Reversible unfolding of the major fraction of ovalbumin by guanidine hydrochloride

The guanidine hydrochloride induced unfolding of the major fraction of ovalbumin (i.e. A1 which contains two phosphate groups and constitutes about 77% of the total protein) was investigated systematically by difference spectran and viscosity measurements. As judged by the intrinsic viscosity (3.9 ml/g), the native protein conformation is compact and globular. Difference spectral results showed extensive disruption of the native structure by guanidine hydrochloride with and without 0.1 M beta-mercaptoethanol were 31.1 and 27.0 ml/g. These and optical rotation results indicated that the denatured protein existed in a cross-linked random coil conformation in 6 M guanidine hydrochloride alone. Strikingly, in contrast to whole ovalbumin, the denaturation of its A1 fraction by guanidine hydrochloride was fully reversible and obeyed first-order kinetic law under different experimental condit ions of pH, temperature, and the denaturant concentration. The monotonic variation of deltaH for the unfolding of ovalbumin A1 by guanidine hydrochloride with temperature, the coincidence of the two transition curves obtained by measuring two independent properties (namely reduced viscosity and difference in light absorption at 288 nm (or 293 nm) as a function of the denaturant concentration, and finally the adherence of the unfolding as well as refolding reactions to first-order kinetic law suggested that the transition of ovalbumin. A1 can reasonably be approximated by a two-state mode. Analysis of the equilibrium data obtained at pH 7.0 and 25 degrees C according to Aune and Tanford (Aune, K.C.,and Tanford, C. (1969), Biochemistry 8, 4586) showed that 12 additional binding sites for the denaturant with an association constant of 1.12 were freshly exposed by the unfolding process and that the native protein was marginally more stable (approximately 6 kcal/mol) than its unfolded form even under native condition. The temperature dependence of the equilibrium constant for the unfolding of ovalbumin A1 by guanidine hydrochloride which was studied in the range 10-60 degrees C at pH 7.0 can be described by assigning the following values of the thermodynamic parameters for the unfolding process: deltaH = 52 kcal/mol at 25 degrees C; deltaS = 153 cal deg-1 mol-1 at 25 degrees C; and delta Cp = 2700 +/- 400 cal deg-1 mol-1.     

Conformational stability of muscle acylphosphatase: the role of temperature, denaturant concentration, and pH

The conformational stability (delta G) of muscle acylphosphatase, a small alpha/beta globular protein, has been determined as a function of temperature, urea concentration, and pH. A combination of thermally induced and urea-induced unfolding, monitored by far-UV circular dichroism, was used to define the conformational stability over a wide range of temperature. Through analysis of all these data, the heat capacity change upon unfolding (delta Cp) could be estimated, allowing the determination of the temperature dependence of the main thermodynamic functions (delta G, delta H, delta S). Thermal unfolding in the presence of urea made it possible to extend such thermodynamic analysis to examine these parameters as a function of urea concentration. The results indicate that acylphosphatase is a relatively unstable protein with a delta G(H2O) of 22 +/- 1 kJ mol-1 at pH 7 and 25 degrees C. The midpoints of both thermal and chemical denaturation are also relatively low. Urea denaturation curves over the pH range 2-12 have allowed the pH dependence of delta G to be determined and indicate that the maximum stability of the protein occurs near pH 5.5. While the dependence of delta G on urea (the m value) does not vary with temperature, a significant increase has been found at low pH values, suggesting that the overall dimensions of the unfolded state are significantly affected by the number of charges within the polypeptide chain. The comparison of these data with those from other small proteins indicates that the pattern of conformational stability is defined by individual sequences and not by the overall structural fold.     

pH titration of native and unfolded beta-trypsin: evaluation of the delta delta G0 titration and the carboxyl pK values

The stabilizing free energy of beta-trypsin was determined by hydrogen ion titration. In the pH range from 3.0 to 7.0, the change in free energy difference for the stabilization of the native protein relative to the unfolded one (delta delta G0 titration) was 9.51 +/- 0.06 kcal/mol. An isoelectric point of 10.0 was determined, allowing us to calculate the Tanford and Kirkwood electrostatic factor w. This factor presented a nonlinear behavior and indicated more than one type of titratable carboxyl groups in beta-trypsin. In fact, one class of carboxyl group with a pK = 3.91 +/- 0.01 and another one with a pK = 4.63 +/- 0.03 were also found by hydrogen ion titration of the protein in the folded state.     

