found to be able to bind exclusively to either of the grooves or to the phosphate groups of the backbone, or exhibit a mixed binding mode. The located metal cations prefer binding to guanine bases and phosphate groups. The only mispairs investigated in A-DNA are the wobble pairs, yielding structural insight into their effects on helix stabilities and hydration. G · T wobble pairs have been determined in various sequence contexts, where they differentially affect the conformations and stableness of the duplexes. The structure of a G · ^m5C base pair, which surprisingly also adopted the wobble conformation, suggests that a similar geometry may transiently exist for G · C pairs. These results from the crystalline state will be compared to the solution state and discussed in relation to their relevance in biology. © 1997 John Wiley & Sons, Inc. Biopoly 44: 45–63, 1997     

The binding of precipitant ions in the tetragonal crystals of hen egg white lysozyme

Abstract

The bonds between lysozyme molecules and precipitant ions in single crystals grown with chlorides of several metals are analysed on the basis of crystal structure data. Crystals of tetragonal hen egg lysozyme (HEWL) were grown with chlorides of several alkali and transition metals (LiCl, NaCl, KCl, NiCl₂ and CuCl₂) as precipitants and the three-dimensional structures were determined at 1.35?Å resolution by X-ray diffraction method. The positions of metal and chloride ions attached to the protein were located, divided into three groups and analysed. Some of them, in accordance with the recently proposed and experimentally confirmed crystal growth model, provide connections in protein dimers and octamers that are precursor clusters in the crystallization lysozyme solution. The first group, including Cu⁺², Ni⁺² and Na⁺¹ cations, binds specifically to the protein molecule. The second group consists of metal and chloride ions bound inside the dimers and octamers. The third group of ions can participate in connections between the octamers that are suggested as building units during the crystal growth. The arrangement of chloride and metal ions associated with lysozyme molecule at all stages of the crystallization solution formation and crystal growth is discussed.

Communicated by Ramaswamy H. Sarma     

Four-Stranded Intercalated Cytosine-Rich Molecules: Novel Insights into DNA Structure and Stability

Abstract

DNA fragments with stretches of cytosine residues can form four-stranded intercalated i-DNA molecules stabilized by hemiprotonated cytosine·cytosine⁺ (C·C⁺) base pairs. Intriguing features of this motif are the accomodation of base stacking that is unfavorable due to electrostatic repulsion and the close approach of phosphates in narrow grooves of the molecule. Unusual sources of stability in this structure involve sugar-base stacking and CH-O interribose short contacts between the backbones of adjacent strands.     

Structure of a complex between yeast hexokinase A and glucose: II. Detailed comparisons of conformation and active site configuration with the native hexokinase B monomer and dimer

Detailed comparison of the refined crystal structures of the hexokinase A: glucose complex (HKA · G) and native hexokinase B shows that, in addition to the 12 ° rotation of one lobe of the enzyme relative to the other as described previously (Bennett & Steitz, 1978) there are small systematic differences in the conformation of the polypeptide backbones of the two structures adjacent to the glucose binding site and crystal packing contacts. In the HKA · G complex, the cleft between the two lobes of the hexokinase molecule is narrowed, substantially reducing the accessibility of the active site to solvent. The HKA · G structure suggests specific contacts with a bound glucose molecule that cannot form in the more open native structure. The closed conformation of the HKA · G complex can be formed by either subunit in the heterologous dimer configuration of hexokinase B (Anderson et al. 1974); new or different interactions between subunits, or with ligands bound to the intersubunit ATP site, may be made when the upper subunit of the dimer is in the closed conformation and may contribute to the cooperative interactions observed in the crystalline dimer and in solution.     

Influence of ions, hydration, and the transcriptional inhibitor P4N on the conformations of the Sp1 binding site

Three crystal structures containing the entire Sp1 consensus sequence d(GGGGCGGGG) with two or three additional base-pairs on either the 5' or 3' ends and overhangs have been determined. Despite the different lengths of DNA in the pseudo-dodecamers and pseudo-tridecamer, all three structures form A-DNA duplexes that share a common set of crystal contacts, including a T*(G.C) base triplet and a 5'-overhang that flips out and away from the helical axes to form a Hoogsteen base-pair with the 3'-overhang of a symmetry mate. The global conformations of the three structures differ, however, in the widths of their respective major grooves, the lengths of the molecules, and the extent of crystal packing. The structures were determined from crystals grown in an unusual precipitant for A-DNA, polyethylene glycol (PEG) 400, in combination with polyamines or ions; cobalt hexamine for the pseudo-tridecamer, and spermidine for the pseudo-dodecamers. As the Sp1 binding site is a target for antiviral and anticancer drugs, pseudo-dodecamer crystals were soaked with one such antiviral and anticancer compound, P4N. Although P4N was not visualized unambiguously in the electron density maps, the effect of the drug is evident from significant differences in the lattice constants, crystal packing, and overall conformation of the structure.     

