Antimicrobial activity and membrane selective interactions of a synthetic lipopeptide MSI-843

The method of fluorescence resonance energy transfer (FRET) has been employed to monitor cytochrome c interaction with bilayer phospholipid membranes. Liposomes composed of phosphatidylcholine and varying amounts of anionic lipid cardiolipin (CL) were used as model membranes. Trace amount of fluorescent lipid derivative, anthrylvinyl-phosphatidylcholine was incorporated into the membranes to serve energy donor for heme moiety of cytochrome c. Energy transfer efficiency was measured at different lipid and protein concentrations to obtain extensive set of data, which were further analyzed globally in terms of adequate models of protein adsorption and energy transfer on the membrane surface. It has been found that the cytochrome c association with membranes containing 10 mol% CL can be described in terms of equilibrium binding model (yielding dissociation constant Kd = 0.2-0.4 microM and stoichiometry n = 11-13 lipid molecules per protein binding site) combined with FRET model assuming uniform acceptor distribution with the distance of 3.5-3.6 nm between the bilayer midplane and heme moiety of cytochrome c. However, increasing the CL content to 20 or 40 mol% (at low ionic strength) resulted in a different behavior of FRET profiles, inconsistent with the concepts of equilibrium adsorption of cytochrome c at the membrane surface and/or uniform acceptor distribution. To explain this fact, several possibilities are analyzed, including cytochrome c-induced formation of non-bilayer structures and clusters of charged lipids, or changes in the depth of cytochrome c penetration into the bilayer depending on the protein surface density. Additional control experiments have shown that only the latter process can explain the peculiar concentration dependences of FRET at high CL content.     

Cytochrome C interaction with cardiolipin/phosphatidylcholine model membranes: effect of cardiolipin protonation

Resonance energy transfer between anthrylvinyl-labeled phosphatidylcholine as a donor and heme moiety of cytochrome c (cyt c) as an acceptor has been employed to explore the protein binding to model membranes, composed of phosphatidylcholine and cardiolipin (CL). The existence of two types of protein-lipid complexes has been hypothesized where either deprotonated or partially protonated CL molecules are responsible for cyt c attachment to bilayer surface. To quantitatively describe cyt c membrane binding, the adsorption model based on scaled particle and double layer theories has been employed, with potential-dependent association constants being treated as a function of acidic phospholipid mole fraction, degree of CL protonation, ionic strength, and surface coverage. Multiple arrays of resonance energy transfer data obtained under conditions of varying pH, ionic strength, CL content, and protein/lipid molar ratio have been analyzed in terms of the model of energy transfer in two-dimensional systems combined with the adsorption model allowing for area exclusion and electrostatic effects. The set of recovered model parameters included effective protein charge, intrinsic association constants, and heme distance from the bilayer midplane for both types of protein-lipid complexes. Upon increasing CL mole fraction from 10 to 20 mol % (the value close to that characteristic of the inner mitochondrial membrane), the binding equilibrium dramatically shifted toward cyt c association with partially protonated CL species. The estimates of heme distance from bilayer center suggest shallow bilayer location of cyt c at physiological pH, whereas at pH below 6.0, the protein tends to insert into membrane core.     

Charged membrane surfaces impede the protein-mediated transfer of glycosphingolipids between phospholipid bilayers

A lipid transfer protein that facilitates the transfer of glycolipids between donor and acceptor membranes has been investigated using a fluorescence resonance energy transfer assay. The glycolipid transfer protein (23-24 kDa, pI 9.0) catalyzes the high specificity transfer of lipids that have sugars beta-linked to either a ceramide or a diacylglycerol backbone, such as simple glycolipids and gangliosides, but not the transfer of phospholipids, cholesterol, or cholesterol esters. In this study, we examined the effect of different charged lipids on the rate of transfer of anthrylvinyl-labeled galactosylceramide (1 mol %) from a donor to acceptor vesicle population at neutral pH. Compared to neutral donor vesicle membranes, introduction of negatively charged lipid at 5 or 10 mol % into the donor vesicles significantly decreased the transfer rate. Introduction of the same amount of negative charge into the acceptor vesicle membrane did not impede the transfer rate as effectively. Also, positive charge in the donor vesicle membrane was not as effective at slowing the transfer rate as was negative charge in the donor vesicle. Increasing the ionic strength of the buffer with NaCl significantly reversed the charge effects. At neutral pH, the transfer protein (pI congruent with 9.0) is expected to be positively charged, which may promote association with the negatively charged donor membrane. Based on these and other experiments, we conclude that the transfer process follows first-order kinetics and that the off-rate of the transfer protein from the donor vesicle surface is the rate-limiting step in the transfer process.     

