The synthesis and use of thionphospholipids in 31P-NMR studies of lipid polymorphism

(1) Dipalmitoyl- and dioleoylthionphosphatidylcholine, which are phosphatidylcholine analogues in which the double bonded oxygen of the phosphate group is replaced by a sulfur atom, have been synthesized in 50–60% yields by condensation of diacylglycerol with phosphorus thionchloride in the presence of choline toluene-sulfonate. Dioleoylthionphosphatidylethanolamine has been prepared by the phospholipase D-catalyzed base exchange reaction. (2) Freeze-fracturing of aqueous dispersions of the thionphospholipids reveals that the thionphosphatidylcholines are organized in extended bilayers whereas dioleoylthionphosphatidylethanolamine above 0°C forms the hexagonal H_II phase similar to dioleoylphosphatidylethanolamine. The gel → liquid crystalline phase transition of the dipalmitoylthionphosphatidylcholine occurs at 44°C which is only slightly higher than the transition temperature of dipalmitoylphosphatidylcholine which together with other data demonstrates that the thionphospholipids closely resemble the natural phospholipids in physicochemical behaviour. (3) Proton decoupled ³¹P-NMR spectra of aqueous dispersions of thionphosphatidylcholines have the characteristic asymmetrical line-shape with a low-field shoulder and a high-field peak typical of phospholipids organized in extended bilayers in which the phosphate group can undergo fast axial rotation. The ³¹P-NMR spectrum of the thionphosphatidylethanolamine in the hexagonal H_II phase has a line-shape with a reversed asymmetry and an effective chemical shift anisotropy half of that of thionphospholipids organized in bilayers which is caused by fast lateral diffusion of the lipids around the cylinders of the hexagonal H_II phase as has been observed for the corresponding phosphatidylethanolamines. (4) Since the ³¹P-NMR resonance of the thionphospholipids is completely separated from that of natural phospholipids, these lipids can be used to study by ³¹P-NMR the motional and structural properties of individual lipids in mixed systems. This is demonstrated for various lipid mixtures in which non-bilayer lipid structures have been induced by variations in composition, temperature and presence of divalent cations. It is shown that bilayer → non-bilayer transitions can be modulated by gel → liquid crystalline phase transitions and that typical bilayer forming lipids can be incorporated into non-bilayer structures such as the hexagonal H_II phase.     

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.     

Lamellar/inverted cubic (L alpha/QII) phase transition in N-methylated dioleoylphosphatidylethanolamine

Inverted cubic (QII) phases form in hydrated N-methylated dioleoylphosphatidylethanolamine (DOPE-Me). Previous work indicated that QII phases in this and other systems might be metastable structures. Whether or not QII phases are stable has important implications for models of the factors determining the relative stability of bilayer and nonbilayer phases and of the mechanisms of transitions between those phases. Here, using X-ray diffraction and very slow scan rate differential scanning calorimetry (DSC), we show that thermodynamically stable QII phases form slowly during incubation of multilamellar samples of DOPE-Me at constant temperature. The equilibrium L alpha/QII phase transition temperature is 62.2 +/- 1 degree C. The transition enthalpy is 174 +/- 34 cal/mol, about two-thirds of the L alpha/HII transition enthalpy observed at faster scan rates. This implies that the curvature free energy of lipids in QII phases is substantially lower than in L alpha phases and that this reduction is substantial compared to the reduction achieved in the HII phase. The L alpha/QII transition is slow and is not reliably detected with DSC until the temperature scan rate is reduced to ca. 1 degrees C/h. At faster scan rates, the HII phase forms at a reproducible temperature of 66 degrees C. This HII phase is metastable until ca. 72-79 degrees C, where the equilibrium QII/HII transition seems to occur. These results, as well as the induction of QII phases in similar systems by temperature cycling (observed by others), are consistent with a theory of L alpha/QII/HII transition mechanisms proposed earlier (Siegel, 1986c).     