Effect of temperature on retention of enantiomers of beta-methyl amino acids on a teicoplanin chiral stationary phase

The isocratic retention of enantiomers of beta-methyl amino acids (beta-methyltyrosine, beta-methylphenylalanine, beta-methyl-tryptophan and beta-methyl-1,2,3,4-tetrahydroisoquinoline-3-carboxylic acid) was studied on a teicoplanin-containing chiral stationary phase at different temperatures and at different mobile phase compositions, using the reversed-phase mode. With variation of both mobile phase composition and temperature, almost baseline separations could be achieved for all four enantiomers of sterically hindered amino acids. The retention factors and selectivity factors for the enantiomers of all investigated compounds decreased with increasing temperature. The natural logarithms of the retention factors (ln k) of the investigated compounds depended linearly on the inverse of temperature (1/T). van 't Hoff plots afforded thermodynamic parameters, such as the apparent change in enthalpy (delta H degree), the apparent change in entropy (delta S degree) and the apparent change in Gibbs free energy (delta G degree) for the transfer of analyte from the mobile to the stationary phase. The thermodynamic constants (delta H degree, delta S degree and delta G degree) were calculated in order to promote an understanding of the thermodynamic driving forces for retention in this chromatographic system.     

Synthesis and hybridization properties of the conjugates of oligonucleotides and stabilization agents--II

New pyranone derivatives having tri- or pentamethylenamine linker functions were synthesized. These derivatives were covalently attached through the 5'-phosphoramide linkage to heptanucleotide pd(CCAAACA). Complementary complexes of the octanucleotide pd(TGTTTGGC) and above oligonucleotide conjugates were tested for their thermodynamic response. The Tm data and thermodynamic parameters for complex formation have demonstrated the ability of chromone (gamma-pyrone) and coumarin (alpha-pyrone) derivatives to stabilize strongly 7-mer/8-mer complementary complex, most likely through the stacking interaction of the pyran aromatic system with the neighboring nucleotide bases. The effect of chromone (or coumarin) derivatives on the stability of the oligonucleotide complexes (delta delta G at 37 degrees C ranged from -1.0 to -1.7 kcal/mol) was shown to be comparable to the effect of one nucleotide base pair and similar to the effect (delta delta G at 37 degrees C ranged from -1.5 to -2.0 kcal/mol) found for acridineoligonucleotide conjugates served in this study as a reference.     

Thermodynamic cycle between DNA and RNA constituents for conformation of the sugar ring from nuclear magnetic resonance study

The effect of a structural change of ribose to deoxyribose, by replacement of 2'-OH by 2'-H, on the conformational equilibrium of the sugar ring is described in terms of one thermodynamic cycle. The method is based on the observation that conformational correlations of the sugar ring--side chain ensemble in DNA and RNA components show one general pattern, reflecting an intrinsic physical property of this ensemble. The pattern determines a choice of model systems to study. The systems consist of pairs of DNA and RNA components, nucleosides and nucleotides in aqueous solution, where all conformational factors are fully controlled. This approach allowed us to describe the thermodynamic cycle and measure its fundamental parameters, equilibrium constants and free energy differences, delta delta G, from a nuclear magnetic resonance study. The delta delta G values as determined for pairs of ribo- and deoxyribo-nucleosides in classes of syn-constrained and anti-preferred models, are comparable and lie in a narrow range, delta delta G = 1.7 +/- 0.1 [kJ/mol]. For pairs of ribo- and deoxyribo-nucleotides, the delta delta G values also lie in narrow ranges, delta delta G = 1.7 +/- 0.1 [kJ/mol] for 5'-phosphate nucleotides and delta delta G = 1.9 +/- 0.1 [kJ/mol] for 3'-phosphate nucleotides, i.e. similar to those observed for nucleosides. The measured quantity, delta delta G, is generally observed in a relatively narrow range, delta delta G = 1.75 +/- 0.15 [kJ/mol], irrespective of the class of the model system. This quantity represents a "pure" constant contribution, pe one sugar moiety, as a "driving force" for the N-->S shift in the sugar ring conformational equilibrium, when one compares RNA and DNA. This important thermodynamic quantity, delta delta G, has not hitherto been determined for nucleic acids. Ultimately the delta delta G quantity is revealed in the tendency to adopt S(C2'endo) sugar puckering domain by the majority of DNA structures, whereas RNA generally adopt an N(C3'endo) puckering domain. A possible biological significance of the delta delta G quantity may include evolutionary aspects of nucleic acids.     

