FRET study of membrane proteins: determination of the tilt and orientation of the N-terminal domain of M13 major coat protein

A formalism for membrane protein structure determination was developed. This method is based on steady-state FRET data and information about the position of the fluorescence maxima on site-directed fluorescent labeled proteins in combination with global data analysis utilizing simulation-based fitting. The methodology was applied to determine the structural properties of the N-terminal domain of the major coat protein from bacteriophage M13 reconstituted into unilamellar DOPC/DOPG (4:1 mol/mol) vesicles. For our purpose, the cysteine mutants A7C, A9C, N12C, S13C, Q15C, A16C, S17C, and A18C in the N-terminal domain of this protein were produced and specifically labeled with the fluorescence probe AEDANS. The energy transfer data from the natural Trp-26 to AEDANS were analyzed assuming a two-helix protein model. Furthermore, the polarity Stokes shift of the AEDANS fluorescence maxima is taken into account. As a result the orientation and tilt of the N-terminal protein domain with respect to the bilayer interface were obtained, showing for the first time, to our knowledge, an overall alpha-helical protein conformation from amino acid residues 12-46, close to the protein conformation in the intact phage.     

Membrane-anchoring interactions of M13 major coat protein

The response to hydrophobic mismatch of membrane-bound M13 major coat protein is measured using site-directed fluorescence and ESR spectroscopy. For this purpose, we investigate the membrane-anchoring interactions of M13 coat protein in model systems consisting of phosphatidylcholine bilayers that vary in hydrophobic thickness. Mutant coat proteins are prepared with an AEDANS-labeled single cysteine residue in the hinge region of the protein or at the C-terminal side of the transmembrane helix. In addition, the fluorescence of the tryptophan residue is studied as a monitor for the N-terminal side of the transmembrane helix. The fluorescence results show that the hinge region and C-terminal side of the transmembrane helix hardly respond to hydrophobic mismatch. In contrast, the N-terminal side of the helical transmembrane domain shifts to a more apolar environment, when the hydrophobic thickness is increased. The apparent strong membrane-anchoring interactions of the C-terminus are confirmed using a mutant that contains a longer transmembrane domain. As a result of this mutation, the tryptophan residue at the N-terminal side of the helical domain clearly shifts to a more polar environment, whereas the labeled position 46 at the C-terminal side is not affected. The phenylalanines in the C-terminal part of the protein play an important role in these apparent strong anchoring interactions. This is demonstrated with a mutant in which both phenylalanines are replaced by alanine residues. The phenylalanine residues in the C-terminus affect the location in the membrane of the entire transmembrane domain of the protein.     

Transmembrane extension and oligomerization of the CLIC1 chloride intracellular channel protein upon membrane interaction

Chloride intracellular channel proteins (CLICs) differ from most ion channels as they can exist in both soluble and integral membrane forms. The CLICs are expressed as soluble proteins but can reversibly autoinsert into the membrane to form active ion channels. For CLIC1, the interaction with the lipid bilayer is enhanced under oxidative conditions. At present, little evidence is available characterizing the structure of the putative oligomeric CLIC integral membrane form. Previously, fluorescence resonance energy transfer (FRET) was used to monitor and model the conformational transition within CLIC1 as it interacts with the membrane bilayer. These results revealed a large-scale unfolding between the C- and N-domains of CLIC1 as it interacts with the membrane. In the present study, FRET was used to probe lipid-induced structural changes arising in the vicinity of the putative transmembrane region of CLIC1 (residues 24-46) under oxidative conditions. Intramolecular FRET distances are consistent with the model in which the N-terminal domain inserts into the bilayer as an extended α-helix. Further, intermolecular FRET was performed between fluorescently labeled CLIC1 monomers within membranes. The intermolecular FRET shows that CLIC1 forms oligomers upon oxidation in the presence of the membranes. Fitting the data to symmetric oligomer models of the CLIC1 transmembrane form indicates that the structure is large and most consistent with a model comprising approximately six to eight subunits.     

