Fluorescence anisotropy decay of ethidium bound to nucleosome core particles. 1. Rotational diffusion indicates an extended structure at low ionic strength

The fluorescence decay of ethidium intercalated into the DNA of nucleosome core particles increases in average lifetime from about 22 ns in H2O to about 39 ns in D2O. This increase, combined with the acquisition of large amounts of data (on the order of 10(8) counts per decay), allows measurement of anisotropy decays out to more than 350 ns. The overall slow rotational motions of the core particle may thereby be more clearly distinguished from the faster torsional motions of the DNA. In 10 mM NaCl at 20 degrees C, we recover a long correlation time of 198 ns in D2O (159 ns when corrected to a viscosity of 1.002 cP), in agreement with the value of 164 ns obtained in H2O. These values are consistent with hydrodynamic calculations based on the expected size and shape of the hydrated particle. To support our conclusion that this long correlation time derives from Brownian rotational diffusion, we show that the value is directly proportional to the viscosity and inversely proportional to the temperature. No significant changes in the rotational correlation time are observed between 1 and 500 mM ionic strength. Below 1 mM, the particle undergoes the "low-salt transition" as measured by steady-state tyrosine fluorescence anisotropy. However, we observe little change in shape until the ionic strength is decreased below approximately 0.2 mM, where the correlation time increases nearly 2-fold, indicating that the particle has opened up into an extended form. We have previously shown that the transition becomes nonreversible below 0.2 mM salt.     

Fluorescence anisotropy of labelled F-actin: Influence of Ca2+ on the flexibility of F-actin

We measured the fluorescence static anisotropy and the time-resolved fluorescence anisotropy decay of F-actin labelled with N-iodoacetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine at 20°C in solutions containing 100 mM KCl and free Ca²⁺ at various concentrations. The average fluorescence anisotropy and the fluorescence rotational correlation time of actin decreased in the presence of micromolar concentrations of free Ca²⁺. The change of the rotational correlation time of labelled actin could not be explained by a variation of the actin critical concentration. We concluded therefore that F-actin undergoes a conformational change induced by Ca²⁺ binding. The binding constant was 6 × 10⁶ M^?1.     

Study of actin and its interactions with heavy meromyosin and the regulatory proteins by the pulse fluorimetry in polarized light of a fluorescent probe attached to an actin cysteine.

The decay of anisotropy of the N-iodoacetyl-N'-(5-sulfo-1-naphthyl)-ethylenediamine fluorescence attached to cysteine-373 of actin can be characterized by two correlation times theta1 and theta2. theta1 has a value of several nanoseconds and is thought to represent some local protein motion. theta2 is of the order of several hundreds of nanoseconds. Its value increases with actin concentration. It represents an average of the G and F actin correlation times. When actin interacts with heavy meromyosin, theta2 increases and becomes infinite at a molar ratio of one heavy meromyosin molecule per four actin protomers. It is concluded that a definite complex is then formed between F actin and heavy meromyosin. In the same time, G actin concentration becomes equal to zero. Finally, when F actin forms a complex with the regulatory proteins tropomyosin and troponin, the value of theta2 is greater in the absence than in the presence of Ca2+. This result indicates that micromolar concentrations of Ca2+ induces a conformation change of the complex of F actin with the regulatory proteins.     

Enhanced resolution of fluorescence anisotropy decays by simultaneous analysis of progressively quenched samples. Applications to anisotropic rotations and to protein dynamics.

Enhanced resolution of rapid and complex anisotropy decays was obtained by measurement and analysis of data from progressively quenched samples. Collisional quenching by acrylamide was used to vary the mean decay time of indole or of the tryptophan fluorescence from melittin. Anisotropy decays were obtained from the frequency-response of the polarized emission at frequencies from 4 to 2,000 MHz. Quenching increases the fraction of the total emission, which occurs on the subnanosecond timescale, and thereby provides increased information on picosecond rotational motions or local motions in proteins. For monoexponential subnanosecond anisotropy decays, enhanced resolution is obtained by measurement of the most highly quenched samples. For complex anisotropy decays, such as those due to both local motions and overall protein rotational diffusion, superior resolution is obtained by simultaneous analysis of data from quenched and unquenched samples. We demonstrate that measurement of quenched samples greatly reduces the uncertainty of the 50-ps correlation time of indole in water at 20 degrees C, and allows resolution of the anisotropic rotation of indole with correlation times of 140 and 720 ps. The method was applied to melittin in the monomeric and tetrameric forms. With increased quenching, the anisotropy data showed decreasing contributions from overall protein rotation and increased contribution from picosecond tryptophan motions. The tryptophan residues in both the monomeric and the tetrameric forms of melittin displayed substantial local motions with correlation times near 0.16 and 0.06 ns, respectively. The amplitude of the local motion is twofold less in the tetramer. These highly resolved anisotropy decays should be valuable for comparison with molecular dynamics simulations of melittin.     

