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Molecular dynamics simulations of a mixed DOPC/DOPG bilayer.

We have constructed a mixed dioleoylphosphatidylcholine (DOPC) and dioleoylphosphatidylglycerol bilayer (DOPG) bilayer utilizing MD simulations. The aim was to develop an explicit molecular model of biological membranes as a complementary technique to neutron diffraction studies that are well established within the group. A monolayer was constructed by taking a previously customized PDB file of each molecule and arranging them in a seven rows of ten molecules and duplicated and rotated to form a bilayer. The 140-molecule bilayer contained 98 DOPC molecules and 42 DOPG molecules, in a 7:3 ratio in favour of DOPC. Sodium counter ions were placed near the phosphate moiety of DOPG to counteract the negative charge of DOPG. This was representative of the lipid ratio in a sample used for neutron diffraction. The MD package GROMACS was used for confining the bilayer in a triclinic box, adding Simple Polar Charge water molecules, energy minimization (EM). The bilayer/solvent system was subjected to EM using the steepest descent method to nullify bad contacts and reduce the potential energy of the system. Subsequent MD simulation using an initial NVT (constant number of particles, volume and temperature) for a 20 ps MD run followed by a NPT (constant number of particles, pressure and temperature) was performed. Structural parameters including volume of lipid, area of lipid, order parameter of the fatty acyl carbons and electron density profiles generated by the MD simulation were verified with values obtained from experimental data of DOPC, as there are no comparable experimental data available for the mixed bilayer.

Electrons↗

Diffraction techniques for nonlamellar phases of phospholipids.

A neutron diffraction method applicable to nonlamellar phases of substrate-supported lipid membranes is described and validated. When prepared on a flat substrate, the resulting nonlamellar phases have layered symmetry which provides some advantages over powder diffraction for detailed structure determination. This approach recently led to the detection of a rhombohedral phase and a distorted hexagonal phase of lipids. Here the determination of intensity and phase information for such phases is demonstrated by application to the hexagonal phase of diphytanoyl phosphatidylcholine (DPhPC). The hexagonal symmetry is used to verify the data reduction procedure for the intensities of the diffraction peaks. Diffraction intensities measured while varying the D2O/H2O ratio in the relative humidity was used to solve the phase problem. The neutron scattering length density distribution of the hexagonal phase was constructed and analyzed to elucidate the packing of the lipid molecules. The structure of DPhPC in the hexagonal phase is of interest in connection with its stalk structure in the rhombohedral phase. We also found that the incorporation of tetradecane into the DPhPC hexagonal phase is limited, similar to the case for dioleoyl phosphatidylethanolamine.

Neutron Diffraction↗

Analysis of pulsed-neutron powder diffraction patterns of the icosahedral quasicrystals Pd3Siu and AlCuLiMg (three alloys) as twinned cubic crystals with large units.

The low-Q peaks on three pulsed-neutron powder patterns (total, U differential, and Pd differential) of the icosahedral quasicrystal Pd3SiU have been indexed on the basis of an assumed cubic structure of the crystals that by icosahedral twinning form the quasicrystal. The primitive unit cube is found to have edge length 56.20 A and to contain approximately 12,100 atoms. Similar analyses of pulsed-neutron patterns of Al55Cu10Li35, Al55Cu10Li30Mg5, and Al510Cu125Li235Mg130 give values of the cube edge length 58.3, 58.5, and 58.4 A, respectively, with approximately 11,650 atoms in the unit cube. It is suggested that the unit contains eight complexes in the beta-W positions, plus some small interstitial groups of atoms, with each complex consisting of a centered icosahedron of 13 clusters, each of 116 atoms with the icosahedral structure found in the body-centered cubic crystal Mg32(Al,Zn)49.

Journal Article↗

Ab initio molecular dynamics simulation of the structure and proton transport dynamics of methanol-water solutions.