Real Time Observation of Single Membrane Protein Insertion Events by the Escherichia coli Insertase YidC

Membrane protein translocation and insertion is a central issue in biology. Here we focus on a minimal system, the membrane insertase YidC of Escherichia coli that inserts small proteins into the cytoplasmic membrane. In a reconstituted system individual insertion processes were followed by single-pair fluorescence resonance energy transfer (FRET), with a pair of fluorophores on YidC and the substrate Pf3 coat protein. After addition of N-terminally labeled Pf3 coat protein a close contact to YidC at its cytoplasmic label was observed. This allowed to monitor the translocation of the N-terminal domain of Pf3 coat protein across the membrane in real time. Translocation occurred within milliseconds as the label on the N-terminal domain rapidly approached the fluorophore on the periplasmic domain of YidC at the trans side of the membrane. After the close contact, the two fluorophores separated, reflecting the release of the translocated Pf3 coat protein from YidC into the membrane bilayer. When the Pf3 coat protein was labeled C-terminally, no translocation of the label was observed although efficient binding to the cytoplasmic positions of YidC occurred.     

Asymmetric dipping of bacteriophage M13 coat protein with increasing lipid bilayer thickness

Knowledge about the vertical movement of a protein with respect to the lipid bilayer plane is important to understand protein functionality in the biological membrane. In this work, the vertical displacement of bacteriophage M13 major coat protein in a lipid bilayer is used as a model system to study the molecular details of its anchoring mechanism in a homologue series of lipids with the same polar head group but different hydrophobic chain length. The major coat proteins were reconstituted into 14:1PC, 16:1PC, 18:1PC, 20:1PC, and 22:1PC bilayers, and the fluorescence spectra were measured of the intrinsic tryptophan at position 26 and BADAN attached to an introduced cysteine at position 46, located at the opposite ends of the transmembrane helix. The fluorescence maximum of tryptophan shifted for 700 cm^-1 on going from 14:1PC to 22:1PC, the corresponding shift of the fluorescence maximum of BADAN at position 46 was approximately 10 times less (∼ 70 cm^-1). Quenching of fluorescence with the spin label CAT 1 indicates that the tryptophan is becoming progressively inaccessible for the quencher with increasing bilayer thickness, whereas quenching of BADAN attached to the T46C mutant remained approximately unchanged. This supports the idea that the BADAN probe at position 46 remains at the same depth in the bilayer irrespective of its thickness and clearly indicates an asymmetrical nature of the protein dipping in the lipid bilayer. The anchoring strength at the C-terminal domain of the protein (provided by two phenylalanine residues together with four lysine residues) was estimated to be roughly 5 times larger than the anchoring strength of the N-terminal domain.     

Proximity of the protein moiety of a GPI-anchored protein to the membrane surface: a FRET study

GPI-anchored proteins are ubiquitous on the eukaryotic cell surface, where they are involved in a variety of functions ranging from adhesion to enzymatic catalysis. Indirect evidence suggests that the GPI anchor may hold the protein close to the plasma membrane; however, there is a lack of direct information on the proximity of the protein portion of GPI-anchored proteins to the bilayer surface. The present study uses fluorescence resonance energy transfer (FRET) to address this important problem. The GPI-anchored ectoenzyme placental alkaline phosphatase (PLAP) was purified from a plasma membrane extract of human placental microsomes without the use of butanol. The protein was fluorescently labeled at the N-terminus with 7-(dimethylamino)coumarin-4-acetic acid succinimidyl ester (DMACA-SE) or Oregon Green 488 succinimidyl ester (OG488-SE), and each was reconstituted by detergent dilution into defined lipid bilayer vesicles containing an increasing mole fraction of a fluorescent lipid probe. The fluorescence of the labeled PLAP donors was quenched in a concentration-dependent manner by the lipid acceptors. The energy transfer data were analyzed using an approach that describes FRET between a uniform distribution of donors and acceptors in an infinite plane. The distance of closest approach between the protein moiety of PLAP and the lipid-water interfacial region of the bilayer was estimated to be smaller than 10-14 A. This indicates that the protein portion of PLAP is located very close to the lipid bilayer, possibly resting on the surface. This contact may allow transmission of structural changes from the membrane surface to the protein, which could influence the behavior and catalytic properties of GPI-anchored proteins.     

