Fluorescence and 13C NMR determination of side-chain and backbone dynamics of synthetic melittin and melittin analogues in isotropic solvents

The dynamics in isotopic solvents of selectively 13C labeled synthetic melittin and three analogues have been investigated by using NMR and fluorescence techniques both separately and in combination. In conjunction with the "model-free" approach to interpretation of NMR relaxation data [Lipari, G., & Szabo, A. (1982) J. Am. Chem. Soc. 104, 4546-4570], the availability of steady-state fluorescence anisotropy and lifetime data augment T1, T2, and NOE data to provide quantitative information about fluorophore dynamics in these peptides. A method is presented for using combined fluorescence and NMR data to obtain technique- and model-independent values for parameters describing local motion of 13C-labeled fluorophores in peptides and proteins. The dynamics of melittin and melittin analogues are found to be consistent with structural characteristics inferred from CD, fluorescence, and NMR spectral information presented in the preceding paper (Weaver et al., 1989). In particular, the mobility of the random coil peptide monomers is shown to be quite similar, while side-chain as well as peptide backbone motion in the aggregated or oligomeric species differs markedly among the analogues. For melittin itself, experimentally determined overall rotational correlation times for the monomer and tetramer agree very well with values predicted on the basis of solvent-accessible protein surface area. The local dynamics of selectively 13C-labeled Trp-19 and Gly-12 residues of melittin are also found to be consistent with peptide structure. In random coil melittin monomer, a specific model for the motion indicates that the Trp side chain moves through an approximate angle of +/- 71 degrees about the beta-gamma bond with a correlation time of 159 +/- 24 ps. In melittin tetramer, the indole moiety is spatially more confined with a flip angle of +/- 37 degrees, yet demonstrates an increased rate of motion with a correlation time of 56 +/- 8 ps. The constrained mobility of the Trp-19 side chain is consistent with motional constraints inferred from the X-ray structure of melittin tetramer. These results show that protein side-chain motion, even of moieties as large as indole, can occur on the picosecond time scale and that these motions are reasonably similar to those inferred from molecular dynamics simulations.     

Characterization of selectively 13C-labeled synthetic melittin and melittin analogues in isotropic solvents by circular dichroism, fluorescence, and NMR spectroscopy

The spectroscopic and functional characterization of 13C-labeled synthetic melittin and three analogues is described. Selectively 13C-enriched tryptophan ( [13C delta 1]-L-Trp) and glycine ( [13C alpha]Gly) were incorporated into melittin and three analogues by de novo peptide synthesis. 13C-Labeled tryptophan was incorporated into melittin at position 19 and into single-tryptophan analogues of melittin at positions 17, 11, and 9, respectively. Each of the synthetic peptides contained 13C-labeled glycine at position 12 only. The peptides were characterized functionally in a cytolytic assay, and spectroscopically by CD, fluorescence, and NMR. The behavior of 13C-labeled synthetic melittin was, in all respects, indistinguishable from that of the naturally occurring peptide. All of the analogues were found to be efficient lytic agents and thus were functionally similar to the native peptide, yet no evidence was found for formation of a melittin-like tetramer by any of the analogues in aqueous media, although there was a propensity for apparently nonspecific peptide aggregation, especially for MLT-W9. Since the analogues did exhibit fractional helicities by CD comparable to or even greater than melittin itself in the presence of methanol, we infer that tetramer assembly requires not only the ability to form alpha-helix but also a very precise packing of amino acid side chains of the constituent monomers. The 13C chemical shift of the Gly-12 C alpha was found to be a sensitive marker for helix formation in all of the peptides. For melittin itself, 13C NMR spectra revealed a downfield shift of approximately 1.8 ppm for the Gly-12 13C alpha resonance of the tetramer relative to that observed for the free monomer in D2O. In mixed samples containing melittin monomer and tetramer, two discrete Gly-12 13C alpha peaks were observed simultaneously, suggestive of slow exchange between the two species. We conclude that melittin's ability to form a soluble tetramer is not a prerequisite for cytolytic activity, nor is cytolytic potential precisely correlated with the ability to form an amphiphilic helix.     

Structure and dynamics of melittin in lysomyristoyl phosphatidylcholine micelles determined by nuclear magnetic resonance.

