Interaction of melittin with membrane cholesterol: a fluorescence approach

We have monitored the organization and dynamics of the hemolytic peptide melittin in membranes containing cholesterol by utilizing the intrinsic fluorescence properties of its functionally important sole tryptophan residue and circular dichroism spectroscopy. The significance of this study is based on the fact that the natural target for melittin is the erythrocyte membrane, which contains high amounts of cholesterol. Our results show that the presence of cholesterol inhibits melittin-induced leakage of lipid vesicles and the extent of inhibition appears to be dependent on the concentration of membrane cholesterol. The presence of cholesterol is also shown to reduce binding of melittin to membranes. Our results show that fluorescence parameters such as intensity, emission maximum, and lifetime of membrane-bound melittin indicate a change in polarity in the immediate vicinity of the tryptophan residue probably due to increased water penetration in presence of cholesterol. This is supported by results from fluorescence quenching experiments using acrylamide as the quencher. Membrane penetration depth analysis by the parallax method shows that the melittin tryptophan is localized at a relatively shallow depth in membranes containing cholesterol. Analysis of energy transfer results using melittin tryptophan (donor) and dehydroergosterol (acceptor) indicates that dehydroergosterol is not randomly distributed and is preferentially localized around the tryptophan residue of membrane-bound melittin, even at the low concentrations used. Taken together, our results are relevant in understanding the interaction of melittin with membranes in general, and with cholesterol-containing membranes in particular, with possible relevance to its interaction with the erythrocyte membrane.     

Aggregation state of melittin in lipid vesicle membranes

We have performed time-resolved fluorescence energy transfer measurements using melittin as donor and a modified melittin as acceptor. The melittin molecules were bound to fluid vesicle membranes of dimyristoylphosphatidylcholine. Analysis of the temporal decay of the energy transfer and of its variation with the donor and acceptor concentrations led to the conclusion that melittin in fluid membranes is usually monomeric. Only at the high melittin/lipid molar ratio of 1/200 and high ionic strength evidence for aggregation was obtained, the percentage of aggregated melittin molecules being of the order of 10%. The shortcomings of previous steady-state measurements of fluorescence energy transfer between melittin molecules are discussed.     

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.     

Structural and thermodynamic analyses of the interaction between melittin and lipopolysaccharide

Lipopolysaccharide (LPS), the major constituent of the outer membrane of Gram-negative bacteria, is the very first site of interactions with the antimicrobial peptides. In this work, we have determined a solution conformation of melittin, a well-known membrane active amphiphilic peptide from honey bee venom, by transferred nuclear Overhauser effect (Tr-NOE) spectroscopy in its bound state with lipopolysaccharide. The LPS bound conformation of melittin is characterized by a helical structure restricted only to the C-terminus region (residues A15-R24) of the molecule. Saturation transfer difference (STD) NMR studies reveal that several C-terminal residues of melittin including Trp19 are in close proximity with LPS. Isothermal titration calorimetry (ITC) data demonstrates that melittin binding to LPS or lipid A is an endothermic process. The interaction between melittin and lipid A is further characterized by an equilibrium association constant (Ka) of 2.85 x 10(6) M(-1) and a stoichiometry of 0.80, melittin/lipid A. The estimated free energy of binding (delta G0), -8.8 kcal mol(-1), obtained from ITC experiments correlates well with a partial helical structure of melittin in complex with LPS. Moreover, a synthetic peptide fragment, residues L13-Q26 or mel-C, derived from the C-terminus of melittin has been found to contain comparable outer membrane permeabilizing activity against Escherichia coli cells. Intrinsic tryptophan fluorescence experiments of melittin and mel-C demonstrate very similar emission maxima and quenching in presence of LPS micelles. The Red Edge Excitation Shift (REES) studies of tryptophan residue indicate that both peptides are located in very similar environment in complex with LPS. Collectively, these results suggest that a helical conformation of melittin, at its C-terminus, could be an important element in recognition of LPS in the outer membrane.     

