Tilted hydrocarbon chains of dipalmitoyl lecithin become perpendicular to the bilayer before melting.

Differential scanning calorimetry studies of dipalmitoyl lecithin show two reversible transitions as the temperature is changed between 20 and 50 degrees C. A pretransition endotherm occurs at 35 degrees C prior to the main chain melting endotherm which occurs at 42 degrees C. X-ray diffraction studies show that below 33 degrees C the chains of the lecithin are fully extended, packed in a hexagonal crystalline lattice but tilted with respect to the plane of the bilayer. Between 35 and 42 degrees C the chains are similarly packed but oriented perpendicular to the bilayer plane. Above 44 degrees C the chains are "melted" or disordered. Monolayer studies of dipalmitoyl lecithin using continuous recording of pressure with molecular area reveal the existence of two solid condensed phases corresponding to these tilted and verticle chain structures. The tilted to perpendicular transition would account for the pretransition endotherm of the lipid; the crystalline to melted change corresponds to the larger transition observed at 42 degrees C.     

Lipid thermotropic transitions in Triatoma infestans lipophorin

The structure and lipid thermotropic transitions of highly purified lipophorin of Triatoma infestans were examined by several techniques: steady-state fluorescence polarization of 1,6-diphenyl-1,3,5-hexatriene (DPH), cis-parinaric acid (cis-PnA) and trans-parinaric acid (trans-PnA), light scattering fluorescence energy transfer between the lipophorin tryptophan residues and the bound chromophores, DPH, trans-parinaric acid cis-parinaric acid, gel electrophoresis, and gel filtration. Fluorescence polarization of PnAs and DPH revealed a reversible lipid thermotropic transition in intact lipophorin at about 20 degrees C and 18 degrees C, respectively. In lipophorin, lipid dispersion fluorescence polarization of DPH detected a lipid transition approximately at 20 degrees C, while trans-PnA showed a gel phase formation at a temperature below 30 degrees C. Similar experiments in which trans-PnA was incorporated into diacylglycerols and phospholipids extracted from the lipophorin revealed gel phase formation below 30 degrees C and 24 degrees C, respectively. Light scattering measurements showed that lipophorin particles aggregate irreversibly at 45 degrees C, increasing the molecular weight, as determined by gel filtration on Sephacryl S-300, from 740,000 to values larger than 1,500,000. The particle aggregation did not change the physical properties of the lipophorin studied by fluorescence polarization, indicating that the aggregation is apparently a non-denaturing process. Energy transfer between the lipophorin tryptophans and the bound chromophores cis-PnA, trans-PnA, and DPA revealed a different location of the fluorescent probes within the lipophorin. Temperature-dependence on the energy transfer efficiency for all probes confirmed a change in the ordering of the lipophorin lipids at 24 degrees C.     

The effect of osmotic pressure on the membrane fluidity of Saccharomyces cerevisiae at different physiological temperatures

Membrane fluidity in whole cells of Saccharomyces cerevisiae W303-1A was estimated from fluorescence polarization measurements using the membrane probe, 1,6-diphenyl-1,3,5-hexatriene, over a wide range of temperatures (6-35 degrees C) and at seven levels of osmotic pressure between 1.38 MPa and 133.1 MPa. An increase in phase transition temperatures was observed with increasing osmotic pressure. At 1.38 MPa, a phase transition temperature of 12 +/- 2 degrees C was observed, which increased to 17 +/- 4 degrees C at 43.7 MPa, 21+/- 7 degrees C at 61.8 MPa, and 24 +/- 9 degrees C at an osmotic pressure of 133.1 MPa. From these results we infer that, with increases in osmotic pressure, the change in phospholipid conformation occurs over a larger temperature range. These results allow the representation of membrane fluidity as a function of temperature and osmotic pressure. Osmotic shocks were applied at two levels of osmotic pressure and at nine temperatures, in order to relate membrane conformation to cell viability.     

