Intrinsic tyrosine fluorescence as a tool to study the interaction of the shaker B "ball" peptide with anionic membranes

Steady-state and time-resolved fluorescence from the single tyrosine in the inactivating peptide of the Shaker B potassium channel (ShB peptide) and in a noninactivating peptide mutant, ShB-L7E, has been used to characterize their interaction with anionic phospholipid membranes, a model target mimicking features of the inactivation site on the channel protein. Partition coefficients derived from steady-state anisotropy indicate that both peptides show a high affinity for anionic vesicles, being higher in ShB than in ShB-L7E. Moreover, differential quenching by lipophilic spin-labeled probes and fluorescence energy transfer using trans-parinaric acid as the acceptor confirm that the ShB peptide inserts deep into the membrane, while the ShB-L7E peptide remains near the membrane surface. The rotational mobility of tyrosine in membrane-embedded ShB, examined from the decay of fluorescence anisotropy, can be described by two different rotational correlation times and a residual constant value. The short correlation time corresponds to fast rotation reporting on local tyrosine mobility. The long rotational correlation time and the high residual anisotropy suggest that the ShB peptide diffuses in a viscous and anisotropic medium compatible with the aliphatic region of a lipid bilayer and support the hypothesis that the peptide inserts into it as a monomer, to configure an intramolecular beta-hairpin structure. Assuming that this hairpin structure behaves like a rigid body, we have estimated its dimensions and rotational dynamics, and a model for the peptide inserted into the bilayer has been proposed.     

Conformation and environment of channel-forming peptides: a simulation study

Ion channel-forming peptides enable us to study the conformational dynamics of a transmembrane helix as a function of sequence and environment. Molecular dynamics simulations are used to study the conformation and dynamics of three 22-residue peptides derived from the second transmembrane domain of the glycine receptor (NK4-M2GlyR-p22). Simulations are performed on the peptide in four different environments: trifluoroethanol/water; SDS micelles; DPC micelles; and a DMPC bilayer. A hierarchy of alpha-helix stabilization between the different environments is observed such that TFE/water < micelles < bilayers. Local clustering of trifluoroethanol molecules around the peptide appears to help stabilize an alpha-helical conformation. Single (S22W) and double (S22W,T19R) substitutions at the C-terminus of NK4-M2GlyR-p22 help to stabilize a helical conformation in the micelle and bilayer environments. This correlates with the ability of the W22 and R19 side chains to form H-bonds with the headgroups of lipid or detergent molecules. This study provides a first atomic resolution comparison of the structure and dynamics of NK4-M2GlyR-p22 peptides in membrane and membrane-mimetic environments, paralleling NMR and functional studies of these peptides.     

Microsecond rotational dynamics of spin-labeled Ca-ATPase during enzymatic cycling initiated by photolysis of caged ATP.

We have measured the microsecond rotational motions of the sarcoplasmic reticulum (SR) Ca-ATPase as a function of enzyme-specific ligands, including those that induce active calcium transport. We labeled the Ca-ATPase with a maleimide spin probe and detected rotational dynamics using saturation-transfer electron paramagnetic resonance (ST-EPR). This probe's ST-EPR spectra have been shown to be sensitive to microsecond protein rotational motion, corresponding to large-scale protein rotations that should be affected by changes in the enzyme's shape, flexibility, protein-protein interactions (oligomeric state), and protein-lipid interactions. We found that the motions of the enzyme-nucleotide and the enzyme-nucleotide/Ca states are indistinguishable from the motions in the absence of ligands. Rotational mobility does decrease in response to the addition of DMSO, a solvent that inhibits Ca-ATPase activity and stabilizes the phosphoenzyme. However, the addition of phosphate to form phosphoenzyme, in the presence or absence of DMSO, does not change the motions significantly. During the steady state of active calcium transport, the microsecond rotational mobility is indistinguishable from that of the resting enzyme. In order to detect any transient changes in mobility that might not be detectable in the steady state and to improve the precision of steady-state measurements, we photolyzed caged ATP with a laser pulse in the presence of calcium and detected the ST-EPR response from the spin-labeled enzyme, with a time resolution of 1 s.(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformational dynamics of bovine Cu, Zn superoxide dismutase revealed by time-resolved fluorescence spectroscopy of the single tyrosine residue.