Evaluation of surface energy of W and AlNi by the results of their milling

A method is proposed which is an alternative to existing methods of determining of the surface tension of solids and is based on a generalization of the Rittinger law and the Gibbs thermodynamic equations, as well as on a diffraction analysis of the granulometric characteristics of finely dispersed powders of templates (Fe, Co) and originals (W, AlNi). The surface tension coefficients of tungsten and AlNi are evaluated. The confidence intervals of varying their values are found.     

Energetics of drug-DNA interactions

Understanding the thermodynamics of drug binding to DNA is of both practical and fundamental interest. The practical interest lies in the contribution that thermodynamics can make to the rational design process for the development of new DNA targeted drugs. Thermodynamics offer key insights into the molecular forces that drive complex formation that cannot be obtained by structural or computational studies alone. The fundamental interest in these interactions lies in what they can reveal about the general problems of parsing and predicting ligand binding free energies. For these problems, drug-DNA interactions offer several distinct advantages, among them being that the structures of many drug-DNA complexes are known at high resolution and that such structures reveal that in many cases the drug acts as a rigid body, with little conformational change upon binding. Complete thermodynamic profiles (delta G, delta H, delta S, delta Cp) for numerous drug-DNA interactions have been obtained, with the help of high-sensitivity microcalorimetry. The purpose of this article is to offer a perspective on the interpretation of these thermodynamics parameters, and in particular how they might be correlated with known structural features. Obligatory conformational changes in the DNA to accommodate intercalators and the loss of translational and rotational freedom upon complex formation both present unfavorable free energy barriers for binding. Such barriers must be overcome by favorable free energy contributions from the hydrophobic transfer of ligand from solution into the binding site, polyelectrolyte contributions from coupled ion release, and molecular interactions (hydrogen and ionic bonds, van der Waals interactions) that form within the binding site. Theoretical and semiempirical tools that allow estimates of these contributions to be made will be discussed, and their use in dissecting experimental data illustrated. This process, even at the current level of approximation, can shed considerable light on the drug-DNA binding process.     

Positive feedback hypothesis on development of essential hypertension

A hypothesis is presented on a possible mechanism of development of the essential hypertension. The present theoretical consideration with Laplace's law and Poiseuille's law indicates that arteriolar constriction increases, unless the blood flow is reduced, both arterial blood pressure and vascular circumferential wall tension which is considered a trigger of medial hypertrophy of the constricted arteriole. If the medial hypertrophy aggravates the vascular constriction, it all the more increases arterial pressure and wall tension. Therefore, the initial arteriolar constriction, however slight, may progressively produce hypertension and augment medial hypertrophy by such a positive feedback mechanism.     

Interaction of minor groove ligands to an AAATT/AATTT site: correlation of thermodynamic characterization and solution structure

A combination of circular dichroism spectroscopy, titration calorimetry, and optical melting has been used to investigate the association of the minor groove ligands netropsin and distamycin to the central A3T2 binding site of the DNA duplex d(CGCAAATTGGC).d(GCCAATTTGCG). For the complex with netropsin at 20 degrees C, a ligand/duplex stoichiometry of 1:1 was obtained with Kb approximately 4.3 x 10(7) M-1, delta Hb approximately -7.5 kcal mol-1, delta Sb approximately 9.3 cal K-1 mol-1, and delta Cp approximately 0. Previous NMR studies characterized the distamycin complex with A3T2 at saturation as a dimeric side-by-side complex. Consistent with this result, we found a ligand/duplex stoichiometry of 2:1. In the current study, the relative thermodynamic contributions of the two distamycin ligands in the formation of this side-by-side complex (2:1 Dst.A3T2) were evaluated and compared with the thermodynamic characteristics of netropsin binding. The association of the first distamycin molecule of the 2:1 Dst.A3T2 complex yielded the following thermodynamic profile: Kb approximately 3.1 x 10(7) M-1, delta Hb = -12.3 kcal mol-1, delta Sb = -8 cal K-1 mol-1, and delta Cp = -42 cal K-1 mol-1. The binding of the second distamycin molecule occurs with a lower Kb of approximately 3.3 x 10(6) M-1, a more favorable delta Hb of -18.8 kcal mol-1, a more unfavorable delta Sb of -34 cal K-1 mol-1, and a higher delta Cp of -196 cal K-1 mol-1. The latter term indicates an ordering of electrostricted and structural water molecules by the complexes. These results correlate well with the NMR titrations and are discussed in context of the solution structure of the 2:1 Dst.A3T2 complex.     