Thermodynamics of DNA binding and distortion by the hyperthermophile chromatin protein Sac7d

Sac7d is a hyperthermophile chromatin protein which binds non-specifically to the minor groove of duplex DNA and induces a sharp kink of 66 degrees with intercalation of valine and methionine side-chains. We have utilized the thermal stability of Sac7d and the lack of sequence specificity to define the thermodynamics of DNA binding over a wide temperature range. The binding affinity for poly(dGdC) was moderate at 25 degrees C (Ka = 3.5(+/-1.6) x 10(6) M(-1)) and increased by nearly an order of magnitude from 10 degrees C to 80 degrees C. The enthalpy of binding was unfavorable at 25 degrees C, and decreased linearly from 5 degrees C to 60 degrees C. A positive binding heat at 25 degrees C is attributed in part to the energy of distorting DNA, and ensures that the temperature of maximal binding affinity (75.1+/-5.6 degrees C) is near the growth temperature of Sulfolobus acidocaldarius. Truncation of the two intercalating residues to alanine led to a decreased ability to bend and unwind DNA at 25 degrees C with a small decrease in binding affinity. The energy gained from intercalation is slightly greater than the free energy penalty of bending duplex DNA. Surprisingly, reduced distortion from the double alanine substitution did not lead to a significant decrease in the heat of binding at 25 degrees C. In addition, an anomalous positive DeltaCp of binding was observed for the double alanine mutant protein which could not be explained by the change in polar and apolar accessible surface areas. Both the larger than expected binding enthalpy and the positive heat capacity can be explained by a temperature dependent structural transition in the protein-DNA complex with a Tm of 15-20 degrees C and a DeltaH of 15 kcal/mol. Data are discussed which indicate that the endothermic transition in the complex is consistent with DNA distortion.     

Triple-helix formation by an oligonucleotide containing one (dA)12 and two (dT)12 sequences bridged by two hexaethylene glycol chains.

The triple-helix formation by the oligonucleotide (dA)12-x-(dT)12-x-(dT)12, where x is a hexaethylene glycol group, was investigated by thermal denaturation analysis and circular dichroism spectroscopy. Thermal denaturation analysis showed that this single-stranded oligonucleotide is able to fold back on itself twice to give a triple helix at low temperature. Upon an increase in the temperature, two cooperative transitions were observed: formation of a double-stranded structure with a dangling x-(dT)12 extremity, then formation of a single-stranded coil structure. Due to the intramolecular character of the transition, the triplex is much more stable than that formed by the reference mixture (dA)12 + 2(dT)12. In 0.1 M NaCl, the triplex-to-coil transition occurred at about 30 degrees C whereas the duplex-to-coil was at about 60 degrees C. Upon an increase in the salt, the increase of temperature corresponding to the triplex-to-duplex transition was larger than that of the duplex-to-coil transition. MgCl2 showed higher efficiency than NaCl to promote triplex or duplex formation. The thermodynamic parameters delta H and delta S were determined at various ionic strengths for both transitions. Both the enthalpy change and entropy change associated with triplex-to-duplex transition (Hoogsteen base pairing) were smaller than those associated to the duplex-to-coil transition (Watson-Crick base pairing). When the ionic strength increased, the parameters -delta H and -delta S showed a very small decrease for the duplex-to-coil transition whereas a strong increase was observed with the triplex-to-duplex transition.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of phospholipids on the thermal stability of microsomal UDP-glucuronosyltransferase