Lipid specific penetration of melittin into phospholipid model membranes

The relative depth of penetration of melittin into egg phosphatidylcholine and bovine heart cardiolipin model membranes was investigated using fluorescence spectroscopy techniques. The tryptophan intrinsic fluorescence shift suggests a more hydrophobic surrounding of this residue in cardiolipin, while the accessibility for charged and uncharged aqueous quenchers is decreased in the cardiolipin system when compared with the phosphatidylcholine-bound situation. A lipid incorporated hydrophobic, collisional quencher and a resonance energy transfer acceptor on the other hand are more effective in quenching the tryptophan fluorescence of cardiolipin bound melittin. The combination of these results is interpreted as prove of a deeper positioning of the tryptophan containing part of the peptide molecule in the cardiolipin system in comparison with the situation in phosphatidylcholine. Models that take this difference into account are presented, which try to explain the opposite effect of melittin binding to the two lipid systems with respect to supramolecular structure, as reported in the preceding article (Batenburg, A.M., Hibbeln, J.C.L., Verkleij, A.J. and De Kruijff, B. (1987) Biochim. Biophys. Acta 903, 142-154).     

Conformational distributions of melittin in water/methanol mixtures from frequency-domain measurements of nonradiative energy transfer

We used fluorescence energy transfer to examine the effects of solvent composition on the distribution of distances between the single tryptophan residue of melittin (residue 19) to the N-terminal alpha-amino group, which was labeled with a dansyl residue. The tryptophan intensity decays, with and without the dansyl acceptor, were measured by the frequency-domain method. The data were analyzed by a least-squares algorithm which accounts for correlation between the parameters. A wide distribution of tryptophan to dansyl distances was found for the random-coil state, with a Gaussian half-width of 25 A. Increasing concentrations of methanol, which were shown to induce and alpha-helical conformation, resulted in a progressive decrease in the width of the distribution, reaching a limiting half-width of 3 A at 80% (v/v) methanol. The distance from the indole moiety of Trp-19 to the dansyl group in 80% (v/v) methanol/water was found to be 25 A, as assessed from the center of the distance distribution. A distance of 24-25 A was recovered from the X-ray crystal structure of the tetramer, which is largely alpha-helical. At low ionic strength (less than 0.01) the CD spectra revealed a small fraction or amount of alpha-helix for melittin in water, which implies a small fraction of residual structure. This residual structure is apparently lost in guanidine hydrochloride as demonstrated by a further broadening in the distribution of distances. These results demonstrate the usefulness of frequency-domain measurements of resonance transfer for resolution of conformational distributions of proteins.     

Different states of self-association of melittin in phospholipid bilayers

Melittin is known to self-associate as tetramers in solutions of high ionic strength. Here, an N-bromosuccinimide oxidized-Trp₁₉ melittin is prepared. This derivative can act as an acceptor of the fluorescence of native melittin and is used in order to observe a possible self-association of melittin in phospholipid bilayers.Resonance energy transfer was shown to occur in solutions of high ionic strength, showing that oxidized melittin can associate with native melittin.In phospholipid bilayers, no association is detected in the absence of NaCl. In its presence, an equilibrium between monomeric melittin and oligomeric species is observed. These species are not dimers, but any other degree of association may account for our experimental results. Significant differences in characteristic transfer efficiency reveal differences in the structure of these oligomers according to the length or state of phospholipids (fluid or at the transition temperature). These bound complexes are also different from the soluble hetero-oligomer.Some models of bound complexes are proposed which may explain the leakage and the further disruption of vesicles or cells induced by melittin.Abbreviations NBS N-bromosuccinimide - NATA N-acetyl tryptophanamide - DMPC dimyristoyl phosphatidylcholine - DPPC dipalmitoyl phosphatidylcholine - PG phosphatidylglycerol - EPC egg phosphatidylcholine - O-melittin oxindole-melittin - RET resonance energy transfer - EDTA ethylene diamine tetracetic acid - Mel melittin     

Structural and thermodynamic analyses of the interaction between melittin and lipopolysaccharide

