Characterization of photo-intermediates in the photo-reaction pathways of a bacteriorhodopsin Y185F mutant using in situ photo-irradiation solid-state NMR spectroscopy.

Photo-reaction pathways of a bacteriorhodopsin Y185F mutant were examined using in situ photo-irradiation solid-state NMR spectroscopy. (13)C CP MAS NMR spectra were recorded at -40 °C in the dark (D1), under irradiation with 520 nm light (L1), subsequently in the dark (D2), and again under irradiation with 520 nm light (L2). In the process from D1 to L1, the 13-cis, 15-syn (CS; bR548) state changed to a CS*- (13-cis, 15-syn) intermediate, which was highly stable at -40 °C, and the all-trans (AT; bR568) state transformed to an N-intermediate. Under the D2 conditions, the N-intermediate transformed to an O-intermediate, which was highly stable at -40 °C in the dark. During subsequent irradiation with 520 nm light (L2), the O-intermediate transformed to the N-intermediate through the AT state, whereas the CS*-intermediate did not change. The CS*-intermediate was converted to the AT state (or O-intermediate) after the temperature was increased to -20 °C. Upon subsequent increase of the temperature to 20 °C, the AT state (or O-intermediate) was converted to the CS state until reaching equilibrium. In this experiment, the chemical shift values of [20-(13)C, 14-(13)C]retinal provided the 13C[double bond, length as m-dash]C and 15C[double bond, length as m-dash]N configurations, respectively. From these data, the configurations of the AT and CS states and the CS*-, N-, and O-intermediates were determined to be (13-trans, 15-anti), (13-cis, 15-syn), (13-cis, 15-syn), (13-cis, 15-anti), and (13-trans, 15-anti), respectively. (13)C NMR signals of the CS*- and O-intermediates were observed for the first time for the Y185F bR mutant by in situ photo-irradiation solid-state NMR spectroscopy and the configuration of the CS*-intermediate was revealed to be significantly twisted from that of the CS state although both were assigned as (13-cis, 15-syn) configurations.

Formation of highly twisted ribbons in a carboxymethylcellulase gene-disrupted strain of a cellulose-producing bacterium.

Cellulases are enzymes that normally digest cellulose; however, some are known to play essential roles in cellulose biosynthesis. Although some endogenous cellulases of plants and cellulose-producing bacteria are reportedly involved in cellulose production, their functions in cellulose production are unknown. In this study, we demonstrated that disruption of the cellulase (carboxymethylcellulase) gene causes irregular packing of de novo-synthesized fibrils in Gluconacetobacter xylinus, a cellulose-producing bacterium. Cellulose production was remarkably reduced and small amounts of particulate material were accumulated in the culture of a cmcax-disrupted G. xylinus strain (F2-2). The particulate material was shown to contain cellulose by both solid-state (13)C nuclear magnetic resonance analysis and Fourier transform infrared spectroscopy analysis. Electron microscopy revealed that the cellulose fibrils produced by the F2-2 cells were highly twisted compared with those produced by control cells. This hypertwisting of the fibrils may reduce cellulose synthesis in the F2-2 strains.

Role of aromatic residues in amyloid fibril formation of human calcitonin by solid-state 13C NMR and molecular dynamics simulation.

Calcitonin (CT) is an amyloid fibril forming peptide. Since salmon calcitonin (sCT), having Leu residues (Leu12, Leu16 or Leu19) instead of Tyr12, Phe16 or Phe19 for human calcitonin (hCT), is known to form the fibrils much slower than hCT, hCTs mutated to Leu residues at the position of 16 (F16L-hCT), 19 (F19L-hCT), and 12, 16 and 19 (TL-hCT) were examined to reveal the role of aromatic side-chains on amyloid fibrillation using solid-state (13)C NMR. The detailed kinetics were analyzed using a two-step reaction mechanism such as nucleation and fibril elongation with the rate constants of k1 and k2, respectively. The k2 values of hCT mutants were significantly slower than that of hCT at a neutral pH, although they were almost the same at an acidic pH. The (13)C chemical shifts of the labeled sites showed that the conformations of monomeric hCT mutants take α-helices as viewed from the Gly10 moiety. The hCT mutants formed fibrils and during the fibril formation, the α-helix around Gly10-Phe22 changed to the ß-sheet, and the major structures around Ala26-Ala31 were random coil in the fibrils. Molecular dynamics simulation was performed for the ß-sheet system of hCT9-23 and its mutants F16L-hCT9-23, F19L-hCT9-23 and TL-hCT9-23. In one of the stable fibril structures, Phe16 of hCT interacts with Phe19 of the next strand alternatively. In the hCT mutants, lack of Phe16 and Phe19 interaction causes significant instability as compared with the hCT fibril, leading to the reduction of k2 values, as observed experimentally in the hCT mutants at a neutral pH.