A fluorescence resonance energy transfer approach for monitoring protein-mediated glycolipid transfer between vesicle membranes

A lipid transfer protein, purified from bovine brain (23.7 kDa, 208 amino acids) and specific for glycolipids, has been used to develop a fluorescence resonance energy transfer assay (anthrylvinyl-labeled lipids; energy donors and perylenoyl-labeled lipids; energy acceptors) for monitoring the transfer of lipids between membranes. Small unilamellar vesicles composed of 1 mol% anthrylvinyl-galactosylceramide, 1.5 mol% perylenoyl-triglyceride, and 97.5% 1-palmitoyl-2-oleoyl phosphatidylcholine (POPC) served as donor membranes. Acceptor membranes were 100% POPC vesicles. Addition of glycolipid transfer protein to mixtures of donor and acceptor vesicles resulted in increasing emission intensity of anthrylvinyl-galactosylceramide and decreasing emission intensity of the nontransferable perylenoyl-triglyceride as a function of time. The behavior was consistent with anthrylvinyl-galactosylceramide being transferred from donor to acceptor vesicles. The anthrylvinyl and perylenoyl energy transfer pair offers advantages over frequently used energy transfer pairs such as NBD and rhodamine. The anthrylvinyl emission overlaps effectively the perylenoyl excitation spectrum and the fluorescence parameters of the anthrylvinyl fluorophore are nearly independent of the medium polarity. The nonpolar fluorophores are localized in the hydrophobic region of the bilayer thus producing minimal disturbance of the bilayer polar region. Our results indicate that this method is suitable for assay of lipid transfer proteins including mechanistic studies of transfer protein function.     

Intermembrane transfer of polyethylene glycol-modified phosphatidylethanolamine as a means to reveal surface-associated binding ligands on liposomes

In order to explore the use of exchangeable poly(ethylene glycol) (PEG)-modified diacylphosphatidylethanolamines (PE) to temporarily shield binding ligands attached to the surface of liposomes, a model reaction based on inhibition and subsequent recovery of biotinylated liposome binding to streptavidin immobilized on superparamagnetic iron oxide particles (SA magnetic particles) was developed. PEG-lipid incorporation into biotinylated liposomes decreased liposome binding to SA magnetic particles in a non-linear fashion, where as little as 0.1 mol% PEG-PE resulted in a 20% decrease in binding. Using an assay based on inhibition of binding, PEG(2000)-PE transfer from donor liposomes to biotinylated acceptor liposomes could be measured. The influence of temperature and acyl chain composition on the transfer of PEG-diacyl PEs from donor liposomes to acceptor liposomes, consisting of 1,2-dioleoyl-sn-glycero-3-phosphocholine, cholesterol and N-((6-biotinoyl)amino)hexanoyl)-1,2-distearoyl-sn-glycero-3-phosphoethanolamine (54.9:45:0.1 mole ratio), was measured. Donor liposomes were prepared using 1,2-distearoyl-sn-glycero-3-phosphocholine (50 mol%), cholesterol (45 mol%) and 5 mol% of either PEG-derivatized 1,2-dimyristoyl-sn-glycero-3-phosphoethanolamine (DMPE-PEG(2000)), 1,2-dipalmitoyl-sn-glycero-3-phosphoethanolamine (DPPE-PEG(2000)), or 1,2-distearoyl-sn-glycero-3-phosphoethanolamine (DSPE-PEG(2000)). Transfer of DSPE-PEG(2000) to the donor liposomes was not detected under the conditions employed. In contrast, DMPE-PEG(2000) was transferred efficiently even at 4 degrees C. Using an acceptor to donor liposome ratio of 1:4, the time required for DMPE-PEG(2000) to become evenly distributed between the two liposome populations (T(EQ)) at 4 degrees C and 37 degrees C was approx. 2 and <0.5 h, respectively. An increase in acyl chain length from C14:0 to C16:0 of the PEG-lipid resulted in a significant reduction in the rate of transfer as measured by this assay. The transfer of PEG-lipid out of biotinylated liposomes was also studied in mice following intravenous administration. The relative rates of transfer for the various PEG-lipids were found to be comparable under in vivo and in vitro conditions. These results suggest that it is possible to design targeted liposomes with the targeting ligand protected while in the circulation through the use of PEG-lipids that are selected on the basis of exchange characteristics which result in exposure of the shielded ligand following localization within a target tissue.     

