Interaction of a mitochondrial presequence with lipid membranes: role of helix formation for membrane binding and perturbation

The binding of a peptide to a biological membrane is often accompanied by a transition from a random coil structure to an amphipathic alpha-helix. Recently, we have presented a new approach which allows the determination of the thermodynamic parameters of membrane-induced helix formation [Wieprecht et al. (1999) J. Mol Biol. 294, 785]. It involves a systematic variation of the helix content of a given peptide by double D-substitution and a correlation of the binding parameters with the helicity. Here we have used this method to study membrane-induced helix formation for the presequence of rat mitochondrial rhodanese (RHD). The thermodynamic parameters of binding of the peptide RHD and of four of its double D-isomers were determined for 30 nm (SUVs) and 100 nm (LUVs) unilamellar vesicles composed of phosphatidylcholine/phosphatidylglycerol (3:1) using circular dichroism spectroscopy, fluorescence spectroscopy, and isothermal titration calorimetry. The incremental changes of the thermodynamic parameters of helix formation were found to be very similar for SUVs and LUVs. Membrane-induced helix formation of RHD entailed a negative enthalpy of Delta H(helix) = -0.5 to -0.6 kcal/mol/residue and was opposed by an entropy of about Delta S(helix) = -1 to -1.4 cal/mol K/residue. The free energy of helix formation, Delta G(helix), was about -0.2 kcal/mol, and helix formation accounted for 50-60% of the total free energy of membrane binding. Dye-release experiments were used to assess the role of helix formation for the membrane perturbation potential of the peptides. While helix formation plays a major role for membrane binding, it appears to have little importance for inducing membrane leakiness.     

Thermodynamics of the alpha-helix-coil transition of amphipathic peptides in a membrane environment: implications for the peptide-membrane binding equilibrium

Amphipathic alpha-helices are the membrane binding motif in many proteins. The corresponding peptides are often random coil in solution but are folded into an alpha-helix upon interaction with the membrane. The energetics of this ubiquitous folding process are still a matter of conjecture. Here, we present a new method to quantitatively analyze the thermodynamics of peptide folding at the membrane interface. We have systematically varied the helix content of a given amphipathic peptide when bound to the membrane and have correlated the thermodynamic binding parameters determined by isothermal titration calorimetry with the alpha-helix content obtained by circular dichroism spectroscopy. The peptides investigated were the antibiotic magainin 2 amide and three analogs in which two adjacent amino acid residues were substituted by their d-enantiomers. The thermodynamic parameters controlling the alpha-helix formation were found to be linearly related to the helicity of the membrane-bound peptides. Helix formation at the membrane surface is characterized by an enthalpy change of DeltaH(helix) approximately -0.7 kcal/mol per residue, an entropy change of DeltaS(helix) approximately -1.9 cal/molK residue and a free energy change of DeltaG(helix)=-0.14 kcal/mol residue. Helix formation is a strong driving force of peptide insertion into the membrane and accounts for about 50 % of the free energy of binding. An increase in temperature entails an unfolding of the membrane-bound helix. The temperature dependence can be described with the Zimm-Bragg theory and the enthalpy of unfolding agrees with that deduced from isothermal titration calorimetry.     

Association of a protein with membrane vesicles at the collisional limit: studies with blood coagulation factor Va light chain also suggest major differences between small and large unilamellar vesicles

Vesicle size can be a very sensitive modulator of protein-membrane association. In addition, reactions at the collisional limit may be characteristic of many types of protein-membrane or protein-receptor interactions. To probe these effects quantitatively, we analyzed the association of blood clotting factor Va light chain (Va-LC) with phospholipid vesicles of 15-150-nm radius. The number of protein binding sites per vesicle was approximately proportional to vesicle surface area. Association rates approached the collisional limit, and the activation energy for the association reaction was 4.5 +/- 0.5 kcal/mol. In agreement with diffusional theory for this type of interaction at the collisional limit, the observed association rate constant for filling all sites was approximately proportional to the inverse of vesicle radius. This general property has important implications for many systems such as blood coagulation including possible slower association rates and higher Km values for reactions involving whole cells relative to those obtained for phospholipid vesicles. Dissociation rate constants for reactions that are near the collisional limit should also be proportional to the inverse of vesicle size if diffusional parameters are the only factors influencing dissociation. However, Va-LC bound to small unilamellar vesicles (SUVs, less than or equal to 15-nm radius) gave slower dissociation rates than Va-LC bound to large unilamellar vesicles (LUVs, greater than or equal to 35-nm radius). This indicated a change in KI, the intrinsic protein-phospholipid affinity constant for LUVs vs SUVs. The cumulative effect of association and dissociation rates resulted in higher affinity of Va-LC for SUVs than LUVs under equilibrium conditions. The latter was corroborated by competition binding studies. Furthermore, the temperature dependence of both rate constants indicated an entirely entropy-driven binding to LUVs but a largely enthalpy-driven binding to SUVs. Interactions which are largely entropic are thought to be ionic in nature. The differences observed between binding to LUVs and SUVs may reflect thermodynamic differences between these types of phospholipid structures.     