Binding of nogalamycin to model tetranucleotides

Intercalated complexes of the antitumor antibiotic nogalamycin (NGM) with the double-stranded oligonucleotides d(GCGC)₂, d(ATAT)₂, and d(ACAC) · d(GTGT) are investigated with the theoretical method SIBFA. The amino sugar part of the drug locates preferentially in the minor groove. An intrinsic preference for the d(ATAT)₂ sequence over the d(ACAC) · d(GTGT) and d(GCGC)₂ sequences is obtained, corresponding to relative energies 0, 11, and 15 kcal/mole, respectively. A mixed sugar-puckering pattern is preferred in the d(ATAT)₂ complex while a uniform sugar-puckering pattern is preferred for the other sequences. No direct specific interaction involves the N⁺—H part of protonated NGM. The location of the amino sugar as well as the sequence selectivity is due to the global electrostatic interaction of the dimethylammonium group with the given groove. The two hydroxyl groups of the amino sugar and the carbonyl of the carbomethoxy group encounter partners for hydrogen bonding at the intercalation site, but these interactions do not appear to govern the base sequence selectivity. The nogalose part is not found to be directly involved in the binding or in the selectivity. The conformations of isolated and intercalated NGM are discussed.     

Structural variability and new intermolecular interactions of Z-DNA in crystals of d(pCpGpCpGpCpG).

We have determined the single crystal x-ray structure of the synthetic DNA hexamer d(pCpGpCpGpCpG) in two different crystal forms. The hexamer pCGCGCG has the Z-DNA conformation and in both cases the asymmetric unit contains more than one Z-DNA duplex. Crystals belong to the space group C222(1) with a = 69.73, b = 52.63, and c = 26.21 A, and to the space group P2(1) with a = 49.87, b = 41.26, c = 21.91 A, and gamma = 97.12 degrees. Both crystals show new crystal packing modes. The molecules also show striking new features when compared with previously determined Z-DNA structures: 1) the bases in one duplex have a large inclination with respect to the helical axis, which alters the overall shape of the molecule. 2) Some cytosine nitrogens interact by hydrogen bonding with phosphates in neighbor molecules. Similar base-phosphate interactions had been previously detected in some B-DNA crystals. 3) Basepair stacking between the ends of neighbor molecules is variable and no helical continuity is maintained between contiguous hexamer duplexes.     

A few low-frequency normal modes predominantly contribute to conformational responses of hen egg white lysozyme in the tetragonal crystal to variations of molecular packing controlled by environmental humidity

The structures of proteins in crystals are fixed by molecular interactions with neighboring molecules, except in non-contacting flexible regions. Thus, it is difficult to imagine what conformational changes occur in solution. However, if molecular interactions can be changed by manipulating molecular packing in crystals, it may be possible to visualize conformational responses of proteins at atomic resolution by diffraction experiments. For this purpose, it is suitable to control the molecular packing in protein crystals by changing the volume of solvent channels through variation of the environmental relative humidity. Here, we studied conformational responses of hen egg white lysozyme (HEWL) in the tetragonal crystal by X-ray diffraction experiments using a humidity-control apparatus, which provided air flow of 20-98%rh at 298 K. First, we monitored the lattice parameters and crystalline order during dehydration and rehydration of HEWL crystal between 61 and 94%rh at 300 K. Then two crystal structures at a resolution of 2.1 ? using diffraction data obtained at 84.2 and 71.9%rh were determined to discuss the conformational responses of HEWL against the external perturbation induced by changes in molecular packing. The structure at 71.9%rh displayed a closure movement that was likely induced by the molecular contacts formed during dehydration and could be approximated by ten low-frequency normal modes for the crystal structure obtained at 84.2%rh. In addition, we observed reorganization of hydration structures at the molecular interfaces between symmetry neighbors. These findings suggest that humidity-controlled X-ray crystallography is an effective tool to investigate the responses of inherent intramolecular motions of proteins to external perturbations.     