Suppressed or recovered intensities analysis in site-directed (13)C NMR: assessment of low-frequency fluctuations in bacteriorhodopsin and D85N mutants revisited.

The first proton transfer of bacteriorhodopsin (bR) occurs from the protonated Schiff base to the anionic Asp 85 at the central part of the protein in the L to M states. Low-frequency dynamics accompanied by this process can be revealed by suppressed or recovered intensities (SRI) analysis of site-directed (13)C solid-state NMR spectra of 2D crystalline preparations. First of all, we examined a relationship of fluctuation frequencies available from [1-(13)C]Val- and [3-(13)C]Ala-labeled preparations, by taking the effective correlation time of internal methyl rotations into account. We analyzed the SRI data of [1-(13)C]Val-labeled wild-type bR and D85N mutants, as a function of temperature and pH, respectively, based on so-far assigned peaks including newly assigned or revised ones. Global conformational change of the protein backbone, caused by neutralization of the anionic D85 by D85N, can be visualized by characteristic displacement of peaks due to the conformation-dependent (13)C chemical shifts. Concomitant dynamics changes if any, with fluctuation frequencies in the order of 10(4) Hz, were evaluated by the decreased peak intensities in the B-C and D-E loops of D85N mutant. The resulting fluctuation frequencies, owing to subsequent, accelerated dynamics changes in the M-like state by deprotonation of the Schiff base at alkaline pH, were successfully evaluated based on the SRI plots as a function of pH, which were varied depending upon the extent of interference of induced fluctuation frequency with frequency of magic angle spinning or escape from such interference. Distinguishing fluctuation frequencies between the higher and lower than 10(4) Hz is now possible, instead of a simple description of the data around 10(4) Hz available from one-point data analysis previously reported.

Influence of membrane curvature on the structure of the membrane-associated pleckstrin homology domain of phospholipase C-delta1.

The effects of geometric properties of membranes on the structure of the phospholipase C-delta1 (PLC-delta1) pleckstrin homology (PH) domain were investigated using solid state (13)C NMR spectroscopy. Conformations of the PLC-delta1 PH domain at the surfaces of multilamellar vesicles (MLV), small unilamellar vesicles (SUV), and micelles were examined to evaluate the effects of membrane curvature on the PH domain. An increase in curvature of the water-hydrophobic layer interface hinders membrane-penetration of the amphipathic alpha2-helix of the PH domain that assists the membrane-association of the PH domain dominated by the phosphatidylinositol 4,5-bisphosphate (PIP(2)) specific lipid binding site. The solid state (13)C NMR signal of Ala88 located at the alpha2-helix indicates that the conformation of the alpha2-helix at the micelle surface is similar to the solution conformation and significantly different from those at the MLV and SUV surfaces which were characterized by membrane-penetration and re-orientation. The signal of Ala112 which flanks the C-terminus of the beta5/beta6 loop that includes the alpha2-helix, showed downfield displacement with decrease in the interface curvature of the micelles, SUV and MLV. This reveals that the conformation of the C-terminus of the beta5/beta6 loop connecting the beta-sandwich core containing the PIP(2) binding site and the amphipathic alpha2-helix is sensitive to alterations of the curvature of lipid bilayer surface. It is likely that these alterations in the conformation of the PLC-delta1 PH domain contribute to the regulatory mechanisms of the intracellular localization of PLC-delta1 in a manner dependent upon the structure of the molecular complex containing PIP(2).

Participation of the BC loop in the correct folding of bacteriorhodopsin as revealed by solid-state NMR.