Binding of the antibacterial peptide magainin 2 amide to small and large unilamellar vesicles

The thermodynamics of binding of the antibacterial peptide magainin 2 amide (M2a) to negatively charged small (SUVs) and large (LUVs) unilamellar vesicles has been studied with isothermal titration calorimetry (ITC) and CD spectroscopy at 45 degrees C. The binding isotherms as well as the ability of the peptide to permeabilize membranes were found to be qualitatively and quantitatively similar for both model membranes. The binding isotherms could be described with a surface partition equilibrium where the surface concentration of the peptide immediately above the plane of binding was calculated with the Gouy-Chapman theory. The standard free energy of binding was deltaG0 approximately -22 kJ/mol and was almost identical for LUVs and SUVs. However, the standard enthalpy and entropy of binding were distinctly higher for LUVs (deltaH0 = -15.1 kJ/mol, deltaS0 = 24.7 J/molK) than for SUVs (deltaH0 = -38.5 kJ/mol, deltaS0 = -55.3 J/molK). This enthalpy-entropy compensation mechanism is explained by differences in the lipid packing. The cohesive forces between lipid molecules are larger in well-packed LUVs and incorporation of M2a leads to a stronger disruption of cohesive forces and to a larger increase in the lipid flexibility than peptide incorporation into the more disordered SUVs. At 45 degrees C the peptide easily translocates from the outer to the inner monolayer as judged from the simulation of the ITC curves.     

CD Spectroscopy of Peptides and Proteins Bound to Large Unilamellar Vesicles

Circular dichroism (CD) spectroscopy is an essential tool for determining the conformation of proteins and peptides in membranes. It can be particularly useful for measuring the free energy of partitioning of peptides into lipid vesicles. The belief is broadly held that such CD measurements can only be made using sonicated small unilamellar vesicles (SUVs) because light scattering associated with extruded large unilamellar vesicles (LUVs) is unacceptably high. We have examined this issue using several experimental approaches in which a chiral object (i.e., peptide or protein) is placed both on the membrane and outside the membrane. We show that accurate CD spectra can be collected in the presence of LUVs. This is important because SUVs, unlike LUVs, are metastable and consequently unsuitable for equilibrium thermodynamic measurements. Our data reveal that undistorted CD spectra of peptides can be measured at wavelengths above 200 nm in the presence of up to 3 mM LUVs and above 215 nm in the presence of up to 7 mM LUVs. We introduce a simple way of characterizing the effect on CD spectra of light scattering and absorption arising from suspensions of vesicles of any diameter. Using melittin as an example, we show that CD spectroscopy can be used to determine the fractional helical content of peptides in LUVs and to measure their free energy of partitioning of into LUVs.     

Thermodynamics of the coil <==> beta-sheet transition in a membrane environment

Biologically important peptides such as the Alzheimer peptide Abeta(1-40) display a reversible random coil <==>beta-structure transition at anionic membrane surfaces. In contrast to the well-studied random coil left arrow over right arrow alpha-helix transition of amphipathic peptides, there is a dearth on information on the thermodynamic and kinetic parameters of the random coil left arrow over right arrow beta-structure transition. Here, we present a new method to quantitatively analyze the thermodynamic parameters of the membrane-induced beta-structure formation. We have used the model peptide (KIGAKI)(3) and eight analogues in which two adjacent amino acids were substituted by their d-enantiomers. The positions of the d,d pairs were shifted systematically along the three identical segments of the peptide chain. The beta-structure content of the peptides was measured in solution and when bound to anionic lipid membranes with circular dichroism spectroscopy. The thermodynamic binding parameters were determined with isothermal titration calorimetry and the binding isotherms were analysed by combining a surface partition equilibrium with the Gouy-Chapman theory. The thermodynamic parameters were found to be linearly correlated with the extent of beta-structure formation. beta-Structure formation at the membrane surface is characterized by an enthalpy change of DeltaH(beta)=-0.23 kcal/mol per residue, an entropy change of DeltaS(beta)=-0.24 cal/mol K residue and a free energy change of DeltaG(beta)=-0.15 kcal/mol residue. An increase in temperature induces an unfolding of beta-structure. The residual free energy of membrane-induced beta-structure formation is close to that of membrane-induced alpha-helix formation.     