Packing interface energetics in different crystal forms of the λ Cro dimer

Variation among crystal structures of the λ Cro dimer highlights conformational flexibility. The structures range from a wild type closed to a mutant fully open conformation, but it is unclear if each represents a stable solution state or if one may be the result of crystal packing. Here we use molecular dynamics (MD) simulation to investigate the energetics of crystal packing interfaces and the influence of site‐directed mutagenesis on them in order to examine the effect of crystal packing on wild type and mutant Cro dimer conformation. Replica exchange MD of mutant Cro in solution shows that the observed conformational differences between the wild type and mutant protein are not the direct consequence of mutation. Instead, simulation of Cro in different crystal environments reveals that mutation affects the stability of crystal forms. Molecular Mechanics Poisson‐Boltzmann Surface Area binding energy calculations reveal the detailed energetics of packing interfaces. Packing interfaces can have diverse properties in strength, energetic components, and some are stronger than the biological dimer interface. Further analysis shows that mutation can strengthen packing interfaces by as much as ～5 kcal/mol in either crystal environment. Thus, in the case of Cro, mutation provides an additional energetic contribution during crystal formation that may stabilize a fully open higher energy state. Moreover, the effect of mutation in the lattice can extend to packing interfaces not involving mutation sites. Our results provide insight into possible models for the effect of crystallization on Cro conformational dynamics and emphasize careful consideration of protein crystal structures. Proteins 2014; 82:1128–1141. © 2013 Wiley Periodicals, Inc.     

Crystallographic studies of drug-nucleic acid interactions: Proflavine intercalation between the non-complementary base-pairs of cytidilyl-3′,5′-adenosine

In order to get insights into the binding of dyes and mutagens with denatured and single-stranded nucleic acids and the possible implications in frameshift mutagenesis, a 1:1 complex between the non-self-complementary dinucleoside monophosphate cytidilyl-3′,5′-adenosine (CpA) and proflavine was crystallized. The crystals belong to the tetragonal space group P4₂2₁2 with cell constants $\text{a = b = 19.38(1)}\text{A}\text{?}\text{and}\text{c = 27.10(1)}\text{A}\text{?}$. The asymmetric unit contains one CpA, one proflavine and nine water molecules by weight. The structure was determined using Patterson and direct methods and refined to an R-value of 11% using 2454 diffractometer intensities.The non-self-complementary dinucleoside monophosphate CpA forms a selfpaired parallel chain dimer with a proflavine molecule intercalated between the protonated cytosine-cytosine (C · C) pair and the neutral adenine-adenine (A · A) pair. The dimer complex exhibits a right-handed helical twist and an irregular girth. The neutral A · A pair is doubly hydrogen-bonded through the N(6) and N(7) sites (C(1′)C(1′) distance: 10.97(2) Å) and the protonated C · C pair is triply hydrogen-bonded with a proton shared between the N(3) sites (C(1′)C(1′) distance: 9.59(2) Å). To accommodate the intercalating dye, the sugars of successive nucleotide residues adopt the two fundamental conformations (5′ end: 3′-endo, 3′ end: 2′-endo), the backbone adopts torsion angle values that fluctuate within their preferred conformational domains: the PO bonds (ω, ω′) adopt the characteristic helical (gauche^?-gauche^?) conformation, the CO bonds (φ, φ′) are both in the trans domain and the C(4′)C(5′) bonds (ψ) are in the gauche⁺ region. The bases of both residues are disposed in the preferred anti domain with the glycosyl torsion angles (χ) correlated to the puckering mode of the sugar so that the cytidine residue is C(3′)-endo, low χ (12 dg), and the adenosine residue is C(2′)-endo, high χ (84 °). The intercalated proflavine stacks more extensively with the C · C pair than the A · A pair. Between 4₂-related CpA proflavine units there is a second proflavine which stacks well with both the A · A and the C · C pairs sandwiching it. Both proflavine molecules are positionally disordered. In each of its two disordered sites, the intercalated proflavine forms hydrogen-bonded interactions with only one sugar-phosphate backbone. A total of 26 water sites has been characterized of which only two are fully occupied. These hydration sites are involved in an intricate network of hydrogen bonds with both the dye and CpA and provide insights on the various modes of interactions between water molecules and between water molecules and nucleic acids.The structure of the proflavine-CpA complex shows that intercalation of planar drugs can occur between non-complementary base-pairs. This result can be relevant for understanding the strong binding of acridine dyes to denatured DNA, single-stranded RNA, and single-stranded polynucleotides. Also, the ability of proflayine to promote self-pairs of adenine and cytosine bases could provide a chemical basis for an alternative mechanism of frameshift mutagenesis.     