Mixed micelles of the 26-residue, lytic peptide melittin (MLT) and 1-myristoyl-2-hydroxyl-sn-glycero-3-phosphocholine (MMPC) in aqueous solution at 25 degrees C were investigated by (13)C- and (31)P-NMR spectroscopy. (13)C alpha chemical shifts of isotopically labeled synthetic MLT revealed that MLT in the micelle is predominantly alpha-helical and that the peptide secondary structure is stable from pH 4 to pH 11. Although the helical transformation of MLT as determined from NMR is evident at lipid:peptide molar ratios as low as 1:2, tryptophan fluorescence measurements demonstrate that well-defined micellar complexes do not predominate until lipid:peptide ratios exceed 30:1. (31)P linewidth measurements indicate that the interaction between phosphate ions in solution and cationic groups on MLT is pH dependent, and that the phosphoryl group of MMPC senses a constant charge, most likely +2, on MLT from pH 4 to pH 10. (13)C-NMR relaxation data, analyzed using the model-free formalism, show that the peptide backbone of MLT is partially, but not completely, immobilized in the mixed micelles. Specifically, order parameters (S(2)) of C alpha-H vectors averaged 0.7 and were somewhat larger for residues in the N-terminal half of the molecule. The amino terminal glycine had essentially the same range of motion as the backbone carbons. Likewise, order parameters for the trp side chain were similar to those found for the peptide C alpha moieties, as was verified by trp fluorescence anisotropy decay data. In contrast, the motion of the lysine side chains was less restricted, the average S(2) values for the C epsilon-H vectors being 0.19, 0.30, and 0.44 for lys-7, 21, and 23, respectively, for MLT in the mixed micelles. Values of the effective correlation time of the local motion tau e were in the motional narrowing limit and usually longer for side-chain atoms than for those in the backbone. The dynamics were independent of pH from pH 4 to pH 9, but at pH 11 the correlation time for the rotational motion of the mixed micelles as a whole increased from 10 ns to 16 ns, and S(2) for the lys side chains increased. Overall it appears that the MLT helix lies near the surface of the micelle at low to neutral pH, but at higher pH its orientation changes, accompanied by deeper penetration of the lysine side chains into the micelle interior. It is apparent, however, that the MLT-lipid interaction is not dependent on deprotonation of any of the titratable cationic groups in the peptide in the pH 4-10 range, and that there is substantial backbone and side-chain mobility in micelle-bound MLT.     

Binding and folding of melittin in the presence of ganglioside GM1 micelles

In this work we examine the binding and folding of the membrane-active peptide, melittin in the presence of ganglioside GM1 micelle. The membrane bilayer is capable of inducing folding to small proteins and peptides upon binding. Using two-dimensional NMR techniques we have shown that at low concentration, GM1 micelle is able to induce an extended helical conformation to MLT. The pulsed-field gradient diffusion NMR study indicates that the peptide partition into GM1 micelle along with about 32% binding. While looking for the binding between MLT and GM1 using saturation transfer difference NMR spectroscopy, Val5, Leu9, Thr11, Ile17, Ser18, and Trp19 have been identified as the residues that are in close proximity to GM1 micelles.     

Investigation of the membrane-active peptides melittin and glucagon by photochemically induced dynamic-nuclear-polarization (photo-CIDNP) NMR

The photochemically induced dynamic-nuclear-polarization (photo-CIDNP) NMR technique was used to investigate the membrane-active peptides melittin and glucagon. The experiments were performed both in the absence and presence of phospholipid vesicles in order to study the topography of the membrane-bound state. From the results it can be concluded that the melittin peptide chain is oriented in such a way that the single tryptophan residue (Trp19) reaches into the membrane. In the case of glucagon, a binding interaction with vesicle membranes is indicated within the pH range 2-10, whereby the single tryptophan residue (Trp25) is buried in the lipid bilayer and the tyrosine and histidine residues are exposed to the aqueous solvent.     

