Transition processes in stratum corneum model lipid membranes with a mixture of free fatty acids

The hydration of model membranes based on ceramide 6 with a mixture of free fatty acids most commonly encountered in the native lipid matrix of stratum corneum, the outermost layer of the mammalian skin, has been studied by neutron diffraction. Membrane hydration with water vapor at a temperature of 25°C is characterized by a small increase in the repeat distance Δd ₀ = 1.0 Å, which is comparable with membrane swelling in the presence of excess water. The kinetics of changes in the repeat distance, connected with an increase of the water layer between bilayers during hydration, and water exchange during the processes of hydration and H-D isotopic substitution, consists of a fast initial and a subsequent slow stage and is well described by exponentials with two characteristic times lying in the range from a few tens of minutes to several hundreds of minutes. During hydration at a temperature of 57°C, the repeat distance increases by Δd ₀ = 1.6 Å, after which the membrane irreversibly separates into two phases. One of the phases is formed mainly by long-chain free fatty acids and is characterized by a large decrease in the repeat distance Δd _ph = 8.3 Å on dehydration. The investigation of the structure of model membranes in the temperature range 20–72°C indicated that the system with 20% (w) of cholesterol in the range of 63–67°C undergoes a structural phase transition caused by the melting of hydrocarbon chains of lipids. In the system with a smaller content of cholesterol, no phase transition was observed up to a temperature of 72°C.     

Dye permeability at phase transitions in single and binary component phospholipid bilayers

By encapsulating a pH-sensitive dye, phenol red, in multilamellar liposomes of DMPC, DPPC and DMPC/DPPC mixtures, the permeability of these phospholipid bilayers to dye as a function of temperature has been studied. For both DMPC and DPPC liposomes, dye release begins well below the main gel-to-liquid-crystalline phase transition (24°C and 42°C, respectively) at temperatures corresponding to the onset of the pretransition (about 14°C and 36°C, respectively) with DPPC liposomes exhibiting a permeability anomaly at the main phase transition (42°C). The perturbation occurring in the bilayer structure that allows the release of encapsulated phenol red (approx. 5 Å diameter) is not sufficient to permit the release of encapsulated haemoglobin (approx. 20 Å diameter, negatively charged). In liposomes composed of a range of DMPC/DPPC mixtures, dye release commences at the onset of the pretransition range (determined by optical absorbance measurements) and increases with increasing temperature until the first appearance of liquid crystalline phase after which no further dye release occurs. Interestingly, the dye retaining properties of DMPC and DPPC liposomes well below their respective pretransition temperature regions are very different: DMPC liposomes release much encapsulated dye at incubation temperatures of 5°C whilst DPPC liposomes do not.     

Monitoring Phase Transformations in Intact Tablets of Trehalose by FT-Raman Spectroscopy

The purpose of this study is to monitor phase transformations in intact trehalose tablets using FT-Raman spectroscopy. Tablets of trehalose dihydrate, amorphous trehalose (obtained by freeze-drying aqueous trehalose solutions), and anhydrous trehalose (β-trehalose) were prepared. The tablets were exposed to different conditions [11% and 0% RH (60°C); 75% RH (25°C)] and monitored periodically over 96 h using Raman spectroscopy. Within 96 h of storage, the following phase transformations were observed: (1) trehalose dihydrate → β-trehalose (11% RH, 60°C), (2) trehalose dihydrate → α-trehalose (0% RH, 60°C), (3) β-trehalose → trehalose dihydrate (75% RH, 25°C), and (4) amorphous trehalose → trehalose dihydrate (75% RH, 25°C). FT-Raman spectroscopy was a useful technique to identify the solid form and monitor multiple-phase transformations in intact trehalose tablets stored at different conditions.     

Temperature-induced transitions in the structure and interfacial rheology of human meibum

Meibomian lipids are the primary component of the lipid layer of the tear film. Composed primarily of a mixture of lipids, meibum exhibits a range of melt temperatures. Compositional changes that occur with disease may alter the temperature at which meibum melts. Here we explore how the mechanical properties and structure of meibum from healthy subjects depend on temperature. Interfacial films of meibum were highly viscoelastic at 17°C, but as the films were heated to 30°C the surface moduli decreased by more than two orders of magnitude. Brewster angle microscopy revealed the presence of micron-scale inhomogeneities in meibum films at higher temperatures. Crystalline structure was probed by small angle x-ray scattering of bulk meibum, which showed evidence of a majority crystalline structure in all samples with lamellar spacing of 49 Å that melted at 34°C. A minority structure was observed in some samples with d-spacing at 110 Å that persisted up to 40°C. The melting of crystalline phases accompanied by a reduction in interfacial viscosity and elasticity has implications in meibum behavior in the tear film. If the melt temperature of meibum was altered significantly from disease-induced compositional changes, the resultant change in viscosity could alter secretion of lipids from meibomian glands, or tear-film stabilization properties of the lipid layer.     