Synthesis and polymorphic phase behaviour of polyunsaturated phosphatidylcholines and phosphatidylethanolamines

A series of phosphatidylcholines and phosphatidylethanolamines was synthesized containing two acyl chains of the following polyunsaturated fatty acids: linoleic acid (18:2), linolenic acid (18:3), arachidonic acid (20:4) and docosahexaenoic acid (22:6). In addition two phospholipids with mixed acid composition were synthesized: 16:0/18:1_c phosphatidylcholine and 16:0/18:1_c phosphatidylethanolamine. The structural properties of these lipids in aqueous dispersions in the absence and in the presence of equimolar cholesterol were studied using ³¹P-NMR, freeze fracturing and differential scanning calorimetry (DSC).The phosphatidylcholines adopt a bilayer configuration above 0°C. Incorporation of 50 mol% of cholesterol in polyunsaturated species induces a transition at elevated temperatures into structures with ³¹P-NMR characteristics typical of non-bilayer organizations. When the acyl chains contain three or more double bonds, this non-bilayer organization is most likely the hexagonal H_II phase, 16:0/15:1_c phosphatidylethanolamine shows a bilayer to hexagonal transition temperature of 75°C. The polyunsaturated phosphatidylethanolamines exhibit a bilayer to hexagonal transition temperature below 0°C which decreases with increasing unsaturation and which is lowered by approximately 10°C upon incorporation of 50 mol% of cholesterol. Finally, it was found that small amounts of polyunsaturated fatty acyl chains in a phosphatidylethanolamine disproportionally lower its bilayer to hexagonal transition temperature.     

Calorimetric and optical characterization of sickle cell hemoglobin gelation.

We have used two techniques to characterize the gelation of deoxyhemoglobin S, a high sensitivity heat-flow calorimeter to measure the heat of gelation and a simple light-transmission method to measure the optical birefringence resulting from the alignment of deoxyhemoglobin S fibers in the gel. A theory for the interpretation of the birefringence measurements is presented. We combine the results of the calorimetric and optical measurements with those of sedimentation experiments to obtain enthalpy changes for gelation. The enthalpy change obtained from scanning and isothermal calorimetric measurements (0.25 m-potassium phosphate, 0.05 m-sodium dithionite, pH 6.9) varies from 4000 to 2200 cal mol⁻¹ hemoglobin between 16 and 25 °C. There is a large apparent heat capacity change of −130 to −190 cal deg.⁻¹ mol⁻¹. The apparent enthalpy change estimated from solubility measurements and birefringence melting experiments is 2200 ± 500 cal mol⁻¹ in qualitative agreement with the calorimetric results. Analysis of the time dependence of the calorimetric and optical progress curves at 20 °C leads to a rough estimate of 1800 to 4000 and −800 to 1500 cal mol⁻¹ hemoglobin for the enthalpies of polymerization and alignment of fibers, respectively. The small magnitude of the observed enthalpy change is in accord with the view that no large conformational change takes place in the deoxyhemoglobin S molecule upon gelation.     

P-31 nuclear magnetic resonance studies of the appearance of an isotropic component in dielaidoylphosphatidylethanolamine.

We have utilized phosphorus nuclear magnetic resonance, which provides an excellent means of characterizing the physical state of lipids, to investigate the polymorphic phase behavior of pure dielaidoylphosphatidylethanolamine (DEPE). We have observed a sharp isotropic component in the typical bilayer and inverted hexagonal P-31 NMR spectra. This component appears in the spectra of both the bilayer and inverted hexagonal lipid phases after several cycles through the bilayer-to-hexagonal phase transition. The magnitude of the isotropic component increased as a function of the number of cycles through the transition. The appearance of this component was not a function of time at constant temperature, but only a function of the number of cycles through the transition. The isotropic component is stable at all temperatures above the gel-to-liquid crystal transition, but it abruptly disappears when the lipid is cooled below the gel-to-liquid crystal phase transition. It is suggested that this isotropic phase is similar to the isotropic phase observed in dioleoylphosphatidylethanolamine (DOPE) by x-ray diffraction and identified as a cubic phase (Shyamsunder, E., S. M. Gruner, M. W. Tate, D. C. Turner, P. T. C. So, and C. P. S. Tilcock. 1988. Biochemistry. 27:2332-2336).     