Membrane assembly of M13 major coat protein: evidence for a structural adaptation in the hinge region and a tilted transmembrane domain

New insights into the low-resolution structure of the hinge region and the transmembrane domain of the membrane-bound major coat protein of the bacteriophage M13 are deduced from a single cysteine-scanning approach using fluorescence spectroscopy. New mutant coat proteins are labeled and reconstituted into phospholipid bilayers with varying headgroup compositions (PC, PE, and PG) and thicknesses (14:1PC, 18:1PC, and 22:1PC). Information about the polarity of the local environment around the labeled sites is deduced from the wavelength of maximum emission using AEDANS attached to the SH groups of the cysteines as a fluorescent probe. It is found that the protein is almost entirely embedded in the membrane, whereas the phospholipid headgroup composition of the membrane hardly affects the overall embedment of the protein in the membrane. From the assessment of a hydrophobic and hydrophilic face of the transmembrane helix, it is concluded that the helix is tilted with respect to the membrane normal. As compared to the thicker 18:1PC and 22:1PC membranes, reconstitution of the protein in the thin 14:1PC membranes results in a loss of helical structure and in the formation of a stretched conformation of the hinge region. It is suggested that the hinge region acts as a flexible spring between the N-terminal amphipathic arm and transmembrane hydrophobic helix. On average, the membrane-bound state of the coat protein can be seen as a gently curved and tilted, "banana-shaped" molecule, which is strongly anchored in the membrane-water interface at the C-terminus. From our experiments, we propose a rather small conformational adaptation of the major coat protein as the most likely reversible mechanism for responding to environmental changes during the bacteriophage disassembly and assembly process.     

Fluorescence resonance energy transfer shows a close helix-helix distance in the transmembrane M13 procoat protein

During the membrane insertion process the major coat protein of bacteriophage M13 assumes a conformation in which two transmembrane helices corresponding to the leader sequence and the anchor region in the mature part of the protein coming into close contact with each other. Previous studies on the molecular mechanism of membrane insertion of M13 procoat protein have shown that this interaction between the two helices might drive the actual translocation process. We investigated the intramolecular distance between the two helices of the transmembrane procoat protein by measuring fluorescence resonance energy transfer (FRET) between the donor (Tyr) placed in one helix and the acceptor (Trp) placed in the other helix. Various mutant procoat proteins with differently positioned donor-acceptor pairs were generated, purified, and reconstituted into artificial lipid bilayers. The results obtained from the FRET measurements, combined with molecular modeling, show that the transmembrane helices are in close contact on the order of 1-1.5 nm. The present approach might be of general interest for determining the topology and the folding of membrane proteins.     

Interaction of a two-transmembrane-helix peptide with lipid bilayers and dodecyl sulfate micelles

To probe structural changes that occur when a membrane protein is transferred from lipid bilayers to SDS micelles, a fragment of bacteriorhodopsin containing transmembrane helical segments A and B was studied by fluorescence spectroscopy, molecular dynamics (MD) simulation, and stopped flow kinetics. In lipid bilayers, F?rster resonance energy transfer (FRET) was observed between tyrosine 57 on helix B and tryptophans 10 and 12 on helix A. FRET efficiency decreased substantially when the peptide was transferred to SDS. MD simulation showed no evidence for significant disruption of helix-helix interactions in SDS micelles. However, a cluster of water molecules was observed to form a hydrogen-bonded network with the phenolic hydroxyl group of tyrosine 57, which probably causes the disappearance of tyrosine-to-tryptophan FRET in SDS. The tryptophan quantum yield decreased in SDS, and the change occurred at nearly the same rate as membrane solubilization. The results provide a clear example of the importance of corroborating distance changes inferred from FRET by using complementary methods.     

Membrane-bound conformation of M13 major coat protein: a structure validation through FRET-derived constraints

M13 major coat protein, a 50-amino-acid-long protein, was incorporated into DOPC/DOPG (80/20 molar ratio) unilamellar vesicles. Over 60% of all amino acid residues was replaced with cysteine residues, and the single cysteine mutants were labeled with the fluorescent label I-AEDANS. The coat protein has a single tryptophan residue that is used as a donor in fluorescence (or F?rster) resonance energy transfer (FRET) experiments, using AEDANS-labeled cysteines as acceptors. Based on FRET-derived constraints, a straight alpha-helix is proposed as the membrane-bound conformation of the coat protein. Different models were tested to represent the molecular conformations of the donor and acceptor moieties. The best model was used to make a quantitative comparison of the FRET data to the structures of M13 coat protein and related coat proteins in the Protein Data Bank. This shows that the membrane-bound conformation of the coat protein is similar to the structure of the coat protein in the bacteriophage that was obtained from x-ray diffraction. Coat protein embedded in stacked, oriented bilayers and in micelles turns out to be strongly affected by the environmental stress of these membrane-mimicking environments. Our findings emphasize the need to study membrane proteins in a suitable environment, such as in fully hydrated unilamellar vesicles. Although larger proteins than M13 major coat protein may be able to handle environmental stress in a different way, any membrane protein with water exposed parts in the C or N termini and hydrophilic loop regions should be treated with care.     