Comparison of 15N- and 13C-determined parameters of mobility in melittin

Backbone and tryptophan side-chain mobilities in the 26-residue, cytolytic peptide melittin (MLT) were investigated by ¹⁵N and ¹³C NMR. Specifically, inverse-detected ¹⁵N T₁ and steady-state NOE measurements were made at 30 and 51 MHz on MLT at 22 °C enriched with ¹⁵N at six amide positions and in the Trp¹⁹ side chain. Both the disordered MLT monomer (1.2 mM peptide at pH 3.6 in neat water) and -helical MLT tetramer (4.0 mM peptide at pH 5.2 in 150 mM phosphate buffer) were examined. The relaxation data were analyzed in terms of the Lipari and Szabo model-free formalism with three parameters: _m, the correlation time for the overall rotation; S², a site-specific order parameter which is a measure of the amplitude of the internal motion; and _e, a local, effective correlation time of the internal motion. A comparison was made of motional parameters from the ¹⁵N measurements and from ¹³C measurements on MLT, the latter having been made here and previously [Kemple et al. (1997) Biochemistry, 36, 1678–1688]. _m and _e values were consistent from data on the two nuclei. In the MLT monomer, S² values for the backbone N-H and C-H vectors in the same residue were similar in value but in the tetramer the N-H order parameters were about 0.2 units larger than the C-H order parameters. The Trp side-chain N-H and C-H order parameters, and _e values were generally similar in both the monomer and tetramer. Implications of these results regarding the dynamics of MLT are examined.     

Fluorescence analysis of tryptophan-containing variants of the LamB signal sequence upon insertion into a lipid bilayer

To investigate the interaction of the LamB signal sequence with lipid bilayers, we have synthesized three tryptophan-containing analogues of the wild-type signal peptide. The tryptophan residues were used as intrinsic fluorescent probes of the N-terminal (position 5), central (position 18), and C-terminal (position 24) regions of the 25-residue peptide. The tryptophan substitutions did not significantly alter the physical properties of the wild-type signal peptide. In the presence of lipid vesicles which mimic the composition of the Escherichia coli inner membrane, the peptides adopt alpha-helical structure, and the tryptophan fluorescence emission maximum is shifted to shorter wavelength, indicating that the peptides insert into the acyl chain region of the lipid bilayer. Fluorescence quenching by soluble, aqueous-phase (I-), and membrane-resident (nitroxide-labeled lipids) quenchers was used to locate the tryptophans in each peptide within the bilayer. The C-terminus was interfacial while the central region of the signal sequence was deeply buried within the acyl chain region of the bilayer. The tryptophan at position 5 was buried but less deeply than the tryptophan at position 18. This topology is consistent with either a looped or a transmembrane orientation of signal peptide. However, either structure must accommodate the high helical content of the peptides in vesicles. These results indicate that the LamB signal sequence spontaneously inserts into the acyl chain region of lipid membranes in the absence of any of the proteins involved in protein secretion.     

Site-specific tryptophan fluorescence spectroscopy as a probe of membrane peptide structure and dynamics

The fluorescence from tryptophan contains valuable information about the environment local to the indole side-chain. This environment sensitivity coupled with the ability to synthetically or genetically incorporate a single tryptophan residue at specific sites in a polypeptide sequence has provided the membrane biophysicist with powerful tools for examining the structure and dynamics of membrane peptides and proteins. Here we briefly review the use of site-specific tryptophan fluorescence spectroscopy to probe aspects of peptide orientation, structure, and dynamics in lipid bilayers, focusing on recent developments in the literature.     

Fluorescence studies of the secondary structure and orientation of a model ion channel peptide in phospholipid vesicles.

A 21-residue peptide of the sequence (LSSLLSL)3 forms ion channels when incorporated into planar lipid bilayer membranes of diphytanoylphosphatidylcholine (diPhy-PC). The frequency of channel openings increases with the applied voltage gradient. We investigated the molecular and structural mechanisms underlying this voltage dependence. A series of seven peptides, each containing a tryptophan substituted for a single residue in the middle heptad, was synthesized, purified, and incorporated into small, unilamellar, diPhy-PC vesicles. We measured circular dichroism, maximum fluorescence emission wave-lengths, and fluorescence quenching by both aqueous and lipid hydrocarbon-associated quenchers. Circular dichroism spectra and the observed sequence periodicity of all fluorescence and fluorescence quenching data are consistent with an alpha-helical peptide secondary structure. Energy transfer quenching measurements using N-terminally labeled (LSSLLSL)3 co-incorporated at lipid/peptide ratios greater than 100 into vesicles with one of the Trp-substituted peptides showed that the vesicle-associated peptide, in the absence of a voltage gradient across the bilayer, exists as an equilibrium mixture of monomers and dimers. Static fluorescence quenching measurements using different lipid-bound quenchers indicate that the helical axis of a representative lipid-associated peptide is, on average, oriented parallel to the surface of the membrane and located a few angstroms below the polar head group/hydrocarbon boundary. This surface orientation for the peptide is confirmed by the complementary sequence periodicity observed for Trp fluorescence emission wavelength shifts and collisional quenching by aqueous CsCl.(ABSTRACT TRUNCATED AT 250 WORDS)     