Lipopolysaccharide (LPS), the major constituent of the outer membrane of Gram-negative bacteria, is the very first site of interactions with the antimicrobial peptides. In this work, we have determined a solution conformation of melittin, a well-known membrane active amphiphilic peptide from honey bee venom, by transferred nuclear Overhauser effect (Tr-NOE) spectroscopy in its bound state with lipopolysaccharide. The LPS bound conformation of melittin is characterized by a helical structure restricted only to the C-terminus region (residues A15-R24) of the molecule. Saturation transfer difference (STD) NMR studies reveal that several C-terminal residues of melittin including Trp19 are in close proximity with LPS. Isothermal titration calorimetry (ITC) data demonstrates that melittin binding to LPS or lipid A is an endothermic process. The interaction between melittin and lipid A is further characterized by an equilibrium association constant (K_a) of 2.85 × 10⁶ M^− 1 and a stoichiometry of 0.80, melittin/lipid A. The estimated free energy of binding (ΔG⁰), − 8.8 kcal mol^− 1, obtained from ITC experiments correlates well with a partial helical structure of melittin in complex with LPS. Moreover, a synthetic peptide fragment, residues L13-Q26 or mel-C, derived from the C-terminus of melittin has been found to contain comparable outer membrane permeabilizing activity against Escherichia coli cells. Intrinsic tryptophan fluorescence experiments of melittin and mel-C demonstrate very similar emission maxima and quenching in presence of LPS micelles. The Red Edge Excitation Shift (REES) studies of tryptophan residue indicate that both peptides are located in very similar environment in complex with LPS. Collectively, these results suggest that a helical conformation of melittin, at its C-terminus, could be an important element in recognition of LPS in the outer membrane.     

Melittin-induced alterations in dynamic properties of human red blood cell membranes.

The interaction of bee venom melittin with erythrocyte membrane ghosts has been investigated by means of fluorescence quenching of membrane tryptophan residues, fluorescence polarization and ESR spectroscopy. It has been revealed that melittin induces the disorders in lipid-protein matrix both in the hydrophobic core of bilayer and at the polar/non-polar interface of melittin complexed with erythrocyte membranes. The peptide has been found to act most efficiently at the concentration of the order of 10(-10) mol/mg membrane protein. The apparent distance separating the membrane tryptophan and bound 1-anilino-8-naphthalenesulphonate (ANS) molecules is decreased upon melittin binding, which results in a significant increase of the maximum energy transfer efficiency. Significant changes in the fluorescence anisotropy of both 1,6-diphenyl-1,3,5-hexatriene and 1-anilino-8-naphthalenesulphonate bound to erythrocyte ghosts, which have been observed in the presence of melittin and crude venom, indicate membrane lipid bilayer rigidization. The effect of crude honey bee venom has been found to be of similar magnitude as the effect of pure melittin at the concentration of 10(-10) mol/mg membrane protein. Using two lipophilic spin labels, methyl 5-doxylpalmitate and 16-doxylstearic acid, we found that melittin at its increasing concentrations induces a well marked rigidization in the deeper regions of lipid bilayer, whereas the effect of rigidization near the membrane surface maximizes at the melittin concentration of 10(-10) mol/mg (10(-4) mol melittin per mole of membrane phospholipid). The decrease in the ratio hw/hs of maleimide and the rise in relative rotational correlation time (tau c) of iodacetamid spin label, indicate that melittin effectively immobilizes membrane proteins in the plane of the lipid bilayer. We conclude that melittin-induced rigidization of the lipid bilayer may induce a reorganization of lipid assemblies as well as the rearrangements in membrane protein pattern and consequently the alterations in lipid-protein interactions. Thus, the interaction of melittin with erythrocyte membranes is supposed to produce local conformational changes in membranes, which are discussed in the connection with their significance during the synergistic action of melittin and phospholipase of bee venom on red blood cells.     

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.     

Dynamics of melittin in water and membranes as determined by fluorescence anisotropy decay.

Fluorescence anisotropy decay measurements were performed on melittin in water and in membranes of dimyristoylphosphatidylcholine. The fluorescence of the single tryptophan residue of melittin and of a pyrene label attached to melittin was detected. In water, the slowest relaxation process in the anisotropy decay occurs with a relaxation time of 1.5 or 5.5 ns in the case of low or high ionic strength and corresponds to rotational diffusion of monomeric or tetrameric melittin. Superimposed on this slow process are fast processes in the subnanosecond range reflecting fluctuations of the fluorophores relative to the polypeptide backbone. In membranes, the fast relaxation processes are not much altered. A slow process with a relaxation time of 35 ns is observed and assigned to orientational fluctuations of the melittin helices in membranes.     