The GT2P isoform of microsomal UDP-glucuronosyltransferase from pig liver is a lipid-dependent enzyme. The data in the present work indicate that, in addition to regulation of activity, the thermal stability of the enzyme also is modulated by the acyl chain composition of phosphatidylcholines (PC) used to reconstitute the activity of pure enzyme. There was a reversible, temperature-dependent change in the state of the pure enzyme to an inactive form with onset at T greater than 38 degrees C, depending on the environment of the enzyme. The midpoint for the transition shifted from 39.8 degrees C for enzyme in a bilayer of distearoylphosphatidylcholine (DSPC) to 47.5 degrees C for enzyme in a bilayer of 1-stearoyl-2-oleoylphosphatidylcholine (SOPC). For all lipids, the transition from a catalytically active to an inactive form of the enzyme was associated with large compensating changes in H and S. Lipid-induced stabilization of the active form of UDP-glucuronosyltransferase at T greater than 37 degrees C was associated with decreases in delta H and delta S, but the decreases in delta S were larger, indicating that lipid-induced stabilization of the active form of the enzyme was entropic. The transition between the active and inactive forms of the enzyme was too rapid in either direction to measure in a standard spectrophotometer. In addition to reversible inactivation of the enzyme, there was a slower irreversible, temperature-dependent inactivation. The rate of this process depended on the acyl chains of the phosphocholines interacting with the enzyme. However, there was no obvious correlation between the structures of lipids that stabilized the different inactivation reactions.     

Pressure-induced unfolding of lysozyme in aqueous guanidinium chloride solution.

The pressure-induced unfolding of lysozyme was investigated in an aqueous guanidinium chloride solution by means of ultraviolet spectroscopy. Assuming a two-state transition model, volume changes were calculated from the slope of free energy vs. pressure plots over a temperature range of 10 to 60 degrees C. Between 25 and 60 degrees C, almost constant volume changes were observed in the transition region, which was reflected in almost identical slopes of the free energy change vs. pressure plots. On the other hand, the different slopes were observed in the pressure dependence of free energy change at temperatures lower than 25 degrees C. These data were interpreted as suggesting that a two-state model is not appropriate at low temperature, but instead one or more intermediates are present under these conditions. The volume changes for unfolding became less negative at temperatures higher than 25 degrees C.     

Kinetics and in vitro origin of the temperature-dependent transition of the estrogen receptor monomer

Partitioning of estrogen receptors in aqueous two-phase polymer systems has provided the basis for a detailed kinetic analysis of the effects of temperature on estrogen receptor (ER) structure in vitro. Exposure to temperatures of 0-30 degrees C increased the rate of change in ER partition coefficients by up to 100-fold but did not affect the final extent of the process. The temperature-dependent change in ER partition coefficients was characterized by a linear Arrhenius plot and an activation energy of 25 kcal/mol. The rate of the temperature-dependent ER transition (28 degrees C) was found to be unaffected by greater than 50-fold changes in receptor concentration, which indicates that the temperature-dependent change in partition coefficients reflects a first-order process. The partition coefficients of heated ER were unaffected by subsequent 18-h incubations at 0 degree C, indicating that the temperature-dependent ER transition is irreversible in vitro. Direct heating of the unoccupied ER resulted in both a change in ER partition coefficients and a loss of ER binding sites. The temperature-dependent change in unoccupied ER partition coefficients was complete within 30 min at 28 degrees C and yielded a first-order rate constant that was the same as that obtained for heating the receptor-estradiol complex at 28 degrees C. In contrast, the loss of unoccupied ER binding sites that occurred during 28 degrees C incubations did not reach completion after 150 min of heating and was found to behave as a second-order process.(ABSTRACT TRUNCATED AT 250 WORDS)     

Elongation of tandem repetitive DNA by the DNA polymerase of the hyperthermophilic archaeon Thermococcus litoralis at a hairpin-coil transitional state: a model of amplification of a primordial simple DNA sequence

