Interaction of nucleic acids with lipid membranes

The thermodynamics of nucleic acids which were enclosed in reverse-phase evaporation vesicles was studied by thermal denaturation with optical recording. The denaturation curves were recorded with a dual wavelength spectrophotometer. The sum of the hypochromicity of the nucleic acid and of the change in turbidity of the vesicles was measured at 260 nm and was corrected for the change in turbidity at 320 nm. Cloned fragments of double-stranded DNA containing 180 base pairs and poly A:poly U were enclosed in REV with a yield up to every vesicle containing five nucleic acid molecules. Vesicles were prepared from egg-lecithin, and the surface charge of the vesicles was varied by addition of stearic acid, phosphatidyl-glycerol and phosphatidyl-serine. The helix-coil transition of the nucleic acid enclosed in the vesicle could be resolved from that of the free nucleic acid. Due to the enclosure into the egg-lecithin REV the transition is stabilized from 70.5 degrees to 74 degrees C, the transition is broadened from 0.7 degrees C to 2.7 degrees C. Varying the phosphatidyl-serine-lecithin-ratio from 0-100%, an optimum in the yield of enclosure at 20% was obtained, a further broadening of the transition to 5.5 degrees C and a decrease of the stabilization down to a small destabilization at 100% phosphatidyl serine was observed. Qualitatively, similar effects were observed with poly A:poly U. Variation of the ionic strength led to the conclusion that the replacement of the counterions of the phosphate backbone by the surface charge of the membrane, as well as a direct contact between the nucleic acid and the membrane have to be assumed.(ABSTRACT TRUNCATED AT 250 WORDS)     

Interaction of Nucleic Acids with Lipid Membranes

Abstract

The thermodynamics of nucleic acids which were enclosed in reverse-phase evaporation vesicles was studied by thermal denaturation with optical recording. The denaturation curves were recorded with a dual wavelength spectrophotometer. The sum of the hypochromicity of the nucleic acid and of the change in turbidity of the vesicles was measured at 260 nm and was corrected for the change in turbidity at 320 nm. Cloned fragments of double-stranded DNA containing 180 base pairs and poly A:poly U were enclosed in REV with a yield up to every vesicle containing five nucleic acid molecules. Vesicles were prepared from egg- lecithin, and the surface charge of the vesicles was varied by addition of stearic acid, phosphatidyl-glycerol and phosphatidyl-serine. The helix-coil transition of the nucleic acid enclosed in the vesicle could be resolved from that of the free nucleic acid. Due to the enclosure into the egg-lecithin REV the transition is stabilized from 70.5° to 74°C, the transition is broadened from 0.7°C to 2.7°C. Varying the phosphatidyl-serine-lecithin-ratio from 0–100%, an optimum in the yield of enclosure at 20% was obtained, a further broadening of the transition to 5.5°C and a decrease of the stabilization down to a small destabilization at 100% phosphatidyl serine was observed. Qualitatively, similar effects were observed with poly A:poly U. Variation of the ionic strength led to the conclusion that the replacement of the counterions of the phosphate backbone by the surface charge of the membrane, as well as a direct contact between the nucleic acid and the membrane have to be assumed. At present, the biological relevance of the results may be more in the drastic decrease in cooperativity than in the slight modulation of the stability. From nearly 180 base pairs opening up cooperatively in free nucleic acid this number is lowered to less than 50, a size in the range of promotor regions.     

Calorimetric and spectroscopic investigation of the unfolding of human apolipoprotein B