Phase properties of binary mixtures of monogalactosyldiacylglycerols differing in hydrocarbon chain substituents dispersed in aqueous systems

Monogalactosyldiacylglycerols isolated from spinach leaves contain a high proportion of polyunsaturated fatty acyl substituents and form hexagonal-II structures when dispersed in excess water. Catalytic hydrogenation of the lipid in the presence of Adam's catalyst completely saturates the hydrocarbon chains and the lipid forms typical open sheet bilayer structures in water at 20°C. Binary mixtures of the native and hydrogenated lipid tend to phase separate at 20°C. Freeze-fracture electron microscopy reveals lamellar phase lipid indispersed with regions of hexagonal-II structure and the proportions of each reflect the composition of the mixture. X-ray diffraction in both wide- and low-angle regions show that the saturated lipid forms the typical stable gel-phase structure in mixtures that are allowed to equilibrate over three days at 20°C. The phase transition behaviour of binary mixtures of the two galactolipids was investigated by differential scanning calorimetry and fluorescence probe methods. Thermal studies indicate that the phase-separated gel structure undergoes an anomalous transition compared with the saturated pure lipid in that the transition temperature is reduced from about 57°C to 41°C and the enthalpy of the transition is also somewhat reduced. Furthermore, the transition appears to involve the conversion of the completely phase-separated system into bilayer coexisting with phases intermediate between bilayer and hexagonal-II. A homogeneous hexagonal-II phase is presumably formed at higher temperatures. The thermal and structural studies were consistent with fluorescence polarization measurements of 1,6-diphenyl-1,3,5-hexatriene interpolated into the hydrocarbon domain of the structure.     

The ternary phase diagram of lecithin, cholesteryl linolenate and water: phase behavior and structure

The ternary phase diagram of cholesteryl linolenate-egg lecithin-water has been determined by polarizing light microscopy, calorimetry and X-ray diffraction at 23 °C. Hydrated lecithin forms a lamellar liquid-crystalline structure into which small amounts of cholesteryl linolenate are incorporated. The maximum incorporation of cholesterol ester into this lamellar structure varies with the degree of hydration. Increasing the water concentration from 10 to 15% (w/w) increased the limiting molar ratio of cholesteryl linolenate to lecithin in the lamellar phase from 1:50 to 1:22. At intermediate concentrations (15 to 30% water) the cholesteryl linolenate:lecithin ratio remains constant at 1:22. When water is increased to 42.5%, the maximum water content in the lamellar phase, the molar ratio decreased to 1:32. At low water concentrations the cholesterol ester appears to be entirely in the apolar region of the lecithin bilayer, while at higher water concentrations the ester groups of cholesteryl linolenate may be located at the lipid-water interface. At high water concentrations the ester appears to disorder the alkyl chains of the lecithin, giving rise to a thinner lipid layer and an increased surface area per lipid molecule when compared to the lecithin-water system in the absence of cholesteryl linolenate.The lamellar phase is the only phase (except at water concentrations less than 5%) in which all three components mutually interact. All mixtures of the three components having compositions outside the one-phase (lamellar) zone produce additional phases of cholesteryl linolenate or water, or both. Between 23 °C and 60 °C only minor changes in the phase diagram are observed.     

Structure of β,D(1–>4′)-xylan hydrate

A structure is proposed for xylan hydrate as a result of investigations by x-ray fiber diffraction and computer-aided chain-packing methods. The unit-cell dimensions are a = b = 9.16 Å, c (fiber axis) = 14.85Å, γ = 120° and the proposed anti-parallel chain arrangement corresponds to a space group symmetry of P3₂21. Left-handed threefold screw helices are stabilized in this conformation by their interaction with chains of water molecules, so that a satisfactory hydrogen-bonding scheme is achieved. The proposed structure provides an explanation of the changes in the x-ray diagram with relative humidity and yields a very good structure factors agreement. An x-ray fiber diagram corresponding to a higher hydrate (xylan dihydrate) is presented. Comments are made on the possible role of xylan in nature and in technological processes.     