DNA is replicated by DNA polymerase semiconservatively in many organisms. Accordingly, the replicated DNA does not become larger than the original DNA (template DNA), implying that replicative synthesis by DNA polymerase alone cannot explain the diversification of primordial simple DNA. We demonstrate that a single-stranded tandem repetitive oligodeoxyribonucleic acid (oligoDNA) composed of a palindromic or quasi-palindromic motif sequence and 25-50% GC content is elongated in vitro to more than 20,000 bases at 70-74 degrees C by the DNA polymerase of the hyperthermophilic archaeon Thermococcus litoralis without a bimolecular primer-template complex. The efficiency of elongation decreased when the palindromic structure of the oligoDNA was destroyed or when the GC content of the oligoDNA was outside the range of 25-50%. The thermal melting transition profile of the oligoDNA, as observed by ultraviolet spectroscopy, exhibited a biphasic curve, reflecting a duplex-hairpin transition at 31-40 degrees C and a hairpin-coil transition at 70-77 degrees C. The optimal reaction temperature for the elongation, for instance, of oligoDNA (AGATATCT)(6) (72 degrees C) was very close to its hairpin-coil transition melting temperature (70.4 degrees C), but was markedly higher than the temperature at which duplex oligoDNA can exist stably (<35.9 degrees C). These results suggest that a hairpin-based "intramolecular primer-template structure" is formed transiently in the oligoDNA, and it is elongated by the DNA polymerase to long DNA through repeated cycles of folding and melting of the hairpin structure. We discuss the implication of this phenomenon, "hairpin elongation", from the standpoint of potential amplification of simple DNA sequences during the evolution of the genome.     

The effect of selected anions on dipalmitoylphosphatidylcholine phase transitions

The effect of three anions, Cl-, Br- and I-, on the phase transitions of dipalxnitoylphosphatidyicholine (DPPC) was measured. Main phase transition was modestly affected by these anions in the salt concentration range 0.2 M. For Cl- and Br- the temperature of main phase transition was lower (by about 0.5 degrees C), its half-width modestly larger and enthalpy practically unchanged, all three parameters were altered to a much larger deuce. Main phase transition temperature was 1.5 degrees C lower and the peak hall-width significantly smaller. These changes were not accompanied by any alteration in main phase transition enthalpy. Iodide shifted the pretransition temperature toward lower values and increased its half-width to such an extent that at concentrations above 100 mM it was practically undetectable. Besides cations, the presence of anions also has a distinct effect on lipid bilayer interface properties.     

Inactivation of calcium uptake by EGTA is due to an irreversible thermotropic conformational change in the calcium binding domain of the Ca(2+)-ATPase.

Calcium uptake by rabbit skeletal sarcoplasmic reticulum (SR) is inhibited with an effective inactivation temperature (TI) of 37 degrees C in EGTA with no effect on ATPase activity. Since the Ca-ATPase denatures at a much higher temperature (49 degrees C) in EGTA, this suggests that a small or localized conformational change of the Ca-ATPase at 37 degrees C results in inability to accumulate calcium by the SR. Using a fluorescent analogue of dicyclohexylcarbodiimide, N-cyclohexyl-N'-[4-(dimethylamino)-alpha-naphthyl]-carbodiimide (NCD-4), the region of the calcium binding sites of the SR Ca-ATPase was labeled. Steady-state and frequency-resolved fluorescence measurements were subsequently performed on the NCD-4-labeled Ca-ATPase. Site-specific information pertaining to the hydrophobicity and segmental flexibility of the region of the calcium binding sites was derived from the steady-state fluorescence intensity, lifetime, and rotational rate of the covalently bound NCD-4 label as a function of temperature (0-50 degrees C). A reversible transition at approximately 15 degrees C and an irreversible transition at approximately 35 degrees C were deduced from the measured fluorescence parameters. The low-temperature transition agrees with the previously observed break in the Arrhenius plot of ATPase activity of the native Ca-ATPase at 15-20 degrees C. The high-temperature transition conforms well with the conformational transition, resulting in uncoupling of Ca translocation from ATP hydrolysis as predicted from the irreversible inactivation of Ca uptake at 31-37 degrees C in 1 mM EGTA.(ABSTRACT TRUNCATED AT 250 WORDS)     

Temperature and pH dependent changes of immunoglobulin G structure.