Phosphatidylcholine exchange protein catalyzes the net transfer of phosphatidylcholine to model membranes

2-Stearoyl spin-labeled phosphatidylcholine (PC*) has been introduced into the phosphatidylcholine exchange protein from bovine liver and its electron spin resonance (ESR) spectrum determined. The spin-labeled group in the PC*- exchange protein complex was strongly immobilized. Addition of sodium deoxycholate micelles released PC* from its binding site, producing a mobile signal. This was also observed when micelles of lysophosphatidylcholine and vesicles of phosphatidic acid were added, indicating that the exchange protein can insert its endogenous PC* into interfaces devoid of phosphatidylcholine. ESR spectroscopy was used to measure transfer of PC* from spin-labeled "donor" vesicles to unlabeled "acceptor" vesicles as described by Machida & Ohnishi [Machida, K., & Ohnishi, S. (1978) Biochim. Biophys. Acta 507, 156-164]. The donor vesicles consisted of PC* and phosphatidic acid (75:25 mol%) and the acceptor vesicles of phosphatidylethanolamine and phosphatidic acid (81:19 mol%). Addition of exchange protein catalyzed a net transfer of PC* from donor to acceptor vesicles. This transfer proceeded until the acceptor vesicles contained approximately 2 mol% of PC*. A spontaneous transfer of PC* was not observed. As for the mode of action, it appears that the exchange protein, after insertion of its endogenous PC* into the acceptor, leaves the interface without a bound phospholipid molecule yet continues to shuttle PC* from donor to acceptor.     

Fluorescent energy transfer measurements on fluorescein isothiocyanate modified cytochrome P-450 LM2

The distance between the heme iron and the N-terminus of cytochrome P-450 LM2 was determined by fluorescence energy transfer measurements. Fluorescein isothiocyanate which was covalently bound to the N-terminal methionine was used as donor chromophor. The Ro value between fluorescein isothiocyanate and the heme was calculated to be 3.98 nm. The distance between the nitrogen of the N-terminal methionine and the heme was estimated with 2.84 +/- 0.23 nm excluding most likely the N-terminal amino acid of cytochrome P-450 LM2 to participate in the electron transfer to the heme iron. A cytochrome P-450 LM2 membrane model is proposed.     

Estimation of surface area in very low density human serum lipoproteins

The surface area of very low density lipoproteins (VLDL) from the serum of 15 healthy donors and the surface area of artificial lipid particles have been estimated. The artificial particles were prepared as a mixture of egg phosphatidylcholine and triolein. Two fluorescent probes - energy donor and acceptor - were placed on the surface, and Forster's nonradiative energy transfer was measured; the transfer efficiency is a function of surface area. The fluorescent probe K-68 (4-[5-(phenyloxazolyl-2)-1-pentadecyl)pyridinium) was used as a donor, and DSP-12 (dimethylamino)styryl-N-dodecylpyridinium) was used as an acceptor. The specific surface area of the artificial lipid particles was estimated to be 0.585 +/- 0.015 nm2 per phosphatidylcholine molecule, which is 15% less than in lipid bilayers. The specific area of VLDL particles was 259 +/- 65 m2 per g of total VLDL. This value is close to the specific area of low density lipoproteins (LDL), and corresponds to the area of a spherical particle 10-12 nm in radius. However, VLDL are assumed to be much larger particles as compared with LDL. Therefore, the new data of the VLDL surface area raise a problem of revision of the existing VLDL models.     

Quenching of tryptophan phosphorescence in Escherichia coli alkaline phosphatase by long-range transfer mechanisms to external agents in the rapid-diffusion limit.