Structure of the complex formed by bovine trypsin and bovine pancreatic trypsin inhibitor. II. Crystallographic refinement at 1.9 A resolution

The crystal structure of the complex formed by bovine trypsin and bovine pancreatic trypsin inhibitor has been refined with data to 1.9 Å resolution, using a procedure described by Deisenhofer &; Steigemann (1974) in their refinement of the crystal structure of the free inhibitor. This procedure involves cycles consisting of phase calculation using the current atomic model, Fourier synthesis using these phases and the observed structure factor amplitudes and Diamond's real-space refinement (Diamond, 1971,1974). At various stages, difference Fourier syntheses are calculated to detect and correct gross errors in the model and to localize solvent molecules.The refinement progressed smoothly, starting with the model obtained from the isomorphous Fourier map at 2.6 Å resolution. The R-factor is 0.23 for 20,500 significantly measured reflections to 1.9 Å resolution, using an over-all temperature factor of 20 Ų. The estimated standard deviation of atomic positions is 0.09 Å.An objective assessment of the upper limit of the error in the atomic coordinates of the final model is possible by comparing the inhibitor component in the model of the complex with the refined structure of the free inhibitor (Deisenhofer &; Steigemann, 1974). The mean deviation of main-chain atoms of the two molecular models in internal segments is 0.25 Å, of main-chain dihedral angles 5.1 ° and side-chain dihedral angles 6.5 °.A comparison of the trypsin component with α-chymotrypsin (Birktoft &; Blow, 1972) showed a mean deviation of main-chain atoms of 0.75 Å. The structures are closely similar and the various deletions and insertions cause local structural differences only.     

Effect of storage time and temperature on steroid and protein hormone concentrations in porcine plasma and serum

The effect of storage time and temperature of porcine blood prior to quantitation of hormone concentrations by radioimmunoassay (RIA) was evaluated. Blood from each of four luteal phase gilts was used to determine cortisol (CS) and progesterone (P) concentrations, while blood from each of four ovariectomized gilts and each of four lactating sows was used to determine luteinizing hormore (LH) and prolactin (PRL) concentrations, respectively. Blood was collected via jugular puncture from each animal within a 30-sec time period and placed into 18 heparinized and 18 nonheparinized tubes. One sample with and without heparin was stored in ice water (4°C) or at 28°C for 0.25, 2, 4, 6, 8, 12, 24, 36 or 48 hours. After storage, blood was centrifuged at 4°C and plasma or serum was collected and stored at ?20°C until quantitated by RIA. There were no differences (P>0.05) between plasma and serum concentrations (X ± SE, ng/ml) of CS (26.9 ± 0.8 vs 28.5 ± 0.8), P (24.7 ± 0.7 vs 24.8 ± 0.8), LH (2.1 ± 0.1 vs 2.2 ± 0.1) or PRL (53.2 ± 2.3 vs 52.6 ± 2.1). Similarly, storage temperature (4 vs 28°C) did not affect the concentrations of P (25.7 ± 0.8 vs 23.9 ± 0.7), LH (2.2 ± 0.1 vs 2.2 ± 0.1) or PRL (53.7 ± 2.1 vs 53.2 ± 2.3). Howver, CS concentrations decreased (P<0.05) from 28.5 ± 0.5 (4°C) to 26.9 ± 0.8 ng/ml (28°C). There was an animla x time interaction for CS concentration when plasma and serum were stored at both 4°C (P<0.001) and 28°C (P<0.003). There was also and animal x time interaction (P<0.03) for LH concentrations. The P and PRL concentrations decreased linearly by 0.0615 ng/hr (P<0.001) and 0.0625 ng/hr (P<0.004), respectively, with increased storage time.     

Protein structure refinement: Streptomyces griseus serine protease A at 1.8 A resolution.