Structural and thermodynamic characterization of the interaction of the SH3 domain from Fyn with the proline-rich binding site on the p85 subunit of PI3-kinase

The interaction of the Fyn SH3 domain with the p85 subunit of PI3-kinase is investigated using structural detail and thermodynamic data. The solution structure complex of the SH3 domain with a proline-rich peptide mimic of the binding site on the p85 subunit is described. This indicates that the peptide binds as a poly(L-proline) type II helix. Circular dichroism spectroscopic studies reveal that in the unbound state the peptide exhibits no structure. Thermodynamic data for the binding of this peptide to the SH3 domain suggest that the weak binding (approximately 31 microM) of this interaction is, in part, due to the entropically unfavorable effect of helix formation (delta S0 = -78 J.mol-1.K-1). Binding of the SH3 domain to the intact p85 subunit (minus its own SH3 domain) is tighter, and the entropic and enthalpic contributions are very different from those given by the peptide interaction (delta S0 = +252 J.mol-1.K-1; delta H0 = +44 kJ.mol-1). From these dramatically different thermodynamic measurements we are able to conclude that the interaction of the proline-rich peptide does not effectively mimic the interaction of the intact p85 subunit with the SH3 domain and suggest that other interactions could be important.     

A new stochastic model for auditory-nerve discharge

This paper investigates the mechanisms for history-dependent probability of eight-nerve discharge, which is modeled as the probability that the excitatory postsynaptic potential (EPSP) process crosses afferent membrane threshold, with the discharge history dependence due to the dependence of postsynaptic threshold voltage on time since previous action potential. The model parameters are the Poisson intensity alpha t of vesicle release, the duration epsilon and probability density PV(upsilon) of single-vesicle EPSP's, and the threshold voltage curve theta (tau) for spiking. It is proven that the infinitesimal conditional probabilities of discharge exhibit two distinct behaviors. The first is associated with the time tau = T D, exactly the time the neuron releases from absolute refractory where there is no intensity [theta(tau) = infinity, for tau < T D]. At this time the neuron has a nonzero probability of discharge [symbol:see text] (T D) = lim delta-->0 Pr(Nt,t+delta = 1/t - wNt = T D). The second regime corresponds to the time since previous spike being greater than dead time, tau > T D, during which time the intensity exists lambda t(tau) = lim delta-->0(1/delta) Pr(Nt,t+delta = 1/t - wNt = tau > T D). The fact that there is a nonzero probability of discharge following passage from the absolute refractory period predicts the nonmonotonic hazard intensity seen in high spontaneous neurons [R. P. Gaumond, Ph.D. thesis, Washington University, St. Louis (1980)] and high driven rate neurons. It is shown that for the lowest range of vesicle release intensities where the vesicle-release-rate/membrane-integration-time product alpha t epsilon small, the nonzero probability of discharge at a point is approximately equal to 0. The discharge intensity is dominated by a term linear in vesicle release intensity: lambda t(tau) approximately alpha t exp(-integral of t-epsilon t alpha sigma d sigma) integral of theta (tau) infinity Pv(upsilon)d upsilon. This is precisely the Siebert-Gaumond intensity product form with monotonic recovered discharge probability. At high vesicle release rates, such as for driven rate responses, the nonzero probability of discharging at a point becomes of nonsignificant size, and the intensity of discharge grows nonlinearly with alpha t, implying the product model does not hold. The model is demonstrated via the analysis of auditory nerve fibers from the cat.     

High-temperature,high-pressure nitrogen concentration in Fe-Cr-Mn-Ni alloys

The thermodynamic expressions used to express the nitrogen concentration in iron based alloys prepared under high pressure requires the explicit use of pressure terms. The nitrogen concentration follows Sievert's law for low alloy additions, but significant deviations are observed at higher alloy additions. This Bureau of Mines study extends these new thermodynamic results to higher pressures (200 MPa) and to a greater range of iron alloys: Fe-(0-30)Cr-(0-30)Mn-(0-30)Ni. The experimental results also show that pressure-alloy concentration effects exist.     