Quenching of the room-temperature phosphorescence of Escherichia coli alkaline phosphatase by several freely diffusing molecules was studied, each of whose absorption spectrum overlaps the long-lived emission of this protein and which therefore can quench the excited triplet state by diffusion-enhanced F?rster energy transfer. The presence of additional nonresonance transfer mechanisms was also detected, from a lack of linear dependence of quenching rate on spectral overlap. The quenching agents used were the dye molecules methyl red, methyl orange, and 2-[(4-hydroxyphenyl)azo]benzoic acid, as well as the embedded heme groups of myoglobin, metmyoglobin, and the reduced and oxidized forms of cytochrome c. Quenching was found to be greatly diminished upon reduction of each acceptor, indicating that electron transfer occurs efficiently from the excited tryptophan to the oxidized form of the acceptors. The elimination of this electron transfer in the reduced form affords the opportunity to separately measure the F?rster transfer rates for the heme proteins. When the transfer rate constant thus measured for myoglobin is applied to a model where both donor and acceptor proteins are taken to be spherical with both tryptophan and the heme group placed off center (a model whose quenching rate equation is newly presented here), the depth of the phosphorescent tryptophan beneath the surface of alkaline phosphatase is found to be 16 A. This value is close to the depth of tryptophan 109 (which is known to be the phosphorescent residue in alkaline phosphatase), showing that with properly chosen probes this technique is indeed valuable for distance determinations in protein structure studies.(ABSTRACT TRUNCATED AT 250 WORDS)     

Cholesterol transfer from small and large unilamellar vesicles

The rates of transfer of [14C]cholesterol from small and large unilamellar cholesterol/egg yolk phosphatidylcholine vesicles to a common vesicle acceptor were compared at 37 degrees C. The rate of exchange of cholesterol between vesicles of identical cholesterol concentrations (20 mol%) did not differ from the rate of transfer from donor vesicles containing 20 mol% cholesterol to egg yolk PC vesicles. Further, the rate of transfer of [14C]cholesterol from vesicles containing 15 mol% dicetyl phosphate (to confer a negative charge) was not different from the rate of transfer from neutral vesicles. However, the half-time for transfer of [14C]cholesterol from large unilamellar donor vesicles was about 5-times greater (10.2 h, 80 nm diameter) than from small unilamellar vesicles (2.3 h, 23 nm diameter). These data suggest that increased curvature in small unilamellar vesicles reduces cholesterol-nearest neighbor interactions to allow a more rapid transfer of cholesterol into the aqueous phase.     

Fluorescence resonance energy transfer study of the associative state of membrane-bound complexes of complement proteins C5b-8

Human complement protein C8 was labeled with the fluorescent chromophores fluorescein-5-isothiocyanate (FITC), 3-(4-isothiocyanatophenyl)-7-diethylamine-4-methyl coumarin (IPM), eosin-5-isothiocyanate (EOS), or Texas Red (sulforhodamine-101-sulfonyl chloride; TR) with only minor reduction in the specific hemolytic activity of the protein. The distribution of C5b-8 complexes bound to sheep erythrocyte membranes was investigated by monitoring fluorescence resonance energy transfer (RET) between the following RET donor/acceptor pairs of labeled C8: FITC-C8/EOS-C8, IPM-C8/EOS-C8, and FITC-C8/TR-C8. On binding to membranes containing pre-formed C5b67 complexes, specific RET was detected for each of the donor/acceptor pairs of labeled C8 investigated. In contrast, no energy transfer was observed for these RET donor/acceptor pairs of labeled C8 incubated in the presence of control membranes or in membrane-free solution. On the basis of a consideration of the transfer efficiency that would be expected for donor/acceptor pairs of labeled C8 that were uniformly dispersed on the membrane surface, these results suggest that C5b-8 complexes are aggregated into polymeric clusters when membrane-bound. The efficiency of donor-C8 to acceptor-C8 RET--and the hemolytic activity of membrane-bound C5b-8 (in the absence of C9)--are both related to the surface density of membrane-bound C5b67, suggesting that the physical clustering of the membrane-inserted C5b-8 complex may be related to the expression of its cytolytic activity.     

Intermembrane phospholipid transfer mediated by cell-free extracts of Rhodopseudomonas sphaeroides.