Effect of membrane microheterogeneity and domain size on fluorescence resonance energy transfer

Studies of multicomponent membranes suggest lateral inhomogeneity in the form of membrane domains, but the size of small (nanoscale) domains in situ cannot be determined with current techniques. In this article, we present a model that enables extraction of membrane domain size from time-resolved fluorescence resonance energy transfer (FRET) data. We expand upon a classic approach to the infinite phase separation limit and formulate a model that accounts for the presence of disklike domains of finite dimensions within a two-dimensional infinite planar bilayer. The model was tested against off-lattice Monte Carlo calculations of a model membrane in the liquid-disordered (l(d)) and liquid-ordered (l(o)) coexistence regime. Simulated domain size was varied from 5 to 50 nm, and two fluorophores, preferentially partitioning into opposite phases, were randomly mixed to obtain the simulated time-resolved FRET data. The Monte Carlo data show clear differences in the efficiency of energy transfer as a function of domain size. The model fit of the data yielded good agreement for the domain size, especially in cases where the domain diameter is <20 nm. Thus, data analysis using the proposed model enables measurement of nanoscale membrane domains using time-resolved FRET.     

Dysferlin forms a dimer mediated by the C2 domains and the transmembrane domain in vitro and in living cells

Dysferlin was previously identified as a key player in muscle membrane repair and its deficiency leads to the development of muscular dystrophy and cardiomyopathy. However, little is known about the oligomerization of this protein in the plasma membrane. Here we report for the first time that dysferlin forms a dimer in vitro and in living adult skeletal muscle fibers isolated from mice. Endogenous dysferlin from rabbit skeletal muscle exists primarily as a ～460 kDa species in detergent-solubilized muscle homogenate, as shown by sucrose gradient fractionation, gel filtration and cross-linking assays. Fluorescent protein (YFP) labeled human dysferlin forms a dimer in vitro, as demonstrated by fluorescence correlation spectroscopy (FCS) and photon counting histogram (PCH) analyses. Dysferlin also dimerizes in living cells, as probed by fluorescence resonance energy transfer (FRET). Domain mapping FRET experiments showed that dysferlin dimerization is mediated by its transmembrane domain and by multiple C2 domains. However, C2A did not significantly contribute to dimerization; notably, this is the only C2 domain in dysferlin known to engage in a Ca-dependent interaction with cell membranes. Taken together, the data suggest that Ca-insensitive C2 domains mediate high affinity self-association of dysferlin in a parallel homodimer, leaving the Ca-sensitive C2A domain free to interact with membranes.     

The activation energy for insertion of transmembrane alpha-helices is dependent on membrane composition

The physical mechanisms that govern the folding and assembly of integral membrane proteins are poorly understood. It appears that certain properties of the lipid bilayer affect membrane protein folding in vitro, either by modulating helix insertion or packing. In order to begin to understand the origin of this effect, we investigate the effect of lipid forces on the insertion of a transmembrane alpha-helix using a water-soluble, alanine-based peptide, KKAAAIAAAAAIAAWAAIAAAKKKK-amide. This peptide binds to preformed 1,2-dioleoyl-l-alpha-phosphatidylcholine (DOPC) vesicles at neutral pH, but spontaneous transmembrane helix insertion directly from the aqueous phase only occurs at high pH when the Lys residues are de-protonated. These results suggest that the translocation of charge is a major determinant of the activation energy for insertion. Time-resolved measurements of the insertion process at high pH indicate biphasic kinetics with time constants of ca 30 and 430 seconds. The slower phase seems to correlate with formation of a predominantly transmembrane alpha-helical conformation, as determined from the transfer of the tryptophan residue to the hydrocarbon region of the membrane. Temperature-dependent measurements showed that insertion can proceed only above a certain threshold temperature and that the Arrhenius activation energy is of the order of 90 kJ mol(-1). The kinetics, threshold temperature and the activation energy change with the mole fraction of 1,2-dioleoyl-l-alpha-phosphatidylethanolamine (DOPE) introduced into the DOPC membrane. The activation energy increases with increasing DOPE content, which could reflect the fact that this lipid drives the bilayer towards a non-bilayer transition and increases the lateral pressure in the lipid chain region. This suggests that folding events involving the insertion of helical segments across the bilayer can be controlled by lipid forces.     