Ab initio molecular dynamics simulations are employed to study the structural and proton transport properties of methanol-water mixtures. Structural characteristics analyzed at two different methanol mole fractions (X(M) = 0.25 and X(M) = 0.5) reveal enhanced structuring of water as the methanol mole fraction increases in agreement with recent neutron diffraction experiments. The simulations reveal the existence of separate hydrogen-bonded water and methanol networks, also in agreement with the neutron diffraction data. The addition of a single proton to the X(M) = 0.5 mixture leads to an anomalous structural or Grotthuss-type diffusion mechanism of the charge defect in which water-to-water, methanol-to-water, and water-to-methanol proton transfer reactions play the dominant role with methanol-to-methanol transfers being much less significant. Unlike in bulk water, where coordination number fluctuations drive the proton transport process, suppression of the coordination number of waters in the first solvation shell of the defect diminish the importance of coordination number fluctuations as a driving force in the structural diffusion process. The charge defect is found to reside preferentially at the interface between water and methanol networks. The length of the ab initio molecular dynamics run (approximately 120 ps), allowed the diffusion constant of the charge defect to be computed, yielding a value of D = 4.2 x 10(-5) cm2/s when deuterium masses are assigned to all protons in the system. The relation of this value to excess proton diffusion in bulk water is discussed. Finally, a kinetic theory is introduced to identify the relevant time scales in the proton transfer/transport process.

Journal Article↗

The hydration structure of guanidinium and thiocyanate ions: implications for protein stability in aqueous solution.

Neutron diffraction experiments were carried out on aqueous solutions containing either guanidinium or thiocyanate ions. The first-order difference method of neutron diffraction and isotopic substitution was applied, and the hydration structures of two of nature's strongest denaturant ions were determined. Each ion is shown to interact weakly with water: Guanidinium has no recognizable hydration shell and is one of the most weakly hydrated cations yet characterized. Hydration of thiocyanate is characterized by a low coordination number involving around one hydrogen-bonded water molecule and approximately two water molecules weakly interacting through "hydration bonds." The weak hydration of these denaturant ions strongly supports suggestions that a major contribution to the denaturant effect is the preferential interaction of the denaturant with the protein surface. By contrast, solute species such as many sugars and related polyols that stabilize proteins are strongly hydrated and are thus preferentially retained in the bulk solvent and excluded from the protein surface.

Biophysical Phenomena↗

Structure of insulin: results of joint neutron and X-ray refinement.

Neutron diffraction data for porcine 2Zn insulin were collected to 2.2 A resolution from a single crystal deuterated by slow exchange of mother liquor. A joint neutron/X-ray restrained-least-squares refinement was undertaken using the neutron data, as well as the 1.5 A resolution X-ray data collected previously. The final R factors were 0.182 for the X-ray data and 0.191 for the neutron data. Resulting atomic coordinates were compared with the initial X-ray model, showing a total r.m.s. shift of 0.36 A for the protein and 0.6 A for the solvent. Protonation of a number of individual amino acids was investigated by analysis of the neutron maps. No D atoms were found between the carboxylates of Glu B13 which make an intermolecular contact, suggesting nonbonded interaction rather than the predicted hydrogen bond. Amide hydrogen exchange was investigated in a refinement of their atomic occupancies. Regions of unexchanged amide groups were found in the center of the B helices. The results of this study emphasize the limited amount of information available in neutron diffraction studies of proteins at resolution lower than 2 A.

Animals↗

Detergent organisation in crystals of monomeric outer membrane phospholipase A.

The structure of the detergent in crystals of outer membrane phospholipase A (OMPLA) has been determined using neutron diffraction contrast variation. Large crystals were soaked in stabilising solutions, each containing a different H(2)O/D(2)O contrast. From the neutron diffraction at five contrasts, the 12 A resolution structure of the detergent micelle around the protein molecule was determined. The hydrophobic beta-barrel surfaces of the protein molecules are covered by rings of detergent. These detergent belts are fused to neighbouring detergent rings forming a continuous three-dimensional network throughout the crystal. The thickness of the detergent layer around the protein varies from 7-20 A. The enzyme's active site is positioned just outside the hydrophobic detergent zone and is thus in a proper location to catalyse the hydrolysis of phospholipids in a natural membrane. Although the dimerisation face of OMPLA is covered with detergent, the detergent density is weak near the exposed polar patch, suggesting that burying this patch in the enzyme's dimer interface may be energetically favourable. Furthermore, these results indicate a crucial role for detergent coalescence during crystal formation and contribute to the understanding of membrane protein crystallisation.