Spontaneous transfer of ganglioside GM1 from its micelles to lipid vesicles of differing size.

The spontaneous incorporation of II3-N-acetylneuraminosylgangliotetraosylceramide (GM1) from its micelles into phospholipid bilayer vesicles has been investigated to determine whether curvature-induced changes in membrane lipid packing influence ganglioside uptake. Use of conventional liquid chromatography in conjunction with technically-improved molecular sieve gels permits ganglioside micelles to be separated from phospholipid vesicles of different average size including vesicles with diameters smaller than 40 nm and, thus, allows detailed study of native ganglioside GM1 incorporation into model membranes under conditions where complicating processes like fusion are readily detected if present. At 45 degrees C, the spontaneous transfer rate of GM1 from its micelles to small unilamellar vesicles (SUVs) comprised of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) is at least 3-fold faster than that to similar composition large unilamellar vesicles (LUVs) prepared by octyl glucoside dialysis. Careful analysis of ganglioside GM1 distribution among vesicle populations of differing average size reveals that GM1 preferentially incorporates into the smaller vesicles of certain populations. This behavior is observed in SUVs as well as in LUV-SUV mixtures and actually serves as a sensitive indicator for the presence of trace quantities of SUVs in various LUV preparations. Analysis of the results shows that both differences in the diffusional collision frequency between GM1 monomers and either SUVs or LUVs and curvature-induced changes in the interfacial lipid packing in either SUVs or LUVs can dramatically influence spontaneous ganglioside uptake.(ABSTRACT TRUNCATED AT 250 WORDS)     

Spectrin-like repeats 11-15 of human dystrophin show adaptations to a lipidic environment

Dystrophin is essential to skeletal muscle function and confers resistance to the sarcolemma by interacting with cytoskeleton and membrane. In the present work, we characterized the behavior of dystrophin 11-15 (DYS R11-15), five spectrin-like repeats from the central domain of human dystrophin, with lipids. DYS R11-15 displays an amphiphilic character at the liquid/air interface while maintaining its secondary α-helical structure. The interaction of DYS R11-15 with small unilamellar vesicles (SUVs) depends on the lipid nature, which is not the case with large unilamellar vesicles (LUVs). In addition, switching from anionic SUVs to anionic LUVs suggests the lipid packing as a crucial factor for the interaction of protein and lipid. The monolayer model and the modulation of surface pressure aim to mimic the muscle at work (i.e. dynamic changes of muscle membrane during contraction and relaxation) (high and low surface pressure). Strikingly, the lateral pressure modifies the protein organization. Increasing the lateral pressure leads the proteins to be organized in a regular network. Nevertheless, a different protein conformation after its binding to monolayer is revealed by trypsin proteolysis. Label-free quantification by nano-LC/MS/MS allowed identification of the helices in repeats 12 and 13 involved in the interaction with anionic SUVs. These results, combined with our previous studies, indicate that DYS R11-15 constitutes the only part of dystrophin that interacts with anionic as well as zwitterionic lipids and adapts its interaction and organization depending on lipid packing and lipid nature. We provide strong experimental evidence for a physiological role of the central domain of dystrophin in sarcolemma scaffolding through modulation of lipid-protein interactions.     