The crystal structure of the bacterial serine protease from Streptomyces griseus (SGPA) has been refined at 1.8 Å resolution by a restrained parameter least-squares procedure (Konnert, 1976) to a conventional R factor of 0.139 for 12662 statistically significant reflections [I > 3σ(I)]. The number of variable parameters in the final model was 5912 which included positional and individual thermal parameters of the enzyme, and positions, B factors and occupancies of 175 solvent molecules. The algorithm used for this refinement allows for the simultaneous restraint on bond distances and distances related to interbond angles, the coplanarity of atoms in planar groups, the conservation of chirality of asymmetric centres, non-bonded contact distances, conformational torsional angles and individual isotropic temperature factors.The refined structure of SGPA differs from ideal bond lengths by an overall root-mean-square deviation of 0.02 Å; the corresponding value for angle distances is 0.038 Å. Comparison of the phase angles for the shell of data, 8.0 to 2.8 Å, between the multiple isomorphous replacement phases (Brayer et al., 1978a) and the refined phases, indicates an overall difference (r.m.s.) of 56.6 °. The average conformational angle of the peptide bond (ω) is 179.7 ° (root-mean-square deviation ± 2.5 °) for the 180 peptide bonds of SGPA. Of the 175 solvent molecules included during the course of the refinement, 22 with occupancies ranging from 1.00 to 0.38 are located in the active site and the substrate binding region. It was not until these water molecules were included in the refinement process that the active Ser195 adopted its final conformation (χ¹ = ?77 °). The resulting distance from O^γ of Ser195 to N^ε2 of His57 is 3.1 Å, which, when taken with the observed distortion from linearity (50 °), indicates a rather weak interaction.     

Lamellar dispersion and phase separation of chloroplast membrane lipids by negative staining electron microscopy

Aqueous dispersions of lipids isolated from spinach chloroplast membranes were studied by electron microscopy after negative staining with phosphotungstic acid. Influence of low temperature (5°C for 24 h) was also investigated. It was observed that when contacted with water, these lipids, as such, formed multilamellar structures. Upon sonication, these multilamellar structures gave rise to a clear suspension of unilamellar vesicles varying in size (diameter) between 250 and 750 Å. When samples of sonicated unilamellar vesicles were stored at 5°C for 24 h or more, they revealed a variety of lipid aggregates including liposomes, cylindrical rods (about 100 Å wide and up to 3600 Å long), and spherical micellar structures (100–200 Å in diameter)—thus indicating phase separation of lipids.     

Charge-induced tilt in ordered-phase phosphatidylglycerol bilayers Evidence from x-ray diffraction

X-ray diffraction studies have been performed, as a function of water content, on dipalmitoyl phosphatidyl-glycerol bilayers, both in the charged state at pH 8.0 and in the protonated state at pH 1.5, using buffers of 1.5 M salt concentration. Measurements were made at 20°C, and the high-angle reflections indicated that the bilayers were in the ordered phase at both pH values. Lamellar diffractions were observed under all conditions studied. The lamellar repeat reached a limiting value of 62.4 Å (6.24 nm) at a water/lipid ratio of 0.24 at pH 8.0, and a limiting value of 67.3 Å (6.73 nm) at a water/lipid ratio of 0.22 at pH 1.5. The area per lipid molecule in the plane of the bilayer, deduced from the bilayer thickness and the lipid partial specific volume, is 48 Ų (0.48 nm²) at pH 8.0 and 37 Ų (0.37 nm²) at pH 1.5. The area per molecule in the plane perpendicular to the chain axes, deduced from the X-ray short spacings, is 40.5 Ų (0.405 nm²) at pH 8.0 and 39.2 Ų (0.392 nm²) at pH 1.5. Thus the lipid molecules are tilted by approx. 30° relative to the bilayer normal at pH 8.0, but are not essentially untilted at pH 1.5.     

Molecular and crystal structure of hexaaquamanganese(II) bis{bis(N-salicylideneglycinato)manganate(III)} dihydrate, [MnII(H2O)6][MnIII(Sal = Gly)2]2·2H2O

The crystal structure of hexaaquamanganese(II) bis{bis(N-salicylideneglycinato)manganate(III)} dihydrate has been determined by X-ray analysis. The complex crystallizes in the monoclinic space group I2|a, with unit-cell dimensions a = 37.431(5), b = 12.100(1), c = 9.448(1) Å, β = 92.31(1)°. The structure was deduced by the direct method and refined by the block-diagonal least-squares technique to a final R value of 0.062 for 3904 observed reflections. The Mn(II) is octahedrally ligated by six water molecules, while Mn(III) is octahedrally chelated by two salicylideneglycinate ligands, of which one is nearly planar and the other considerably bent.It was discovered that the crystal is, as a whole, of a ‘sandwich’ structure made of one central sheet containing hexaaquamanganese(II)'s and the water molecules of crystallization, and two outside sheets containing bis(N-salicylideneglycinato)manganate(III)'s.     