Structural changes in bacteriorhodopsin (bR) in two different processes of retinal reconstitutions were investigated by observing the (13)C and (15)N solid-state NMR spectra of [1-(13)C]Val- and [(15)N]Pro-labeled bR. We found that NMR signals of the BC loop were sensitive to changes in protein structure and dynamics, from wild-type (WT) bR to bacterio-opsin (bO), regenerated bR and E1001 bR. Regenerated bR was prepared following the addition of retinal into bO obtained from photobleached WT-bR. E1001 bR was cultured from a retinal-deficient strain termed E1001 following the addition of retinal to growing cells. (15)N NMR signal at Pro70 in the BC loop in WT-bR was observed at 122.4 p.p.m., whereas signals were not apparent or partly suppressed in bO and regenerated bR, respectively. Similarly, the (13)C NMR signal at Val69 in the BC loop at 172.0 p.p.m. that was observed in WT-bR was significantly decreased in both regenerated bR and bO. These results suggest that the dynamic structure of the BC loop in bO was substantially altered following the removal of retinal. As a consequence, the correct protein structure failed to be recovered via the regenerating process of retinal to bO. On the other hand, (13)C and (15)N NMR signals at the BC loop in E1001 bR appeared at positions identical to those of WT-bR. The results of the current study indicate that the BC loop may not always fold correctly in the regenerated bR, which leads to different properties in the regenerated bR compared to that of WT-bR.

Dynamic aspects of extracellular loop region as a proton release pathway of bacteriorhodopsin studied by relaxation time measurements by solid state NMR.

Local dynamics of interhelical loops in bacteriorhodopsin (bR), the extracellular BC, DE and FG, and cytoplasmic AB and CD loops, and helix B were determined on the basis of a variety of relaxation parameters for the resolved 13C and 15N signals of [1-13C]Tyr-, [15N]Pro- and [1-13C]Val-, [15N]Pro-labeled bR. Rotational echo double resonance (REDOR) filter experiments were used to assign [1-13C]Val-, [15N]Pro signals to the specific residues in bR. The previous assignments of [1-13C]Val-labeled peaks, 172.9 or 171.1 ppm, to Val69 were revised: the assignment of peak, 172.1 ppm, to Val69 was made in view of the additional information of conformation-dependent 15N chemical shifts of Pro bonded to Val in the presence of 13C-15N correlation, although no assignment of peak is feasible for 13C nuclei not bonded to Pro. 13C or 15N spin-lattice relaxation times (T1), spin-spin relaxation times under the condition of CP-MAS (T2), and cross relaxation times (TCH and TNH) for 13C and 15N nuclei and carbon or nitrogen-resolved, 1H spin-lattice relaxation times in the rotating flame (1H T1 rho) for the assigned signals were measured in [1-13C]Val-, [15N]Pro-bR. It turned out that V69-P70 in the BC loop in the extracellular side has a rigid beta-sheet in spite of longer loop and possesses large amplitude motions as revealed from 13C and 15N conformation-dependent chemical shifts and T1, T2, 1H T1 rho and cross relaxation times. In addition, breakage of the beta-sheet structure in the BC loop was seen in bacterio-opsin (bO) in the absence of retinal.

Dynamics change of phoborhodopsin and transducer by activation: study using D75N mutant of the receptor by site-directed solid-state 13C NMR.

Pharaonis phoborhodopsin (ppR or sensory rhodopsin II) is a negative phototaxis receptor of Natronomonas pharaonis, and forms a complex, which transmits the photosignal into cytoplasm, with its cognate transducer (pHtrII). We examined a possible local dynamics change of ppR and its D75N mutant complexed with pHtrII, using solid-state (13)C NMR of [3-(13)C]Ala- and [1-(13)C]Val-labeled preparations. We distinguished Ala C(beta) (13)C signals of relatively static stem (Ala221) in the C-terminus of the receptors from those of flexible tip (Ala228, 234, 236 and 238), utilizing a mutant with truncated C-terminus. The local fluctuation frequency at the C-terminal tip was appreciably decreased when ppR was bound to pHtrII, while it was increased when D75N, that mimics the signaling state because of disrupted salt bridge between C and G helices prerequisite for the signal transfer, was bound to pHtrII. This signal change may be considered with the larger dissociation constant of the complex between pHtrII and M-state of ppR. At the same time, it turned out that fluctuation frequency of cytoplasmic portion of pHtrII is lowered when ppR is replaced by D75N in the complex with pHtrII. This means that the C-terminal tip partly participates in binding with the linker region of pHtrII in the dark, but this portion might be released at the signaling state leading to mutual association of the two transducers in the cytoplasmic regions within the ppR/pHtrII complex.

