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Thermodynamic stability of the 5' dangling-ended DNA hairpins formed from sequences 5'-(XY)2GGATAC(T)4GTATCC-3', where X, Y = A, T, G, C.

Expressions for the partition function Q (T) of DNA hairpins are presented. Calculations of Q (T), in conjunction with our previously reported numerically exact algorithm [T. M. Paner, M. Amaratunga, M. J. Doktycz, and A. S. Benight (1990) Biopolymers, 29, 1715-1734], yield a numerical method to evaluate the temperature dependence of the transition enthalpy, entropy, and free energy of a DNA hairpin directly from its optical melting curve. No prior assumptions that the short hairpins melt in a two-state manner are required. This method is then applied in a systematic manner to investigate the stability of the six basepair duplex stem 5'-GGATAC-3' having four-base dangling single-strand ends with the sequences (XY)2, where X, Y = A, T, G, C, on the 5' end and a T4 loop on the 3' end. Results show that all dangling ends of the sample set stabilize the hairpin against melting. Increases in transition temperatures as great as 4.0 degrees C above the blunt-ended control hairpin were observed. The hierarchy of the hairpin transition temperatures is dictated by the identity of the first base of the dangling end adjoining the duplex in the order: purine greater than T greater than C. Calculated melting curves of every hairpin were fit to experimental curves by adjustment of a single parameter in the numerically exact theoretical algorithm. Exact fits were obtained in all cases. Experimental melting curves were also calculated assuming a two-state melting process. Equally accurate fits of all dangling-ended hairpin melting curves were obtained with the two-state model calculation. This was not the case for the melting curve of the blunt-ended hairpin, indicating the presence of a four-base dangling-end drives hairpin melting to a two-state process. Q (T) was calculated as a function of temperature for each hairpin using the theoretical parameters that provided calculated curves in exact agreement with the experimentally obtained optical melting curves. From Q (T), the temperature dependence of the transition enthalpy delta H, entropy delta S, and free energy delta G were calculated for every hairpin providing a quantitative assessment of the effects of dangling ends on hairpin thermodynamics. Comparisons of our results are made with those of the Breslauer group [M. Senior, R. A. Jones, and K. J. Breslauer (1988) Biochemistry 27, 3879-3885] on the T2 5' dangling-ended d(GC)3 duplexes.(ABSTRACT TRUNCATED AT 400 WORDS)

Base Sequence↗

[Study of the penicillin amidase from E. coli. An ultrasonic method of studying the ph- and temperature-conformational transitions in the active center of the enzyme].

pH and temperature conformation transitions in the active center of penicillin amidase i.e. penicillinamidohydrolase E.C. 3.5.I.II were investigated by means of the kinetic method and a new ultrasonic method. It was shown that the catalytic activity of the enzyme was controlled by 2 ionogenic groups with pK 6.1 and 10.2. The study of penicillinamidase by means of the ultrasonic method showed that the ionogenic group with pK 10 was responsible for maintaining the catalytically active conformation of the enzyme active center. Investigation of the temperature relation between the kinetic parameters of the enzymatic hydrolysis of benzylpenicillin catalyzed by penicillin amidase and the data on the effect of ultrasound on the enzyme showed that the enzyme was subjected to the temperature conformation transiton. The temperature and thermodynamic parameters of the conformation transition were determinded (T=318 degrees K, delta H=81 kcal/mole and delta S=255 e.u.). The structure of the active center of the enzyme is discussed on the basis of the data obtained.

Amidohydrolases↗

Permeability of lipid-coated polymer capsule membranes to solutes: effects of temperature and chemical structure of solutes.

The permeability of di-stearyldimethylammonium-coated polyamide capsule membranes to KCl, and tetra-methylammonium (4C1N), tetra-propylammonium (4C3N), and tetra-butylammonium (4C4N) bromides was investigated at temperatures below and above the phase transition temperature of the amphiphile coat and compared with that of non-coated polyamide capsule membranes. The rate of solute permeation through the non-coated capsule membranes for all permeants increased gradually with rise in temperature. When the capsule was coated with the amphiphile, the rate was reduced by a factor of 2-200 relative to that through the non-coated semipermeable capsule membranes and changed drastically or slightly at the phase transition temperature of the amphiphile coat, depending on the chemical structure of permeants. The permeation of hydrophilic KCl and slightly hydrophobic 4C1N was greatly supressed by the amphiphile coat below the phase transition temperature while it was enhanced above that temperature. On the contrary, the permeation rate of the moderately hydrophobic and bulky 4C3N increased monotonically with rising temperature. No change in the permeation rate was observed with the highly hydrophobic and bulky 4C4N at all temperatures.