Fluorescence polarization study of the alpha-ketoglutarate dehydrogenase complex from Escherichia coli

The lipoic acids of the alpha-ketoglutarate dehydrogenase multienzyme complex from Escherichia coli have been modified with two fluorescent probes, N-(1-pyrenyl)-maleimide and 5-[[[(iodoacetyl)amino]ethyl]amino]-naphthylene-1-sulfonic acid. Time-resolved fluorescence polarization of partially labeled complexes (18-77% inhibition of enzyme activity) reveals a complex depolarization process: one component of the anisotropy is characterized by a rotational correlation time much longer than the time scale of the measurements (less than or equal to 400 ns), reflecting the overall rotation of the complex, while a second component of the anisotropy decays with a rotational correlation time of 320 (+/- 50) ns. This decay is essentially independent of viscosity and is consistent with a model in which the depolarization is due to the dissociation from and rotation of lipoic acids between binding sites on the multienzyme complex. The sum of the rate constants characterizing the association and dissociation with the binding sites is approximately 3 x 10(6) s-1. In addition, approximately 5% of the anisotropy of the N-(1-pyrenyl)maleimide-labeled complex decays with a rotational correlation time of 25 ns; this can be attributed to local motion of the probe. At high extents of N-(1-pyrenyl)maleimide labeling (90-95% inhibition of enzyme activity), the anisotropy decay can be described by a constant term plus a rotational correlation time of about 1 microseconds. The increase in the correlation time probably reflects interactions between pyrene moieties. The N-(1-pyrenyl)maleimide-labeled dihydrolipoyl transsuccinylase core of the multienzyme complex has been isolated, and the anisotropy is constant over the observed time range of 300 ns. This suggests that the native structure is necessary for observation of lipoic acid movement within the complex. Fluorescent-labeled limited trypsin digestion fragments of the alpha-ketoglutarate dehydrogenase complex also have been isolated, and anisotropy measurements reveal substantial mobility of the label within the fragments. The time-resolved anisotropy of FAD in the native complex and in the isolated dihydrolipoyl dehydrogenase indicates some rapid local mobility of the FAD (rotational correlation time of 12 ns) that is viscosity independent, as well as a component of the anisotropy that is constant over the 35-ns time scale of the experiments.     

Application of a reference convolution method to tryptophan fluorescence in proteins. A refined description of rotational dynamics

A reference method for the deconvolution of polarized fluorescence decay data is described. Fluorescence lifetime determinations for p-terphenyl, p-bis[2-(5-phenyloxazolyl)]benzene and N-acetyltryptophanamide (AcTrpNH2) show that with this method more reliable fits of the decays can be made than with the scatterer method, which is most frequently used. Analysis of the AcTrpNH2 decay with p-terphenyl as the reference compound yields an excellent fit with lifetimes of 2.985 ns for AcTrpNH2 and 1.099 ns for p-terphenyl (20 degrees C), whereas the AcTrpNH2 decay cannot be satisfactorily fitted when the scatterer method is used. The frequency of the detected photons is varied to determine the conditions where pulse pile-up starts to affect the measured decays. At detection frequencies of 5 kHz and 15 kHz, which corresponds to 1.7% and 5% respectively of the rate of the excitation photons no effects are found. Decays measured at 30 kHz (10%) are distorted, indicating that pile-up effects play a role at this frequency. The fluorescence and fluorescence anisotropy decays of the tryptophan residues in the proteins human serum albumin, horse liver alcohol dehydrogenase and lysozyme have been reanalysed with the reference method. The single tryptophan residue of the albumin is shown to be characterized by a triple-exponential fluorescence decay. The anisotropy decay of albumin was found to be mono-exponential with a rotational correlation time of 26 ns (20 degrees C). The alcohol dehydrogenase has two different tryptophan residues to which single lifetimes are assigned. It is found that the rotational correlation time for the dehydrogenase changes with excitation wavelength (33 ns for lambda ex = 295 nm and 36 ns for lambda ex = 300 nm at 20 degrees C), indicating a nonspherical protein molecule. Lysozyme has six tryptophan residues, which give rise to a triple-exponential fluorescence decay. A single-exponential decay with a rotational correlation time of 3.8 ns is found for the anisotropy. This correlation time is significantly shorter than that arising from the overall rotation and probably originates from intramolecular, segmental motion.     