Proline Metabolism and Cross-Tolerance to Salinity and Heat Stress in Germinating Wheat Seeds

Germination/growth of wheat (Triticum aestivum L., cv. Zimai 1) seeds and changes in the levels of proline and protein as well as in activities of key enzymes involved in proline metabolism in response to salinity-, heat-stresses and their cross-stress were studied. With decreasing water potential caused by increasing concentrations of NaCl, germination percentage, fresh weight of seedlings and protein amount markedly decreased, whereas proline amount slightly increased. The activities of pyrroline-5-carboxylate synthetase (P5CS), ornithine aminotransferase (OAT), and proline dehydrogenase (PDH) peaked at ?0.2 MPa water potential. Germination percentage and amounts of proline and protein increased as germination temperature elevated to 25°C from 15°C, and decreased above 25°C; fresh weight of seedlings increased to 30°C from 15°C, and decreased above 30°C. However, the activities of P5CS, OAT and PDH gradually decreased with elevaing temperature. Seeds pretreated at 33°C or in ?0.8 MPa NaCl solution for various time length increased tolerance to subsequent salt + water stress or heat stress, as measured by germination percentage and fresh weight of seedlings 5 days after beginning of experiment. The acquisition of cross-tolerance resulting in limitation of negative stress effects does not relate directly to proline level and activities of P5CS, OAT and PDH involved in proline metabolism. Proline amount as measured four days or later after stress imposition cannot be considered a symptom of salt-, water- and heat-stress injury or an indicator of the resistance.     

Structure of GlyGly peptide in the crystalline state as studied by X-ray diffraction and solid state 13C-NMR methods

A new type of crystal of glycylglycine (GlyGly) hydrate was crystallized from an aqueous solution, and the structure of the crystal has been determined by x-ray diffraction. The crystal is monoclinic, and the space group is C2/c, with the cell constants of a = 15.941(2) Å, b = 4.774(2) Å, c = 19.428(2) Å and β = 109.884(7)° at 296 K. There are eight GlyGly molecules and six water solvent in the cell. The GlyGly molecules are packed in a parallel β-sheet arrangement. The single crystal was obtained with a maximum size of 10 × 7 × 4 mm and is not stable under atmospheric conditions. The transparent crystal turned to turbid with the elapse of time. The isotropic ¹³C chemical shifts obtained from the ¹³C cross polarization magic angle spinning nmr experiments reveal that GlyGly hydrate was changed into GlyGly (form α) by dehydration. © 1998 John Wiley & Sons, Inc. Biopoly 45: 333–339, 1998     

Reconstitution of collagen-fold structure with stretching of gelatin film

The gelatin film is stretched more 100% over 75% relative humidity, while the dried gelatin extended only several percent. In this experiment the gelatin film was stretched in a solution of water and ethanol. The sample was extended to 650% of its initial length when ethanol/water was 1.5(w/w) at 30°C. The wide-angle X-ray diffraction photographs of drawn samples showed the three important layer lines with approximate spacing of 10 Å, 4 Å, and 3 Å, which verify the reconstitution of collagen triple helical structure. The sharp spots appeared near 10 Å on the equatirial axis, indicating the high orientation of peptide chains. These patterns become sharp and clear on increasing the extension ratio. The content of the triple helix was investigated by wide-angle X-ray diffraction and differential scanning calorimetry. The maximum renaturation percentage is 25% at the draw ratio of 7.5. Since the formation of a collagen triple helix requires three chains, in which each chain has only three repeatin amino acids, (Gly-Pro-X)_n, and glycoprotein and other impurities interrupt helix formation, the more advanced renaturation will not be expected.     

Temperature management strategy for efficient gene expression in a thermally inducible <Emphasis Type="Italic">Escherichia coli</Emphasis>/bacteriophage system

In a two-phase operation, E. coli containing λSNNU1 (Q ⁻ S ⁻) in the chromosome is typically cultured at 33°C and cloned gene expression is induced by elevating the temperature. At least 40°C is necessary for complete induction of cloned gene expression; however, temperatures above 40°C have been shown to inhibit cloned gene expression. This suggests that a three-phase operation, which has an induction phase between the growth and production phases, may result in higher gene expression. In this study, optimal temperature management strategies were investigated for the three-phase operation of cloned gene expression in thermally inducible E. coli/bacteriophage systems. The optimal temperature for the induction phase was determined to be 40°C. When the temperature of the production stage was 33°C, the optimal time period for the induction phase at 40°C was determined to be 60 min. In contrast, when the temperature of the production phase was 37°C, the optimal period for the induction phase at 40°C was 20∼30 min. When the three-phase temperature and temporal profile were set at a growth phase of 33°C, an induction phase at 40°C for 30 min, and a production phase at 37°C, the highest level of cloned gene expression was achieved.     