Diacylglycerols, lysolecithin, or hydrocarbons markedly alter the bilayer to hexagonal phase transition temperature of phosphatidylethanolamines

The bilayer to hexagonal phase transition temperatures of dielaidoylphosphatidylethanolamine and 1-palmitoyl-2-oleoylphosphatidylethanolamine are 65.6 and 71.4 degrees C, respectively. Using high-sensitivity differential scanning calorimetry, I have shown that these transition temperatures are extremely sensitive to the presence of small amounts of other lipid components. For example, at a mole fraction of only 0.01, dilinolenin lowers the bilayer to hexagonal phase transition temperature of 1-palmitoyl-2-oleoyl-phosphatidylethanolamine by 8.5 degrees C. Other diacylglycerols have similar effects on this transition temperature, although the degree of unsaturation of the acyl chains has some effect, with distearin being less potent. In comparison, the 20-carbon alkane eicosane lowers this transition temperature by 5 degrees C, while palmitoyl-lysolecithin raises it by 2.5 degrees C. Similar effects of these additives on the bilayer to to hexagonal phase transition temperature are observed with dielaidoylphosphatidylethanolamine. At these concentrations of additive, there is no effect on the gel-state to liquid-crystalline-state transition temperature. The observed shifts in the temperature of the bilayer to the hexagonal phase transition can be qualitatively interpreted in terms of the effects of these additives on the hydrophilic surface area and on the hydrophobic volume. Substances expanding the hydrophobic domain promote hexagonal phase formation and lower the bilayer to hexagonal phase transition temperature. The sensitivity of the bilayer to hexagonal phase transition temperature to the presence of additives is at least as great as that which has been observed for any other lipid phase transition.     

The phase behaviour of 1,2-diacyl-3-monogalactosyl-sn-glycerol derivatives

Monogalactosyldiacylglycerol was isolated from the blue-green alga Anacystis nidulans. Part of this lipid, which is rich in the 1–16:1/2–16:0 derivative, was hydrogenated to yield a lipid fraction rich in the 1–16:0/2–16:0 derivative. The phase behaviour of the two fractions were studied using differential scanning calorimetry, wide-angle X-ray diffraction and freeze-fracture electron microscopy. Both fractions exhibited complex polymorphic behaviour. Two distinct gel phases were identified; a stable form (MGDG₁) and a metastable form (MGDG_II). The transition temperatures for the two forms were 345 K and 325 K for the 1–16:0/2–16:0 fraction and 311 K and 279 K for the 1–16:1/2–16:0 fraction, respectively. The corresponding enthalpy values were 59.3 and 24.5 kJ · mol⁻¹ and 51.4 and 11.5 kJ · mol⁻¹. Inverted hexagonal (H₁₁) phases were seen at higher temperatures. The transition to the H₁₁ phase appears to occur directly from MGDG₁ gel phase, but may involve the formation of a lamellar liquid -crystalline phase existing between the melting points of the two gel phases in the case of the transitions from the MGDG₁₁ gel phase.     

Interaction of melittin with dimyristoyl phosphatidylcholine liposomes. Evidence for boundary lipid by raman spectroscopy