MgATP-induced conformational change of the catalytic subunit of cAMP-dependent protein kinase

Conformational changes of the cAMP-dependent protein kinase (PKA) catalytic (C) subunit are critical for the catalysis of gamma-phosphate transfer from adenosine 5'-triphosphate (ATP) to target proteins. Time-resolved fluorescence anisotropy (TRFA) was used to investigate the respective roles of Mg(2+), ATP, MgATP, and the inhibitor peptide (IP20) in the conformational changes of a 5,6-carboxyfluorescein succinimidyl ester (CF) labeled C subunit ((CF)C). TRFA decays were fit to a biexponential equation incorporating the fast and slow rotational correlation times phi(F) and phi(S). The (CF)C apoenzyme exhibited the rotational correlation times phi(F)=1.8+/-0.3 ns and phi(S)=20.1+/-0.6 ns which were reduced to phi(F)=1.1+/-0.2 ns and phi(S)=13.3+/-0.9 ns in the presence of MgATP. The reduction in rotational correlation times indicated that the (CF)C subunit adopted a more compact shape upon formation of a (CF)C.MgATP binary complex. Neither Mg(2+) (1-3 mM) nor ATP (0.4 mM) alone induced changes in the (CF)C subunit conformation equivalent to those induced by MgATP. The effect of MgATP was removed in the presence of ethylenediaminetetraacetic acid (EDTA). The addition of IP20 and MgATP to form the (CF)C x MgATP x IP20 ternary complex produced rotational correlation times similar to those of the (CF)C x MgATP binary complex. However, IP20 alone did not elicit an equivalent reduction in rotational correlation times. The results indicate that binding of MgATP to the C subunit may induce conformation changes in the C subunit necessary for the proper stereochemical alignment of substrates in the subsequent phosphorylation.     

Ionic effects on the rotational dynamics of cross-bridges in myosin filaments, measured by triplet absorption anisotropy

We have measured the rotational motion of myosin heads in synthetic thick filaments at 4 degrees C in the time range from 10(-7) to 10(-4) seconds, by measuring transient absorption anisotropy of an eosin probe attached to a reactive sulfhydryl on the myosin head. Under conditions that result in monomeric myosin (500 mM ionic strength), the anisotropy decay is independent of pH in the range from 7.0 to 8.2 and [Mg2+] in the range from 0.1 to 10 mM; the anisotropy decays bi-exponentially with correlation times of 0.4 and 2 microseconds to a constant value of 0.016. Under more physiological conditions (115 mM ionic strength), resulting in filament formation, the anisotropy decay is sensitive to both pH and [Mg2+]. The anisotropy at pH 8.2 and 0.1 mM-Mg2+ decays with correlation times of 0.5 and 3.8 microseconds to a constant limiting anisotropy of 0.038. When the [Mg2+] is increased to 10 mM, the correlation times are 0.6 and 5.7 microseconds and the limiting anisotropy value is 0.055. Identical changes in the anisotropy decay are caused by an increase in [H+] to pH 7.0, in the presence of 0.1 mM-Mg2+. Increasing the total ionic strength to 187 mM decreases the amplitude of the cation effects. These results provide direct evidence that the rotational dynamics of myosin heads in thick filaments are influenced by physiological concentrations of cations. The results are qualitatively consistent with the proposal that these and other ionic conditions regulate transitions between "spread" and "compact" cross-bridge conformations, but the quantitative results indicate that cross-bridges undergo large-amplitude microsecond rotations even under conditions where the compact state should predominate.     