Bilayer acyl chain dynamics and lipid-protein interaction: the effect of the M13 bacteriophage coat protein on the decay of the fluorescence anisotropy of parinaric acid.

Nanosecond fluorescence polarization anisotropy decay is used to determine the effect of the bacteriophage M13 coat protein on lipid bilayer acyl chain dynamics and order. The fluorescent acyl chain analogues cis- and trans-parinaric acid were used to determine the rate and extent of the angular motion of acyl chains in liquid crystalline (39 degrees C) dimyristoylphosphatidylcholine bilayers free of coat protein or containing the coat protein at a protein:lipid ratio of 1:30. Subnanosecond time resolution was obtained by using synchrotron radiation as the excitation source for single photon counting detection. Previous measurements of Förster energy transfer from coat protein tryptophan to cis- or trans-parinaric acid have shown that these probes are randomly distributed in the bilayer with respect to the protein. The anisotropy decay observed for pure bilayers has the form of a rapid drop, followed by a nonzero constant region extending from roughly 3 ns to at least 12 ns. The magnitude of the anisotropy in the plateau region is simply related to the acyl chain order parameter. The effect of the M13 coat protein is to increase the acyl chain order parameter significantly while having only a small effect on the rate of angular relaxation. This behavior is rationalized in terms of a simple microscopic model. The order parameters for pure lipid and coat protein containing bilayers are compared to 2H-NMR values.     

Peptide inhibitors of melittin action

The sequence of peptides necessary to inhibit melittin-induced lysis was studied using 13 peptide analogues of the inhibitor Ac-IVIFDC-NH₂. Although this inhibitor is a disulfide-linked dimer, inhibition was equally effective if the thiol SH was blocked or replaced by methionine or lysine. The substitution of phenylalanine with other aromatic residues preserved activity, as did the replacement of aspartic acid by asparagine. The results suggest that the cytolytic activity of melittin can be inhibited by a short peptide of four hydrophobic residues followed by two other nonspecific residues. Fluorescence studies showed that the inhibitor caused a blue shift in the Trp emission spectrum. A spin label attached to the N-terminus of the inhibitor significantly quenched the fluorescence. These data confirmed the involvement of Trp 19 with the inhibitor, also predicted by molecular modeling of the probable binding site. Density gradient studies with large unilamellar vesicles indicated that the inhibitor prevented melittin from reacting with the lipid bilayer.     

Conformation and dynamics of melittin bound to magnetically oriented lipid bilayers by solid-state (31)P and (13)C NMR spectroscopy

The conformation and dynamics of melittin bound to the dimyristoylphosphatidylcholine (DMPC) bilayer and the magnetic orientation in the lipid bilayer systems were investigated by solid-state (31)P and (13)C NMR spectroscopy. Using (31)P NMR, it was found that melittin-lipid bilayers form magnetically oriented elongated vesicles with the long axis parallel to the magnetic field above the liquid crystalline-gel phase transition temperature (T(m) = 24 degrees C). The conformation, orientation, and dynamics of melittin bound to the membrane were further determined by using this magnetically oriented lipid bilayer system. For this purpose, the (13)C NMR spectra of site-specifically (13)C-labeled melittin bound to the membrane in the static, fast magic angle spinning (MAS) and slow MAS conditions were measured. Subsequently, we analyzed the (13)C chemical shift tensors of carbonyl carbons in the peptide backbone under the conditions where they form an alpha-helix and reorient rapidly about the average helical axis. Finally, it was found that melittin adopts a transmembrane alpha-helix whose average axis is parallel to the bilayer normal. The kink angle between the N- and C-terminal helical rods of melittin in the lipid bilayer is approximately 140 degrees or approximately 160 degrees, which is larger than the value of 120 degrees determined by x-ray diffraction studies. Pore formation was clearly observed below the T(m) in the initial stage of lysis by microscope. This is considered to be caused by the association of melittin molecules in the lipid bilayer.     