Thermodynamics of fusion peptide-membrane interactions

The fusion peptides of viral membrane fusion proteins play a key role in the mechanism of viral spike glycoprotein mediated membrane fusion. These peptides insert into the lipid bilayers of cellular target membranes where they adopt mostly helical secondary structures. To better understand how membranes may be converted to high-energy intermediates during fusion, it is of interest to know how much energy, enthalpy and entropy, is provided by the insertion of fusion peptides into lipid bilayers. Here, we describe a detailed thermodynamic analysis of the binding of analogues of the influenza hemagglutinin fusion peptide of different lengths and amino acid compositions. In small unilamellar vesicles, the interaction of these peptides with lipid bilayers is driven by enthalpy (-16.5 kcal/mol) and opposed by entropy (-30 cal mol(-1) K(-1)). Most of the driving force (deltaG = -7.6 kcal/mol) comes from the enthalpy of peptide insertion deep into the lipid bilayer. Enthalpic gains and entropic losses of peptide folding in the lipid bilayer cancel to a large extent and account for only about 40% of the total binding free energy. The major folding event occurs in the N-terminal segment of the fusion peptide. The C-terminal segment mainly serves to drive the N-terminus deep into the membrane. The fusion-defective mutations G1S, which causes hemifusion, and particularly G1V, which blocks fusion, have major structural and thermodynamic consequences on the insertion of fusion peptides into lipid bilayers. The magnitudes of the enthalpies and entropies of binding of these mutant peptides are reduced, their helix contents are reduced, but their energies of self-association at the membrane surface are increased compared to the wild-type fusion peptide.     

Membrane insertion pathway of annexin B12: thermodynamic and kinetic characterization by fluorescence correlation spectroscopy and fluorescence quenching

Experimental determination of the free energy stabilizing the structure of membrane proteins in their native lipid environment is undermined by the lack of appropriate methods and suitable model systems. Annexin B12 (ANX) is a soluble protein which reversibly inserts into lipid membranes under mildly acidic conditions, which makes it a good experimental model for thermodynamic studies of folding and stability of membrane proteins. Here we apply fluorescence correlation spectroscopy for quantitative analysis of ANX partitioning into large unilamellar vesicles containing either 25% or 75% anionic lipids. Membrane binding of ANX results in changes of autocorrelation time and amplitude, both of which are used in quantitative analysis. The thermodynamic scheme describing acid-induced membrane interactions of ANX considers two independent processes: pH-dependent formation of a membrane-competent form near the membrane interface and its insertion into the lipid bilayer. Our novel fluorescence lifetime topology method demonstrates that the insertion proceeds via an interfacial refolded intermediate state, which can be stabilized by anionic lipids. Lipid titration measurements are used to determine the free energy of both transmembrane insertion and interfacial penetration, which are found to be similar, approximately -10-12 kcal/mol. The formation of the membrane-competent form, examined in a lipid saturation experiment, was found to depend on the local proton concentration near the membrane interface, occurring with pK = 4.3 and involving the protonation of two residues. Our results demonstrate that fluorescence correlation spectroscopy is a convenient tool for the quantitative characterization of the energetics of transmembrane insertion and that pH-triggered ANX insertion is a useful model for studying the thermodynamic stability of membrane proteins.     

Peptide:lipid ratio and membrane surface charge determine the mechanism of action of the antimicrobial peptide BP100. Conformational and functional studies

The cecropin-melittin hybrid antimicrobial peptide BP100 (H-KKLFKKILKYL-NH2) is selective for Gram-negative bacteria, negatively charged membranes, and weakly hemolytic. We studied BP100 conformational and functional properties upon interaction with large unilamellar vesicles, LUVs, and giant unilamellar vesicles, GUVs, containing variable proportions of phosphatidylcholine (PC) and negatively charged phosphatidylglycerol (PG). CD and NMR spectra showed that upon binding to PG-containing LUVs BP100 acquires α-helical conformation, the helix spanning residues 3–11. Theoretical analyses indicated that the helix is amphipathic and surface-seeking. CD and dynamic light scattering data evinced peptide and/or vesicle aggregation, modulated by peptide:lipid ratio and PG content. BP100 decreased the absolute value of the zeta potential (ζ) of LUVs with low PG contents; for higher PG, binding was analyzed as an ion-exchange process. At high salt, BP100-induced LUVS leakage requires higher peptide concentration, indicating that both electrostatic and hydrophobic interactions contribute to peptide binding. While a gradual release took place at low peptide:lipid ratios, instantaneous loss occurred at high ratios, suggesting vesicle disruption. Optical microscopy of GUVs confirmed BP100-promoted disruption of negatively charged membranes. The mechanism of action of BP100 is determined by both peptide:lipid ratio and negatively charged lipid content. While gradual release results from membrane perturbation by a small number of peptide molecules giving rise to changes in acyl chain packing, lipid clustering (leading to membrane defects), and/or membrane thinning, membrane disruption results from a sequence of events – large-scale peptide and lipid clustering, giving rise to peptide-lipid patches that eventually would leave the membrane in a carpet-like mechanism.     