Effects of temperature on the fluorescence intensity and anisotropy decays of staphylococcal nuclease and the less stable nuclease-conA-SG28 mutant

Frequency-domain fluorescence spectroscopy was used to investigate the effects of temperature on the intensity and anisotropy decays of the single tryptophan residues of Staphylococcal nuclease A and its nuclease-conA-SG28 mutant. This mutant has the beta-turn forming hexapeptide, Ser-Gly-Asn-Gly-Ser-Pro, substituted for the pentapeptide Tyr-Lys-Gly-Gln-Pro at positions 27-31. The intensity decays were analyzed in terms of a sum of exponentials and with Lorentzian distributions of decay times. The anisotropy decays were analyzed in terms of a sum of exponentials. Both the intensity and anisotropy decay parameters strongly depend on temperature near the thermal transitions of the proteins. Significant differences in the temperature stability of Staphylococcal nuclease and the mutant exist; these proteins show characteristic thermal transition temperatures (Tm) of 51 and 30 degrees C, respectively, at pH 7. The temperature dependence of the intensity decay data are shown to be consistent with a two-state unfolding model. For both proteins, the longer rotational correlation time, due to overall rotational diffusion, decreases dramatically at the transition temperature, and the amplitude of the shorter correlation time increases, indicating increased segmental motions of the single tryptophan residue. The mutant protein appears to have a slightly larger overall rotational correlation time and to show slightly more segmental motion of its Trp than is the case for the wild-type protein.     

Anisotropy decays of indole, melittin monomer and melittin tetramer by frequency-domain fluorometry and multi-wavelength global analysis

We used frequency-domain fluorescence spectroscopy to measure the fluorescence lifetime and anisotropy decays of indole in propylene glycol, and of the tryptophan emission of melittin monomer and tetramer in water solutions at 5 degrees C. We obtained an increase in resolution of the anisotropy decays by using multiple excitation wavelengths, chosen to provide a range of fundamental anisotropy values. The multi-excitation wavelength anisotropy decays were analyzed globally to recover a single set of correlation times with wavelength-dependent anisotropy amplitudes. Simulated data and kappaR2 surfaces are shown to reveal the effect of multi-wavelength data on the resolution of complex anisotropy decays. For both indole and melittin, the anisotropy decays are heterogeneous and require two correlation times to fit the frequency-domain data. For indole in propylene glycol at 5 degrees C we recovered correlation times of 0.59 and 4.10 ns, which appear to be characteristic of the rigid and asymmetric indole molecule. For melittin monomer the correlation times were 0.13 and 1.75 ns, and for melittin tetramer 0.12 and 3.96 ns. The shorter and longer correlation times of melittin are due to segmental motions and overall rotational diffusion of the polypeptide.     

Torsional motion of eosin-labeled F-actin as detected in the time-resolved anisotropy decay of the probe in the sub-millisecond time range

The internal motion of F-actin in the time range from 10(-6) to 10(-3) second has been explored by measuring the transient absorption anisotropy of eosin-labeled F-actin using laser flash photolysis. The transient absorption anisotropy of eosin-F-actin at 20 degrees C has a component that decays in the submicrosecond time scale to an anisotropy of about 0.3. This anisotropy then decays with a relaxation time of about 450 microseconds to a residual anisotropy of about 0.1 after 2 ms. When the concentration of eosin-F-actin was varied in the range from 7 to 28 microM, the transient absorption anisotropy curves obtained were almost indistinguishable from each other. These results show that the anisotropy decay arises from internal motion of eosin-F-actin. Analysis of the transient absorption anisotropy curves indicates that the internal motion detected by the decay in anisotropy is primarily a twisting of actin protomers in the F-actin helix; bending of the actin filament makes a minor contribution only to the measured decay. The torsional rigidity calculated from the transient absorption anisotropy is 0.2 X 10(-17) dyn cm2 at 20 degrees C, which is about an order of magnitude smaller than the flexural rigidity determined from previous studies. Thus, we conclude that F-actin is more flexible in twisting than in bending. The calculated root-mean-square fluctuation of the torsional angle between adjacent actin protomers in the actin helix is about 4 degrees at 20 degrees C. We also found that the torsional rigidity is approximately constant in the temperature range from 5 to approximately 35 degrees C, and that the binding of phalloidin does not appreciably affect the torsional motion of F-actin.     

The viscoelastic properties of actin solutions

The viscoelastic properties in actin solutions were investigated by measuring their elastic modulus and viscous modulus using a rheometer. The polymerization/gelation process of actin solutions was accompanied by an increase of both parameters, indicating the formation of a protein network. High shear rotational motion destroyed this network which, however, would reanneal if left undisturbed. At 25 °C under low ionic strength conditions, the viscoelastic moduli of a Spudich-Watt globular (G) actin preparation increased with time, while G-actin, purified by gel filtration maintained low viscoelastic moduli. The rigidity of the filamentous (F) actin network in a solution of Spudich-Watt actin, measured by the elastic modulus, was somewhat lower than that of gel-filtration-purified actin at the same protein concentration. The crosslink density of these F-actin networks was estimated, using models from rubber elasticity theory. The calculated density was 1 crosslink/50 actin monomers for the purified actin and 1 crosslink/120 actin monomers for Spudich-Watt actin. The results are consistent with the idea that a small amount of regulatory factor(s), which could be removed by the gel filtration step, modulates the structure of an actin network.     