The unfolding of human apolipoprotein B-100 in its native lipid environment, low density lipoprotein (LDL), and in a soluble, lipid-free complex with sodium deoxycholate (NaDC) has been examined using differential scanning calorimetry (DSC) and near UV circular dichroic (CD) spectroscopy. High resolution DSC shows that LDL undergoes three thermal transitions. The first is reversible and corresponds to the order-disorder transition of the core-located cholesteryl esters (CE) (Tm = 31.1 degrees C, delta H = 0.75 cal/g CE). The second, previously unreported, is reversible with heating up to 65 degrees C (Tm = 57.1 degrees C, delta H = 0.20 cal/g apoB) and coincides with a reversible change in the tertiary structure of apoB as shown by near UV-CD. No alteration in the secondary structure of apoB is observed over this temperature range. The third transition is irreversible (Tm = 73.5 degrees C, delta H = 0.99 cal/g apoB) and coincides with disruption of the LDL particle and denaturation of apoB. The ratio of delta H/delta HvH for the reversible protein-related transition suggests that this is a two-state event that correlates with a change in the overall tertiary structure of the entire apoB molecule. The second protein-related transition is complex and coincides with irreversible denaturation. ApoB solubilized in NaDC undergoes three thermal transitions. The first two are reversible (Tm = 49.7 degrees C, delta H = 1.13 cal/g apoB; Tm = 56.4 degrees C, delta H = 2.55 cal/g apoB, respectively) and coincide with alterations in both secondary and tertiary structure of apoB. The changes in secondary structure reflect an increase in random coil conformation with a concomitant decrease in beta-structure, while the change in tertiary structure suggests that the conformation of the disulfide bonds is altered. The third transition is irreversible (Tm = 66.6 degrees C, delta H = 0.54 cal/g apoB) and coincides with complete denaturation of apoB and disruption of the NaDC micelle. The ratio of delta H/delta HvH for the two reversible transitions indicates that each of these transitions is complex which may suggest that several regions or domains of apoB are involved in each thermal event.     

Thermal unfolding and aggregation of human complement protein C9: a differential scanning calorimetry study

The thermotropic behavior of purified human complement protein C9 was investigated by high-sensitivity differential scanning calorimetry. When dissolved in physiological buffers (pH 7.2, 150 mM NaCl), C9 underwent three endothermic transitions with transition temperatures (Tm) centered at about 32, 48, and 53 degrees C, respectively, and one exothermic transition above 64 degrees C that correlated with protein aggregation. The associated calorimetric enthalpies of the three endothermic transitions were about 45, 60, and 161 kcal/mol with cooperative ratios (delta Hcal/delta HvH) close to unity. The total calorimetric enthalphy for the unfolding process was in the range of 260-280 kcal/mol under all conditions. The exothermic aggregation temperature was strongly pH dependent, changing from 60 degrees C at pH 6.6 to 81.4 degrees C at pH 8.0, whereas none of the three endothermic transitions was significantly affected by pH changes. They were, however, sensitive to addition of calcium ions; most affected was Tm1 which shifted from 32 to 35.8 degrees C in the presence of 3 mM calcium, i.e., the normal blood concentration. Kosmotropic ions stabilized the protein by shifting the endothermic transitions to slightly higher temperatures whereas inclusion of chaotropic ions (such as choline), removal of bound calcium by addition of EDTA, or proteolysis with thrombin lowered the transition temperatures. Previous studies had indicated the formation of at least three different forms of C9 during membrane insertion or during heat polymerization, and it is suggested that the three endothermic transitions reflect the formation of such C9 conformers. Choline, which is present at high concentrations on the surface of biological membranes, and calcium ions have the ability to shift the transition temperatures of the first two transitions to be either close to or below body temperature. Thus, it is very likely that C9 is present in vivo in a partially unfolded state when bound to a membrane surface, and we propose that this facilitates membrane insertion and refolding of the protein into an amphiphilic conformation.     

Differences in thermal stability between reduced and oxidized cytochrome b562 from Escherichia coli

The thermal stabilities of ferri- and ferrocytochrome b562 were examined. Thermally induced spectral changes, monitored by absorption and second-derivative spectroscopies, followed the dissociation of the heme moiety and the increased solvation of tyrosine residue(s) located in close proximity to the heme binding site. All observed thermal transitions were independent of the rate of temperature increase (0.5-2 degrees C/min), and the denatured protein exhibited partial to near-complete reversibility upon return to ambient temperature. The extent of renaturation of cytochrome b562 is dependent on the amount of time the unfolded conformer is exposed to temperatures above the transition temperature, Tm. All thermally induced spectra changes fit a simple two-state model, and the thermal transition was assumed to be reversible. The thermal transition for ferrocytochrome b562 yielded Tm and van't Hoff enthalpy (delta HvH) values of 81.0 degrees C and 137 kcal/mol, respectively. In contrast, Tm and delta HvH values obtained for the ferricytochrome were 66.7 degrees C and 110 kcal/mol, respectively. The estimated increase in the stabilization free energy at the Tm of ferricytochrome b562 following the one-electron reduction to the ferrous form, where delta delta G = delta Tm delta Sm [delta Sm = 324 cal/(K.mol), delta Tm = 14.3 degrees C] [Becktel, W. J., & Schellman, J. A. (1987) Biopolymers 26, 1859-1877], is 4.6 kcal/mol.     