The structural dynamics of bovine erythrocyte Cu, Zn superoxide dismutase (BSOD) was studied by time-resolved fluorescence spectroscopy. BSOD is a homodimer containing a single tyrosine residue (and no tryptophan) per subunit. Frequency-domain fluorometry revealed a heterogeneous fluorescence decay that could be described with a Lorentzian distribution of lifetimes. The lifetime distribution parameters (center and width) were markedly dependent on temperature. The distribution center (average lifetime) displayed Arrhenius behavior with an Ea of 4.2 kcal/mol, in contrast with an Ea of 7.4 kcal/mol for the single-exponential decay of L-tyrosine. This indicated that thermal quenching of tyrosine emission was not solely responsible for the effect of temperature on the lifetimes of BSOD. The distribution width was broad (1 ns at 8 degrees C) and decreased significantly at higher temperatures. Furthermore, the width of the lifetime distribution increased in parallel to increasing viscosity of the medium. The combined effects of temperature and viscosity on the fluorescence decay suggest the existence of multiple conformational substrates in BSOD that interconvert during the excited-state lifetime. Denaturation of BSOD by guanidine hydrochloride produced an increase in the lifetime distribution width, indicating a larger number of conformations probed by the tyrosine residue in the denatured state. The rotational mobility of the tyrosine in BSOD was also investigated. Analysis of fluorescence anisotropy decay data enabled resolution of two rotational correlation times. One correlation time corresponded to a fast (picosecond) rotation that contributed 62% of the anisotropy decay and likely reported local mobility of the tyrosine ring. The longer correlation time was 50% of the expected value for rotation of the whole (dimeric) BSOD molecule and appeared to reflect segmental motions in the protein in addition to overall tumbling. Comparison between rotational correlation times and fluorescence lifetimes of BSOD indicates that the heterogeneity in lifetimes does not arise from mobility of the tyrosine per se, but rather from dynamics of the protein matrix surrounding this residue which affect its fluorescence decay.     

An EPR study of the rotational dynamics of actins from striated and smooth muscle and their complexes with heavy meromyosin

The rotational motions of the actin from rabbit skeletal muscle and from chicken gizzard smooth muscle were measured by conventional and saturation transfer electron paramagnetic resonance (EPR) spectroscopy using maleimide spin-label rigidly bound at Cys-374. The conventional EPR spectra indicate a slight difference in the polarity of the environment of the label and in the rotational mobility of the monomeric gizzard actin compared to its skeletal muscle counterpart. These differences disappear upon polymerization. The EPR spectra of the two actins in their F form and in their complexes with heavy meromyosin (HMM) did not reveal any difference in the rotational dynamic properties that might be correlated with the known differences in the activation of myosin ATPase activity by smooth and skeletal muscle actin. Our results agree with earlier EPR studies on skeletal muscle actin in showing that polymerization stops the nanosecond rotational motion of actin monomers and that F-actin undergoes rotational motion having an effective correlation time of the order of 0.1 ms. However, our measurements show that complete elimination of the nanosecond motions requires prolonged incubation of F-actin, suggesting that the slow formation of interfilamental cross-links in concentrated F-actin solutions contributes to this process. We have also used the EPR spectroscopy to study the interaction between HMM and actin in the F and G form. Our results show that in the absence of salt one HMM molecule can cooperatively interact with eight monomers to produce a polymer which closely resembles F-actin in its rotational mobility but differs from the complex of F-actin with HMM. The results indicate that salt is necessary for further slowing down, in a cooperative manner, the sub-millisecond internal motion in actin polymer and for a non-cooperative change in the intramonomer conformation around Cys-374 on the binding of HMM.     

Single-Molecule Motions of MHC Class II Rely on Bound Peptides

The major histocompatibility complex (MHC) class II protein can bind peptides of different lengths in the region outside the peptide-binding groove. Peptide-flanking residues (PFRs) contribute to the binding affinity of the peptide for MHC and change the immunogenicity of the peptide/MHC complex with regard to T cell receptor (TCR). The mechanisms underlying these phenomena are currently unknown. The molecular flexibility of the peptide/MHC complex may be an important determinant of the structures recognized by certain T cells. We used single-molecule x-ray analysis (diffracted x-ray tracking (DXT)) and fluorescence anisotropy to investigate these mechanisms. DXT enabled us to monitor the real-time Brownian motion of the peptide/MHC complex and revealed that peptides without PFRs undergo larger rotational motions than peptides with PFRs. Fluorescence anisotropy further revealed that peptides without PFRs exhibit slightly larger motions on the nanosecond timescale. These results demonstrate that peptides without PFRs undergo dynamic motions in the groove of MHC and consequently are able to assume diverse structures that can be recognized by T cells.     