Outer membrane phospholipase A is dimeric in phospholipid bilayers: a cross-linking and fluorescence resonance energy transfer study.

In the cell, the activity of outer membrane phospholipase A (OMPLA) is strictly regulated to prevent uncontrolled breakdown of the membrane lipids. Previously, it has been shown that the enzymatic activity is modulated by reversible dimerization. The current studies were carried out to define the oligomeric state of OMPLA in a membrane and to investigate the activation process. Three single-cysteine variant proteins H26C, H234C, and S144C were produced and purified to homogeneity. Using maleimido-based homo-bifunctional cross-linking reagents, H26C could be efficiently cross-linked as assessed by SDS-PAGE, whereas S144C and H234C could not be cross-linked. These data suggest that residue 26 is located close to the dimer symmetry axis. H26C was specifically labeled with 5-({[(2-iodoacetyl)amino]ethyl}amino)naphthalene-1-sulfonic acid and N,N'-dimethyl-N-(iodoacetyl)-N-(7-nitrobenz-2-oxa-1, 3-diazol-4-yl)ethylenediamine as the fluorescent energy donor and acceptor, respectively, and dimerization was investigated using fluorescence resonance energy transfer (FRET). Quenching of the donor in the presence of the acceptor demonstrated the dimeric nature of OMPLA, in agreement with cross-linking data. The observed FRET effect was dependent on the cofactor calcium, and the presence of substrate, indicating the specificity of the dimerization process. The labeled protein was reconstituted in phospholipid vesicles. In bilayers, OMPLA exhibited low activity and was dimeric as assessed by FRET. Addition of detergent resulted in a 70-fold increase in activity, while the protein remained dimeric. The results are discussed in terms of the activation of dimeric OMPLA due to changes in the physical state of the bilayer which occur upon perturbation of the membrane integrity.     

Adventures in membrane protein topology. A study of the membrane-bound state of colicin E1.

The molecular aggregate size of the closed state of the colicin E1 channel was determined by fluorescence resonance energy transfer experiments involving a fluorescence donor (three tryptophans, wild-type protein) and a fluorescence acceptor (5-(((acetyl)amino)ethyl)aminonaphthalene-1-sulfonic acid (AEDANS), Trp-deficient protein). There was no evidence of energy transfer between the donor and acceptor species when bound to membrane large unilamellar vesicles. These experiments led to the conclusion that the colicin E1 channel is monomeric in the membrane-bound closed channel state. Experiments were also conducted to study the membrane topology of the closed colicin channel in membrane large unilamellar vesicles using acrylamide as the membrane-impermeant, nonionic quencher of tryptophan fluorescence in a battery of single tryptophan mutant proteins. Furthermore, additional fluorescence parameters, including fluorescence emission maximum, fluorescence quantum yield, and fluorescence decay times, were used to assist in mapping the topology of the closed channel. Results suggest that the closed channel comprises most of the polypeptide of the channel domain and that the hydrophobic anchor domain does not transverse the membrane bilayer but nonetheless is deeply embedded within the hydrocarbon core of the membrane. Finally, a model is proposed which features at least two states that are in rapid equilibrium with each other and in which one state is more heavily populated than the other.     

Membrane topology of the colicin E1 channel using genetically encoded fluorescence

The membrane topology of the colicin E1 channel domain was studied by fluorescence resonance energy transfer (FRET). The FRET involved a genetically encoded fluorescent amino acid (coumarin) as the donor and a selectively labeled cysteine residue tethered with DABMI (4-(dimethylamino)phenylazophenyl-4'-maleimide) as the FRET acceptor. The fluorescent coumarin residue was incorporated into the protein via an orthogonal tRNA/aminoacyl-tRNA synthetase pair that allowed selective incorporation into any site within the colicin channel domain. Each variant harbored a stop (TAG) mutation for coumarin incorporation and a cysteine (TGT) mutation for DABMI attachment. Six interhelical distances within helices 1-6 were determined using FRET analysis for both the soluble and membrane-bound states. The FRET data showed large changes in the interhelical distances among helices 3-6 upon membrane association providing new insight into the membrane-bound structure of the channel domain. In general, the coumarin-DABMI FRET interhelical efficiencies decreased upon membrane binding, building upon the umbrella model for the colicin channel. A tentative model for the closed state of the channel domain was developed based on current and previously published FRET data. The model suggests circular arrangement of helices 1-7 in a clockwise direction from the extracellular side and membrane interfacial association of helices 1, 6, 7, and 10 around the central transmembrane hairpin formed by helices 8 and 9.     