Relationship of hyperthermia-induced hemolysis of human erythrocytes to the thermal denaturation of membrane proteins

Hemolysis of human erythrocytes as a function of time of exposure to 47.4-54.5 degrees C was measured and correlated to thermal transitions in the membranes of intact erythrocytes as determined by differential scanning calorimetry (DSC). Curves of hemoglobin leakage (a measure of hemolysis) as a function of time have a shoulder region exhibiting no leakage, indicative of the ability to accumulate sublethal damage (i.e., damage not sufficient to cause lysis), followed by a region of leakage approximating pseudo-first-order kinetics. Inverse leakage rates (Do) of 330-21 min were obtained from 47.4-54.5 degrees C, respectively. A relatively high activation energy of 304 +/- 22 kJ/mol was obtained for leakage, eliminating the involvement of metabolic processes but implicating a transition as the rate-limiting step. Membrane protein involvement was suggested by the very low rate (10(-2) of the rate from erythrocytes) and low activation energy (50 +/- 49 kJ/mol) of hemoglobin leakage from liposomes containing no membrane protein. A model was developed that predicts a transition temperature (Tm) for the critical target (rate-limiting step) of 60 degrees C when measured at a scan rate of 1 K/min. DSC scans were obtained from intact erythrocytes and a procedure developed to fit and remove the transition for hemoglobin denaturation which dominated the scan. Three transitions remained (transitions A, B, and C) with Tm values of 50.0, 56.8, and 63.8 degrees C, respectively. These correspond to, but occur at slightly different temperatures than, the A, B, and C transitions of isolated erythrocyte membranes in the same salt solution (Tm = 49.5, 53-58, and 65.5 degrees C, respectively). In addition, the relative enthalpies of the three transitions differ between isolated membranes and erythrocytes, suggestive of membrane alterations occurring during isolation. Thus, all analyses were conducted on DSC scans of intact erythrocytes. The B transition is very broad and probably consists of several transitions. An inflection, which is seen as a distinct peak (transition B3) in fourth-derivative curves, occurs at 60.8 degrees C and correlates well with the predicted Tm of the critical target. Ethanol (2.2%) lowers the Tm of B3 by 4.0-4.5 K, close to the shift of 3.3 K predicted from its effect on hemolysis. Glycerol (10%) has very little effect on both hemolysis and the Tm of B3, but it stabilizes spectrin (delta Tm = 1.5 K) against thermal denaturation.(ABSTRACT TRUNCATED AT 400 WORDS)     

Effect of polynucleotide adsorption on characteristics of a planar phosphatidylcholine bilayer membrane

Interaction of DNA with planar bilayer phosphatidylcholine membrane in the presence of CaCl2 increases electric conductance of the membrane several times as a result of the formation of DNA-membrane complex. The same effect was observed in the cases of ribosomal RNA and synthetic homopolymers polyA, polyU and polyA X polyU double helix.     

Effects of pressure and temperature on the M412 intermediate of the bacteriorhodopsin photocycle. Implications for the phase transition of the purple membrane

The effects of pressure and temperature on the decay kinetics of the M412 (M) intermediate in the photocycle of bacteriorhodopsin were studied to provide information about the phase transitions of the purple membrane lipids. The activation volume (delta V++) for the decay of M is expected to be different below and above a phase transition. However, no abrupt change in delta V++ was found from 3.5 degrees to 60 degrees C. But a sharp break was observed in a plot of the logarithm of the rate of M decay vs. pressure. Extrapolation of this break point to standard atmospheric pressure gives a temperature of -42 degrees C, which probably corresponds to the phase transition of the purple membrane lipids. This conclusion is supported by studies of the effect of pressure on the M kinetics of bacteriorhodopsin incorporated into dimyristoylphosphatidylcholine vesicles, whose phase transition has previously been characterized.     