Isothermal titration microcalorimetric studies for the binding of octenoyl-CoA to medium chain acyl-CoA dehydrogenase

We investigated the binding of octenoyl-CoA to pig kidney medium chain acyl-CoA dehydrogenase (MCAD) by isothermal titration microcalorimetry under a variety of experimental conditions. At 25 degrees C in 50 mM phosphate buffer at pH 7.6 (ionic strength of 175 mM), the binding is characterized by the stoichiometry (n) of 0.89 mole of octenoyl-CoA/(mole of MCAD subunit), delta G = -8.75 kcal/mol, delta H = -10.3 kcal/mol, and delta S = -5.3 cal mol(-1) K(-1), suggesting that formation of MCAD-octenoyl-CoA is enthalpically driven. By employing buffers with various ionization enthalpies, we discerned that formation of the MCAD-octenoyl-CoA complex, at pH 7.6, accompanies abstraction (consumption) of 0.52 +/- 0.15 proton/(MCAD subunit) from the buffer media. We studied the effects of pH, ionic strength, and temperature on the thermodynamics of MCAD-octenoyl-CoA interaction. Whereas the ionic strength does not significantly influence the above interaction, the pH of the buffer media exhibits a pronounced effect. The pH dependence of the association constant of MCAD +octenoyl-CoA <==> MCAD-octenoyl-CoA yields a pKa for the free enzyme of 6.2. Among thermodynamic parameters, whereas delta G remains invariant as a function of temperature, delta H and deltaS(standard) both decrease with an increase in temperature. At temperatures of < 25 degrees C, delta G is dominated by favorable entropic contributions. As the temperature increases, the entropic contributions progressively decrease, attain a value of zero at 23.8 degrees C, and then becomes unfavorable. During this transition, the enthalpic contributions become progressively favorable, resulting in an enthalpy-entropy compensation. The temperature dependence of delta H yields the heat capacity change (delta Cp(0)) of -0.37 +/- 0.05 kcal mol(-1) K(-1), attesting to the fact that the binding of octenoyl-CoA to MCAD is primarily dominated by the hydrophobic forces. The thermodynamic data presented herein are rationalized in light of structural-functional relationships in MCAD catalysis.     

Thermodynamic parameters of opioid binding in the presence and absence of G-protein coupling

We have investigated the thermodynamic parameters of various opioid ligands interacting with their receptors in rat brain membranes. Affinity constants (Ka), enthalpy and entropy values were obtained from homologous displacement experiments performed at 0, 24 and 33 degrees C. It was found that all the opioid agonists tested ([3H]dihydromorphine (DHM) mu alkaloid; [3H]DAMGO mu peptide; [3H]deltorphin-B delta peptide) display endothermic binding accompanied with a large entropy increase, regardless of their chemical structure (alkaloid or peptide), or of their mu or delta receptor selectivity. In contrast, binding of the antagonist naloxone is exothermic, mainly enthalpy driven. Na+ or Mg2+ results only in quantitative changes of the thermodynamic parameters. In the presence of the GTP-analog Gpp(NH)p; or Gpp(NH)p + Na+; or Gpp(NH)p + Na- + Mg2+ the affinity of DHM binding dramatically decreases which might reflect functional uncoupling of the receptor-ligand complex and G-proteins. This altered molecular interactions are also indicated by curvilinear van't Hoff plot and entropy increase. It is concluded that the thermodynamic analysis provides means of determining the underlying driving forces of ligand binding and helps to delineate its mechanism.     

Exchange of monooleoylphosphatidylcholine as monomer and micelle with membranes containing poly(ethylene glycol)-lipid

Surface-grafted polymers, such as poly(ethylene glycol) (PEG), provide an effective steric barrier against surface-surface and surface-macromolecule interactions. In the present work, we have studied the exchange of monooleoylphosphatidylcholine (MOPC) with vesicle membranes containing 750 mol wt surface-grafted PEG (incorporated as PEG-lipid) from 0 to 20 mol % and have analyzed the experimental results in terms of thermodynamic and stationary equilibrium models. Micropipette manipulation was used to expose a single lipid vesicle to a flow of MOPC solution (0.025 microM to 500 microM). MOPC uptake was measured by a direct measure of the vesicle area change. The presence of PEG(750) lipid in the vesicle membrane inhibited the partitioning of MOPC micelles (and to some extent microaggregates) into the membrane, while even up to 20 mol % PEG-lipid, it did not affect the exchange of MOPC monomers both into and out of the membrane. The experimental data and theoretical models show that grafted PEG acts as a very effective molecular scale "filter" and prevents micelle-membrane contact, substantially decreasing the apparent rate and amount of MOPC taken up by the membrane, thereby stabilizing the membrane in a solution of MOPC that would otherwise dissolve it.     