Calorimetry, Differential Scanning↗

Phase transition characteristics of diphosphatidyl-glycerol (cardiolipin) and stereoisomeric phosphatidyldiacylglycerol bilayers. Mono- and divalent metal ion effects.

Synthesis and phase transition chaaracteristics of aqueous dispersions of the homologous (12 : 0, 14 : 0, 16 : 0) diphosphatidylglycerols (cardiolipins) and phosphatidyldiacylglycerols are reported. Electron microscopy of the negatively stained aqueous dispersions reveals a characteristic lamellar structure suggesting that these phospholipid molecules are organized as bilayers in the aqueous dispersions. The phase transition temperature (Tm) and the enthalpy of transition (delta H) increase monotonically with chain length in the cardiolipin and phosphatidyldiacylglycerol series; Tm for phosphatidyldiacylglycerol is higher than that for cardiolipin of the same chain-length. The transition temperatures for the enantiomeric sn-3,3- and sn-1,1-phosphatidyldiacylglycerol and for the diastereomeric, meso-sn-1,3-phosphatidyldiacylglycerol are approximately the same. The molar enthalpy for the transition of cardiolipin-NH+4 bilayers is approximately twice the value for the phosphatidylcholines of the same chain length, i.e., the molar enthalpy per acyl chain is approximately the same in the two systems. The transition temperatures for metal ion salts of C16-cardiolipin exhibit a biphasic dependence upon the unhydrated ionic radii, i.e., the highest Tm is observed for Ca2+-cardiolipin and decreases for the salts of ions with smaller and larger ionic radii than that of Ca2+. The lowest Tm is observed for Rb+-cardiolipin. Monovalent metal salts of cardiolipin exhibit two phase transitions. This effect may result from different conformational packing of the four acyl chains due to differences in metal-phosphate binding.

Cardiolipins↗

Molecular characteristics of astaxanthin and beta-carotene in the phospholipid monolayer and their distributions in the phospholipid bilayer.

The molecular characteristics of the monolayers of astaxanthin with polar group on the beta-ionone ring in the molecule and beta-carotene without polar group and their interactions in mixed carotenoid-phospholipid monolayers and the effects of carotenoids on the phase behavior of the phospholipid bilayers were examined by the monolayer technique and differential scanning calorimetry (DSC). We found from the monolayer study that beta-carotene had an amphiphilic nature. The molecular assembly of astaxanthin in the monolayer at the hydrophobic/hydrophilic interface was more stable than that of beta-carotene. Dimyristoylphosphatidylcholine (DMPC) in the monolayer was miscible with astaxanthin in the range of 0-0.4 mol fractions of astaxanthin, but not fully miscible with beta-carotene even at low concentrations below 0.1 mol fraction of beta-carotene. Surface potential and compression/expansion cycles of beta-carotene monolayer indicated the formation of molecular aggregates by itself. DSC study showed that when small amount of astaxanthin was added, the transition temperature of dipalmitoylphosphatidylcholine (DPPC) was markedly shifted to lower temperatures and that the transition peak was asymmetrically broadened, indicative of a significant depression in cooperativity of the gel to liquid-crystalline transition. The asymmetric DSC endothermic bands of DPPC incorporating small amounts of astaxanthin were well fit by deconvolution into two to three domains containing different concentrations of astaxanthin. On the contrary, the incorporation of beta-carotene resulted in a small depression of the main transition temperature with a slight broadening of the transition peak, suggesting a small miscibility of beta-carotene with the phospholipid bilayer or a formation of aggregates of beta-carotene in the membranes. These results suggest that there would be a high localized concentration in the phase separated membrane for astaxanthin or beta-carotene to function effectively as scavenger.