Studies of Receptor Tyrosine Kinase Transmembrane Domain Interactions: The EmEx-FRET Method

The energetics of transmembrane (TM) helix dimerization in membranes and the thermodynamic principles behind receptor tyrosine kinase (RTK) TM domain interactions during signal transduction can be studied using Förster resonance energy transfer (FRET). For instance, FRET studies have yielded the stabilities of wild-type fibroblast growth factor receptor 3 (FGFR3) TM domains and two FGFR3 pathogenic mutants, Ala391Glu and Gly380Arg, in the native bilayer environment. To further our understanding of the molecular mechanisms of deregulated FGFR3 signaling underlying different pathologies, we determined the effect of the Gly382Asp FGFR3 mutation, identified in a multiple myeloma cell line, on the energetics of FGFR3 TM domain dimerization. We measured dimerization energetics using a novel FRET acquisition and processing method, termed “emission-excitation FRET (EmEx-FRET),” which improves the precision of thermodynamic measurements of TM helix association. The EmEx-FRET method, verified here by analyzing previously published data for wild-type FGFR3 TM domain, should have broad utility in studies of protein interactions, particularly in cases when the concentrations of fluorophore-tagged molecules cannot be controlled.     

Ciprofloxacin interactions with bacterial protein OmpF: modelling of FRET from a multi-tryptophan protein trimer

The outer membrane protein F (OmpF) is known to play an important role in the uptake of fluoroquinolone antibiotics by bacteria. In this study, the degree of binding of the fluoroquinolone antibiotic ciprofloxacin to OmpF in a lipid membrane environment is quantified using a methodology based on F?rster resonance energy transfer (FRET). Analysis of the fluorescence quenching of OmpF is complex as each OmpF monomer presents two tryptophans at different positions, thus sensing two different distributions of acceptors in the bilayer plane. Specific FRET formalisms were derived accounting for the different energy transfer contributions to quenching of each type of tryptophan of OmpF, allowing the recovery of upper and lower boundaries for the ciprofloxacin-OmpF binding constant (K(B)). log (K(B)) was found to lie in the range 3.15-3.62 or 3.58-4.00 depending on the location for the ciprofloxacin binding site assumed in the FRET modelling, closer to the centre or to the periphery of the OmpF trimer, respectively. This methodology is suitable for the analysis of FRET data obtained with similar protein systems and can be readily adapted to different geometries.     

Role of helix nucleation in the kinetics of binding of mastoparan X to phospholipid bilayers

Many antimicrobial peptides undergo a coil-to-helix transition upon binding to membranes. While this conformational transition is critical for function, little is known about the underlying mechanistic details. Here, we explore the membrane-mediated folding mechanism of an antimicrobial peptide, mastoparan X. Using stopped-flow fluorescence techniques in conjunction with a fluorescence resonance energy transfer (FRET) pair, p-cyanophenylalanine (donor) and tryptophan (acceptor), we were able to probe, albeit in an indirect manner, the membrane-mediated folding kinetics of this peptide. Our results show that the association of mastoparan X with model lipid vesicles proceeds with biphasic kinetics. The first step shows a large change in the FRET signal, indicating that the helix forms early in the time course of the interaction, while the second step where a further increase in tryptophan fluorescence is observed presumably reflects deeper insertion of the peptide into the bilayer. Additional kinetic studies on a double mutant of mastoparan X, designed to form a nucleation site for alpha-helix formation through coordination with a metal ion (e.g., Zn2+ or Ni2+), indicate that while the coil-to-helix transition occurs in the first step, it follows the rate-determining docking of the peptide onto the membrane surface. Taken together, these results indicate that the initial association of the peptide with the membrane occurs in a nonhelical conformation, which rapidly converts to a helical state within the anisotropic environment of the bilayer surface.     

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.