The transfer of phospholipids between two membrane substrates catalyzed by a soluble protein fraction from Rhodopseudomonas sphaeroides has been demonstrated. The assay employs purified intracytoplasmic membrane (ICM) vesicles derived from cells of R. sphaeroides grown on [3H]acetate as the phospholipid donor substrate and phosphatidylcholine (70%)/phosphatidylethanolamine (30%) unilamellar liposomes containing [14C]triolein, a nontransferable marker, as the acceptor substrate for transferred phospholipids. Incubation of these two membrane substrates with a 40 to 80% (NH4)2SO4 protein fraction from R. sphaeroides results in the transfer of tritium-labeled ICM phospholipids to the acceptor membrane substrate. Upon completion of the incubation period, the donor ICM vesicles are quantitatively separated from the acceptor liposomes by precipitation with antibody prepared against whole, purified ICM vesicles. Phospholipid transfer is linear with respect to time and protein concentration, is inhibited by trypsin and heat, and shows an absolute dependence upon the presence of acceptor liposomes and the 40 to 80% (NH4)2SO4 protein fraction. Control experiments indicate that no fusion of the donor and acceptor membrane occurs during the incubation period and that, following prolonged incubation there is no detectable degradation of the labeled lipid components. Preliminary data on the phospholipid specificity of the transfer reaction is also presented.     

Structural mapping of chloroplast coupling factor

Fluorescence resonance energy transfer measurements have been used to investigate the spatial relationships between the nucleotide binding sites and the gamma-subunit of the H+-ATPase from chloroplasts and the orientation of these sites with respect to the membrane surface. Fluorescent maleimides reacted covalently at specific sulfhydryl sites on the gamma-subunit served as energy donors. One sulfhydryl site can be labeled only under energized conditions on the thylakoid membrane surface (light site). The two gamma-sulfhydryls exposed after catalytic activation served as a second donor site (disulfide site). In one set of experiments, the nucleotide analogue 2'(3')-(trinitrophenyl)adenosine triphosphate, selectively bound at each of the three nucleotide binding sites of the solubilized coupling factor, was used as an energy acceptor; in another, octadecylrhodamine with its acyl chain inserted in the vesicle bilayer and the rhodamine fluorophore exposed along the membrane surface was the energy acceptor. The distance between the sulfhydryl and disulfide sites was also obtained by sequentially labeling the sites with coumarin (donor) and fluorescein (acceptor) maleimide derivatives, respectively. The results indicate that all three nucleotide sites are approximately equal to 50 A from the light-labeled gamma-sulfhydryl. Two of the nucleotide sites are very far from the gamma-disulfide (greater than 74 A), while the third site, which binds nucleotides reversibly under all conditions, is 62 A from this sulfhydryl. The light-labeled sulfhydryl and disulfide sites are about 42-47 A apart. Finally, the distance of closest approach between the membrane surface of the reconstituted system and the gamma-disulfide is 31 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fluorescence energy transfer studies of transmembrane location of retinal in purple membrane

A diffusion-enhanced energy transfer technique was employed for the determination of transmembrane location of the retinal chromophore in the purple membrane. Theoretical considerations showed that the rate of energy transfer from an energy donor embedded within a membrane to acceptors dissolved in solvent could be described by an analytical function of the distance a of closest approach between the donor and acceptor, if the "rapid-diffusion limit" was attained. The criterion for this limit was given by the relation: (RO)6 much less than 20D tau Da4, where RO is the characteristic distance of energy transfer, D is the diffusion coefficient of the acceptor and tau D is the fluorescence lifetime of the donor in the absence of acceptor. By photo-reduction of the purple membrane with sodium borohydride, the retinal chromophore was converted to a highly fluorescent derivative, which showed a broad emission band in the visible region. From analysis of the fluorescence decay curves of the photo-reduced purple membrane in the presence of various concentrations of cobalt-ethylenediamine tetraacetate (Co-EDTA: energy acceptor), the depth of the chromophore from the membrane surface was estimated to be 8 (+/-3) A. This result was supported by investigations of energy transfer processes in a system where the native purple membranes and the photo-reduced membranes were stacked in parallel: the energy acceptor in this system was the native retinal chromophore.     