Molecular dynamics simulations of pentapeptides at interfaces: salt bridge and cation-pi interactions

Peptide-membrane interactions are important for understanding the binding, partitioning, and folding of membrane proteins; the activity of antimicrobial and fusion peptides; and a number of other processes. We describe molecular dynamics simulations (10-25 ns) of two pentapeptides Ace-WLXLL (with X = Arg or Lys side chain) (White, S. H., and Wimley, W.C. (1996) Nat. Struct. Biol. 3, 842-848) in water and three different membrane mimetic systems: (i) a water/cyclohexane interface, (ii) water-saturated octanol, and (iii) a solvated dioleoylphosphatidylcholine bilayer. A salt bridge is found between the protonated Arg or Lys side chains with the carboxyl terminus at the three interfaces. In water/cyclohexane, the salt bridge is most exposed to the water phase and least stable. In water/octanol and the lipid bilayer systems, the salt bridge once formed persists throughout the simulations. In the lipid bilayer, the salt bridge is more stable when the peptide penetrates deeper into the bilayer. In one of two peptides, a cation-pi interaction between the Arg and the Trp side chains is stable in the lipid bilayer for about 15 ns before breaking. In all cases, the conformations of the peptides are restricted by their presence at the interface and can be assigned to a few major conformational clusters. Side chains facing the water phase are most mobile. In the lipid bilayer, the peptides remain in the interface area, where they overlap with the carbonyl area of the lipid bilayer and perturb the local density profile of the bilayer. The tryptophan side chain remains in the water-lipid interface, where it interacts with the lipid choline group and forms hydrogen bonds with the ester carbonyl of the lipid and with water in the interface.     

An NMR database for simulations of membrane dynamics

Computational methods are powerful in capturing the results of experimental studies in terms of force fields that both explain and predict biological structures. Validation of molecular simulations requires comparison with experimental data to test and confirm computational predictions. Here we report a comprehensive database of NMR results for membrane phospholipids with interpretations intended to be accessible by non-NMR specialists. Experimental 13C-1H and 2H NMR segmental order parameters (S(CH) or S(CD)) and spin-lattice (Zeeman) relaxation times (T(1Z)) are summarized in convenient tabular form for various saturated, unsaturated, and biological membrane phospholipids. Segmental order parameters give direct information about bilayer structural properties, including the area per lipid and volumetric hydrocarbon thickness. In addition, relaxation rates provide complementary information about molecular dynamics. Particular attention is paid to the magnetic field dependence (frequency dispersion) of the NMR relaxation rates in terms of various simplified power laws. Model-free reduction of the T(1Z) studies in terms of a power-law formalism shows that the relaxation rates for saturated phosphatidylcholines follow a single frequency-dispersive trend within the MHz regime. We show how analytical models can guide the continued development of atomistic and coarse-grained force fields. Our interpretation suggests that lipid diffusion and collective order fluctuations are implicitly governed by the viscoelastic nature of the liquid-crystalline ensemble. Collective bilayer excitations are emergent over mesoscopic length scales that fall between the molecular and bilayer dimensions, and are important for lipid organization and lipid-protein interactions. Future conceptual advances and theoretical reductions will foster understanding of biomembrane structural dynamics through a synergy of NMR measurements and molecular simulations.     

Structural-dynamic properties of the tryptophan residue environment in melittin

The structural dynamics of the environment of the single tryptophan residue in melittin was studied by site-selective red-edge-excitation fluorescence spectroscopy. The dependence of the spectral shift on transition from excitation in a maximum (at 280 nm) to long-wavelength edge (305 nm) was studied as a function of temperature. It was shown, that for melittin at high ionic strength (tetramer), the three regions of temperature dependence of the red-edge effect are observed: retarded relaxation (up to +30 degrees C), relaxational changes of spectra (from +30 to +50 degrees C) and thermal changes of structure (above +50 degrees C). The dipolar-re-orientational relaxation time and activation energy of orientation motions in the environment of indolic ring in the tetrameric melittin structure were estimated. Extrapolation from relaxational region to room temperature results in relaxation time 40 ns. In monomeric melittin (at low ionic strength) the red-edge shift of spectra is absent. The distinct differences in character of thermal quenching of fluorescence between monomeric and tetrameric forms of melittin are observed. It follows, that the short-wave-length fluorescence shift on monomer-tetramer transition is due to both the reduction of polarity, and the increase in rigidity of tryptophan environment, the absence of relaxation motions at nanosecond times.     