Action of phospholipases on the cytoplasmic membrane of Escherichia coli. Stimulation by melittin

The emission maximum of the single tryptophan residue of melittin was measured in the presence of phosphatidylethanolamine liposomes and Escherichia coli cytoplasmic membranes. In both cases, the fluorescence maximum was shifted to shorter wavelengths indicating a transfer of the indole ring to an apolar environment. E. coli membranes were labelled in position 2 of their phospholipids with [¹⁴C]oleic acid. These membranes were used for measuring the activity of an endogenous phospholipase A₂. A slow hydrolysis is observed, which can be accelerated by adding melittin. The extent of the stimulation depends on the molar ratio of melittin to membrane phospholipid. Under suitable conditions, the initial rate of hydrolysis is six to seven times higher in the presence than in the absence of melittin. The action of the phospholipase A₂ from bee venom is also stimulated by melittin. An identical stimulation was observed with either E. coli membranes or pure phosphatidylethanolamine liposomes as substrate.     

Effect of micellar charge on the conformation and dynamics of melittin

Electrostatic interactions play a crucial role in modulating and stabilizing molecular interactions in membranes and membrane-mimetic systems such as micelles. We have monitored the change in the conformation and dynamics of the cationic hemolytic peptide melittin bound to micelles of various charge types, utilizing fluorescence and circular dichroism (CD) spectroscopy. The sole tryptophan of melittin displays a red-edge excitation shift (REES) of 3-6 nm when bound to anionic, nonionic, and zwitterionic micelles. This suggests that melittin is localized in a restricted environment, probably in the interfacial region of the micelles, and this region offers considerable restriction to the reorientational motion of the solvent dipoles around the excited state tryptophan in melittin. Further, the rotational mobility of melittin is considerably reduced in these micelles and is found to be dependent on the surface charge of micelles. Interestingly, our results show that melittin does not partition into cetyltrimethylammonium bromide (CTAB) micelles owing to electrostatic repulsion between melittin and CTAB micelles, both of which carry a positive charge. In addition, the fluorescence lifetime of melittin is modulated in micelles of different charge types. The lowest mean fluorescence lifetime is observed in the case of melittin bound to anionic sodium dodecyl sulfate (SDS) micelles. CD spectroscopy shows that micelles induce significant helicity to melittin, with maximum helicity being induced in the case of melittin bound to SDS micelles. Fluorescence quenching measurements using the neutral aqueous quencher acrylamide show differential accessibility of melittin in various types of micelles. Taken together, our results show that micellar surface charge can modulate the conformation and dynamics of melittin. These results could be relevant to understanding the role of the surface charge of membranes in the interaction of membrane-active, amphiphilic peptides with membranes.     

丙酮酸氧化酶激活机制的研究——α-肽与磷脂囊的结合

 丙酮酸氧化酶既能被两性脂类激活,也能被蛋白酶从羧基端切下一个23肽(称α-肽)激活,而且这两种激活方式相互排斥。本文用分离纯化的α-肽,通过测定色氨酸荧光能量转移的方法,证明α-肽能与磷脂囊(vesicle)结合。我们选用两种不同类型的荧光探针,发现α-肽对它们表现不同的色氨酸能量转移效率。α-肽对Dan-syl-DPPE为7.4±1.0％对Dansyl-UAPC为12.5±2.0％。由此推测α-肽的色氨酸残基易与磷脂双层内部疏水区结合,说明α-肽是一种较为疏水的肽。我们推测α-肽在这种外膜酶的激活过程中,提供了与膜结合的部位,在生理过程中起着重要作用。     

Detection of energy transfer between tryptophan residues in the tubulin molecule and bound bis(8-anilinonaphthalene-1-sulfonate), an inhibitor of microtubule assembly, that binds to a flexible region on tubulin