1,2-Dipalmitoylphosphatidylcholine↗

Targeting a genetically engineered elastin-like polypeptide to solid tumors by local hyperthermia.

Elastin-like polypeptides (ELPs) are biopolymers of the pentapeptide repeat Val-Pro-Gly-Xaa-Gly that undergo an inverse temperature phase transition. They are soluble in aqueous solutions below their transition temperature (T1) but hydrophobically collapse and aggregate at temperatures greater than T1. We hypothesized that ELPs conjugated to drugs would enable thermally targeted drug delivery to solid tumors if their T1 were between body temperature and the temperature in a locally heated region. To test this hypothesis, we synthesized a thermally responsive ELP with a T1 of 41 degrees C and a thermally unresponsive control ELP in Escherichia coli using recombinant DNA techniques. In vivo fluorescence videomicroscopy and radiolabel distribution studies of ELP delivery to human tumors (SKOV-3 ovarian carcinoma and D-54MG glioma) implanted in nude mice demonstrated that hyperthermic targeting of the thermally responsive ELP for 1 h provides a approximately 2-fold increase in tumor localization compared to the same polypeptide without hyperthermia. We observed aggregates of the thermally responsive ELP by fluorescence videomicroscopy within the heated tumor microvasculature but not in control experiments, which demonstrates that the phase transition of the thermally responsive ELP carrier can be engineered to occur in vivo at a specified temperature. By exploiting the phase transition-induced aggregation of these polypeptides, this method provides a new way to thermally target polymer-drug conjugates to solid tumors.

Amino Acid Sequence↗

Thermal stability of proteins in the presence of poly(ethylene glycols).

Thermal unfolding of ribonuclease, lysozyme, chymotrypsinogen, and beta-lactoglobulin was studied in the absence or presence of poly(ethylene glycols). The unfolding curves were fitted to a two-state model by a nonlinear least-squares program to obtain values of delta H, delta S, and the melting temperature Tm. A decrease in thermal transition temperature was observed in the presence of poly(ethylene glycol) for all of the protein systems studied. The magnitude of such a decrease depends on the particular protein and the molecular size of poly(ethylene glycol) employed. A linear relation can be established between the magnitude of the decrease in transition temperature and the average hydrophobicity of these proteins; namely, the largest observable decrease is associated with the protein of the highest hydrophobicity. Further analysis of the thermal unfolding data reveals that poly(ethylene glycols) significantly effect the relation between delta H degrees of unfolding and temperature for all the proteins studied. For beta-lactoglobulin, a plot of delta H versus Tm indicates a change in slope from a negative to a positive value, thus implying a change in delta Cp in thermal unfolding caused by the presence of poly(ethylene glycols). Results from solvent-protein interaction studies indicate that at high temperature poly(ethylene glycol) 1000 preferentially interacts with the denatured state of protein but is excluded from the native state at low temperature. These observations are consistent with the fact that poly(ethylene glycols) are hydrophobic in nature and will interact favorably with the hydrophobic side chains exposed upon unfolding; thus, it leads to a lowering of thermal transition temperature.

Chymotrypsinogen↗

Reversibility of the effects of gossypol acetic acid, an antispermatogenic/antifertility agent on the intestinal structure and functions of male albino rats.

The effects of Gossypol acetic acid (10 mg/kg b. wt. daily for 15 days), an experimental male antifertility agent and its subsequent withdrawal for another 15 days, on the structure and functions of the rat small intestinal tract have been investigated. Gossypol feeding causes a reduction in body weight and intestinal weight, length, protein, and nucleic acid contents. A 27%-50% reduction in the uptake of glucose, alanine, leucine, and calcium is observed after Gossypol feeding which is found to be reversible after 15 days of withdrawal of the drug. Gossypol also causes a significant reduction in the activities of sucrase, lactase, maltase and alkaline phosphatase in the intestinal homogenates as well as in the purified brush border membrane of the microvillus. A decrease in the maximum of apparent enzyme velocity and no change in the substrate affinity constant in these digestive hydrolases are observed on Gossypol treatment. It also causes a shift in the transition temperature in these enzymes and predictably changes the energy of activation both below and above the temperature of transition, although the Arrhenius expression of the temperature dependence still shows proximity, non-linearity, and is parallel to the control group. These changes are reversed on withdrawal of the drug and during the subsequent recovery period. Recovery experiments also show near identical values in kinetic parameters (Kt and Jmax) of 14C-glucose uptake in jejunal segments both in the presence and absence of Na+ ions. Also, no difference is observed between the control and recovery groups with respect to body and intestinal weight, intestinal length, and DNA, RNA, protein, lactate dehydrogenase and glucose-6-phosphate phosphohydrolase values in the intestinal homogenates. Phospholipid, cholesterol and sialic acid levels in both the groups also show nearly identical values. Molecular mechanism of the effects of Gossypol on brush border membrane-bound enzyme/carrier molecules operation is discussed in view of the kinetic and thermodynamic data obtained.