Time-resolved fluorescence of the single tryptophan residue in rat alpha-fetoprotein and rat serum albumin: analysis by the maximum-entropy method.

The time-resolved fluorescence emissions of the lone tryptophan residues in rat alpha-fetoprotein (RFP) and rat serum albumin (RSA) were studied. The total fluorescence intensity decays in both proteins were multiexponential. Analysis of the data by nonlinear least squares as a sum of discrete exponentials showed that four exponentials were needed for a satisfactory fit for both proteins. Analysis by the maximum entropy method using 150 logarithmically equally spaced exponentials yielded four well-resolved excited-state lifetime classes with barycenters and relative amplitudes values (ci) that corresponded to those obtained from the nonlinear least-squares method. Changing the temperature affected the relative amplitudes of the lifetime classes but had little effect on the lifetime values themselves. This suggests that the four classes reflect local conformational substates that exchange slowly with respect to the time window of observation defined by the longest lifetime. The internal rotational dynamics of the tryptophan in each protein was monitored by fluorescence anisotropy decay measurements. The mobility of the tryptophan appeared to be larger and faster in RFP than in RSA. The nonlinear least-squares analysis suggests the existence of three rotational correlation times of 0.1, 3, and 55 ns for this protein. As a function of temperature, the long correlation time did not follow the Perrin's law expected for a rigid rotating body. This suggests that this correlation time may reflect not only the Brownian rotation of the whole protein but also the flexibilities of domains in the protein. For RSA a two-component model with correlation times of 0.4 and 31 ns was sufficient to describe the data.(ABSTRACT TRUNCATED AT 250 WORDS)     

Isolation and characterization of actin and myosin from B-lymphocytic guinea pig leukemia cells.

Actin and myosin have been isolated from a guinea pig B cell leukemia line, L2C. The m.w. and amino acid compositions of these proteins are similar to actin and myosin from other nonmuscle cell types. L2C actin polymerizes to form filaments and activates the ATPase activity of skeletal muscle myosin. Actin in crude lymphocyte extracts does not polymerize as well as predicted from the critical concentration of purified lymphocyte actin suggesting that other factors in lymphocyte extracts regulate actin polymerization. Lymphocyte myosin polymerizes to form synthetic filaments at low ionic strength. Lymphocyte myosin binds to actin, but its ATPase activity is not activated by actin. Possible mechanisms for regulation of the lymphocyte contractile apparatus and its importance in a number of lymphocyte functions are discussed.     

Strong impact of ionic strength on the kinetics of fibrilar aggregation of bovine beta-lactoglobulin

We investigate the effect of ionic strength on the kinetics of heat-induced fibrilar aggregation of bovine beta-lactoglobulin at pH 2.0. Using in situ light scattering we find an apparent critical protein concentration below which there is no significant fibril formation for all ionic strengths studied. This is an independent confirmation of our previous observation of an apparent critical concentration for 13 mM ionic strength by proton NMR spectroscopy. It is also the first report of such a critical concentration for the higher ionic strengths. The critical concentration decreases with increasing ionic strength. Below the critical concentration mainly "dead-end" species that cannot aggregate anymore are formed. We prove that for the lowest ionic strength this species consists of irreversibly denatured protein. Atomic force microscopy studies of the morphology of the fibrils formed at different ionic strengths show shorter and curvier fibrils at higher ionic strength. The fibril length distribution changes non-monotonically with increasing ionic strength. At all ionic strengths studied, the fibrils had similar thicknesses of about 3.5 nm and a periodic structure with a period of about 25 nm.     