Enthalpy-driven apolipoprotein A-I and lipid bilayer interaction indicating protein penetration upon lipid binding

The interaction of lipid-free apolipoprotein A-I (apoA-I) with small unilamellar vesicles (SUVs) of 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) with and without free cholesterol (FC) was studied by isothermal titration calorimetry and circular dichroism spectroscopy. Parameters reported are the affinity constant (K(a)), the number of protein molecules bound per vesicle (n), enthalpy change (DeltaH degrees), entropy change (DeltaS degrees ), and the heat capacity change (DeltaC(p) degrees). The binding process of apoA-I to SUVs of POPC plus 0-20% (mole) FC was exothermic between 15 and 37 degrees C studied, accompanied by a small negative entropy change, making enthalpy the main driving force of the interaction. The presence of cholesterol in the vesicles increased the binding affinity and the alpha-helix content of apoA-I but lowered the number of apoA-I bound per vesicle and the enthalpy and entropy changes per bound apoA-I. Binding affinity and stoichiometry were essentially invariant of temperature for binding to SUVs of POPC/FC at a molar ratio of 6/1 at (2.8-4) x 10(6) M(-1) and 2.4 apoA-I molecules bound per vesicle or 1.4 x 10(2) phospholipids per bound apoA-I. A plot of DeltaH degrees against temperature displayed a linear behavior, from which the DeltaC(p) degrees per mole of bound apoA-I was calculated to be -2.73 kcal/(mol x K). These results suggested that binding of apoA-I to POPC vesicles is characterized by nonclassical hydrophobic interactions, with alpha-helix formation as the main driving force for the binding to cholesterol-containing vesicles. In addition, comparison to literature data on peptides suggested a cooperativity of the helices in apoA-I in lipid interaction.     

Reversible refolding of the diphtheria toxin T-domain on lipid membranes

The catalytic domain of diphtheria toxin (DT) is translocated across endosomal membranes by the T-domain (DTT) in response to acidification. Understanding the energetics of translocation, besides clarifying the mechanism of translocation, should provide insights into general principles of membrane protein stability and assembly. As a first step, we have evaluated the energetics of DTT binding to lipid vesicles using three single-cysteine mutants (L350C, Q369C, and Y280C) labeled with a 7-nitrobenz-2-oxa-1,3-diazol-4-yl (NBD) fluorophore sensitive to polarity changes. Remarkably strong association with the vesicles was detected for all mutants, even at pH 7 at which DTT is believed to be in a fully folded membrane-incompetent state. Lowering the pH in the presence of anionic membranes resulted in a strong but reversible increase in emission of NBD-labeled mutants, consistent with reversible membrane insertion. This reversibility permitted free energies of DTT interactions with vesicles to be determined for the first time. Free energy values for the three mutants ranged from -8 to -10 kcal mol(-1) at pH 4.3 and from -7 to -8 kcal mol(-1) at pH 7. Insights into the disposition of DTT on membranes were obtained using a novel hydropathy analysis that considers the relative free energies of transmembrane and interfacial interactions as a function of pH. This analysis suggests that interactions at the membrane interface dominate pH-triggered insertion of DTT, implying that the folding pathway involves interfacial intermediates.     

Preparation and Properties of Asymmetric Large Unilamellar Vesicles: Interleaflet Coupling in Asymmetric Vesicles Is Dependent on Temperature but Not Curvature

Asymmetry of inner and outer leaflet lipid composition is an important characteristic of eukaryotic plasma membranes. We previously described a technique in which methyl-β-cyclodextrin-induced lipid exchange is used to prepare biological membrane-like asymmetric small unilamellar vesicles (SUVs). Here, to mimic plasma membranes more closely, we used a lipid-exchange-based method to prepare asymmetric large unilamellar vesicles (LUVs), which have less membrane curvature than SUVs. Asymmetric LUVs in which sphingomyelin (SM) or SM + 1-palmitoyl-2-oleoyl-phosphatidylcholine was exchanged into the outer leaflet of vesicles composed of 1,2-dioleoyl-phosphatidylethanolamine (DOPE) and 1-palmitoyl-2-oleoyl-phosphatidylserine (POPS) were prepared with or without cholesterol. Approximately 80–100% replacement of outer leaflet DOPE and POPS was achieved. At room temperature, SM exchange into the outer leaflet increased the inner leaflet lipid order, suggesting significant interleaflet interaction. However, the SM-rich outer leaflet formed an ordered state, melting with a midpoint at ∼37°C. This was about the same value observed in pure SM vesicles, and was significantly higher than that observed in symmetric vesicles with the same SM content, which melted at ∼20°C. In other words, ordered state formation by outer-leaflet SM in asymmetric vesicles was not destabilized by an inner leaflet composed of DOPE and POPS. These properties suggest that the coupling between the physical states of the outer and inner leaflets in these asymmetric LUVs becomes very weak as the temperature approaches 37°C. Overall, the properties of asymmetric LUVs were very similar to those previously observed in asymmetric SUVs, indicating that they do not arise from the high membrane curvature of asymmetric SUVs.     