Monolayer coupling in phosphatidylserine bilayers: distinct phase transitions induced by magnesium interacting with one or both monolayers

We have investigated the thermotropic behavior of phospatidylserine bilayers interacting with Mg2+ either on one side or both sides, using differential scanning calorimetry. Large unilamellar vesicles (LUV) of phosphatidylserine exposed to Mg2+ on the external side only displayed an upward shift of the gel-liquid transition temperature (Tm) of about 6-8 degrees C relative to the Tm of LUV in Na+. Mg2+ was shown not to enter the vesicle interior, by means of fluorescence measurements on encapsulated 8-hydroxyquinoline-5-sulfonate. Multilamellar vesicles prepared in the presence of Mg2+, or vesicles prepared by Mg2+-induced fusion of small unilamellar vesicles, had Tm values that were shifted upward by about 16-17 C degrees. When the latter preparation was treated with EDTA to produce vesicles with Mg2+ inside and Na+ outside, the Tm was found to be shifted again by only 6-8 degrees C. These observations indicate that the monolayer interacting with Na+ fluidizes the monolayer interacting with Mg2+, and that the latter tends to solidify the former. The two monolayers thus appear to be coupled, possibly by hydrocarbon chain interdigitation.     

Characterization of thermotropic structural transitions of the erythrocyte membrane: a biochemical and electron-paramagnetic resonance approach

The relationship between membrane structural properties and functions has been generally inferred from observed thermotropic phenomena. By the use of 16-dinyloxyl stearic acid spin probe we investigated the red blood cell membrane components involved in three characteristic thermotropic structural transitions occurring at 8, 20, and 40 degrees C. The transition at 8 degrees C is removed by chymotrypsin treatment at the cytoplasmic membrane layer. The 20 degrees C phase transition is unmodified after chymotrypsin treatment and occurs at 15 degrees C after complete proteolysis of intramembrane chymotrypsin-insensitive peptides. Liposomes from the total lipid extract of RBC show only one thermotropic transition at 15 degrees C. The 40 degrees C phase transition is absent in vesicles free of skeletal proteins, in vesicles obtained after RBC storage, and in low-ionic-strength resealed ghosts. Transitions at 8 degrees C and 40 degrees C appear to be due to the interactions of cytoplasmic exposed proteins with membrane, whereas the 20 degrees C transition is intrinsic to the lipid component.     

Cholesterol affects divalent cation-induced fusion and isothermal phase transitions of phospholipid membranes

The influence of cholesterol on divalent cation-induced fusion and isothermal phase transitions of large unilamellar vesicles composed of phosphatidylserine (PS) was investigated. Vesicle fusion was monitored by the terbium/dipicolinic acid assay for the intermixing of internal aqueous contents, in the temperature range 10-40 degrees C. The fusogenic activity of the cations decreases in the sequence Ca2+ greater than Ba2+ greater than Sr2+ much greater than Mg2+ for cholesterol concentrations in the range 20-40 mol%, and at all temperatures. Increasing the cholesterol concentration decreases the initial rate of fusion in the presence of Ca2+ and Ba2+ at 25 degrees C, reaching about 50% of the rate for pure PS at a mole fraction of 0.4. From 10 to 25 degrees C, Mg2+ is ineffective in causing fusion at all cholesterol concentrations. However, at 30 degrees C, Mg2+-induced fusion is observed with vesicles containing cholesterol. At 40 degrees C, Mg2+ induces slow fusion of pure PS vesicles, which is enhanced by the presence of cholesterol. Increasing the temperature also causes a monotonic increase in the rate of fusion induced by Ca2+, Ba2+ and Sr2+. The enhancement of the effect of cholesterol at high temperatures suggests that changes in hydrogen bonding and interbilayer hydration forces may be involved in the modulation of fusion by cholesterol. The phase behavior of PS/cholesterol membranes in the presence of Na+ and divalent cations was studied by differential scanning calorimetry. The temperature of the gel-liquid crystalline transition (Tm) in Na+ is lowered as the cholesterol content is increased, and the endotherm is broadened. Addition of divalent cations shifts the Tm upward, with a sequence of effectiveness Ba2+ greater than Sr2+ greater than Mg2+. The Tm of these complexes decreases as the cholesterol content is increased. Although the transition is not detectable for cholesterol concentrations of 40 and 50 mol% in the presence of Na+, Sr2+ or Mg2+, the addition of Ba2+ reveals endotherms with Tm progressively lower than that observed at 30 mol%. Although the presence of cholesterol appears to induce an isothermal gel-liquid crystalline transition by decreasing the Tm, this change in membrane fluidity does not enhance the rate of fusion, but rather decreases it. The effect of cholesterol on the fusion of PS/phosphatidylethanolamine (PE) vesicles was investigated by utilizing a resonance energy transfer assay for lipid mixing. The initial rate of fusion of PS/PE and PS/PE/cholesterol vesicles is saturated at high Mg2+ concentrations. With Ca2+, saturation is not observed for cholesterol-containing vesicles.(ABSTRACT TRUNCATED AT 400 WORDS)     