Neutron diffraction studies of oral stratum corneum model lipid membranes

In this work we have investigated model lipid mixtures simulating a lipid component of oral stratum corneum (OSC). Neutron diffraction experiments on oriented samples have revealed that SM (bovine brain)/dipalmitoylphosphatidylethanolamine/dipalmitoylphosphatidylcholine (DPPE/DPPC) mixtures at molar ratios of 1/2/1 and 1/1/1 are one-phase membranes. The incorporation of low concentrations of ceramide 6 and cholesterol into SM/DPPC/DPPE bilayers does not result in a phase separation, affecting membrane hydration. The model OSC membrane composed of ceramide 6/cholesterol/fatty acids/cholesterol sulfate/SM (bovine brain)/DPPE/DPPC is characterized by coexistence of several lamellar phases, that behave differently during their hydration in water excess. The phase with lamellar repeat distance of about 45 Å is likely a ceramide-rich phase and shows a restricted swelling in water, while another phase with repeat distance of 50 Å swells very quickly on 15 Å and then disappears. Our results indicate that phospholipid-rich and ceramide-rich domains could possibly coexist in the intercellular space of oral epithelium.     

Refinement of human lysozyme at 1.5 Å resolution analysis of non-bonded and hydrogen-bond interactions

The structure of human lysozyme has been crystallographically refined at 1.5 Å resolution by difference map and restrained least-squares procedures to an R factor of 0.187. A comprehensive analysis of the non-bonded and hydrogen-bonded contacts in the lysozyme molecule, which were not restrained, revealed by the refinement has been carried out. The non-bonded CC contacts begin at ~3.45 Å, and the shorter contacts are dominated, as expected, by interactions between trigonal and tetrahedral carbon atoms. The CO contact distances have a “foot” at 3.05 Å. The CN distance plot shows a significant peak at 3.25 Å, which results from close contact between peptide NHs and carbonyl carbons involved in N_iC′_{i ? 2} interactions in α-helices and reverse turns. The distances involving sulphur atoms discriminate SC trigonal interactions at 3.4 to 3.6 Å from SC tetrahedral interactions at 3.7 Å. All these types of non-bonded interactions show minimum distances close to standard van der Waals' separations.Analysis of hydrogen-bond distances has been carried out by using standard geometry to place hydrogen atoms and measuring the XHO distances. On this basis, there are 130 intramolecular hydrogens: 111 NHO bonds, of which 69 are between main-chain atoms, 13 between side-chain atoms and 29 between mainchain and side-chain atoms. If a cluster of four well-defined internal water molecules is included in the protein structure, there is a total of 19 OHO hydrogen bonds. The mean NO, NHO distances and HN?O angles are 2.96 ± 0.17 Å, 2.05 ± 0.18 Å and 18.5 ± 9.6 °, and the mean OO, OHO distances and HÔO angles are 2.83 ± 0.19 Å, 1.98 ± 0.26 Å and 23.8 ± 13.4 °. The distances agree well with standard values, although the hydrogen bonds are consistently more non-linear than in equivalent small molecules. An analysis of the hydrogen-bond angles at the receptor atom indicates that the α-helix, β-sheet and reverse turn have characteristic angular values. A detailed analysis of the regularity of the α-helices and reverse turns shows small but consistent differences between the α-helices in lysozyme and the current standard model, which may now need revision. Of the 21 reverse turns that include a hydrogen bond, the conformations of 19 agree very closely with four of the five standard types. We conclude that the restrained least-squares method of refinement has been validated by these analyses.     

Localization of repetitive and unique DNA sequences neighbouring the rabbit beta-globin gene

The structure of oxymyoglobin has been refined at 1·6 Å resolution, using diffractometer data collected at ?12 °C. The crystallographic R factor is 0·159, and the atomic positions are known to 0·1 Å accuracy in internal segments of the molecule.The iron atom lies 0·22(3) Å from the plane of the porphyrin, 0·25 Å closer than in deoxymyoglobin, and the F helix has moved by a similar amount. Oxygen binds to the iron in a bent, end-on arrangement, with FeOO = 115(5) ° and FeO = 1·83(6) Å. The mean FeN(porphyrin) bond length is 1·95(6) Å, 0·08 Å shorter than in deoxymyoglobin, but the difference is not significant compared to the experimental error. FeN_ε(His8F) is 2·07(6) Å, the same as in model compounds. Movements of the haem, iron, F helix and FG corner on oxygenation are similar to those found in the T-R state transition in haemoglobin, but are smaller in magnitude.