1. The temperature and pH functions of the myeloma IgG(K) conformation were studied by optical rotatory dispersion, circular dichroism, thermal perturbation difference spectroscopy, solvent perturbation difference spectroscopy, electrochemical iodination and difference adiabatic scanning microcalorimetry. 2. The IgG studied was found to be capable of a fully reversible structural change between pH 6.5 and 6.0. A transition occurring at low pH is accompanied by an increase of exposure of the chromophores to the solvent. 3. The "alkaline state" was found to be capable of a fully reversible S-like transition at temperatures between 25 and 35 degrees C. The changes occurring at the higher temperature are accompanied by the screening of 14-15 tyrosine residues and probably by a small increase in the helicity of the protein. These changes are not accompanied by an appreciable heat effect. The thermal denaturation of the "alkaline state" occurs only at 64 degrees C in the narrow temperature interval (3-4 degrees C). 4. The "acid state" is not accompanied by S-like transition at 25-35 degrees C. The thermal denaturation of the "acid state" occurs at 54 degrees C in the wide temperature interval (8-9 degrees C). 5. It was proposed that the ionisation of the invariant histidine residues situated in the "cavity" between the constant and variable domains causes the pH transition studied. The temperature changes in the interval 25-35 degrees C are explained by the alteration of the domains interposition. Similar alterations were investigated as a result of antigen-antibody reaction.     

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)     

Electrical capacitance of lipid bilayer membranes of hydrogenated egg lecithin at the temperature phase transition

Electrical capacitance of the planar bilayer lipid membrane (BLM) formed from hydrogenated egg lecithin (HEL) has been studied during many passages through the phase transition temperature. In contrast to the BLM from individual synthetic phospholipids, membranes from HEL did not demonstrate any capacitance change at the phase transition temperature maximum, as measured by differential scanning calorimeter at 52 degrees C. Instead, two temperatures have been discerned by capacitance records: thickening at 42-43 degrees C and thinning at 57-59 degrees C. The first temperature region is close to the transition temperature of dipalmitoyllecithin, whereas the second is close to that of distearoyllecithin, two main components of the HEL. It was suggested that capacitance measurements were able to reveal a phase separation in the BLM from HEL which was not detected by differential scanning calorimetry. The phase transition of the BLM from the liquid crystal state to the gel state is followed by thickening of the bilayer structure, partly due to a gauche- trans transition of lipid molecules but mainly due to redistribution of the solvent n-decane.     

Corticosteroids as effectors of lipid polymorphism of dielaidoylglycerophosphoethanolamine. A study using 31P NMR and differential scanning calorimetry

The influence of corticosteroids on the lipid polymorphism of dielaidoylglycerophosphoethanolamine was studied by 31P NMR spectroscopy and differential scanning calorimetry. Both techniques evidenced two transitions in the pure lipid samples. The first one corresponded to the gel----liquid crystalline phase transition. It occurred at a temperature of 38.9 degrees C, as measured by differential scanning calorimetry and at 35-40 degrees C as detected by 31P NMR. The second transition corresponded to the bilayer----hexagonal HII phase transition. It occurred at 64.2 degrees C as measured by differential scanning calorimetry and at 60 degrees C as detected by NMR. Addition of corticosteroids led to different specific effects on the bilayer----hexagonal HII phase transition, according to their chemical structure. These effects appear to be the result of low amounts of incorporated steroids, according to binding studies (partition coefficient values range between 5 and 54). The presence of a conjugated 3-keto group in the steroid molecule (progesterone) promoted a downward shift in the bilayer----hexagonal HII phase transition temperature by about 6 -7 degrees C as compared to the 3 beta-OH-bearing compound (pregnenolone), which did not exhibit any appreciable effect. No change in the delta H of transition could be measured. The presence of the 21-OH group (like in deoxycorticosterone) induced the formation of a structure, characterized by an isotropic lineshape of the 31P NMR spectrum at temperatures where the 'hexagonal' type of lineshape is present, without steroid. The transition from the bilayer to this other structure occurred at a slightly higher temperature than the bilayer----hexagonal HII phase transition. It corresponded to a peak in differential scanning calorimetry scans with a delta H of 2.1 kJ X mol-1. The presence of the 17 beta-OH group as present in 17 beta-OH-progesterone and 11-deoxycortisol suppressed the two former effects. These compounds had no influence on the bilayer----hexagonal HII phase HII phase transition. The additional presence of the 11 beta-OH group like in corticosterone and cortisol, evoked a stabilization of the bilayer organization as the bilayer----hexagonal HII phase transition temperature is shifted upward by about 10 degrees C. This was accompanied by a decrease of the delta H to 0.8 kJ X mol-1. Besides this, the corticosteroids did not affect to a large extent the gel----liquid crystalline phase transition: a general slight downward shift of the transition temperature and a small broadening of the transition were observed without significant change in the delta H.(ABSTRACT TRUNCATED AT 400 WORDS)     