Amino Acids↗

Effect of fatty acyl chain length and structure on the lamellar gel to liquid-crystalline and lamellar to reversed hexagonal phase transitions of aqueous phosphatidylethanolamine dispersions.

The lamellar gel/liquid-crystalline and the lamellar liquid-crystalline/reversed hexagonal phase transitions of aqueous dispersions of a number of synthetic phosphatidylethanolamines containing linear saturated, branched chain, and alicyclic fatty acyl chains of varying length were studied by differential scanning calorimetry, 31P nuclear magnetic resonance spectroscopy, and X-ray diffraction. For any given homologous series of phosphatidylethanolamines containing a single chemical class of fatty acids, the lamellar gel/liquid-crystalline phase transition temperature increases and the lamellar liquid-crystalline/reversed hexagonal phase transition temperature decreases with increases in hydrocarbon chain length. For a series of phosphatidylethanolamines of the same hydrocarbon chain length but with different chemical structures, both the lamellar gel/liquid-crystalline and the lamellar liquid-crystalline/reversed hexagonal phase transition temperatures vary markedly and in the same direction. In particular, at comparable effective hydrocarbon chain lengths, both the lamellar gel/liquid-crystalline and the lamellar liquid-crystalline/reversed hexagonal phase transition temperatures vary in parallel, such that the temperature difference between these two phase transitions is nearly constant. Moreover, at comparable effective acyl chain lengths, the d spacings of the lamellar liquid-crystalline phases and of the inverted hexagonal phases are all similar, implying that the thickness of the phosphatidylethanolamine bilayers at the onset of the lamellar liquid-crystalline/reversed hexagonal phase transition and the diameter of the water-filled cylinders formed at the completion of this phase transition are comparable and independent of the chemical structure of the acyl chain.(ABSTRACT TRUNCATED AT 250 WORDS)

Calorimetry, Differential Scanning↗

Effects of thermosensitivity of poly (N-isopropylacrylamide) hydrogel upon the duration of a lag phase at the beginning of drug release from the hydrogel.

The release rates of three kinds of drugs, with different charges, from poly (N-isopropylacrylamide) hydrogels were studied. The release rate was observed to be temperature dependent for the types of drug. When the temperature was lower than the phase transition temperature, the release rate was higher at lower temperatures and increased as the temperature rose. The amount of drugs released from a poly (N-isopropylacrylamide) hydrogel disk was plotted against the square root of time. It was found that the amount of drugs released was proportional to the square root of time over a certain time interval. A lag phase was observed before the amount of drug released became proportional to the square root of time. The longest time lag was observed at the phase transition temperature of poly (N-isopropylacrylamide); LCST (33 degrees C). This suggests that the penetration rate of water into the hydrogels is lowest at the phase transition temperature and drastically changes around it. The release rates of drugs was also affected by the charges of the drug molecules. This may be caused by the interaction of drug molecules with polymer chains. When anionic drugs are released, the electrostatic repulsion seems to act between polymer chains and drug molecules. Therefore, the lag phase observed at the beginning of the release of anionic drugs was shorter, as compared with other kinds of drugs at any temperatures between 25 and 40 degrees C. On the other hand, when cationic drugs are released, the time lag was longer at temperatures higher than 33 degrees C as compared with the time lag at lower temperatures. At temperatures higher than 33 degrees C, drugs are released from the surface skin layer of the hydrogel where water molecules are less mobile than those in bulk distilled water. The drug release thus shows a long lag phase.