Crystal and Molecular Structure of the Sodium Salt of the Dinucleotide Duplex d(CpG)

Abstract

The crystal and molecular structure of the sodium salt of deoxycytidylyl-{3′ ?5′)-deoxyguanosine has been determined from X-ray diffraction data. The crystals, obtained from an aqueous y- butyrolactone solution at pH = 5.3, are orthorhombic, P2₁2₁2₁, a= 10.640(2), b= 11.184(2) and c=44.618(4) A. The structure was refined to an R = 0.041. The d(CpG) structure is similar to the ammonium salt solved by Cruse et al.(1). Both structures form a parallel self base paired mini-double helix. In d(CpG).Na⁺, one of the two paired cytosines is protonated on N(3). The cytosines form 3 hydrogen bonds while the guanines form only 2. The Na⁺ ion is coordinated with five groups: two water molecules, 0(6) of guanine A, N(7) of guanine B and 0(5′) of cytosine B, forming a square pyramid. The hydration shell around the mini-helix is analysed and compared with that of the ammonium salt. d(CpG).Na⁺ is the second d(CpG) oligonucleotide found with a self base pairing arrangement despite of the fact that the crystallization conditions and counterion were different in both cases. The hypothesis that self base pairing is not only a crystallization artifact but may play a role under physiological conditions as a source of transversion mutations is discussed.     

The absence of tertiary interactions in a self-assembled DNA crystal structure

DNA is a highly effective molecule for controlling nanometer-scale structure. The convenience of using DNA lies in the programmability of Watson-Crick base-paired secondary interactions, useful both to design branched molecular motifs and to connect them through sticky-ended cohesion. Recently, the tensegrity triangle motif has been used to self-assemble three-dimensional crystals whose structures have been determined; sticky ends were reported to be the only intermolecular cohesive elements in those crystals. A recent communication in this journal suggested that tertiary interactions between phosphates and cytosine N(4) groups are responsible for intermolecular cohesion in these crystals, in addition to the secondary and covalent interactions programmed into the motif. To resolve this issue, we report experiments challenging this contention. Gel electrophoresis demonstrates that the tensegrity triangle exists in conditions where cytosine-PO(4) tertiary interactions seem ineffective. Furthermore, we have crystallized a tensegrity triangle using a junction lacking the cytosine suggested for involvement in tertiary interactions. The unit cell is isomorphous with that of a tensegrity triangle crystal reported earlier. This structure has been solved by molecular replacement and refined. The data presented here leave no doubt that the tensegrity triangle crystal structures reported earlier depend only on base pairing and covalent interactions for their formation.     

Modification of protein crystal packing by systematic mutations of surface residues: Implications on biotemplating and crystal porosity

Bioinspired nano‐scale biotemplating for the development of novel composite materials has recently culminated in several demonstrations of nano‐structured hybrid materials. Protein crystals, routinely prepared for the elucidation of protein 3D structures by X‐ray crystallography, present an ordered and highly accurate 3D array of protein molecules. Inherent to the 3D arrangement of the protein “building blocks” in the crystal, a complementary 3D array of interconnected cavities—voids array, exhibiting highly ordered porosity is formed. The porous arrays of protein crystal may serve as a nano‐structured, accurate biotemplate by a “filling” process. These cavities arrays are shaped by the mode of protein packing throughout the crystallization process. Here we propose and demonstrate feasibility of targeting site specific mutations to modify protein's surface to affect protein crystal packing, enabling the generation of a series of protein crystal “biotemplates” all originating from same parent protein. The selection of these modification sites was based on in silico analysis of protein–protein interface contact areas in the parent crystal. The model protein selected for this study was the N‐terminal type II cohesin from the cellulosomal scaffold in ScaB subunit of Acetivibrio cellulolyticus and mutations were focused on lysine residues involved in protein packing as prime target. The impact of systematically mutating these lysine residues on protein packing and its resulting interconnected cavities array were found to be most significant when surface lysine residues were substituted to tryptophan residues. Our results demonstrate the feasibility of using pre‐designed site directed mutations for the generation of a series of protein crystal biotemplates from a “parent” protein. Biotechnol. Bioeng. 2009; 104: 444–457 © 2009 Wiley Periodicals, Inc.     