Conformation and dynamics changes of bacteriorhodopsin and its D85N mutant in the absence of 2D crystalline lattice as revealed by site-directed 13C NMR.

13C NMR spectra of [3-(13)C]Ala- and [1-(13)C]Val-labeled D85N mutant of bacteriorhodopsin (bR) reconstituted in egg PC or DMPC bilayers were recorded to gain insight into their secondary structures and dynamics. They were substantially suppressed as compared with those of 2D crystals, especially at the loops and several transmembrane alphaII-helices. Surprisingly, the 13C NMR spectra of [3-(13)C]Ala-D85N turned out to be very similar to those of [3-(13)C]Ala-bR in lipid bilayers, in spite of the presence of globular conformational and dynamics changes in the former as found from 2D crystalline preparations. No further spectral change was also noted between the ground (pH 7) and M-like state (pH 10) as far as D85N in lipid bilayers was examined, in spite of their distinct changes in the 2D crystalline state. This is mainly caused by that the resulting 13C NMR peaks which are sensitive to conformation and dynamics changes in the loops and several transmembrane alphaII-helices of the M-like state are suppressed already by fluctuation motions in the order of 10(4)-10(5) Hz interfered with frequencies of magic angle spinning or proton decoupling. However, 13C NMR signal from the cytoplasmic alpha-helix protruding from the membrane surface is not strongly influenced by 2D crystal or monomer. Deceptively simplified carbonyl 13C NMR signals of the loop and transmembrane alpha-helices followed by Pro residues in [1-(13)C]Val-labeled bR and D85N in 2D crystal are split into two peaks for reconstituted preparations in the absence of 2D crystalline lattice. Fortunately, 13C NMR spectral feature of reconstituted [1-(13)C]Val and [3-(13)C]Ala-labeled bR and D85N was recovered to yield characteristic feature of 2D crystalline form in gel-forming lipids achieved at lowered temperatures.

Phosphatidylserine induces functional and structural alterations of the membrane-associated pleckstrin homology domain of phospholipase C-delta1.

The membrane binding affinity of the pleckstrin homology (PH) domain of phospholipase C (PLC)-delta1 was investigated using a vesicle coprecipitation assay and the structure of the membrane-associated PH domain was probed using solid-state (13)C NMR spectroscopy. Twenty per cent phosphatidylserine (PS) in the membrane caused a moderate but significant reduction of the membrane binding affinity of the PH domain despite the predicted electrostatic attraction between the PH domain and the head groups of PS. Solid-state NMR spectra of the PH domain bound to the phosphatidylcholine (PC)/PS/phosphatidylinositol 4,5-bisphosphate (PIP(2)) (75 : 20 : 5) vesicle indicated loss of the interaction between the amphipathic alpha2-helix of the PH domain and the interface region of the membrane which was previously reported for the PH domain bound to PC/PIP(2) (95 : 5) vesicles. Characteristic local conformations in the vicinity of Ala88 and Ala112 induced by the hydrophobic interaction between the alpha2-helix and the membrane interface were lost in the structure of the PH domain at the surface of the PC/PS/PIP(2) vesicle, and consequently the structure becomes identical to the solution structure of the PH domain bound to d-myo-inositol 1,4,5-trisphosphate. These local structural changes reduce the membrane binding affinity of the PH domain. The effects of PS on the PH domain were reversed by NaCl and MgCl(2), suggesting that the effects are caused by electrostatic interaction between the protein and PS. These results generally suggest that the structure and function relationships among PLCs and other peripheral membrane proteins that have similar PH domains would be affected by the local lipid composition of membranes.