Journal Article↗

Interactions of arbutin with dry and hydrated bilayers.

The glycosylated hydroquinone arbutin (4-hydroxyphenyl-beta-D-glucopyranoside) is abundant in certain resurrection plants, which can survive almost complete dehydration for prolonged periods. Little is known about the role of arbutin in vivo, but it is thought to contribute toward survival of the plants in the dry state. We have investigated the interactions of arbutin with model membranes under conditions of high and low hydration, as well as the possible participation of arbutin in carbohydrate glasses formed at low water contents. Retention of a trapped soluble marker inside large unilamellar vesicles and fusion of vesicles was monitored by fluorescence spectroscopy. Effects of arbutin on glass-transition temperatures and hydrated membrane phase-transition temperatures were measured by differential scanning calorimetry. The possible insertion of arbutin into membrane bilayers was estimated by following arbutin auto-fluorescence. Evidence is presented that arbutin does not change the glass-transition temperature of a sucrose/trehalose glass, but that arbutin does interact with hydrated membranes by insertion of the phenol moiety into the lipid bilayer. This interaction causes increased membrane leakage during air-drying by a mechanism other than vesicle-vesicle fusion. Implications of these effects on the dehydrated plant cells, as well as possible methods of obviating the damage, are discussed.

1,2-Dipalmitoylphosphatidylcholine↗

Effect of the gel to liquid crystalline phase transition on the osmotic behaviour of phosphatidylcholine liposomes.

Aspects of osmotic properties of liposomes, prepared from synthetic lecithin, above, at and below the gel to liquid crystalline phase transition temperature are described. The experiments show that liposomal membranes with their lipids in the gel state are still permeable to water. The rate of water permeation changes drastically on passing the transition temperature. The water permeation has activation energies of 9.5 +/- 1.28 and 26.4 +/- 0.9 kcal/mol above and below the transition temperature, respectively, indicating that the diffusion processes take place by different mechanisms. With respect to the barrier properties of the liposomes in the vicinity of the transition temperature, the following conclusions can be made. (1) Studying the osmotic shrinkage of liposomes at a fixed temperature near the transition point, the experiments indicate that dimyristoyl phosphatidylcholine membranes are highly permeable to glucose under these conditions, where liquid and solid domains co-exist. Under the same conditions the osmotic experiments did not indicate a strong increase in glucose permeability of dipalmitoyl phosphatidylcholine membranes as compared to the situation above and below the transition temperature. (2) On the other hand, perturbations of the phase equilibrium by temperature varations resulted in a marked increase of the glucose permeation through dipalmitoyl phosphatidylcholine bilayers. Once a new phase equilibrium of liquid and solid regions is established the permeation rate of glucose is much less.

Binding Sites↗

Improvement of temperature-sensitivity of poly(N-isopropylacrylamide)-modified liposomes.

As a novel temperature-sensitive drug delivery system, we have designed liposomes coated with poly(N-isopropylacrylamide), which exhibits a coil-globule transition at 32-35 degrees C. In a previous study [ K. Kono, H. Hayashi, T. Takagishi, J. Control. Release 30 (1994) 69-75], it was shown that the release of contents from the polymer-coated liposomes is enhanced above the transition temperature of the polymer but the release is not controlled completely by the conformational change of the polymer. In this study, to improve temperature-sensitivity of the poly(N-isopropylacrylamide)-modified liposomes, the influence of lipid composition on the temperature-sensitivity of the liposomes was investigated. A copolymer of N-isopropylacrylamide and N, N-didodecylacrylamide was synthesized by free radical copolymerization. While the copolymer was insoluble in water, it exhibited a coil-globule transition around 28 degrees C when incorporated into an egg yolk phosphatidylcholine membrane. The copolymer-modified egg yolk phosphatidylcholine/dioleoylphosphatidylethanolamine liposomes were prepared by sonication or reverse phase evaporation. Release of calcein from the copolymer-modified liposomes was very slow below the transition temperature of the copolymer, whereas the release was enhanced above the transition temperature. Incorporation of dioleoylphosphatidylethanolamine into liposome membranes enhanced release greatly above the transition temperature of the copolymer. Fluorometric measurements using 8-anilino-1-naphthalenesulfonate and 1,6-diphenyl-1,3,5-hexatriene suggested that the copolymer decreases membrane fluidity of the liposomes near and above the transition temperature of the copolymer and that interaction between the copolymer and the liposome membranes is enhanced by inclusion of dioleoylphosphatidylethanolamine.