Lipid bilayer perturbations induced by simple hydrophobic peptides

Mixtures of tripeptides of the form Ala-X-Ala-O-tert-butyl with 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) bilayers have been used as a model system for studying the influence of hydrophobic peptides on membrane order and dynamic properties by means of deuterium NMR spectroscopy. Tripeptides with X = Ala, Leu, Phe, and Trp have been examined. Lipid 2H NMR spectra of acyl chain perdeuteriated DMPC ([2H54]DMPC) show that the addition of peptide disorders the bilayer lipid acyl chains and that the extent of the perturbation increases as the size of the central residue increases. Moment analyses of the spectra indicate that, while the average acyl chain order parameter decreases with increasing central residue size, the order parameter spread across the bilayer (the mean-squared width of the distribution) increases. Lipid segmental 2H longitudinal relaxation rates, 1/T1(i), exhibit a square-law functional dependence on SCD(i) both with and without the addition of peptide. The addition of peptide causes an increase in the slope of plots of 1/T1(i) vs. (SCD(i))2 with little change in the 1/T1(i) intercept, indicating a complex modulation of the acyl chain motions. 2H NMR spectra of Ala-[2H4]Ala-Ala-O-tert-butyl in DMPC bilayers have both isotropic and powder pattern components that vary as a function of temperature. At 30 degrees C the 2H spin-lattice relaxation times for the labeled Ala residue increase in going from bilayer-incorporated peptide to polycrystalline peptide to polycrystalline Ala.HCl. These experiments provide no information on the location of these peptides in the bilayer.(ABSTRACT TRUNCATED AT 250 WORDS)     

Tryptophan sidechain dynamics in hydrophobic oligopeptides determined by use of 13C nuclear magnetic resonance spectroscopy.

Two oligopeptides, t-boc-LAWAL-OMe and t-boc-LALALW-OMe, were synthesized for the purpose of examining the sidechain dynamics of the tryptophan residue in hydrophobic environments by 13C nuclear magnetic resonance and fluorescence spectroscopy. In both peptides, the tryptophan sidechain was greater than 95% enriched with 13C at the C delta 1 position. Spin-lattice relaxation time (T1) and steady-state nuclear Overhauser effect (NOE) data were obtained at 50.3 and 75.4 MHz for both peptides in CD3OD, and at 75.4 MHz for t-boc-LALALW-OMe in lysolecithin-D2O micelles. We have adapted the model-free approach of G. Lipari and A. Szabo (1982, J. Am. Chem. Soc. 104:4546) to interpret the 13C-NMR data. Computer-generated curves based on experimental data obtained at a single frequency demonstrate relationships between an effective correlation time for tryptophan sidechain motion (tau e), a generalized order parameter (sigma) describing the extent of motional restriction, and an overall correlation time for the peptide (tau m). Assuming predominantly dipolar relaxation, least-squares fits of the dual frequency relaxation data provide values for these parameters for both peptides. The contribution of chemical shift anisotropy (CSA), however, is also explicitly assessed in the data analysis, and is shown to perturb the predicted sigma, tau e, and tau m values and to decrease chi(2) values observed in nonlinear least-squares analysis of the data. Because of uncertainty in the contribution of CSA to the relaxation of the indole ring 13C delta 1 atom, nonlinear least-squares analysis of the relaxation data were performed with and without inclusion of a CSA term in the appropriate relaxation equations. Neglecting CSA, an overall peptide correlation time of 0.69 ns is predicted for t-boc-LAWAL-OMe in CD3OD at 20 degrees C compared with 1.28 ns for t-boc-LALALW-OMe. Given these tau m values and taking into account the effect of measurement error in the T1 and NOE data, the internal dynamics of the tryptophan residue of t-boc-LAWAL-OMe in this isotropic environment are described by a range of tau e values from 70 to 112 ps and sigma values between 0.22 and 0.36. Similarly, for t-boc-LALALW-OMe, 68 less than or equal to tau e less than or equal to 93 ps and 0.09 less than or equal to sigma less than or equal to 0.17. The Ch-terminal position of the tryptophan residue in the hexapeptide may account for its lower order parameter.(ABSTRACT TRUNCATED AT 400 WORDS)     