Packing forces in nine crystal forms of cutinase

During the characterization of mutants and covalently inhibited complexes of Fusarium solani cutinase, nine different crystal forms have been obtained so far. Protein mutants with a different surface charge distribution form new intermolecular salt bridges or long-range electrostatic interactions that are accompanied by a change in the crystal packing. The whole protein surface is involved in the packing contacts and the hydrophobicities of the protein surfaces in mutual contact turned out to be noncorrelated, which indicates that the packing interactions are nonspecific. In the case of the hydrophobic variants, the packing contacts showed some specificity, as the protein in the crystal tends to form either crystallographic or noncrystallographic dimers, which shield the hydrophobic surface from the solvent. The likelihood of surface atoms to be involved in a crystal contact is the same for both polar and nonpolar atoms. However, when taking areas in the 200–600 Ų range, instead of individual atoms, the either highly hydrophobic or highly polar surface regions were found to have an increased probability of establishing crystal lattice contacts. The protein surface surrounding the active-site crevice of cutinase constitutes a large hydrophobic area that is involved in packing contacts in all the various crystalline contexts. Proteins 31:320–333, 1998. © 1998 Wiley-Liss, Inc.     

Control of crystal forms of apoferritin by site-directed mutagenesis

Surface charges of protein molecules are not only important to biological functions but also crucial to the molecular assembly responsible for crystallization. Appropriate alteration in the surface charge distribution of a protein molecule induces new molecular alignment in the proper direction in the crystal and, hence, controls the crystal form. Apoferritin molecules are known to crystallize in two- and three-dimensional forms in the presence of cadmium ions, which bridge neighboring protein molecules. Here we report a controlled transformation of the apoferritin 2-D crystal by site-directed mutagenesis. In mutant apoferritin, two amino acid residues binding a cadmium-ion through their negative charge, were replaced by one type of nonionic amino acid residues. The amino acid residues, Asp-84 and Gln-86 in the sequence of recombinant (i.e., wild-type) horse L -apoferritin, were replaced by Ser. The wild-type apoferritin yielded a hexagonal lattice 2-D crystal in the presence of cadmium ions. In contrast, the mutant apoferritin yielded two types of oblique crystals independent of the presence of cadmium ions. Image reconstruction of electron micrographs of the mutant crystals made clear that the mutant apoferritin molecules oriented themselves with the 2-fold symmetry axis perpendicular to the crystal plane in both crystals, while the wild-type apoferritin molecules oriented themselves with the 3-fold symmetry axis perpendicular to the crystal plane. The changes of crystal forms and molecular orientation in the 2-D crystals were well explained by a change of the electrostatic interactions induced by the mutagenesis. © 1995 Wiley-Liss, Inc.     

A novel form of intercalation involving four DNA duplexes in an acridine-4-carboxamide complex of d(CGTACG)(2)

The structures of the complexes formed between 9-amino-[N-(2-dimethyl-amino)butyl]acridine-4-carboxamide and d(CG^5BrUACG)₂ and d(CGTACG)₂ have been solved by X-ray crystallography using MAD phasing methodology and refined to a resolution of 1.6 Å. The complexes crystallised in space group C222. An asymmetric unit in the brominated complex comprises two strands of DNA, one disordered drug molecule, two cobalt (II) ions and 19 water molecules (31 in the native complex). Asymmetric units in the native complex also contain a sodium ion. The structures exhibit novel features not previously observed in crystals of DNA/drug complexes. The DNA helices stack in continuous columns with their central 4 bp adopting a B-like motif. However, despite being a palindromic sequence, the terminal GC base pairs engage in quite different interactions. At one end of the duplex there is a CpG dinucleotide overlap modified by ligand intercalation and terminal cytosine exchange between symmetry-related duplexes. A novel intercalation complex is formed involving four DNA duplexes, four ligand molecules and two pairs of base tetrads. The other end of the DNA is frayed with the terminal guanine lying in the minor groove of the next duplex in the column. The structure is stabilised by guanine N7/cobalt (II) coordination. We discuss our findings with respect to the effects of packing forces on DNA crystal structure, and the potential effects of intercalating agents on biochemical processes involving DNA quadruplexes and strand exchanges. NDB accession numbers: DD0032 (brominated) and DD0033 (native).     