Developmental profile of a caltrin-like protease inhibitor, P12, in mouse seminal vesicle and characterization of its binding sites on sperm surface

We examined the developmental profile of a kazal-type trypsin inhibitor (P12) of Mr 6126 in mouse seminal vesicle, characterized its binding sites on the surface of sperm, and assessed its effect on Ca2+ uptake by spermatozoa. Among the genital tracts of adult mice, P12 was found only in the male accessory glands including seminal vesicle, coagulating gland, and prostate. It was immunolocalized on the luminal epithelium of the primary and secondary folds in both the seminal vesicle and coagulating gland, and on the folds projecting into the lumen of the glandular alveolus in the prostate. The protein and its RNA message in seminal vesicle did not appear in the prepubertal period, but expression coincided with maturation. Castration of adult mice resulted in cessation of P12 expression. Treatment of the castrated mice with testosterone propionate in corn oil restored the protein expression in the seminal vesicle. Spermatozoa collected from caudal epididymis were devoid of P12. Cytochemical study illustrated a P12-binding region on the anterior acrosomes of cells preincubated with P12. Analysis of equilibrium data from the binding assay using 125I-P12 with a Scatchard plot showed a single type of P12-binding sites on sperm, with an apparent dissociation constant of 70.15 +/- 5.25 nM and the capacity of 1.49 +/- 0.06 x 10(6) binding sites/cell. The protein could serve as a calcium transport inhibitor to suppress a great extent of Ca2+ uptake by spermatozoa. The immunohistochemical staining patterns of testis revealed that the P12-binding sites appeared on postmeiotic cells such as spermatids and spermatozoa, but were absent in Leydig cells, Sertoli cells, spermatogonia, and spermatocytes in seminiferous tubules.     

Calculation Model of Mass Action Concentration for Mg-Al, Sr-Al and Ba-Al Melts and Determination of Their Thermodynamic Parameters

Basedonthermodynamicpropertiesofdifferentkindsofmetallicmelts[1 5] ,ageneralunderstandingofcoexistencetheoryforstructureofmetallicmeltscanbeachieved .ThispaperaimsatdeterminationofthermodynamicparametersofMg Al,Sr AlandBa Almetallicmeltsbycalculationwithmassactionconcentrationsmodel.Therearesomeresearchworksaboutthephasediagramofthesebinarysys tems[6 ,7] ,dataofactivityinthesemelts[8 13 ] aswellasthethermodynamicparametersofSr AlandBa Almelts[12 ,13 ] .Thesedataareusedtobuildcalculationmod…     

External surface and lamellarity of lipid vesicles: a practice-oriented set of assay methods

Three methods are presented for the determination of external surface of large lipid vesicles of different lamellarity with 2% absolute accuracy. These methods (referred to as EPR, NBD and TNBS assays) use different marker lipids which provide signals (electron paramagnetic resonance, fluorescence of N-(7-nitrobenz-2-oxa-1,3-diazol-4-yl) residues, and UV absorption increase of 2,4,6-trinitrobenzenesulfonic acid after reaction with aminolipids, respectively). The signals change upon addition of different membrane-impermeant reagents due to reaction with marker lipids at the external vesicle surface. They were applied to the same vesicle samples, including unilamellar and multilamellar vesicles, both at two different lipid compositions. External surface data matched for the three assays within 2%, but only after appropriate redesign or adaptation of so far published procedures. Main improvements related to slow influx of reagents (TNBS and NBD assays) or to redistribution of marker lipids (EPR assay), obscuring determination of outer vesicle surface from fast reaction between reagent and readily accessible marker lipids. Furthermore, suitable strategies were found to obtain accurate 100% values (reaction of all marker lipids present), required to relate external vesicle surface to total surface. This included corrections for light scattering (NBD assay) and for turbidity (TNBS assay). These three methods appear to close a gap in the methodology to determine external surface of vesicles for typical practical needs. In particular, the reliability range of the NBD assay could be extended to marker lipid densities as low as 1 marker lipid per 3000 lipids.