Surface and dynamic structures of bacteriorhodopsin in a 2D crystal, a distorted or disrupted lattice, as revealed by site-directed solid-state 13C NMR.

The 3D structure of bacteriorhodopsin (bR) obtained by X-ray diffraction or cryo-electron microscope studies is not always sufficient for a picture at ambient temperature where dynamic behavior is exhibited. For this reason, a site-directed solid-state 13C NMR study of fully hydrated bR from purple membrane (PM), or a distorted or disrupted lattice, is very valuable in order to gain insight into the dynamic picture. This includes the surface structure, at the physiologically important ambient temperature. Almost all of the 13C NMR signals are available from [3-13C]Ala or [1-13C]Val-labeled bR from PM, although the 13C NMR signals from the surface areas, including loops and transmembrane alpha-helices near the surface (8.7 angstroms depth), are suppressed for preparations labeled with [1-13C]Gly, Ala, Leu, Phe, Tyr, etc. due to a failure of the attempted peak-narrowing by making use of the interfered frequency of the frequency of fluctuation motions with the frequency of magic angle spinning. In particular, the C-terminal residues, 226-235, are present as the C-terminal alpha-helix which is held together with the nearby loops to form a surface complex, although the remaining C-terminal residues undergo isotropic motion even in a 2D crystalline lattice (PM) under physiological conditions. Surprisingly, the 13C NMR signals could be further suppressed even from [3-13C]Ala- or [1-13C]Val-bR, due to the acquired fluctuation motions with correlation times in the order of 10(-4) to 10(-5) s, when the 2D lattice structure is instantaneously distorted or completely disrupted, either in photo-intermediate, removed retinal or when embedded in the lipid bilayers.

Pressure-induced isomerization of retinal on bacteriorhodopsin as disclosed by fast magic angle spinning NMR.

Bacteriorhodopsin (bR) is a retinal protein in purple membrane of Halobacterium salinarum, which functions as a light-driven proton pump. We have detected pressure-induced isomerization of retinal in bR by analyzing 15N cross polarization-magic angle spinning (CP-MAS) NMR spectra of [zeta-15N]Lys-labeled bR. In the 15N-NMR spectra, both all-trans and 13-cis retinal configurations have been observed in the Lys N(zeta) in protonated Schiff base at 148.0 and 155.0 ppm, respectively, at the MAS frequency of 4 kHz in the dark. When the MAS frequency was increased up to 12 kHz corresponding to the sample pressure of 63 bar, the 15N-NMR signals of [zeta-15N]Lys in Schiff base of retinal were broadened. On the other hand, other [zeta-15N]Lys did not show broadening. Subsequently, the increased signal intensity of [zeta-15N]Lys in Schiff base of 13-cis retinal at 155.0 ppm was observed when the MAS frequency was decreased from 12 to 4 kHz. These results showed that the equilibrium constant of [all-trans-bR]/[13-cis-bR] in retinal decreased by the pressure of 63 bar. It was also revealed that the structural changes induced by the pressure occurred in the vicinity of retinal. Therefore, microscopically, hydrogen-bond network around retinal would be disrupted or distorted by a constantly applied pressure. It is, therefore, clearly demonstrated that increased pressure induced by fast MAS frequencies generated isomerization of retinal from all-trans to 13-cis state in the membrane protein bR.

Participation of the surface structure of Pharaonis phoborhodopsin, ppR and its A149S and A149V mutants, consisting of the C-terminal alpha-helix and E-F loop, in the complex-formation with the cognate transducer pHtrII, as revealed by site-directed 13C solid-state NMR.