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.     

Time-correlation analysis of simulated water motion in flexible and rigid gramicidin channels.

Molecular dynamics simulations have been done on a system consisting of the polypeptide membrane channel former gramicidin, plus water molecules in the channel and caps of waters at the two ends of the channel. In the absence of explicit simulation of the surrounding membrane, the helical form of the channel was maintained by artificial restraints on the peptide motion. The characteristic time constant of the artificial restraint was varied to assess the effect of the restraints on the channel structure and water motions. Time-correlation analysis was done on the motions of individual channel waters and on the motions of the center of mass of the channel waters. It is found that individual water molecules confined in the channel execute higher frequency motions than bulk water, for all degrees of channel peptide restraint. The center-of-mass motion of the chain of channel waters (which is the motion that is critical for transmembrane transport, due to the mandatory single filing of water in the channel) does not exhibit these higher frequency motions. The mobility of the water chain is dramatically reduced by holding the channel rigid. Thus permeation through the channel is not like flow through a rigid pipe; rather permeation is facilitated by peptide motion. For the looser restraints we used, the mobility of the water chain was not very much affected by the degree of restraint. Depending on which set of experiments is considered, the computed mobility of our water chain in the flexible channel is four to twenty times too high to account for the experimentally measured resistance of the gramicidin channel to water flow. From this result it appears likely that the peptide motions of an actual gramicidin channel embedded in a lipid membrane may be more restrained than in our flexible channel model, and that these restraints may be a significant modulator of channel permeability. For the completely rigid channel model the "trapping" of the water molecules in preferred positions throughout the molecular dynamics run precludes a reasonable assessment of mobility, but it seems to be quite low.     

Microsecond rotational motion of spin-labeled myosin heads during isometric muscle contraction. Saturation transfer electron paramagnetic resonance.

We have used saturation transfer electron paramagnetic resonance (ST-EPR) to detect the microsecond rotational motions of spin-labeled myosin heads in bundles of skinned muscle fibers, under conditions of rigor, relaxation, and isometric contraction. Experiments were performed on fiber bundles perfused continuously with an ATP-regenerating system. Conditions were identical to those we have used in previous studies of myosin head orientation, except that the fibers were perpendicular to the magnetic field, making the spectra primarily sensitive to rotational motion rather than to the orientational distribution. In rigor, the high intensity of the ST-EPR signal indicates the absence of microsecond rotational motion, showing that heads are all rigidly bound to actin. However, in both relaxation and contraction, considerable microsecond rotational motion is observed, implying that the previously reported orientational disorder under these conditions is dynamic, not static, on the microsecond time scale. The behavior in relaxation is essentially the same as that observed when myosin heads are detached from actin in the absence of ATP (Barnett and Thomas, 1984), corresponding to an effective rotational correlation time of approximately 10 microseconds. Slightly less mobility is observed during contraction. One possible interpretation is that in contraction all heads have the same mobility, corresponding to a correlation time of approximately 25 microseconds. Alternatively, more than one motional population may be present. For example, assuming that the spectrum in contraction is a linear combination of those in relaxation (mobile) and rigor (immobile), we obtained a good fit with a mole fraction of 78-88% of the heads in the mobile state.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of urea on peptide conformation in water: molecular dynamics and experimental characterization

Molecular dynamics simulations of a ribonuclease A C-peptide analog and a sequence variant were performed in water at 277 and 300 K and in 8 M urea to clarify the molecular denaturation mechanism induced by urea and the early events in protein unfolding. Spectroscopic characterization of the peptides showed that the C-peptide analog had a high alpha-helical content, which was not the case for the variant. In the simulations, interdependent side-chain interactions were responsible for the high stability of the alpha-helical C-peptide analog in the different solvents. The other peptide displayed alpha-helical unwinding that propagated cooperatively toward the N-terminal. The conformations sampled by the peptides depended on their sequence and on the solvent. The ability of water molecules to form hydrogen bonds to the peptide as well as the hydrogen bond lifetimes increased in the presence of urea, whereas water mobility was reduced near the peptide. Urea accumulated in excess around the peptide, to which it formed long-lived hydrogen bonds. The unfolding mechanisms induced by thermal denaturation and by urea are of a different nature, with urea-aqueous solutions providing a better peptide solvation than pure water. Our results suggest that the effect of urea on the chemical denaturation process involves both the direct and indirect mechanisms.     