Studies on the assembly of a spherical plant virus. I. States of aggregation of the isolated protein

The aggregates formed at equilibrium by purified protein from cowpea chlorotic mottle virus have been characterized on the basis of their sedimentation behaviour and appearance in the electron microscope. Between pH 3.5 and 7.5, at ionic strengths greater than 0.2, most of the protein is found in aggregates sedimenting at either 3 S or 50 S. The 50 S aggregate is identified as the reassembled capsid of cowpea ehlorotic mottle virus. Decreasing the ionic strength favours the formation of multi-shelled particles. Below pH 5.5 single- and multishelled particles predominate, while above this pH most of the protein sediments at 3 S.Varying the temperature from 5 °C to 20 °C has little effect on the equilibrium proportions of aggregates although some real differences can be detected. Ionic strength is not as important a variable as pH in determining which protein forms are present (but increasing ionic strength does result in a steady decrease in the proportion of protein in the multi-layer aggregates). The dependence of the equilibrium upon protein concentration shows that capsid formation is a quasi-crystallization: beyond a certain total protein concentration the concentration of 3 S aggregate remains at this “critical” concentration and all further protein goes into 50 S capsid. In addition to shells and variations upon shells, tubes and hexagonal nets of protein subunits have occasionally been seen with the electron microscope.     

The isolation and characterization of actin from porcine brain

Highly purified porcine brain actin has been prepared by a procedure involving anion-exchange chromatography, polymerization-depolymerization, and gel filtration. Electrophoresis of purified brain actin on polyacrylamide gels in the presence of sodium dodecyl sulfate shows a single protein band corresponding to more than 95% of the applied protein and migrating with the relative mobility of skeletal muscle actin. The amino acid composition of brain actin is similar but not identical to that of rabbit skeletal muscle actin. Brain actin activates the low ionic strength Mg²⁺-ATPase of skeletal muscle myosin to the same extent that skeletal muscle actin potentiates the muscle ATPase. Although similar to its skeletal muscle counterpart, brain actin is distinctly different. Isoelectric focusing experiments indicate that brain actin consists of at least two species, each of which is more basic than the α-species of skeletal muscle actin. The polymerization of brain actin was followed by viscometry and sedimentation techniques as a function of protein concentration, temperature, and ionic conditions. The critical actin concentrations of both brain and skeletal muscle actins polymerized at low ionic strength in the presence of 2.0 mm MgCl₂ are similar and show little dependence upon temperature. When polymerized in the presence of 0. 1 m KCl, brain actin has a critical actin concentration that is higher and more dependent upon temperature than the corresponding critical concentration of skeletal muscle actin.     

Purification and kinetic characterisation of human erythrocyte actin

Human erythrocyte actin can be extracted from membrane ghosts by low ionic strength treatment in the presence of protective amounts of calcium and ATP. Purification then involves a single chromatographic step. The erythrocyte actin can be labelled with N-(1-prenyl)iodoacetamide. The fluorescence enhancement which accompanies polymerisation can be used to determine the critical concentration for assembly and to follow the polymerisation reaction time-course. The polymerisation kinetics of erythrocyte actin are compared with those of rabbit skeletal muscle actin. The two are shown to be markedly different.     

A fluorescent sterol probe study of human serum low-density lipoproteins

The fluorescent sterol probe, ergosta-5,7,9,(11),22-tetraen-3 beta-ol (dehydroergosterol), was utilized as a cholesterol analog to label human serum low-density lipoproteins (LDL). Quenching of dehydroergosterol fluorescence by KI indicated that most of the fluorophore was either buried within the outer phospholipid monolayer of LDL or within the neutral lipid core of LDL. The steady-state anisotropy of dehydroergosterol in LDL detected the cholesteric core phase transition near 30 degrees C. Fluorescence lifetime decays for dehydroergosterol contained two components, both below and above the cholesteric phase transition, with the major lifetime component near 1 ns. Neither lifetime component underwent a detectable change in duration at the core phase transition temperature. Time-correlated fluorescence anisotropy decays of dehydroergosterol indicated a single rotational correlation time near 1.7 ns, which was unaffected by the core phase transition. Time-correlated anisotropy decays also suggested hindered rotation of dehydroergosterol in LDL. These results indicate that unesterified cholesterol is primarily located in the outer phospholipid monolayer of LDL, with the majority of cholesterol not in direct contact with the aqueous phase.     

Gelation of globular proteins: effect of pH and ionic strength on the critical concentration for gel formation. A simple model and its application to beta-lactoglobulin heat-induced gelation.

The influence of pH (2-9) and ionic strength (0-0.14 M NaCl) on the sol-gel transition of beta-lactoglobulin was investigated in order to determine the critical gel concentration (C0). The concentration necessary to form a gel near the isoelectric pH remains approximately constant (approximately 1% w/v) independently of the ionic strength. At other pH values, the higher the ionic strength is, the lower the protein concentration must be to form a gel. A theoretical model to relate the effect of the intensity and the range of electrostatic interactions on the critical concentration (C0) is proposed and fits reasonably with the experimental results.