The interaction of melittin, a polypeptide consisting of 26 amino acid residues, with dimyristoyl phosphatidylcholine bilayers was investigated by vibrational Raman spectroscopy. Spectral peak height intensity ratios, involving vibrational transitions in both the 3000 cm^?1 acyl chain methylene carbon-hydrogen stretching mode region and the 1100 cm^?1 acyl chain carbon-carbon skeletal stretching mode interval, served as temperature profile indices for monitoring the bilayer order-disorder processes. For a lipid : melittin molar ratio of 14 : 1 two order-disorder transitions were observed. In comparison to a gel to liquid crystalline phase transition of 22.5°C for the pure lipid, the lower transition, exhibiting a 2°C width, is centered at 17°C and is associated with a depression of the main lipid phase transition of dimyristoyl phosphatidylcholine. The second thermal transition, displaying a 7°C interval, occurs at approx. 29°C and is associated with the melting behavior of approximately seven immobilized boundary lipids which surround the inserted hydrophobic segment of the polypeptide. For a lipid : melittin molar ratio of 10 : 1 two thermal transitions are also observed at 11 and 30°C. As before, they represent, respectively, the main gel to liquid crystalline phase transition and the melting behavior of approximately four boundary lipids attached to melittin. From these data alternative schemes are suggested for disposing the immobilized lipids around the hydrophobic portion of the polypeptide within the bilayer.     

Effects of temperature and molecular interactions on the vibrational infrared spectra of phospholipid vesicles

Infrared spectra were obtained as a function of temperature for a variety of phospholipid/water bilayer assemblies (80% water by weight) in the 3000-950 cm^?1 region. Spectral band-maximum frequency parameters were defined for the 2900 cm^?1 hydrocarbon chain methylene symmetric and asymmetric stretching vibrations. Temperature shifts for these band-maximum frequencies provided convenient probes for monitoring the phase transition behavior of both multilamellar liposomes and small diameter single-shell vesiclesof dipalmitoyl phosphatidylcholine/water dispersions. As examples of the effects of bilayer lipid/cholesterol/water (3 : 1 mol ratio) and lipid/cholesterol/amphotericin B/water (3 : 1 : 0.1 mol ratios) vesicles were examined using the methylene stretching frequency indices. In comparison to the pure vesicle form, the transition width of the lipid/cholesterol system increased by nearly a factor of two (to 8°C) while the phase transition temperature remained approximately the same (41° C). For the lipid/cholesterol/amphotericin B system, the phase transition temperature increased by about 4.5° C (to 45.5°C) with the transition width increasing by nearly a factor of four ($\text{to}\text{≈ 15°}\text{C}$) above that of the pure vesicles. The lipid/cholesterol/amphotericin B data were interpreted as reflecting the formation below 38°C of a cholesterol/amphotericin B complex whose dissociation at higher temperature (38–60°C range) significantly broades the gel-liquid crystalline phase transition.     

Effects of temperature on metabolic rate and lower dissolved oxygen tolerance of juvenile speckled peacock bass Cichla temensis

The speckled peacock bass Cichla temensis is a popular sport and food fish that generates substantial angling tourism and utilitarian harvest within its range. Its popularity and value make this species important for management and a potential aquaculture candidate for both fisheries enhancement and food fish production. However, little is known of optimal physiochemical conditions in natural habitats, which also are important for the development of hatchery protocols for handling, spawning and grow-out. Speckled peacock bass have been documented to have high sensitivity to extreme temperatures, but the metabolic underpinnings have not been evaluated. In this study, the effects of temperature (25, 30 and 35°C) on the standard metabolic rate (SMR) and lower dissolved oxygen tolerance (LDOT) of juvenile speckled peacock bass (mean ± standard error total length 153 ± 2 mm and wet weight 39.09 ± 1.37 g) were evaluated using intermittent respirometers after an acclimation period of 2 weeks. Speckled peacock bass had the highest SMR at 35°C (345.56 ± 19.89 mgO₂ kg⁻¹ h⁻¹), followed by 30°C (208.16 ± 12.45 mgO₂ kg⁻¹ h⁻¹) and 25°C (144.09 ± 10.43 mgO₂ kg⁻¹ h⁻¹). Correspondingly, the Q₁₀, or rate of increase in aerobic metabolic rate (MO₂) relative to 10°C, for 30–35°C was also greater (2.76) than from 25 to 30°C (2.08). Similarly, speckled peacock bass were the most sensitive to hypoxia at the warmest temperature, with an LDOT at pO₂ of 90 mmHg (4.13 mg l⁻¹) at 35°C compared to pO₂ values of 45 mmHg (2.22 mg l⁻¹) and 30 mmHg (1.61 mg l⁻¹) at 30 and 25°C, respectively. These results indicate that speckled peacock bass are sensitive to temperatures near 35°C, therefore we recommend managing and rearing this species at 25–30°C.     