Crystal structure of a tripeptide containing aminocyclododecane carboxylic acid: a supramolecular twisted parallel β‐sheet in crystals

The crystal structure of a tripeptide Boc‐Leu‐Val‐Ac₁₂c‐OMe ( 1 ) is determined, which incorporates a bulky 1‐aminocyclododecane‐1‐carboxylic acid (Ac₁₂c) side chain. The peptide adopts a semi‐extended backbone conformation for Leu and Val residues, while the backbone torsion angles of the C^α,α‐dialkylated residue Ac₁₂c are in the helical region of the Ramachandran map. The molecular packing of 1 revealed a unique supramolecular twisted parallel β‐sheet coiling into a helical architecture in crystals, with the bulky hydrophobic Ac₁₂c side chains projecting outward the helical column. This arrangement resembles the packing of peptide helices in crystal structures. Although short oligopeptides often assemble as parallel or anti‐parallel β‐sheet in crystals, twisted or helical β‐sheet formation has been observed in a few examples of dipeptide crystal structures. Peptide 1 presents the first example of a tripeptide showing twisted β‐sheet assembly in crystals. Copyright © 2016 European Peptide Society and John Wiley & Sons, Ltd.     

Variability of conformations at crystal contacts in BPTI represent true low-energy structures: correspondence among lattice packing and molecular dynamics structures.

The structures of five basic pancreatic trypsin inhibitor (BPTI) molecules are compared to establish the extent and nature of the conformational variability resulting from crystal packing effects. BPTI is an ideal system to evaluate such factors because of the availability of high resolution X-ray models of five different BPTI structures, each in a different crystal packing environment. Differences observed among the structures are found to be distributed throughout the molecule, although the regions that display most variability are associated with the loop structures (residues 14-17 and 24-29). The regions of structure that show the largest rms deviations from the mean of the five packing motifs correlate well with the presence of intermolecular contacts in the crystal lattice. For most of the molecules there is also a correspondence between a larger number of intermolecular contacts and systematically higher B-factors, although it is not apparent whether this is induced by the crystal contact or results from the fact that the contacts are made predominantly through surface loops. The conformational differences seen among the X-ray models constitute more than local shifts at the lattice contact surfaces, and in fact involve in some cases the making and breaking of intramolecular H-bonds. The magnitudes of the differences among packing models are significantly larger than those usually associated with changes induced by mutagenesis; for instance; the structural differences at the site of mutation observed on removing an internal disulfide from the molecule are significantly less than those associated with lattice contact effects. The crystal packing conformations are compared to representative structures of BPTI generated during a 96-psec molecular dynamics (MD) simulation. This comparison shows a high level of correspondence between the protein flexibility indicated by the X-ray and MD analyses, and specifically between those regions that are most variable. This suggests that the regions that show most variability among the crystal packing models are not artifacts of crystallization, but rather represent true low-energy conformers that have been preferentially selected by crystallization factors.     

Interactions and space requirement of the phosphate head group of membrane lipids: The single crystal structures of a triclinic and a monoclinic form of hexadecyl-2-deoxyglycerophosphoric acid monohydrate

The crystal structures of a triclinic form (HPA1) and a monoclinic form (HPA2) of hexadecyl-2-deoxyglycerophosphoric acid monohydrate were determined by single crystal analysis. The unit cell dimensions for HPA1 are $\text{a = 4.75, b = 5.72, c = 44.36}\text{A}\text{?}$ and α = 91.0, β = 101.5, γ = 100.5° (P$\text{1}$) and for HPA2, $\text{a = 4.75, b = 5.72, c = 88.72}\text{A}\text{?}$ and γ = 100.8° (P2₁). In both structures the molecules are fully extended and pack tail-to-tail in bilayers with tilting (47°) hydrocarbon chains. In HPA2, however, the chain tilt alternatingly changes direction in adjacent bilayers, giving rise to a doubled unit cell which spans two bilayers. The dihydrogen phosphate groups interact by hydrogen bonds and are arranged in rows. Laterally between these phosphate rows the water molecules are accommodated producing a compact two-dimensional network of hydrogen bonds. The packing cross-section in the layer plane of the dihydrogen phosphate monohydrate group is 26.7 Ų in both structures. The hydrocarbon chains pack according to the triclinic (T|) chain packing mode. In HPA2, however, the chain packing is somewhat less compact with accounts for a 2% increase in the molecular volume. In both structures the ether oxygen is accommodated into the hydrocarbon matrix without distortion of the chain packing.