The actions of melittin on membranes

The molecular mechanisms underlying the various effects of melittin on membranes have not been completely defined and much of the evidence described indicates that different molecular mechanisms may underlie different actions of the peptide. Ideas about the formation of transbilayer aggregates of melittin under the influence of a transbilayer potential, and for bilayer structural perturbation arising from the location of the peptide helix within the head group region of the membrane have been made based on the crystal structure of the peptide, the kinetics and concentration dependence of melittins membrane actions, together with simple ideas about the conformational properties of amphipathic helical peptides and their interactions with membranes. Physical studies of the interaction of melittin with model membranes have been useful in determining the potential of the peptide to adopt different locations, orientations and association states within membranes under different conditions, but the relationship of the results obtained to the actions of melittin in cell membranes or under the influence of a membrane potential are unclear. Experimental definition of the interaction of melittin with more complex membranes, including the erythrocyte membrane or in bilayers under the influence of a transmembrane potential, will require direct study in these membranes. Experiments employing labeled melittins for ESR, NMR or fluorescence experiments are promising both for their sensitivity (ESR and fluorescence) and the ability to focus on the peptide within the background of endogenous proteins within cell membranes. The study of melittin in model membranes has been useful for the development of methodology for determination of membrane protein structures. Despite the structural complexity of integral membrane proteins, it is interesting that in some respects their study be more straightforward, lacking as they do the elusive properties of melittin (and other structurally labile membrane peptides) which limit the possibility of defining their interaction with membranes in terms of a single conformation, location, orientation and association state within the membrane.     

Mixtures of a series of homologous hydrophobic peptides with lipid bilayers: a simple model system for examining the protein-lipid interface

The interactions of several members of a homologous series of peptides with the phospholipid bilayer have been examined by using fluorescence and deuterium NMR spectroscopy, differential scanning calorimetry, and measurements of water-to-bilayer partition coefficients. 1,2-Dimyristoyl-sn-glycero-3-phosphocholine (DMPC) bilayers and tripeptides of the form Ala-X-Ala-O-tert-butyl are used as a model system to probe the influence of amino acid side-chain substitution on the insertion of peptides into membranes and the behavior of peptide/bilayer mixtures. Tripeptides with X = Gly, Ala, Phe, and Trp have been examined. All of the tripeptides are water soluble, and all partition into DMPC bilayer vesicles to some extent. The Gly-containing peptide is the least soluble and the Trp-containing peptide the most soluble in the bilayer. The extent of perturbation of the bilayer structure induced by the peptides parallels their bilayer solubility: the Gly and Ala peptides act as simple impurities while peptides containing bulky aromatic rings cause a phase separation. Changes in the fluorescence properties of the Trp analogue upon incorporation into the bilayer indicate that the Trp side chain is probably immersed in the hydrocarbon region of the bilayer. Peptides of this form should serve as easily modifiable model systems with which to examine details of how the bilayer environment affects peptide conformation, as well as how hydrophobic peptides affect the bilayer structure.     

Effect of ionic strength on the organization and dynamics of membrane-bound melittin

Melittin, a cationic hemolytic peptide, is intrinsically fluorescent due to the presence of a single functionally important tryptophan residue. We have previously shown that the sole tryptophan of melittin is localized in a motionally restricted environment in the membrane interface. We have monitored the effect of ionic strength on the organization and dynamics of membrane-bound melittin utilizing fluorescence and circular dichroism (CD) spectroscopic approaches. Our results show that red edge excitation shift (REES) of melittin bound to membranes is sensitive to the change in ionic strength of the medium. This could be attributed to a change in the immediate environment around melittin tryptophan with increasing ionic strength due to differential solvation of ions. Interestingly, the rotational mobility of melittin does not appear to be affected with change in ionic strength. In addition, fluorescence parameters such as lifetime and acrylamide quenching of melittin indicate an increase in water penetration in the membrane interface upon increasing ionic strength. Our results suggest that the solvent dynamics and water penetration in the interfacial region of the membranes are significantly affected at physiologically relevant ionic strength. These results assume significance in the overall context of the influence of ionic strength in the organization and dynamics of membrane proteins and membrane-active peptides.