Detection of conformationally changed MBP using intramolecular FRET

The principal objective of this study was to explore protein conformational changes using fluorescence resonance energy transfer (FRET) technology. Maltose binding protein (MBP) was adopted as a target model, due to its well-characterized structure and ligand specificity. To the best of our knowledge, this is the first report to provide information regarding the biological distance between the two lobes of MBP upon maltose binding. For the FRET pair, ECFP and EYFP were used as the donor and the acceptor, and were linked genetically to the C-terminal and N-terminal regions of MBP (ECFP:MBP:EYFP), respectively. After the FRET reaction, maltose-treated MBP was shown to exhibit a considerable energy transfer (FRET efficiency (E) = ∼0.11, Distance (D) = ∼6.93 nm) at the ensemble level, which was regarded as reflective of the increase in donor quenching and the upshift in acceptor emission intensity, thereby suggesting that the donor and the acceptor had been brought close together as the result of structural alterations in MBP. However, upon glucose treatment, no FRET phenomenon was detected, thereby implying the specificity of interaction between MBP and maltose. The in vitro FRET results were also confirmed via the acceptor photobleaching method. Therefore, our data showed that maltose-stimulated conformational changes of MBP could be measured by FRET, thereby providing biological information, including the FRET efficiency and the intramolecular distance.     

Cytochrome c induces lipid demixing in weakly charged phosphatidylcholine/phosphatidylglycerol model membranes as evidenced by resonance energy transfer

Resonance energy transfer (RET) between anthrylvinyl-labeled phosphatidylcholine (AV-PC) or phosphatidylglycerol (AV-PG) as donors and the heme groups of cytochrome c (cyt c) as acceptors was examined in PC/PG model membranes containing 10, 20 or 40 mol% PG with an emphasis on evaluating lipid demixing caused by this protein. The differences between AV-PC and AV-PG RET profiles observed at PG content 10 mol% were attributed to cyt c ability to produce segregation of acidic lipids into lateral domains. The radius of lipid domains recovered using Monte-Carlo simulation approach was found not to exceed 4 nm pointing to the local character of cyt c-induced lipid demixing. Increase of the membrane PG content to 20 or 40 mol% resulted in domain dissipation as evidenced by the absence of any RET enhancement while recruiting AV-PG instead of AV-PC.     

Kinetics and mechanism of exchange of apolipoprotein C-III molecules from very low density lipoprotein particles

Transfer of apolipoprotein (apo) molecules between lipoprotein particles is an important factor in modulating the metabolism of the particles. Although the phenomenon is well established, the kinetics and molecular mechanism of passive apo exchange/transfer have not been defined in detail. In this study, the kinetic parameters governing the movement of radiolabeled apoC molecules from human very low density lipoprotein (VLDL) to high density lipoprotein (HDL3) particles were measured using a manganese phosphate precipitation assay to rapidly separate the two types of lipoprotein particles. In the case of VLDL labeled with human [14C]apoCIII1, a large fraction of the apoCIII1 transfers to HDL3 within 1 minute of mixing the two lipoproteins at either 4 degrees or 37 degrees C. As the diameter of the VLDL donor particles is decreased from 42-59 to 23-25 nm, the size of this rapidly transferring apoCIII1 pool increases from about 50% to 85%. There is also a pool of apoCIII1 existing on the donor VLDL particles that transfers more slowly. This slow transfer follows a monoexponential rate equation; for 35-40 nm donor VLDL particles the pool size is approximately 20% and the t1/2 is approximately 3 h. The flux of apoCIII molecules between VLDL and HDL3 is bidirectional and all of the apoCIII seems to be available for exchange so that equilibrium is attained. It is likely that the two kinetic pools of apoCIII are related to conformational variations of individual apo molecules on the surface of VLDL particles. The rate of slow transfer of apoCIII1 from donor VLDL (35-40 nm) to acceptor HDL3 is unaffected by an increase in the acceptor to donor ratio, indicating that the transfer is not dependent on collisions between donor and acceptor particles. Consistent with this, apoCIII1 molecules can transfer from donor VLDL to acceptor HDL3 particles across a 50 kDa molecular mass cutoff semipermeable membrane separating the lipoprotein particles. These results indicate that apoC molecules transfer between VLDL and HDL3 particles by an aqueous diffusion mechanism.     