The fluorescent apolar probe bis(8-anilinonaphthalene-1-sulfonate) (Bis-ANS) is a potent inhibitor of microtubule assembly that binds to tubulin at a hitherto uncharacterized site distinct from those of the antimitotic drugs. We have found that energy transfer between tryptophan residues and bound Bis-ANS leads to quenching of the intrinsic tubulin fluorescence. The quenching is biphasic, implying two types of Bis-ANS binding sites. The estimated Kd values are 2.7 and 22.2 microM, consistent with reported values for the primary and secondary Bis-ANS binding sites. Preincubation of tubulin at 37 degrees C results in increased quenching of tryptophan fluorescence without any effect on the Kd values, suggesting localized structural change in the protein around the Bis-ANS binding sites. Concentration-dependent depolarization of Bis-ANS fluorescence was observed, suggesting energy transfer among bound Bis-ANS molecules. Such a concentration-dependent decrease in fluorescence polarization was not observed with 8-anilinonaphthalene-1-sulfonate (1,8-ANS), the monomeric form of Bis-ANS. Perrin-Weber plots were obtained for bound Bis-ANS and 1,8-ANS by varying the viscosity with sucrose. The rotational relaxation times calculated for Bis-ANS and 1,8-ANS are 18 and 96 ns, respectively. Comparison with the theoretical value (125 ns) suggests that Bis-ANS binds to a flexible region of tubulin. This, coupled with the fact that Bis-ANS, but not 1,8-ANS, inhibits microtubule assembly, suggests that the region in the tubulin molecule responsible for microtubule assembly is relatively flexible.     

A high-sensitivity differential scanning calorimetric study of the interaction of melittin with dipalmitoylphosphatidylcholine fused unilamellar vesicles

High-sensitivity differential scanning calorimetry has been used to examine the interaction of bee venom melittin with dipalmitoylphosphatidylcholine fused unilamellar vesicles. Experiments were performed under conditions for which melittin in solution is either monomeric (in low salt) or tetrameric (in high salt). It was found that under both sets of conditions melittin abolishes the pretransition at a relatively high lipid-to-protein molar incubation ratio, Ri (about 200) and that at intermediate values of Ri it broadens the main transition profile and reduces the transition enthalpy. This provides evidence which suggests that melittin is at least partially inserted into the apolar region of the bilayer. Evident at low values of Ri are two peaks in the lipid thermal transition profiles, which may arise from a heterogeneous population of lipid vesicles formed through fusion induced by melittin, or by lipid phase separation. For those profiles which exhibited only one peak, transition enthalpies, normalized to those of the lipid in the absence of the protein, are plotted vs. the bound protein-to-lipid molar ratios for the experiments performed under the conditions which give monomeric and tetrameric melittin in solution. These plots yield straight lines, the slopes of which give the number of lipid molecules each protein molecule excludes from participating in the phase transition. These were found to be 9.9 +/- 0.7 and 4.1 +/- 0.5 for monomeric and tetrameric melittin, respectively. The results are discussed in terms of possible models for the binding of melittin to phospholipid vesicles. For simple hexagonal packing of lipid molecules, incorporation as an aggregate is favored when melittin is tetrameric in solution, whereas incorporation as a monomer is favored when melittin is monomeric in solution. For low-salt solutions, evidence is obtained for the contribution of free melittin to lipid fusion, perhaps by the formation of protein bridges between apposed vesicles.     

Fluorescence-quenching-resolved spectra of melittin in lipid bilayers

The interaction of bee venom melittin with dimyristoylphosphatidylcholine (DMPC) unilamellar vesicles has been studied by means of fluorescence quenching of the single tryptophan residue of the protein, at lipid-to-peptide ratio, Ri = 50 and at high ionic strength (2 M NaCl). The method of fluorescence-quenching-resolved spectra (FQRS), applied in this study with potassium iodide as a quencher, enabled us to decompose the tryptophan emission spectrum of liposome-bound melittin into components, at temperatures above as well as below the main phase transition temperature (Tt) of DMPC. One of the two resolved spectra exhibits maximum at 342 and 338 nm for experiments above and below Tt, respectively, and is similar to the maximum of tryptophan emission found for tetrameric melittin in solution (340 nm). This spectrum is characterized by the Stern-Volmer quenching constant, Ksv, of about 4 M-1 and it represents the fraction of melittin molecules whose tryptophan residues are exposed to the solvent to a degree comparable with tetrameric species in solution. The other spectrum component, corresponding to the quencher-inaccessible fraction of tryptophan molecules (Ksv = 0 M-1) has its maximum blue-shifted up to 15 nm, indicating a decrease in polarity of the environment. For experiments above Tt, the blue spectrum component revealed the excitation-wavelength dependence, originating probably from the relaxation processes between the excited tryptophan molecules and lipid polar head groups. We conclude that melittin bound to DMPC liposomes exists in two lipid-associated forms; one, with tryptophan residues exposed to the solvent and the other, penetrating the membrane interior, with tryptophan residues located in close proximity to the phospholipid polar head groups of the outer vesicle lipid layer. We also discuss our data with current models of melittin-bilayer interactions.     