The effects of bilirubin on the thermal properties of phosphatidylcholine bilayers.

The thermotropic properties of multilamellar vesicles of dimyristoylphosphatidylcholine (DMPC), dipalmitoylphosphatidylcholine (DPPC), and distearoylphosphatidylcholine (DSPC), as a function of the concentration of bilirubin in the range of 0.1 to 1 mol%, were measured. The exact effects of bilirubin depended on the chain length of the polymethylene chains. But the general effects of bilirubin were the same in all systems. At the lowest concentrations tested (0.1 mol bilirubin/100 mol phospholipid (0.1 mol%)), bilirubin broadened and shifted to higher temperatures the main phase transitions of all bilayers. For DPPC and DSPC, but not DMPC, this concentration of bilirubin was associated with a new transition at 25 degrees C (DPPC) or 34 degrees C (DSPC). Bilirubin at 0.2 mol% was required for the detection of a similar transition (at 13.7 degrees C) in DMPC. Higher concentrations of bilirubin (> 0.2 mol%) suppressed completely the main phase transitions in all bilayers but increased the enthalpy of the new transition. Maximal values of delta H for these transitions were reached at 0.5, 0.25, and 0.2 mol% bilirubin in DMPC, DPPC, and DSPC, respectively. Values of delta H and delta S for these transitions were far larger than for the corresponding gel-to-liquid crystal transitions in pure lipid bilayers but were equal to those expected for a transition between crystalline and liquid crystalline phases.     

Phospholipid exchange between bilayer membranes.

The mode of interaction of aqueous dispersions of phospholipid vesicles is investigated. The vesicles (average diameter 950 A) are prepared from total lipid extracts of Escherichia coli composed of phosphatidylethanolamine, phosphatidylglycerol and cardiolipin. One type of vesicle contains trans-delta 9-octadecenoate, the other type trans-delta 9-hexadecenoate as predominant acyl chain component. The vesicles show order in equilibrium disorder transitions at transition temperatures, Tt = 42 degrees C and Tt = 29 degrees C, respectively. A mixture of these vesicles is incubated at 45 degrees C and lipid transfer is studied as a function of time using the phase transition as an indicator. The system reveals the following properties: Lipids are transferred between the two vesicle types giving rise to a vesicle population where both lipid components are homogeneously mixed. Lipid transfer is asymmetric, i.e. trans-delta 9-hexadecenoate-containing lipid molecules appear more rapidly in the trans-delta 9-octadecenoate-containing vesicles than vice versa. At a given molar ratio of the two types of vesicles the rate of lipid transfer is independent of the total vesicle concentration. It is concluded that lipid exchange through the water phase by way of single molecules or micelles is the mode of communication of these negatively charged lipid vesicles.     

The effects of lipid composition on the rate and extent of heme binding to membranes

The effects of membrane composition on heme binding to large unilamellar vesicles were examined using 30 separate phospholipid mixtures. Although there was some variation, most lecithins with Tm values less than or equal to 20 degrees C showed overall equilibrium partition constants equal to approximately 5 x 10(5) and association and dissociation partition rate constants equal to approximately 3 x 10(6) s-1 and 7 s-1, respectively, for CO-heme binding at 30 degrees C. A sharp decrease in the association rate for CO-heme uptake was observed as the lipid vesicles changed from liquid-crystalline to the gel phase. The addition of dicetyl phosphate or dimyristoylphosphatidylglycerol, which are negatively charged at neutral pH, decreased the affinity of the vesicles for CO-heme. The association rate and equilibrium partition constants for CO-heme uptake in unsaturated lecithins were unaffected by cholesterol content at levels up to 40%/mol. The affinity of saturated dimyristoylphosphatidylcholine (DMPC) vesicles for CO-heme decreased with increasing cholesterol content at 30 degrees C. This effect appears to be related to the influence of cholesterol on the DMPC phase transition temperature (Tm) since at low temperatures (less than or equal to 20 degrees C) little CO-heme binds to vesicles composed of DMPC even in the absence of cholesterol.     