We have recorded 13C solid state NMR spectra of [3-13C]Ala-labeled pharaonis phoborhodopsin (ppR) and its mutants, A149S and A149V, complexed with the cognate transducer pharaonis halobacterial transducer II protein (pHtrII) (1-159), to gain insight into a possible role of their cytoplasmic surface structure including the C-terminal alpha-helix and E-F loop for stabilization of the 2:2 complex, by both cross-polarization magic angle spinning (CP-MAS) and dipolar decoupled (DD)-MAS NMR techniques. We found that 13C CP-MAS NMR spectra of [3-13C]Ala-ppR, A149S and A149V complexed with the transducer pHtrII are very similar, reflecting their conformation and dynamics changes caused by mutual interactions through the transmembrane alpha-helical surfaces. In contrast, their DD-MAS NMR spectral features are quite different between [3-13C]Ala-A149S and A149V in the complexes with pHtrII: 13C DD-MAS NMR spectrum of [3-13C]Ala-A149S complex is rather similar to that of the uncomplexed form, while the corresponding spectral feature of A149V complex is similar to that of ppR complex in the C-terminal tip region. This is because more flexible surface structure detected by the DD-MAS NMR spectra are more directly influenced by the dynamics changes than the CP-MAS NMR. It turned out, therefore, that an altered surface structure of A149S resulted in destabilized complex as viewed from the 13C NMR spectrum of the surface areas, probably because of modified conformation at the corner of the helix E in addition to the change of hydropathy. It is, therefore, concluded that the surface structure of ppR including the C-terminal alpha-helix and the E-F loops is directly involved in the stabilization of the complex through conformational stability of the helix E.

Backbone dynamics of membrane proteins in lipid bilayers: the effect of two-dimensional array formation as revealed by site-directed solid-state 13C NMR studies on [3-13C]Ala- and [1-13C]Val-labeled bacteriorhodopsin.

We have recorded site-directed solid-state 13C NMR spectra of [3-13C]Ala- and [1-13C]Val-labeled bacteriorhodopsin (bR) as a typical membrane protein in lipid bilayers, to examine the effect of formation of two-dimensional (2D) lattice or array of the proteins toward backbone dynamics, to search the optimum condition to be able to record full 13C NMR signals from whole area of proteins. Well-resolved 13C NMR signals were recorded for monomeric [3-13C]Ala-bR in egg phosphatidylcholine (PC) bilayer at ambient temperature, although several 13C NMR signals from the loops and transmembrane alpha-helices were still suppressed. This is because monomeric bR reconstituted into egg PC, dimyristoylphosphatidylcholine (DMPC) or dipalmytoylphosphatidylcholine (DPPC) bilayers undergoes conformational fluctuations with frequency in the order of 10(4)-10(5) Hz at ambient temperature, which is interfered with frequency of magic angle spinning or proton decoupling. It turned out, however, that the 13C NMR signals of purple membrane (PM) were almost fully recovered in gel phase lipids of DMPC or DPPC bilayers at around 0 degrees C. This finding is interpreted in terms of aggregation of bR in DMPC or DPPC bilayers to 2D hexagonal array in the presence of endogenous lipids at low temperature, resulting in favorable backbone dynamics for 13C NMR observation. It is therefore concluded that [3-13C]Ala-bR reconstituted in egg PC, DMPC or DPPC bilayers at ambient temperature, or [3-13C]Ala- and [1-13C]Val-bR at low temperature gave rise to well-resolved 13C NMR signals, although they are not always completely the same as those of 2D hexagonal lattice from PM.

Secondary structure and backbone dynamics of Escherichia coli diacylglycerol kinase, as revealed by site-directed solid-state 13C NMR.

To gain insight into secondary structure and backbone dynamics, we have recorded (13)C NMR spectra of [3-(13)C]Ala-, [1-(13)C]Val-labeled Escherichia coli diacylglycerol kinase (DGK), using cross-polarization-magic angle spinning (CP-MAS) and single-pulse excitation with dipolar decoupled-magic angle spinning (DD-MAS) methods. DGK was either solubilized in n-decyl-beta-maltoside (DM) micelle or integrated into 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) or 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) bilayers. Surprisingly, the (13)C NMR spectra were broadened to yield rather featureless peaks at physiological temperatures, both in DM solution or lipid bilayers at liquid crystalline phase, due to interference of motional frequencies of DGK with frequencies of magic angle spinning (MAS) or proton decoupling (10(4) or 10(5) Hz, respectively). In gel phase lipids, however, up to six distinct (13)C NMR peaks were well-resolved due to lowered fluctuation frequencies (<10(5) Hz) for the transmembrane region, the amphipathic alpha-helices and loops. While DGK can be tightly packed in gel phase lipids, DGK is less tightly packed at physiological temperatures, where it becomes more mobile. The fact that the enzymatic activity is low under conditions where motion is restricted and high when conformational fluctuations can occur suggests that acquisition of low frequency backbone motions, on the microsecond to millisecond time scale, may facilitate the efficient enzymatic activity of DGK.