The topology of lysine-containing amphipathic peptides in bilayers by circular dichroism, solid-state NMR, and molecular modeling

In order to better understand the driving forces that determine the alignment of amphipathic helical polypeptides with respect to the surface of phospholipid bilayers, lysine-containing peptide sequences were designed, prepared by solid-phase chemical synthesis, and reconstituted into membranes. CD spectroscopy indicates that all peptides exhibit a high degree of helicity in the presence of SDS micelles or POPC small unilamellar vesicles. Proton-decoupled (31)P-NMR solid-state NMR spectroscopy demonstrates that in the presence of peptides liquid crystalline phosphatidylcholine membranes orient well along glass surfaces. The orientational distribution and dynamics of peptides labeled with (15)N at selected sites were investigated by proton-decoupled (15)N solid-state NMR spectroscopy. Polypeptides with a single lysine residue adopt a transmembrane orientation, thereby locating this polar amino acid within the core region of the bilayer. In contrast, peptides with > or = 3 lysines reside along the surface of the membrane. With 2 lysines in the center of an otherwise hydrophobic amino acid sequence the peptides assume a broad orientational distribution. The energy of lysine discharge, hydrophobic, polar, and all other interactions are estimated to quantitatively describe the polypeptide topologies observed. Furthermore, a molecular modeling algorithm based on the hydrophobicities of atoms in a continuous hydrophilic-hydrophobic-hydrophilic potential describes the experimentally observed peptide topologies well.     

Dynamics of the peptide hormone motilin studied by time resolved fluorescence spectroscopy

Time resolved fluorescence was used to study the dynamics on the nanosecond and subnanosecond time scale of the peptide hormone motilin. The peptide is composed of 22 amino acid residues and has one tyrosine residue in position 7, which was used as an intrinsic fluorescence probe. The measurements show that two rotational correlation times, decreasing with increasing temperature, are needed to account for the fluorescence polarization anisotropy decay data. Viscosity measurements combined with the fluorescence measurements show that the rotational correlation times vary approximately as viscosity with temperature. The shorter rotational correlation time (0.08 ns in an aqueous solution with 30% hexafluoropropanol, HFP at 20°C) should be related to internal movement of the tyrosine side chain in the peptide while the longer rotational correlation time (2.2 ns in 30% HFP at 20°C) describes the motion of the whole peptide. In addition, the interaction of motilin or the derivative motilin (Y7F) –23W (with tyrosine substituted by phenylalanine and with a tryptophan fluorophore added to the C-terminal) with negatively charged phospholipid vesicles (DOPG) was studied. The results show the development of a long anisotropy decay time which reflects partial immobilization of the peptide by interaction with the vesicles.Correspondence to: A. Gräslund     

Reorientational dynamics in lipid vesicles and liposomes studied with ESR: effects of hydration, curvature and unsaturation

Electron spin resonance experiments were carried out on 3-doxyl-5 alpha-cholestane spin-label (CSL) molecules embedded in multilamellar liposomes and small unilamellar vesicles (SUVs) of palmitoyloleoylphosphatidylcholine (POPC), dioleoylphosphatidylcholine (DOPC) and dilinoleoylphosphatidylcholine (DLPC). The experimental spectra were analyzed by a numerical solution of the stochastic Liouville equation. Effects of temperature, presence of unsaturated bonds and high bilayer curvature on the dynamic behaviour of the lipid molecules were studied. Our results, combined with results from planar multibilayers with a varying hydration rate (Korstanje et al. (1989) Biochim. Biophys. Acta 980, 225-233), give a consistent picture of the orientational order and rotational dynamics of CSL molecules embedded in lipid matrices with various geometrical configurations. Increase of hydration or temperature reduces molecular ordering and increases molecular dynamics. In highly curved vesicle configurations, SUVs, molecular order is found to be lower than in multilamellar liposomes. In contrast, rotational motion is not affected by increase of curvature. In all lipid configurations studied, increase of the number of unsaturated bonds in the fatty acid chains reduces molecular ordering. We find, however, no effect of unsaturation on the rotational mobility of the CSL probe molecules. These results clearly show that changes in molecular orientational order and reorientational dynamics have to be considered separately, and that they are not necessarily correlated as implied by the common concept of membrane fluidity. Comparing our results with data from a motional narrowing analysis shows that the latter approach seriously overestimates the rate of molecular reorientation.     