Distribution of distances between the tryptophan and the N-terminal residue of melittin in its complex with calmodulin, troponin C, and phospholipids.

We used frequency-domain measurements of fluorescence resonance energy transfer to measure the distribution of distances between Trp-19 of melittin and a 1-dimethylamino-5-sulfonylnaphthalene (dansyl) residue on the N-terminal-alpha-amino group. Distance distributions were obtained for melittin free in solution and when complexed with calmodulin (CaM), troponin C (TnC), or palmitoyloleoyl-L-alpha-phosphatidylcholine (POPC) vesicles. A wide range of donor (Trp-19)-to-acceptor (dansyl) distances was found for free melittin, which is consistent with that expected for the random coil state, characterized by a Gaussian width (full width at half maxima) of 28.2 A. In contrast, narrow distance distributions were found for melittin complexed with CaM, 8.2 A, or with POPC vesicles, 4.9 A. A somewhat wider distribution was found for the melittin complex with TnC, 12.8 A, suggesting the presence of heterogeneity in the mode of binding between melittin and TnC. For all the complexes the mean Trp-19 to dansyl distance was near 20 A. This value is somewhat smaller than expected for the free alpha-helical state of melittin, suggesting that binding with CaM or TnC results in a modest decrease in the length of the melittin molecule.     

Studies of phosphorescent probes for proteins

1. Certain capabilities and limitations of using bound phosphorescent chromophores to study protein structure were investigated. Carbonic anhydrase inhibitors with three different arrangements of singlet and triplet energy levels relative to those of tryptophan were used to determine their ability to transfer triplet energy. 2. Ligands representing each of the three spectroscopic energy level arrangements were found to exhibit triplet-triplet energy transfer with a tryptophan residue at the active site of carbonic anhydrase. This greatly increases the number of ligands which may be useful as phosphorescent probes. 3. The efficiency of energy transfer occurs to varying degrees depending upon the inhibitor. This is a potential source of data for determining the position of the ligand in the binding site.     

Enhanced resolution of fluorescence anisotropy decays by simultaneous analysis of progressively quenched samples. Applications to anisotropic rotations and to protein dynamics.

Enhanced resolution of rapid and complex anisotropy decays was obtained by measurement and analysis of data from progressively quenched samples. Collisional quenching by acrylamide was used to vary the mean decay time of indole or of the tryptophan fluorescence from melittin. Anisotropy decays were obtained from the frequency-response of the polarized emission at frequencies from 4 to 2,000 MHz. Quenching increases the fraction of the total emission, which occurs on the subnanosecond timescale, and thereby provides increased information on picosecond rotational motions or local motions in proteins. For monoexponential subnanosecond anisotropy decays, enhanced resolution is obtained by measurement of the most highly quenched samples. For complex anisotropy decays, such as those due to both local motions and overall protein rotational diffusion, superior resolution is obtained by simultaneous analysis of data from quenched and unquenched samples. We demonstrate that measurement of quenched samples greatly reduces the uncertainty of the 50-ps correlation time of indole in water at 20 degrees C, and allows resolution of the anisotropic rotation of indole with correlation times of 140 and 720 ps. The method was applied to melittin in the monomeric and tetrameric forms. With increased quenching, the anisotropy data showed decreasing contributions from overall protein rotation and increased contribution from picosecond tryptophan motions. The tryptophan residues in both the monomeric and the tetrameric forms of melittin displayed substantial local motions with correlation times near 0.16 and 0.06 ns, respectively. The amplitude of the local motion is twofold less in the tetramer. These highly resolved anisotropy decays should be valuable for comparison with molecular dynamics simulations of melittin.