Acrylic Resins↗

The effect of the phase transition on the hydration and electrical conductivity of phospholipids.

Adsorption isotherms for various saturated phosphatidylcholines have been obtained. Lipids above and below their phase transition temperature differ only in the amount of water adsorbed and not in the nature of their adsorption isotherms. Cholesterol has an effect similar to that of increasing unsaturation in the hydrocarbon chains. Decreasing the length of the hydrocarbon chains for lipids below their phase transition temperature has no effect on the isotherms. If the chain length is short enough so that the lipids are above their transition temperature, however, a large increase in water adsorption occurs. All of the phospholipids exhibit a rapid increase of electrical conductivity for a few water molecules adsorbed per lipid molecule. All of the phospholipids show a saturation in conductivity at greater amounts of adsorbed water; the shape of the saturation region depends on whether the lipids are above or below their phase transition temperature. The activation energy for the electrical conductivity process depends on whether the hydrated lipids are in the "liquid-like" of the crystalline state, being lower for phospholipids in the liquid-like state. If the lipids are hydrated above their phase transition temperatures, their activation energies are lower than if they are hydrated below the transition temperature. Cholesterol lowers the activation energy. The phosphatidylcholines can be characterized by different activation energies, depending both upon their physical state and the presence of unsaturation in their hydrocarbon chains.

Binding Sites↗

Interfacial effects on vitrification of confined glass-forming liquids.

Mesoporous silica phases, with uniform pores of dimensions in the 2-30 nm range, offer a uniquely well-defined environment for the study of the effects of two-dimensional spatial confinement on the properties of glass-forming liquids. We report observations by differential scanning calorimetry of the vitrification of o-terphenyl (OTP), salol, and glycerol in hexagonal mesoporous silica (MCM-41 and SBA-15) in a wide range of pore sizes from 2.6 to 26.4 nm. In agreement with previous studies, where a controlled porous glass is used as a solid matrix, the glass transition temperature for o-terphenyl diminishes with decreasing pore size. In contrast to OTP, glycerol shows a gradual increase in glass transition temperature, while in salol a slight reduction of glass transition temperature is observed, followed by an increase, which results in glass transition temperature indistinguishable from that of the bulk for the smallest pores. These results are discussed in terms of liquid-surface interactions in an interfacial layer, monitored by Fourier-transformed infrared spectroscopy in the study. The hydrogen bonding with silica surface silanols dominates the glass transition trends observed in salol and glycerol.

Calorimetry, Differential Scanning↗

Availability of dinitrophenylated lipid haptens for specific antibody binding depends on the physical properties of host bilayer membranes.

We have measured the binding of two radioiodinated monoclonal anti-dinitrophenyl antibodies (IgE and IgG2a) to two dinitrophenylated lipid haptens in lipid bilayer membranes having various compositions and physical properties. These antibodies bind strongly to the lipophilic dinitrophenyl group in some membranes. Dimyristoylphosphatidylcholine and dipentadecanoylphosphatidylcholine containing 2 mol % dinitrophenyl lipid hapten bind anti-dinitrophenyl antibodies below the chain-melting transition temperatures of these lipids (22 and 35 degrees C, respectively) but not above these temperatures. Evidently, the lipophilic dinitrophenyl group is partially or completely buried in the hydrophobic region of these bilayers at temperatures above the chain-melting transition temperatures. The inclusion of increasing concentrations of cholesterol in such membranes (e.g. in dimyristoylphosphatidylcholine at 37 degrees C) results in a marked enhancement of antibody binding. It was found that a third lipid hapten containing the dinitrophenyl group does not show this strong dependence of antibody binding on the physical state of the lipid membrane. The weak immunologic degranulation of rat basophil leukemia cells by dimyristoylphosphatidylcholine membrane targets at 37 degrees C can be attributed to a weak binding of anti-dinitrophenyl IgE to these membranes (Balakrishnan, K., Hsu, F. J., Cooper, A. D., and McConnell, H. M. (1982) J. Biol. Chem. 257, 6427-6433). However, if the antibody is first allowed to bind to this membrane below the lipid chain-melting transition temperature, these IgE-coated membrane targets are very effective in releasing serotonin from the rat basophil leukemia cells when the temperature is raised to 37 degrees C.