Residue-specific millisecond to microsecond fluctuations in bacteriorhodopsin induced by disrupted or disorganized two-dimensional crystalline lattice, through modified lipid-helix and helix-helix interactions, as revealed by 13C NMR.

We have recorded 13C NMR spectra of [3-13C]-, [1-13C]Ala-, and [1-13C]Val-labeled bacteriorhodopsin (bR), W80L and W12L mutants and bacterio-opsin (bO) from retinal-deficient E1001 strain, in order to examine the possibility of their millisecond to microsecond local fluctuations with correlation time in the order of 10(-4) to 10(-5) s, induced or prevented by disruption or assembly of two-dimensional (2D) crystalline lattice, respectively, at ambient temperature. The presence of disrupted or disorganized 2D lattice for W12L, W80L and bO from E1001 strain was readily visualized by increased relative proportions of surrounding lipids per protein, together with their broadened 13C NMR signals of transmembrane alpha-helices and loops in [3-13C]Ala-labeled proteins, with reference to those of wild-type. In contrast, 13C CP-MAS NMR spectra of [1-13C]Ala- and Val-labeled these mutants were almost completely suppressed, owing to the presence of fluctuations with time scale of 10(-4) s interfered with magic angle spinning. In particular, 13C NMR signals of [1-13C]Ala-labeled transmembrane alpha-helices of wild-type were almost completely suppressed at the interface between the surface and inner part (up to 8.7 A deep from the surface) with reference to those of the similarly suppressed peaks by Mn(2+)-induced accelerated spin-spin relaxation rate. Such fluctuation-induced suppression of 13C NMR peaks from the interfacial regions, however, was less significant for [1-13C]Val-labeled proteins, because fluctuation motions in Val residues with bulky side-chains at the C(alpha) moiety were modified to those of longer correlation time (>10(-4) s), if any, by residue-specific manner. To support this view, we found that such suppressed 13C NMR signals of [1-13C]Ala-labeled peaks in the wild-type were recovered for D85N and bO in which correlation times of fluctuations were shifted to the order of 10(-5) s due to modified helix-helix interactions as previously pointed out [Biochemistry, 39 (2000) 14472; J. Biochem. (Tokyo) 127 (2000) 861].

Dynorphin induced magnetic ordering in lipid bilayers as studied by (31)P NMR spectroscopy.

Lipid bilayers of dimyristoyl phosphatidylcholine (DMPC) containing opioid peptide dynorphin A(1-17) are found to be spontaneously aligned to the applied magnetic field near at the phase transition temperature between the gel and liquid crystalline states (T(m)=24 degrees C), as examined by 31P NMR spectroscopy. The specific interaction between the peptide and lipid bilayer leading to this property was also examined by optical microscopy, light scattering, and potassium ion-selective electrode, together with a comparative study on dynorphin A(1-13). A substantial change in the light scattering intensity was noted for DMPC containing dynorphin A(1-17) near at T(m) but not for the system containing A(1-13). Besides, reversible change in morphology of bilayer, from small lipid particles to large vesicles, was observed by optical microscope at T(m). These results indicate that lysis and fusion of the lipid bilayers are induced by the presence of dynorphin A(1-17). It turned out that the bilayers are spontaneously aligned to the magnetic field above T(m) in parallel with the bilayer surface, because a single 31P NMR signal appeared at the perpendicular position of the 31P chemical shift tensor. In contrast, no such magnetic ordering was noted for DMPC bilayers containing dynorphin A(1-13). It was proved that DMPC bilayer in the presence of dynorphin A(1-17) forms vesicles above T(m), because leakage of potassium ion from the lipid bilayers was observed by potassium ion-selective electrode after adding Triton X-100. It is concluded that DMPC bilayer consists of elongated vesicles with the long axis parallel to the magnetic field, together with the data of microscopic observation of cylindrical shape of the vesicles. Further, the long axis is found to be at least five times longer than the short axis of the elongated vesicles in view of simulated 31P NMR lineshape.