Thermodynamic parameters of the binding of retinol to binding proteins and to membranes

Retinol (vitamin A alcohol) is a hydrophobic compound and distributes in vivo mainly between binding proteins and cellular membranes. To better clarify the nature of the interactions of retinol with these phases which have a high affinity for it, the thermodynamic parameters of these interactions were studied. The temperature-dependence profiles of the binding of retinol to bovine retinol binding protein, bovine serum albumin, unilamellar vesicles of dioleoylphosphatidylcholine, and plasma membranes from rat liver were determined. It was found that binding of retinol to retinol binding protein is characterized by a large increase in entropy (T delta S degrees = +10.32 kcal/mol) and no change in enthalpy. Binding to albumin is driven by enthalpy (delta H degrees = -8.34 kcal/mol) and is accompanied by a decrease in entropy (T delta S degrees = -2.88 kcal/mol). Partitioning of retinal into unilamellar vesicles and into plasma membranes is stabilized both by enthalpic (delta H degrees was -3.3 and -5.5 kcal/mol, respectively) and by entropic (T delta S degrees was +4.44 and +2.91 kcal/mol, respectively) components. The implications of these finding are discussed.     

Alpha-helix formation is required for high affinity binding of human apolipoprotein A-I to lipids

Apolipoprotein (apo) A-I is thought to undergo a conformational change during lipid association that results in the transition of random coil to alpha-helix. Using a series of deletion mutants lacking different regions along the molecule, we examined the contribution of alpha-helix formation in apoA-I to the binding to egg phosphatidylcholine (PC) small unilamellar vesicles (SUV). Binding isotherms determined by gel filtration showed that apoA-I binds to SUV with high affinity and deletions in the C-terminal region markedly decrease the affinity. Circular dichroism measurements demonstrated that binding to SUV led to an increase in alpha-helix content, but the helix content was somewhat less than in reconstituted discoidal PC.apoA-I complexes for all apoA-I variants, suggesting that the helical structure of apoA-I on SUV is different from that in discs. Isothermal titration calorimetry showed that the binding of apoA-I to SUV is accompanied by a large exothermic heat and deletions in the C-terminal regions greatly decrease the heat. Analysis of the rate of release of heat on binding, as well as the kinetics of quenching of tryptophan fluorescence by brominated PC, indicated that the opening of the N-terminal helix bundle is a rate-limiting step in apoA-I binding to the SUV surface. Significantly, the correlation of thermodynamic parameters of binding with the increase in the number of helical residues revealed that the contribution of alpha-helix formation upon lipid binding to the enthalpy and the free energy of the binding of apoA-I is -1.1 and -0.04 kcal/mol per residue, respectively. These results indicate that alpha-helix formation, especially in the C-terminal regions, provides the energetic source for high affinity binding of apoA-I to lipids.     

Glycolipid transfer protein mediated transfer of glycosphingolipids between membranes: a model for action based on kinetic and thermodynamic analyses