Thermodynamic and structural properties of phosphatidylserine bilayer membranes in the presence of lithium ions and protons

The binding of lithium ions to phosphatidylserine has been studied by differential scanning calorimetry for dialkyl and diacyl lipid forms and by X-ray diffraction for dihexadecylphosphatidylserine (DHPS). On first mixing DHPS with LiCl solutions an ordered L_β (L_c) phase is formed with a bilayer repeat distance of 5.55 nm and one strong wide-angle, chain-chain reflection at 0.405 nm (26°C), corresponding to bilayers of little, (mono)hydrated lipid with chains approximately perpendicular to the membrane surface. On heating, this phase transforms to an inverted hexagonal phase (H₁₁, H_α) with a repeat distance of 3.75 nm, at a chain-melting transition temperature of approximately 90°C (DHPS). Cooling, after equilibration of the DHPS⁻·Li⁺ sample in the fluid phase, creates a new low-temperature phase (L_c') which has a repeat distance of 4.0 nm, corresponding to strongly tilted chains (ϕ=42°). The L_c phase also transforms on heating to the H_α phase, but at a considerably lower chain-melting temperature of approx. 70°C (DHPS). The calorimetric behavior as a function of Li⁺ concentration is qualitatively very similar for the different dialkyl- and diacylphosphatidylserines studied, and is analogous to the results obtained on pH titration. After an initial small increase in transition temperature, that is caused by coulombic ion binding and concomitant surface charge neutralization, a much larger increase in the chain-melting transition temperature occurs, caused by dehydration of the lipid, as a consequence of a further stereospecific ion binding. This suggests that Li⁺ and H⁺ have similar binding sites on the PS headgroup.     

Helix-coil dynamics of a Z-helix hairpin

The helix–coil transition of a Z-helix hairpin formed from d(C-G)₅T₄(C-G)₅ has been characterized by equilibrium melting and temperature jump experiments in 5M NaClO₄ and 10 mM Na₂HPO₄, pH 7.0. The melting curve can be represented by a simple all-or-none transition with a midpoint at 81.6 ± 0.4°C and an enthalpy change of 287 ± 15 kJ/mole. The temperature jump relaxation can be described by single exponentials at a reasonable accuracy. Amplitudes measured as a function of temperature provide equilibrium parameters consistent with those derived from equilibrium melting curves. The rate constants of Z-helix formation are found in the range from 1800 s^?1 at 70°C to 800 s^?1 at 90°C and are associated with an activation enthalpy of ?(50 ± 10) kJ/mole, whereas the rate constants of helix dissociation are found in the range from 200 s^?1 at 70°C to 4500 s^?1 at 90°C with an activation enthalpy +235 kJ/mole. These parameters are consistent with a requirement of 3–4 base pairs for helix nucleation. Apparently nucleation occurs in the Z-helix conformation, because a separate slow step corresponding to a B to Z transition has not been observed. In summary, the dynamics of the Z-helix–coil transition is very similar to that of previously investigated right-handed double helices.     

Barrier properties of glycophorin-phospholipid systems prepared by different methods