Dilatometric studies of the subtransition in dipalmitoylphosphatidylcholine

The phase transition between the newly discovered low-temperature subgel phase and the gel phase of dipalmitoylphosphatidylcholine has been studied by using dilatometry. Equilibrium measurements show that the subtransition upon heating is centered at 13.5 degrees C, has a dilatometric half-width of 0.6 degree C, and comprises a specific volume change of 0.009 mL/g (about one-fourth the size of the main transition). When the gel phase is cooled, the subtransition does not occur until below 5 degrees C. The rate of formation as a function of incubation temperature for 1 degree C less than TI less than 6 degrees C was determined; it is not well fit by quantitative theories based upon homogeneous nucleation. However, some form of nucleation is present since temperature-jump studies show that once the subgel phase has started to form, it continues to grow in the range 6 degrees C less than TJ less than 12.8 degrees C. Thus, the true transition temperature lies between 12.8 and 13.5 degrees C, but nucleation of the subgel phase is severely retarded above 6 degrees C, leading to the large hysteresis observed upon cooling.     

A differential scanning calorimetric study of the conformational transitions of schizophyllan in mixtures of water and dimethylsulfoxide

The thermal conformational transitions of two sonicated samples of schizophyllan were studied in water-dimethylsulfoxide (DMSO) mixtures by high-sensitivity differential scanning calorimetry (DSC). Two transitions were observed over most of the range of solvent compositions. These were assigned to an internal change of the triple helix [T. Itou et al. (1986) Macromolecules 19, 1234-1240] and a triple-helix-single-coil transition [T. Sato et al. (1981) Carbohydr. Res. 95, 195-204], respectively. In water, the former transition observed at lower temperature for a low molecular weight sample, U-1, is centered at 3 degrees C and characterized by the specific enthalpy, delta hcal = 3.29 J g-1. A higher molecular weight sample, M-2, showed this transition at 7 degrees C with delta hcal = 4.39 J g-1. The transition temperature for both samples increased with increasing DMSO concentration up to about 50 degrees C at 70 weight % DMSO, and then rapidly decreased with increasing DMSO concentration, with about 3 degrees C higher for M-2 than for U-1 over the DMSO concentration. The transition was not observed when the concentration of DMSO exceeded 87%. It was found that delta hcal for both samples was a linear function of t 1/2, the temperature of half-completion in degrees C, delta hcal = 0.177t + 2.96. The triple helix-coil transition was observed at around 127 degrees C for U-1 and above 130 degrees C for M-2 in the range of DMSO composition below about 70%. The transition temperature decreased with increasing DMSO concentration at above 70%, and the transition finally disappeared when the DMSO concentration exceeded 90%. The plot of delta hcal vs. t 1/2 for the transition of both samples gave a linear relation, delta hcal = 0.253t - 10.58. The reversibility of the transition at lower temperature was demonstrated by the reversibility of the curves when the first heating was stopped before the second transition. Once the heating was performed over the second transition, the reheating DSC curves showed several endothermic peaks, indicating the irreversibility of the transition and heterogeneity in the conformation of the heated schizophyllan.     