Glycolipid transfer protein (GLTP) catalyzes the intermembrane transfer of lipids that have sugars beta-linked to either diacylglycerol or ceramide backbones, including simple glycosphingolipids (GSLs) and gangliosides. The present study provides a quantitative understanding of GLTP action involving bilayer vesicles that have high and low curvature stress, i.e., small and large unilamellar vesicles (SUVs and LUVs). When the GSL intervesicular transfer was monitored in real time using an established fluorescence resonance energy approach, the initial GSL transfer rates (v(0)) and net transfer equilibrium (K(eq)) were determined for GLTP-mediated transfer from SUVs and LUVs over the temperature range of 30-44 degrees C. v(0) exhibited a linear dependence with respect to varying GLTP concentrations (0-143 nM range) in SUVs and LUVs, suggesting a first order dependence on the GLTP bulk concentration. Thermodynamic parameters associated with the GLTP-GSL transition-state complex and GSL net transfer were determined from linear Arrhenius and van't Hoff plots, respectively. Although initial transfer rates were lower for LUVs than for SUVs, the activation energy barriers were higher for LUVs, while the Gibbs's free energy of the transition states were similar. The formation of a transition-state complex was predominantly enthalpy driven, whereas the net transfer of GSLs was mainly entropy driven. The rate-limiting step for GLTP action appeared to be the surface processes leading to the GLTP-GSL complex formation and release associated with a shuttle/carrier mode of action. Because surface processes leading to the GLTP-GSL complex formation were limiting for GLTP action with SUVs and LUVs, it was concluded that GLTP is likely to be a valuable tool to probe and manipulate GSL environments in membranes.     

The use of N-(7-nitrobenz-2-oxa-1,3-diazole-4-yl)-labeled lipids in determining transmembrane lipid distribution

Transbilayer lipid distribution of small unilamellar vesicles (SUVs) and large unilamellar vesicles (LUVs) was measured using ³¹P-nuclear magnetic resonance (NMR) spectroscopy, chemical modification with 2,4,6-trinitrobenzene sulfonic acid (TNBS) and dithionite reduction of N-(7-nitrobenz-2-oxa-1,3-diazole-4-yl)-labeled lipid (NBD-lipid). The dithionite assay was the most reproducible of the three assays, with 1.2% error for SUVs and 3.9% error for LUVs. The dithionite assay also agreed best with theoretical inner:outer leaflet ratios, based on vesicle diameters determined by electron microscopy (Thomas et al. (1989) Biochem. Biophys. Acta 978, 85–90). Dithionite assay measurements were within 2.7% of theoretical ratios for SUVs and 2.3% for LUVs, while the NMR assay for SUVs was 14% lower than theoretical ratios and 23% lower for LUVs. The accuracy of NBD-lipids as markers for total transbilayer lipid was investigated. NBD-labeled phosphatidylserine, phosphatidylcholine and phosphatidylglycerol were accurate markers for total transbilayer lipid distribution, as their distributions were in close agreement with theoretical ratios. However, NBD-labeled phosphatidylethanolamine displayed a slight preference for the inner leaflet at low mole fractions of phosphatidylethanolamine, while native phosphatidylethanolamine showed a preference for the outer leaflet at the same concentration. NBD-labeled phosphatidic acid also showed a slight preference for the inner leaflet. We conclude that although dithionite-based assessment of NBD-labeled lipids across membrane bilayers can be a powerful analytical tool, caution must be used in the interpretation of results.     

Electrostatic interactions in a peptide--RNA complex

Parallel experimental measurements and theoretical calculations have been used to investigate the energetics of electrostatic interactions in the complex formed between a 22 residue, alpha-helical peptide from the N protein of phage lambda and its cognate 19 nucleotide box B RNA hairpin. Salt-dependent free energies were measured for both peptide folding from coil to helix and peptide binding to RNA, and from these the salt-dependence of binding pre-folded, helical peptide to RNA was determined ( partial differential (DeltaG degrees (dock))/ partial differential log[KCl]=5.98(+/-0.21)kcal/mol). (A folding transition taking place in the RNA hairpin loop was shown to have a negligible dependence on salt concentration.) The non-linear Poisson-Boltzmann equation was used to calculate the same salt dependence of the binding free energy as 5.87(+/-0.22)kcal/mol, in excellent agreement with the measured value. Close agreement between experimental measurements and calculations was also obtained for two variant peptides in which either a basic or acidic residue was replaced with an uncharged residue, and for an RNA variant with a deletion of a single loop nucleotide. The calculations suggest that the strength of electrostatic interactions between a peptide residue and RNA varies considerably with environment, but that all 12 positive and negative N peptide charges contribute significantly to the electrostatic free energy of RNA binding, even at distances up to 11A from backbone phosphate groups. Calculations also show that the net release of ions that accompanies complex formation originates from rearrangements of both peptide and RNA ion atmospheres, and includes accumulation of ions in some regions of the complex as well as displacement of cations and anions from the ion atmospheres of the RNA and peptide, respectively.