Glycophorin was incorporated into large unilamellar dioleoylphosphatidylcholine vesicles by either a detergent dialysis method using octylglucoside or a method avoiding the use of detergents. The vesicles were characterized and the permeability properties and transbilayer movement of lipids in both vesicles were investigated as a function of the protein concentration and were compared to protein-free vesicles. An insight in the permeability properties of the vesicles was obtained by monitoring the ratio potassium (permeant): dextran (impermeant) trap immediately after separation of the vesicles from the external medium. Glycophorin incorporated without the use of detergents in 1:300 protein:lipid molar ratio induces a high potassium permeability for the majority of the vesicles as judged from the low potassium trap (K⁺:dextran trap = 0.21). In contrast, the vesicles in which glycophorin is incorporated via the octylglucoside method (1:500 protein:lipid molar ratio) are much less permeable to potassium (K⁺:dextran trap = 0.67 and $\text{t}\text{1}\text{2}$ of potassium efflux at 22°C is 7.5 h.). The relationship between protein-induced bilayer permeability and lipid transbilayer movement in both vesicle preparations is discussed. Addition of wheat-germ agglutinin to glycophorin-containing vesicles comprised of dioleoylphosphatidylcholine and total erythrocyte lipids caused no or just a small effect (less than 20% release of potassium) on the potassium permeability of these vesicles. Also, addition of lectin to dioleoylphosphatidylethanolamine-glycophorin bilayer vesicles in a 25:1 lipid:glycophorin molar ratio had no effect on the permeability characteristics of the vesicles. In contrast, addition of wheat-germ agglutinin to bilayer vesicles made of dioleoylphosphatidylethanolamine and glycophorin in a 200:1 molar ratio resulted in a release of 74% of the enclosed potassium by triggering a bilayer to hexagonal (H_II) phase transition. The role of protein aggregation and the formation of defects in the lipid bilayer on membrane permeability and lipid transbilayer movement is discussed.     

Phase behavior of the major lipids of Tetrahymena ciliary membranes

The major lipids of Tetrahymena membranes have been purified by thin-layer and high pressure liquid chromatography and the phosphatidylethanolamine and aminoethylphosphonate lipids were examined in detail. ³¹P-NMR, X-ray diffraction and freeze-fracture electron microscopy were employed to describe the phase behavior of these lipids. The phosphatidylethanolamine was found to form a hexagonal phase above 10°C. The aminoethylphosphonate formed a lamellar phase up to 20°C, but converted to a hexagonal phase structure at 40°C. Small amounts of phosphatidylcholine stabilized the lamellar phase for the aminoethylphosphonate. ³¹P-NMR spectra of the intact ciliary membranes were consistent with a phospholipid bilayer at 30°C, suggesting that phosphatidylcholine in the membrane stabilized the lamellar form, even though most of the lipid of that membrane prefers a hexagonal phase in pure form at 30°C. ³¹P-NMR spectra also showed a distinctive difference in the chemical shift tensor of the aminoethylphosphonolipid, when compared to that of phosphatidylethanolamine, due to the difference in chemical structure of the polar headgroups of the two lipids.     

Discontinuous gas exchange patterns of beet armyworm pupae, Spodoptera exigua (Lepidoptera: Noctuidae): effects of Bacillus thuringiensis Cry1C toxin, pupal age and temperature

Abstract. Changes in the discontinuous gas exchange cycle of pupal beet armyworm, Spodoptera exigua (Hübner) (Lepidoptera: Noctuidae), exposed or not to Cry1C Bacillus thuringiensis toxin, are examined against developmental age (1–7 days) and at different temperatures (10–25 °C) using flow through respirometry. Both exposed and nonexposed pupae exhibit discontinuous gas exchange, but only at 10 °C; the frequency of cyclic release of CO₂ increases with increasing temperatures. The three phases of the discontinuous gas exchange cycle are distinct for both treatment groups. However, the duration of each phase is significantly greater for pupae exposed previously to toxin. The closed phase is 40 ± 14% longer, the flutter phase 23 ± 19% longer, and the open phase is 28 ± 12% longer when pupae were exposed to toxin. Respiratory water loss is 4.5 ± 1.3% for toxin exposed pupae and 2.1 ± 2.4% for unexposed pupae. Furthermore, the exposed pupae have significantly greater cuticular permeability (26.01 ± 1.9 µg cm⁻² h⁻¹ mmHg⁻¹) than the nonexposed pupae (9.64 ± 0.9 µg cm⁻² h⁻¹ mmHg⁻¹). However, in both strains, cuticular transpiration (>93%) far exceeds respiratory transpiration. Overall, total water loss is significantly greater in pupae whose larvae are exposed to toxin compared with pupae from nontreated larvae. Toxin exposed pupae have a mean cycle duration of 60 ± 2.5 min whereas that of nonexposed pupae is 42 ± 1.8 min.(ml g⁻¹ h⁻¹) of the open phase is greater earlier in pupal life followed by a minimum at mid-pupal stage and an increase at late-pupal development in both treatment groups. Combining all 7 days, closed, flutter and open phase (ml g⁻¹ h⁻¹), pupae exposed to toxin produce significantly more CO₂ during each phase. On average, toxin exposed pupae produce 52 ± 12, 43 ± 10 and 15 ± 37% more CO₂ than the untreated pupae during the closed, flutter and open phases, respectively. Therefore, the present study reinforces the need to use insects of similar developmental age in studies of insect respiration patterns and energy metabolism.     