Animals↗

31P nuclear magnetic resonance and freeze-fracture electron microscopy studies on Escherichia coli. II. Lipopolysaccharide and lipopolysaccharide-phospholipid complexes.

1. Freeze-fracture electron microscopy and 31P-NMR spectroscopy on native and electrodialyzed lipopolysaccharide from Escherichia coli K12 cells, both above and below the phase transition temperature, are described. 2. Freeze-fracture electron microscopy of native lipopolysaccharide shows ribbon-like structures below (0 and 22 degrees C) and large vesicles above (37 degrees C) the phase transition temperature. Electrodialyzed lipopolysaccharide (sodium salt) occurs in ribbon-like structures at 0, 22 and 37 degrees C if sodium lipopolysaccharide is hydrated in water. If sodium lipopolysaccharide is hydrated in Tris-HCL/NaCl buffer these ribbon-like structures occur only below the phase transition temperature. Above the phase transition temperature stacked sheets are observed. Moreover, in the latter case, the fracture planes contain particles and pits. Upon etching, sodium lipopolysaccharide when hydrated in water appears to form rods and when hydrated in buffer appears to form mainly stacked lamellae both above (37 degrees C) and below (0 degrees C) the phase transition temperature. 3. High resolution 31P-NMR spectra show that the chemical shifts of the phosphorus atoms in native lipopolysaccharide differ from those in electrodialyzed lipopolysaccharide, probably due to conformational and compositional (the disappearance of ions and (poly)electrolytes) changes. The 31P-NMR spectra of native lipopolysaccharide dispersed in Tris-HCL/NaCl buffer are very broad at 20 and at 40 degrees C indicating little motion. At 22 degrees C electrodialyzed lipopolysaccharide also gives a broad spectrum; at 40 degrees C the spectrum is narrower, indicating more motion, and two peaks are visible. After dispersion in H2o and subsequent addition of buffer, the spectrum of electrodialyzed lipopolysaccharide is narrow both at 20 and 40 degrees C, which can be correlated with the rods observed in freeze etching. After treatment with Ca2+, electrodialyzed lipopolysaccharide shows a very broad spectrum at 40 degrees C probably due to immobilization of the lipopolysaccharide. 4. Freeze-fracture electron microscopy and 31P-NMR spectroscopy of liposomes consisting of native lipopolysaccharide and total phospholipids indicate that the phospholipids and the lipopolysaccharide are mainly organized in bilayers. Lipopolysaccharide in such liposomes undergoes more motion than in the absence of phospholipids. Ca2+ does not influence this behaviour.

Escherichia coli↗

Superconductivity in single crystals of the fullerene C70.

The observation of superconductivity in doped C60 has attracted much attention, as these materials represent an entirely new class of superconductors. A maximum transition temperature (Tc) of 40 K has been reported for electron-doped C60 crystals, while a Tc of 52 K has been seen in hole-doped crystals; only the copper oxide superconductors have higher transition temperatures. The results for C60 raise the intriguing questions of whether conventional electron-phonon coupling alone can produce such high transition temperatures, and whether even higher transition temperatures might be observed in other fullerenes. There have, however, been no confirmed reports of superconductivity in other fullerenes, though it has recently been observed in carbon nanotubes. Here we report the observation of superconductivity in single crystals of electric-field-doped C70. The maximum transition temperature of about 7 K is achieved when the sample is doped to approximately four electrons per C70 molecule, which corresponds to a half-filled conduction band. We anticipate superconductivity in smaller fullerenes at temperatures even higher than in C60 if the right charge density can be induced.

Journal Article↗