Bacterial Outer Membrane Proteins↗

A pentameric form of human serum amyloid P component. Crystallization, X-ray diffraction and neutron scattering studies.

Human serum amyloid P component crystallizes from sodium acetate buffer (pH 5.5) in the presence of calcium and polyethylene glycol 6000, at 4 degrees C. The space group is P2(1) and the cell parameters are a = 69.0 A (1 A = 0.1 nm), b = 99.3 A, c = 96.8 A, beta = 96.1. Density considerations supported by neutron scattering and gel filtration experiments indicate that the species crystallized is pentameric. The orientation of the pentamer 5-fold axis is determined and a crystal packing for the discs is proposed.

Crystallization↗

X-ray diffraction and neutron scattering studies of amphiphile-lipid bilayer organization.

The lipid bilayer thickness d(L), the transbilayer distance of lipid phosphate groups d(pp/inf> and the lipid surface area A(L) of fluid hydrated bilayers of lamellar phases of egg phosphatidylcholine or dipalmitoylphosphatidylcholine containing N-alkyl-N,N-dimethylamine N-oxides (CnNO), 1,4-butanedi-ammonium-N,N'-dialkyl-N,N,N',N'-tetramethyl dibromides (GSn) or mono-hydrochlorides of [2-(alkyloxy)phenyl]-2-(1-piperidinyl)ethylesters of carbamic acid (CnA) were obtained by X-ray diffraction, and the bilayer thickness in extruded unilamellar dioleoylphosphatidylcholine vesicles containing C12NO was obtained by the neutron scattering. The values of d(L), d(pp/inf> and A(L) change linearly up to the 1:1 amphiphile:lipid molar ratio. The slopes of these dependencies increase for d(L) and d(pp/inf> and decrease for AL) with an increasing number of carbons n in the amphiphile long hydrocarbon substituent (18> or =n> or =8 for CnNO, 16> or =n> or =9 for GSn, 12> or =n> or =5 for CnA), while the opposite trends are observed for the short substituent (8> or =n>/=6 for CnNO, 9> or =n> or =7 for GSn, 5> or =n> or =3 for CnA). In case of long substituents, the effects on dL), dpp/inf> and AL) are caused by the decrease in the difference between the lipid and amphiphile hydrocarbon chain lengths and by the increase in their van der Waals attraction. The short substituent amphiphiles are mobile and exchange between multiple binding sites in the bilayer, minimizing the bilayer surface area.

1,2-Dipalmitoylphosphatidylcholine↗

Influence of local anesthetics on the phosphatidylcholine model membrane: small-angle synchrotron X-ray diffraction and neutron scattering study.

The phase preferences of egg yolk phosphatidylcholine (EYPC) have been examined in the presence of tertiary amine anesthetics [2-(propyloxy)phenyl]-2-(1-piperidinyl)ethyl ester of carbamic acid (C3A) and [2-(heptyloxy)phenyl]-2-(1-piperidinyl)ethyl ester of carbamic acid (C7A, heptacaine). Using the synchrotron small-angle X-ray diffraction (SAXD), it is shown that the C3A anesthetic induces the cubic and hexagonal (H(I)) phases at 2 > or = C3A:EYPC > 0.5 and H2O:EYPC < or = 40 molar ratios. In contrast, longer alkyloxy chain homolog C7A has no effect on the bilayer arrangement of EYPC at C7A:EYPC < = 1 molar ratios as observed by SAXD in C7A + EYPC mixtures hydrated at H2O:EYPC < = 40 molar ratios, as well as in sonicated C7A + EYPC mixtures hydrated in excess water as proved by the small-angle neutron scattering (SANS). The bilayer thickness d(L) decreases and the bilayer C7A surface area SC7A increases with the increase of C7A:EYPC molar ratio. It is suggested that the ability of tertiary amine local anesthetics to influence the dL and SC7A values and EYPC polymorphism is caused by their effective molecular shape and by charge. The possibility that anesthetic molecules may exert some of their biological effects by virtue of these properties is discussed.