Alignment of lysine-anchored membrane peptides under conditions of hydrophobic mismatch: a CD, 15N and 31P solid-state NMR spectroscopy investigation

The secondary structure and alignment of hydrophobic model peptides in phosphatidylcholine membranes were investigated as a function of hydrophobic mismatch by CD and oriented proton-decoupled (15)N solid-state NMR spectroscopies. In addition, the macroscopic phase and the orientational order of the phospholipid headgroups was analyzed by proton-decoupled (31)P NMR spectroscopy. Both, variations in the composition of the polypeptide (10-30 hydrophobic residues) as well as the fatty acid acyl chain of the phospholipid (10-22 carbons) were studied. At lipid-to-peptide ratios of 50, the peptides adopt helical conformations and bilayer macroscopic phases are predominant. The peptide and lipid maintain much of their orientational order even when the peptide is calculated to be 3 A too short or 14 A too long to fit into the pure lipid bilayer. A continuous decrease in the (15)N chemical shift obtained from transmembrane peptides in oriented membranes suggests an increasing helical tilt angle when the membrane thickness is reduced. This response is, however, insufficient to account for the full hydrophobic mismatch. When the helix is much too long to span the membrane, both the lipid and the peptide order are perturbed, an indication of changes in the macroscopic properties of the membrane. In contrast, sequences that are much too short show little effect on the phospholipid headgroup order, but the peptides exhibit a wide range of orientational distributions predominantly close to parallel to the membrane surface. A thermodynamic formalism is applied to describe the two-state equilibrium between in-plane and transmembrane peptide orientations.     

Structure and dynamics of an amphiphilic peptide in a lipid bilayer: a molecular dynamics study

A molecular dynamics simulation of a simple model membrane system composed of a single amphiphilic helical peptide (ace-K2GL16K2A-amide) in a fully hydrated 1,2-dimyristoyl-sn-glycero-3-phosphocholine bilayer was performed for a total of 1060 ps. The secondary structure of the peptide and its stability were described in terms of average dihedral angles, phi and psi, and the C alpha torsion angles formed by backbone atoms; by the average translation per residue along the helix axis; and by the intramolecular peptide hydrogen bonds. The results indicated that residues 6 through 15 remain in a stable right-handed alpha-helical conformation, whereas both termini exhibit substantial fluctuations. A change in the backbone dihedral angles for residues 16 and 17 is accompanied by the loss of two intramolecular hydrogen bonds, leading to a local but long-lived disruption of the helix. The dynamics of the peptide was characterized in terms of local and global helix motions. The local motions of the N-H bond angles were described in terms of the autocorrelation functions of P2[cos thetaNH(t, t + tau)] and reflected the different degrees of local peptide order as well as a variation in time scale for local motions. The chi1 and chi2 dihedral angles of the leucine side chains underwent frequent transitions between potential minima. No connection between the side-chain positions and their mobility was observed, however. In contrast, the lysine side chains displayed little mobility during the simulation. The global peptide motions were characterized by the tilting and bending motions of the helix. Although the peptide was initially aligned parallel to the bilayer normal, during the simulation it was observed to tilt away from the normal, reaching an angle of approximately 25 degrees by the end of the simulation. In addition, a slight bend of the helix was detected. Finally, the solvation of the peptide backbone and side-chain atoms was also investigated.     

Carbon-13 nuclear magnetic resonance studies on tobacco mosaic virus and its protein.

Fourier transform nuclear magnetic resonance studies on 12% 13C-enriched tobacco mosaic virus (TMV) and its rod-like protein oligomers in solution with molecular weights up to 42 X 10(6) are reported. In the virus approximately 17% of the carbons of the protein subunit have line widths of less than or equal to 300 Hz and T1 less than or equal to 1 s and are concluded to be mobile with more than one degree of freedom of internal rotation about a carbon--carbon bond. In the rodlike polymer of TMV protein at pH 5.3, 30% of the carbons are mobile, which implies rotational motions about carbon--carbon bonds and/or motions of the protein subunits within the polymer. The presence of internal mobility is supported by the observation that 20% of the carbons in the double disklike oligomer show decreasing line width upon increasing temperature; the remaining resonances have line widths which are temperature independent during the double disklike polymerization process. Since the molecular weight of TMV protein polymers increases with increasing temperature, this demonstrates that all nuclei within the double dislike oligomer are mobile. NMR and X-ray data on the double disklike polymer reveal differences with respect to internal mobility.