Frequency-dependent electrodeformation of giant phospholipid vesicles in AC electric field

A model of vesicle electrodeformation is described which obtains a parametrized vesicle shape by minimizing the sum of the membrane bending energy and the energy due to the electric field. Both the vesicle membrane and the aqueous media inside and outside the vesicle are treated as leaky dielectrics, and the vesicle itself is modeled as a nearly spherical shape enclosed within a thin membrane. It is demonstrated (a) that the model achieves a good quantitative agreement with the experimentally determined prolate-to-oblate transition frequencies in the kilohertz range and (b) that the model can explain a phase diagram of shapes of giant phospholipid vesicles with respect to two parameters: the frequency of the applied alternating current electric field and the ratio of the electrical conductivities of the aqueous media inside and outside the vesicle, explored in a recent paper (S. Aranda et al., Biophys J 95:L19–L21, 2008). A possible use of the frequency-dependent shape transitions of phospholipid vesicles in conductometry of microliter samples is discussed.     

Energetics of diphtheria toxin membrane insertion and translocation: calorimetric characterization of the acid pH induced transition

The pH and temperature stabilities of diphtheria toxin and its fragments have been studied by high-sensitivity differential scanning calorimetry. These studies demonstrate that the pH-induced conformational transition associated with the mechanism of membrane insertion and translocation of the toxin involves a massive unfolding of the toxin molecule. At physiological temperatures (37 degrees C), this process is centered at pH 4.7 at low ionic strength and at pH 5.4 in the presence of 0.2 M NaCl. At pH 8, the thermal unfolding of the nucleotide-bound toxin is centered at 58.2 degrees C whereas that of the nucleotide-free toxin is centered at 51.8 degrees C, indicating that nucleotide binding (ApUp) stabilizes the native conformation of the toxin. The unfolding profile of the toxin is consistent with two transitions most likely corresponding to the A fragment (Tm = 54.5 degrees C) and the B fragment (Tm = 58.4 degrees C), as inferred from experiments using the isolated A fragment. These two transitions are not independent, judging from the fact that the isolated A fragment unfolds at much lower temperatures (Tm = 44.2 degrees C) and that the B fragment is insoluble in aqueous solutions when separated from the A fragment. Interfragment association contributes an extra -2.6 kcal/mol to the free energy of stabilization of the A fragment. Whereas the unfolding of the entire toxin is irreversible, the unfolding of the A fragment is a reversible process. These findings provide a thermodynamic basis for the refolding of the A fragment after reexposure to neutral pH immediately following translocation across the lysosomal membrane.     

Ion selectivity of temperature-induced and electric field induced pores in dipalmitoylphosphatidylcholine vesicles

Temperature and electric field are known to alter the permeability of the bilayer membrane in phospholipid vesicles. A study of cation selectivity of these membrane pores is reported for multilamellar liposomes (MLV) and unilamellar large vesicles (ULV, 95 +/- 5 nm diameter) of dipalmitoylphosphatidylcholine (DPPC). The permeability of ULV to Rb+ was 1.0 X 10(-6) micrograms/s at 22 degrees C and increased to 1.1 X 10(-5) micrograms/s at the gel to liquid-crystalline transition temperature (Tm) of the bilayer, at 42 degrees C. The permeability of ULV to Rb+ continued to increase beyond the Tm and reached 1.0 X 10(-4) micrograms/s at 56 degrees C, a 100-fold increase over the permeability at 22 degrees C. In contrast, the permeability of ULV to Na+ showed a local maximum of 6.0 X 10(-6) micrograms/s at 42 degrees C and decreased at temperatures higher or lower than the Tm. For MLV, the permeability to both Rb+ and Na+ peaked dramatically at the phase transition temperature, 42 degrees C, and subsided at lower and higher temperatures. When ULV were exposed to an electric field, the permeability to Rb+, Na+, and sucrose surged at a field strength of 30 kV/cm; 30 kV/cm can induce a transmembrane potential of 210 mV. In ULV, the electrically perforated lipid bilayer exhibited selectivity for Rb+ over Na+ only at a narrow electric field range, between 31 and 33 kV/cm. For MLV, no well-defined breakdown voltage was recorded.(ABSTRACT TRUNCATED AT 250 WORDS)     

Solute effects on the colloidal and phase behavior of lipid bilayer membranes: ethanol-dipalmitoylphosphatidylcholine mixtures.