Amines↗

Base crystallization and base stacking in water.

2H2O solutions of 6-methylpurine and N6,N9-dimethyladenine have been examined by neutron diffraction. Comparison of the scattering from various molar solutions of 6-methylpurine with the scattering from its crystalline precipitates indicated base stacking in solution with a separation of approximately 0.34 nm. In particular at 1.75 M the effective stacking number in 6-methylpurine, as seen by neutron diffraction, was found to be approximately nine. Attempts to observe similar scattering from N6, N9-dimethyladenine were hampered because solutions with a molarity greater than or approximately 0.02 tended to form filamentary crystallites as a function of time. An analysis of the autocatalytic reaction involved in the formation of these dendrites is given. The rate constant is found to be 2.12 +/- 0.05 M-1 h-1. By comparing the diffraction from wet and dry crystallites it is concluded that hydrophilic interactions mediate the aggregation of both bases in water.

Crystallization↗

Bicriticality in FexCo1-xTa2O6.

X-ray and neutron-diffraction, dc magnetic susceptibility, magnetization, and specific-heat measurements are reported for FexCo(1-x)Ta2O6 mixed oxides. X-ray refinement indicates homogeneous samples for all the reported concentrations. The neutron-diffraction measurements reveal magnetic structures with double propagation vectors (+/-1/4,1/4,1/4) for CoTa2O6, and (1/2,0,1/2) and (0,1/2,1/2) for FeTa2O6. The latter remain unchanged in the Fe-rich samples, for 0.46< or =x<1.00, while the Co-rich samples show propagation vectors (+/-1/4,1/4,0) for 0.09< or =x<0.46. The temperature vs x phase diagram exhibits a bicritical point at about T=4.9 K and x=0.46. For this concentration, and at low temperatures, the system shows coexistence of both magnetic structures. This novel bicritical behavior is interpreted as induced by competition between the different magnetic and crystallographic structures.

Journal Article↗

Myoglobin solvent structure at different temperatures.

The structure of the solvent surrounding myoglobin crystals has been analyzed using neutron diffraction data, and the results indicate that the water around the protein is not disordered, but rather lies in well-defined hydration shells. We have analyzed the structure of the solvent surrounding the protein by collecting neutron diffraction data at four different temperatures, namely, 80, 130, 180, and 240K. Relative Wilson Statistics applied to low resolution data showed evidence of a phase transition in the region of 180K. A plot of the liquidity factor, Bsn, versus distance from the protein surface begins with a high plateau near the surface of the protein and drops to two minima at distances from the protein surface of about 2.35A and 3.85A. Two distinct hydration shells are observed. Both hydration shells are observed to expand as the temperature is increased.

Crystallography↗

Assignment of segments of the bacteriorhodopsin sequence to positions in the structural map.

Specific amino acid sequence segments have been assigned to locations in the structural map of bacteriorhodopsin using two-dimensional neutron diffraction data and a model building analysis. Models are constructed computationally by building specific regions of the amino acid sequence as alpha helices and then positioning the helices on axes indicated by the density map of Henderson and Unwin (Nature [Lond.]. 1975, 257:28-32). Neutron diffraction data were collected from samples of stacked, oriented "native" purple membranes as well as purple membranes containing different kinds of deuterated amino acids. Models differing in the assignments of helices to specific axes and in rotations of the helices about those axes were tested against the neutron data using a weighted residual factor to rank the models. This residual factor was calculated between observed and predicted intensity differences for pairs of data sets. Using this approach, a small set of related models has been found that predicts the observed intensity changes between five independent data sets. These models are inconsistent with the proposed locations of the retinal chromophore and the carboxyl terminus and with any of the previously proposed models for bacteriorhodopsin.

Amino Acid Sequence↗

Definition of lipid membrane structural parameters from neutronographic experiments with the help of the strip function model.