Dynamic structure of pharaonis phoborhodopsin (sensory rhodopsin II) and complex with a cognate truncated transducer as revealed by site-directed 13C solid-state NMR.

We have recorded (13)C nuclear magnetic resonance (NMR) spectra of [3-(13)C]Ala, [1-(13)C]Val-labeled pharaonis phoborhodopsin (ppR or sensory rhodopsin II) incorporated into egg PC (phosphatidylcholine) bilayer, by means of site-directed high-resolution solid-state NMR techniques. Seven (13)C NMR signals from transmembrane alpha-helices were resolved for [3-(13)C]Ala-ppR at almost the same positions as those of bacteriorhodopsin (bR), except for the suppressed peaks in the loop regions in spite of the presence of at least three Ala residues. In contrast, (13)C NMR signals from the loops were visible from [1-(13)C]Val-ppR but their peak positions of the transmembrane alpha-helices are not always the same between ppR and bR. The motional frequency of the loop regions in ppR was estimated as 10(5) Hz in view of the suppressed peaks from [3-(13)C]Ala-ppR due to interference with proton decoupling frequency. We found that conformation and dynamics of ppR were appreciably altered by complex formation with a cognate truncated transducer pHtr II (1-159). In particular, the C-terminal alpha-helix protruding from the membrane surface is involved in the complex formation and subsequent fluctuation frequency is reduced by one order of magnitude.

Membrane-induced alteration of the secondary structure in the SWAP-70 pleckstrin homology domain.

Differences in the conformation of the pleckstrin homology (PH) domain of switch-associated protein-70 (SWAP-70) in solution and at the lipid bilayer membrane surface were examined using CD, fluorescence and NMR spectroscopy. Intracellular relocalization of SWAP-70 from the cytoplasm to the plasma membrane and then to the nucleus is associated with its cellular functions. The PH domain of SWAP-70 contains a phosphoinositide-binding site and a nuclear localization signal, which localize SWAP-70 to the plasma membrane and nucleus, respectively. CD and fluorescence spectra showed that a significant conformational alteration involving formation of disordered structure occurs when the PH domain binds to D-myo-phosphatidylinositol 3,4,5-trisphosphate or D-myo-phosphatidylinositol 4,5-bisphosphate embedded in lipid bilayer vesicles. NMR spectra indicate that Ala and Trp residues located in the C-terminal α-helix of the PH domain undergo conformational alterations to form a disordered structure at the vesicle surface. These conformational alterations were not induced by association with inositol 1,3,4,5-tetrakisphosphate in solution or coexistence of phosphatidylcholine vesicles. Interaction with the plane of the lipid bilayer via association with the phosphoinositides is required for the unfolding of the C-terminal α-helix of the PH domain. The unwinding of the C-terminal α-helix could regulate the functions of SWAP-70 at the plasma membrane surface.

Morphological behavior of lipid bilayers induced by melittin near the phase transition temperature.

Morphological changes of DMPC, DLPC, and DPPC bilayers containing melittin (lecithin/melittin molar ratio of 10:1) around the gel-to-liquid crystalline phase transition temperatures (Tc) were examined by a variety of biophysical methods. First, giant vesicles with the diameters of approximately 20 microm were observed by optical microscopy for melittin-DMPC bilayers at 27.9 degrees C. When the temperature was lowered to 24.9 degrees C (Tc = 23 degrees C for the neat DMPC bilayers), the surface of vesicles became blurred and dynamic pore formation was visible in the microscopic picture taken at different exposure times. Phase separation and association of melittin molecules in the bilayers were further detected by fluorescent microscopy and mass spectrometry, respectively. These vesicles disappeared completely at 22.9 degrees C. It was thus found that the melittin-lecithin bilayers reversibly undergo their fusion and disruption near the respective Tcs. The fluctuation of lipids is, therefore, responsible for the membrane fusion above the Tc, and the association of melittin molecules causes membrane fragmentation below the Tc. Subsequent magnetic alignments were observed by solid-state (31)P NMR spectra for the melittin-lecithin vesicles at a temperature above the respective Tcs. On the other hand, additional large amplitude motion induced by melittin at a temperature near the Tc breaks down the magnetic alignment.