Production enhancement of poly(3-hydroxybutyrate-co-3-hydroxyvalerate) in Halogeometricum borinquense,characterization of the bioplastic and desalination of the bioreactor effluent

Polyhydroxyalkanoates (PHAs) are a replacement of conventional single-use plastics. Bioprocess conditions of the extreme halophilic archaeon Halogeometricum borinquense strain RM-G1 were selected resulting in the synthesis of 66.80 ± 1.69 % PHA (of cell dry mass) in 72 h using glycerol and tryptone as carbon and nitrogen sources respectively, yielding volumetric productivity of 0.206 ± 0.006 gL⁻¹ h⁻¹ in a repeated batch process in a small-scale bioreactor where 20 % of the production medium was used as the inoculum for the subsequent batch. The purified PHA was characterized as poly(3-hydroxybutyrate-co-3-hydroxyvalerate) with 10.21 mol% 3-hydroxyvalerate content possessing glass transition temperature -12.6 °C, degradation temperature 285 °C, number average molecular weight 156,899 Da, weight average molecular weight 288,723 Da, polydispersity index 1.8 and melting temperatures 139.1 °C and 152.5 °C. Maximum (21.7 ± 0.6 L m^-2 h⁻¹) and average (17.2 ± 0.6 L m^-2 h⁻¹) flux values were their respective highest and crystallization time was its least (3.0 ± 0.16 h) when ΔT was 90 °C and polytetrafluoroethylene membrane was applied for desalination of the bioreactor effluent by Direct Contact Membrane Distillation. While using polyvinylidene fluoride membrane, maximum 25.5 ± 0.5 L m^-2 h⁻¹ and average 18.6 ± 0.2 L m^-2 h⁻¹ fluxes were obtained and crystallization time decreased (3.25 ± 0.16 h) even when ΔT was lowered by 20 °C.     

Intramolecular excimer formation of pyrene-labeled lipids in lamellar and inverted hexagonal phases of lipid mixtures containing unsaturated phosphatidylethanolamine

The rates of intramolecular excimer formation of di(1'-pyrenemyristoyl)phosphatidylcholine (dipyPC) in dioleoylphosphatidylethanolamine (DOPE), egg PE/diolein (DG) and dilinoleoyl-PE (DLPE)/1-palmitoyl-2-oleoyl-PC (POPC) were studied at different temperatures and lipid compositions. Both the excimer-to-monomer intensity ratio and the excimer association rate constant were employed to quantify the rate of excimer formation. The latter was calculated from the measured monomer fluorescence lifetime of dipyPC. We observed that the rate of excimer formation was sensitive to either the temperature-induced or lipid composition-induced lamellar-to-inverted hexagonal phase transition of the above lipid systems. As the lipids entered the inverted hexagonal phase, the rate of excimer formation increased at the temperature-induced phase transition for DOPE, but decreased at the composition-induced phase transition for both TPE/DG and DLPE/POPC systems by increasing the DG% and decreasing the PC%, respectively. We conclude that the rate of intramolecular excimer formation of dipyPC in the non-lamellar phase is influenced both by the intra-lipid free volume of the hydrocarbon region and the intra-rotational dynamics of the two lipid acyl chains.