Neutron diffraction is an effective method for investigating model and biological membranes. Yet, to obtain accurate structural information it is necessary to use deuterium labels and much time is needed to acquire experimental data as there are a large number of diffraction reflections to register. This paper offers a way to define the hydrophobic boundary position in lipid membranes with high accuracy and for this purpose it is sufficient to take into consideration three structural factors. The method is based on modeling the density of the neutron diffraction amplitude rho(x) in the direction of the bilayer plane normal by means of a strip function, but it also takes into consideration the fact that the multiplication of the strip function amplitude rho i by the step width zi-zi-1 makes the sum of neutron scattering amplitudes of the atoms included in the step region. On the basis of the analysis of a large number of experimental data for different membranes, the effectiveness of this method in the determination of the position of hydrophilic/hydrophobic boundary is demonstrated, including the case of various rho(x) modifications in the region of polar heads and also the different phase states of membranes. However, it is shown in the present paper that the strip function model is not an adequate instrument for the determination of other structural parameters of membranes.

1,2-Dipalmitoylphosphatidylcholine↗

Interaction of amphiphilic molecules with biological membranes. A model for nonspecific and specific drug effects with membranes.

The nonspecific interactions of propranolol, timolol, and ethanol with model and sarcoplasmic reticulum membranes were determined utilizing radioisotopic association differential scanning calorimetry, and neutron diffraction. Differential scanning calorimetry performed on mixtures of these amphiphilic compounds and model membrane bilayers composed of dimyristoyllecithin showed that propranolol was approximately 25 times more lipid-soluble than timolol and at least 100 times more lipid-soluble than ethanol. Neutron diffraction showed that the solvation of propranolol was within the fatty acyl chain region of the lipid bilayer. This solvation correlated with the effect of propranolol to inhibit ATP-dependent calcium transport in isolated rabbit skeletal muscle sarcoplasmic reticulum, a membrane that lacks beta-adrenergic receptors. In contrast, the major site of interaction of ethanol was within the aqueous compartment hydrating the sarcoplasmic reticulum membrane. A model for nonspecific drug interaction with the sarcoplasmic reticulum membrane based on the site of interaction of these amphiphiles and their relative potencies to inhibit calcium transport by these membranes is proposed. In principle, this model could be extended to specific drug interactions with membranes.

Animals↗

Preparation, crystal structure, and properties of barium pernitride, BaN(2).

Stoichiometric barium pernitride, BaN(2), was prepared from the elements under N(2) pressure of 5600 bar in an autoclave at 920 K. The compound is isotypic to ThC(2) (space group C2/c, Z = 4) according to powder X-ray (neutron) diffraction data with a = 7.1712(1), b = 4.3946(1), c = 7.2362(1) A, and beta = 104.864(1) degrees (a = 7.1745(1), b = 4.3963(1), c = 7.2393(1) A, beta = 104.876(1) degrees ). The N-N distance of 1.221(4) A (based on the neutron diffraction data) is indicative of a double bond in the N(2)(2-) dumbbells. BaN(2) is metallic according to magnetic susceptibility measurements and TB-LMTO band structure calculations.

Journal Article↗

Pressure-enhanced 3D antiferromagnetic correlations in La(1.4)Sr(1.6)Mn(2)O(7).

Pressure effects on the stability of magnetic phases in La(1.4)Sr(1.6)Mn(2)O(7) have been studied using magnetization measurements and neutron diffraction. At ambient conditions this material is a quasi-two-dimensional ferromagnet. On cooling it becomes ordered three dimensionally: at 90 K La(1.4)Sr(1.6)Mn(2)O(7) it becomes an antiferromagnet, and at 65 K it undergoes a transition into a ferromagnetic phase. Using neutron diffraction techniques on a single crystal of La(1.4)Sr(1.6)Mn(2)O(7) it has been shown that these two magnetic phases belong to a single structural phase and do not coexist at low temperatures. The application of pressure enhances the antiferromagnetic correlations between the Mn(2)O(9) bilayers.

Journal Article↗