By means of the scanning differential calorimetry, x-ray diffractometry, and the dynamic light scattering, we have systematically studied the phase and packing properties of dipalmitoylphosphatidylcholine vesicles or multibilayers in the presence of ethanol. We have also determined the partial ternary phase diagram of such dipalmitoylphosphatidylcholine/water/ethanol mixtures. The directly measured variability of the structural bilayer parameters implies that ethanol binding to the phospholipid bilayers increases the lateral as well as the transverse repulsion between the lipid molecules. This enlarges the hydrocarbon tilt (by up to 23 degrees) and molecular area (by < or = 40%). Ethanol-phospholid association also broadens the interface and, thus, promotes lipid headgroup solvation. This results in excessive swelling (by 130%) of the phosphatidylcholine bilayers in aqueous ethanol solutions. Lateral bilayer expansion, moreover, provokes a successive interdigitation of the hydrocarbon chains in the systems with bulk ethanol concentrations of 0.4-1.2 M. The hydrocarbon packing density as well as the propensity for the formation of lamellar gel phases simultaneously increase. The pretransition temperature of phosphatidylcholine bilayers is more sensitive to the addition of alcohol (initial shift: delta Tp = 22 degrees C/mol) than the subtransition temperature (delta Ts reversible 5 degrees C/mol), whereas the chain-melting phase transition temperature is even less affected (delta Tm = 1.8 degrees C/mol). After an initial decrease of 3 degrees for the bulk ethanol concentrations below 1.2 M, the Tm value increases by 2.5 degrees above this limiting concentration. The gel-phase phosphatidylcholine membranes below Tm are fully interdigitated above this limiting concentration. The chain tilt on the fringe of full chain interdigitation is zero and increases with higher ethanol concentrations. Above Tm, some of the lipid molecules are solubilized by the bound ethanol molecules. More highly concentrated ethanol solutions (> 7 M) solubilize the phosphatidylcholine bilayers with fluid chains fully and result in the formation of mixed lipid-alcohol micelles.     

A magnesium-induced conformational transition in the loop of a DNA analog of the yeast tRNA(Phe) anticodon is dependent on RNA-like modifications of the bases of the stem.

Two single-stranded DNA heptadecamers corresponding to the yeast tRNA(Phe) anticodon stem-loop were synthesized, and the solution structures of the oligonucleotides, d(CCAGACTGAAGATCTGG) and d(CCAGACTGAAGAU-m5C-UGG), were investigated using spectroscopic methods. The second, or modified, base sequence differs from that of DNA by RNA-like modifications at three positions; dT residues were replaced at positions 13 and 15 with dU, and the dC at position 14 with d(m5C), corresponding to positions where these nucleosides occur in tRNA(Phe). Both oligonucleotides form intramolecular structures at pH 7 in the absence of Mg2+ and undergo monophasic thermal denaturation transitions (Tm = 47 degrees C). However, in the presence of 10 mM Mg2+, the modified DNa adopted a structure that exhibited a biphasic "melting" transition (Tm values of 23 and 52 degrees C) whereas the unmodified DNA structure exhibited a monophasic denaturation (Tm = 52 degrees C). The low-temperature, Mg(2+)-dependent structural transition of the modified DNA was also detected using circular dichroism (CD) spectroscopy. No such transition was exhibited by the unmodified DNA. This transition, unique to the modified DNA, was dependent on divalent cations and occurred most efficiently with Mg2+; however, Ca2+ also stabilized the alternative conformation at low temperature. NMR studies showed that the predominant structure of the modified DNA in sodium phosphate (pH 7) buffer in the absence of Mg2+ was a hairpin containing a 7-nucleotide loop and a stem composed of 3 stable base pairs. In the Mg(2+)-stabilized conformation, the loop became a two-base turn due to the formation of two additional base pairs across the loop.(ABSTRACT TRUNCATED AT 250 WORDS)