Conformational changes in bovine heart myosin as studied by EPR and DSC techniques

Thermal behavior of intact and LC-2 deficient myosin obtained from bovine heart was studied using EPR and DSC techniques. The reactive thiol sites (Cys 704) of myosin was labelled with 4-maleimidopiperidine-nitroxyl, and the measurements were taken in X-band in the conventional and saturation transfer EPR time domains. DSC scans were made from 5 degrees up to 60 degrees C with 0.25 degree C/min scan rate. Bovine heart myosin was isolated by standard methods. The LC-2 deficient myosin was prepared by cleaving myosin with alpha-chymotrypsin (400:1 molar ratio) for 1.5 min at 25 degrees. Our basic finding was a conformational change in LC-2 deficient myosin detected at 18 degrees C. It was not observed in intact myosin suggesting that the dissociation of the regulatory light chain resulted in a local structural change in the neighbourhood of the attached label in the 20 kD domain. The rotational correlation time of the label and the microwave saturation behavior of myosin at 25 degrees C exhibited no significant differences after removal of the LC-2 light chain. However, the mobility of the same label was significantly diminished in skeletal muscle. Studying the melting behavior of myosin, six endothermic peaks were detected at 19; 41.3; 43.3; 45.5; 48.5; and 54.3 degrees C (enthalpies: 708.4; 399; 773.8; 1089; 1612.8; and 3304.8 kJ/mol). They were assigned to the segment containing the essential thiols: HMM S-2, HMM S-1 (50kD and 20kD plus 27kD) and LMM. Removal of the LC-2 light chain was associated with the disappearance of the 18 degrees transition showing again a structural change in LC-2 deficient myosin which extended to a larger region.     

Physicochemical characterization of large unilamellar phospholipid vesicles prepared by reverse-phase evaporation

Properties of large unilamellar vesicles (LUV), composed of phosphatidylcholine and prepared by reverse-phase evaporation and subsequent extrusion through Unipore polycarbonate membranes, have been investigated and compared with those of small unilamellar vesicles (SUV) and of multilamellar vesicles (MLV). The unilamellar nature of the LUV is shown by 1H-NMR using Pr3+ as a shift reagent. The gel to liquid-crystalline phase transition of LUV composed of dipalmitoylphosphatidylcholine (DPPC) monitored by differential scanning calorimetry, fluorescence polarization of diphenylhexatriene and 90 degrees light scattering, occurs at a slight lower temperature (40.8 degrees C) than that of MLV (42 degrees C) and is broadened by about 50%. The phase transition of SUV is shifted to considerably lower temperatures (mid-point, 38 degrees C) and extends over a wide temperature range. In LUV a well-defined pretransition is not observed. The permeability of LUV (DPPC) monitored by leakage of carboxyfluorescein, increases sharply at the phase transition temperature, and the extent of release is greater than that from MLV. Leakage from SUV occurs in a wide temperature range. Freeze-fracture electron microscopy of LUV (DPPC) reveals vesicles of 0.1-0.2 micron diameter with mostly smooth fracture faces. At temperatures below the phase transition, the larger vesicles in the population have angled faces, as do extruded MLV. A banded pattern, seen in MLV at temperatures between the pretransition and the main transition, is not observed in the smaller LUV, although the larger vesicles reveal a dimpled appearance.     

Role of latent heat in chiral symmetry breaking transition in the crystallization of 1,1'-binaphthyl

The influence of latent heat dissipated by the crystallization of 1,1'-binaphthyl in its supercooled molten state on the chiral symmetry breaking transition was investigated. Temperature change in the crystallization system was monitored by infrared thermocamera. Temperature rise due to the dissipation of latent heat in the growing front of polycrystalline aggregate was about 2 degrees C in an unstirred crystallization system. The melting point of racemic mixture and racemic compound of 1,1'-binaphthyl is 145 degrees C and 158 degrees C, respectively. The latent heat generated by the crystallization could thus change the crystallization behavior when the initial temperature of the melt was slightly lower than 145 degrees C. The temperature change in both unstirred and stirred crystallization systems was monitored. In the stirred crystallization system, even in the case when the initial temperature of the melt was about 2 degrees C lower than 145 degrees C, the temperature rose by about 4 degrees C immediately after the onset of crystallization. This indicates that the role of stirring as the critical parameter for the chiral symmetry breaking transition is not only to clone the chiral crystals but also to enhance the dissipation of latent heat due to secondary nucleation.