FRET studies with factor X mutants provide insight into the topography of the membrane-bound factor X/Xa

FRET (fluorescence resonance energy transfer) studies have shown that the vitamin K-dependent coagulation proteases bind to membrane surfaces perpendicularly, positioning their active sites above the membrane surfaces. To investigate whether EGF (epidermal growth factor) domains of these proteases play a spacer function in this model of the membrane interaction, we used FRET to measure the distance between the donor fluorescein dye in the active sites of Fl-FPR (fluorescein-D-Phe-Pro-Arg-chloromethane)-inhibited fXa (activated Factor Xa) and its N-terminal EGF deletion mutant (fXa-desEGF1), and the acceptor OR (octadecylrhodamine) dye incorporated into phospholipid vesicles composed of 80% phosphatidylcholine and 20% phosphatidylserine. The average distance of closest approach (L) between fluorescein in the active site and OR at the vesicle surface was determined to be 56+/-1 A (1 A=0.1 nm) and 63+/-1 A for fXa-desEGF1 compared with 72+/-2 A and 75+/-1 A for fXa, in the absence and presence of fVa (activated Factor V) respectively, assuming kappa2=2/3. In comparison, an L value of 95+/-6 A was obtained for a S195C mutant of fXa in the absence of fVa in which fluorescein was attached directly to Cys(195) of fXa. These results suggest that (i) EGF1 plays a spacer function in holding the active site of fXa above the membrane surface, (ii) the average distance between fluorescein attached to Fl-FPR in the active site of fXa and OR at the vesicle surface may not reflect the actual distance of the active-site residue relative to the membrane surface, and (iii) fVa alters the orientation and/or the height of residue 195 above the membrane surface.     

A simplified approach to resonance energy transfer in membranes,lipoproteins and spatially restricted systems

A general model is developed to simulate dipole-dipole resonance energy transfer in spatially restricted systems. At low concentrations of acceptor molecule, the overall quantum yield of a donor population can be defined quantitatively in terms of transfer to multiple defined acceptor regions. Energy transfer at higher acceptor concentrations can be approximated by assuming an exponential dependence of relative quantum yield on the acceptor concentrations. Through geometrical manipulations, this algorithm has been applied using an electronic calculator to systems in which donor-acceptor interaction is limited by unique steric restriction on donor and acceptor distribution within lipid aggregates. The systems that have been analyzed include monomolecular films, bilayer membranes, small cliscoidal lipid-protein complexes and plasma lipoproteins. The observed energy transfer from N-(2-naphthyl)-23.24-dinor-5-cholen-22-amide-3β-ol to N-dansyldimyristoylphosphatidyl-ethanolamine in a dimyristoylphosphatidylcholine bilayer agrees with that predicted by this model.     

The active site of the thrombin-thrombomodulin complex. A fluorescence energy transfer measurement of its distance above the membrane surface

The location of the active site of the membrane-bound anticoagulant complex of thrombin and thrombomodulin has been determined relative to the membrane surface using fluorescence energy transfer. Thrombin was reacted with 5-(dimethylamino)-1-naphthalenesulfonylglutamylglycylarginyl chloromethyl ketone (DEGR-CK) to yield DEGR-thrombin, an analogue of thrombin with a fluorescent dye covalently attached to its active site. When DEGR-thrombin was titrated with thrombomodulin that had been reconstituted into phospholipid vesicles containing octadecylrhodamine, singlet-singlet energy transfer was observed between the donor dyes, each in an active site of a DEGR-thrombin bound to thrombomodulin, and the acceptor dyes at the outer surface of the phospholipid bilayer. The extent of energy transfer reached a maximum when DEGR-thrombin and thrombomodulin were equimolar in the sample, as expected for the formation of a 1:1 complex between thrombin and thrombomodulin. This energy transfer was dependent upon the binding of DEGR-thrombin to thrombomodulin because no energy transfer was observed with vesicles that lacked thrombomodulin, and the extent of energy transfer was reduced greatly by the addition of excess unmodified nonfluorescent thrombin to compete with DEGR-thrombin for binding to the thrombomodulin. From the dependence of the energy transfer upon the acceptor density and assuming kappa 2 = 2/3, the distance of closest approach between a dye in the active site of the thrombin-thrombomodulin complex and a dye at the membrane surface was determined to average 66 A (65 +/- 3 A for phosphatidylcholine vesicles without and 67 +/- 5 A for those with 20% phosphatidylserine). This distance was also insensitive to the presence or absence of Ca2+. These direct measurements indicate that the active site of the membrane-bound thrombin-thrombomodulin complex is located far above the phospholipid surface, that the peptide bond cleaved during the activation of protein C is situated about 66 A above the membrane, that the thrombin binding site on thrombomodulin is positioned more than 45 A above the membrane, ant that thrombin, with a diameter near 40 A, is not positioned alongside thrombomodulin near the membrane to form the thrombin-thrombomodulin complex but is instead bound "on top" of thrombomodulin.