Backbone dynamics of membrane proteins in lipid bilayers: the effect of two-dimensional array formation as revealed by site-directed solid-state C NMR studies on [3-C]Ala- and [1-C]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 α-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 10⁴-10⁵ 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 °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.     

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.     

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

¹³C NMR spectra of [3-¹³C]Ala- and [1-¹³C]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 α_II-helices. Surprisingly, the ¹³C NMR spectra of [3-¹³C]Ala-D85N turned out to be very similar to those of [3-¹³C]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 α_II-helices of the M-like state are suppressed already by fluctuation motions in the order of 10⁴-10⁵ Hz interfered with frequencies of magic angle spinning or proton decoupling. However, ¹³C NMR signal from the cytoplasmic α-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 α-helices followed by Pro residues in [1-¹³C]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 [1-¹³C]Val and [3-¹³C]Ala-labeled bR and D85N was recovered to yield characteristic feature of 2D crystalline form in gel-forming lipids achieved at lowered temperatures.     

Regio-selective detection of dynamic structure of transmembrane alpha-helices as revealed from (13)C NMR spectra of [3-13C]Ala-labeled bacteriorhodopsin in the presence of Mn2+ ion.

13C Nuclear magnetic resonance (NMR) spectra of [3-(13)C]Ala-labeled bacteriorhodopsin (bR) were edited to give rise to regio-selective signals from hydrophobic transmembrane alpha-helices by using NMR relaxation reagent, Mn(2+) ion. As a result of selective suppression of (13)C NMR signals from the surfaces in the presence of Mn(2+) ions, several (13)C NMR signals of Ala residues in the transmembrane alpha-helices were identified on the basis of site-directed mutagenesis without overlaps from (13)C NMR signals of residues located near the bilayer surfaces. The upper bound of the interatomic distances between (13)C nucleus in bR and Mn(2+) ions bound to the hydrophilic surface to cause suppressed peaks by the presence of Mn(2+) ion was estimated as 8.7 A to result in the signal broadening to 100 Hz and consistent with the data based on experimental finding. The Ala C(beta) (13)C NMR peaks corresponding to Ala-51, Ala-53, Ala-81, Ala-84, and Ala-215 located around the extracellular half of the proton channel and Ala-184 located at the kink in the helix F were successfully identified on the basis of (13)C NMR spectra of bR in the presence of Mn(2+) ion and site-directed replacement of Ala by Gly or Val. Utilizing these peaks as probes to observe local structure in the transmembrane alpha-helices, dynamic conformation of the extracellular half of bR at ambient temperature was examined, and the local structures of Ala-215 and 184 were compared with those elucidated at low temperature. Conformational changes in the transmembrane alpha-helices induced in D85N and E204Q and its long-range transmission from the proton release site to the site around the Schiff base in E204Q were also examined.     

Dynamic pictures of membrane proteins in two-dimensional crystal, lipid bilayer and detergent as revealed by site-directed solid-state 13C NMR

We have compared site-directed 13C solid-state NMR spectra of [3-13C]Ala- and/or [1-13C]Val-labeled membrane proteins, including bacteriorhodopsin (bR), pharaonis phoborhodopin (ppR), its cognate transducer (pHtrII) and Escherichia coli diacylglycerol kinase (DGK), in two-dimensional (2D) crystal, lipid bilayers, and detergent. Restricted fluctuation motions of these membrane proteins due to oligomerization of bR by specific protein-protein interactions in the 2D crystalline lattice or protein complex between ppR and pHtrII provide the most favorable environment to yield well-resolved, fully visible 13C NMR signals for [3-13C]Ala-labeled proteins. In contrast, several signals from such membrane proteins were broadened or lost owing to interference of inherent fluctuation frequencies (10(4)-10(5)Hz) with frequency of either proton decoupling or magic angle spinning, if their 13C NMR spectra were recorded as a monomer in lipid bilayers at ambient temperature. The presence of such protein dynamics is essential for the respective proteins to achieve their own biological functions. Finally, spectral broadening found for bR and DGK in detergents were discussed.     

Surface dynamics of bacteriorhodopsin as revealed by (13)C NMR studies on [(13)C]Ala-labeled proteins: detection of millisecond or microsecond motions in interhelical loops and C-terminal alpha-helix

We have recorded (13)C NMR spectra of [2-(13)C]-, [1-(13)C]-, [3-(13)C],- and [1,2,3-(13)C(3)]Ala-labeled bacteriorhodopsin (bR), and its mutants, A196G, A160G, and A103C, by means of cross polarization-magic angle spinning (CP-MAS) and dipolar decoupled-magic angle spinning (DD-MAS) techniques, to reveal the conformation and dynamics of bR, with emphasis on the loop and C-terminus structures. The (13)C NMR signals of the loop (C-D, E-F, and F-G) regions were almost completely suppressed from [2-(13)C]-, [1-(13)C]Ala-, and [1-(13)C]Gly-labeled bR, due to the presence of conformational fluctuation with correlation times of 10(-4) s that interfered with the peak-narrowing by magic angle spinning. The observation of such suppressed peaks for specific residues provides a unique means of detecting intermediate frequency motions on the time scale of ms or micros in the surface loops of membrane proteins. Instead, the three well-resolved (13)C CP-MAS NMR signals of [2-(13)C]Ala-bR, at 50.38, 49.90, and 47.96 ppm, were ascribed to the C-terminal alpha-helix previously proposed from the data for [3-(13)C]Ala-bR: the former two peaks were assigned to Ala 232 and 238, in view of the results of successive proteolysis experiments, while the highest-field peak was ascribed to Ala 235 prior to Pro 236. Even such (13)C NMR signals were substantially broadened when (13)C NMR spectra of fully labeled [1,2,3-(13)C]Ala-bR were recorded, because the broadening and splitting of peaks due to the accelerated transverse relaxation rate caused by the increased number of relaxation pathways through a number of (13)C-(13)C homo-nuclear dipolar interactions and scalar J couplings, respectively, are dominant among (13)C-labeled nuclei. In addition, approximate correlation times for local conformational fluctuations of different domains, including the C-terminal tail, C-terminal alpha-helix, loops, and transmembrane alpha-helices, were estimated by measurement of the spin-lattice relaxation times in the laboratory frame and spin-spin relaxation times under the conditions of cross-polarization-magic angle spinning, and comparative study of suppressed specific peaks between the CP-MAS and DD-MAS experiments.     

A (13)C NMR study on [3-(13)C]-, [1-(13)C]Ala-, or [1-(13)C]Val-labeled transmembrane peptides of bacteriorhodopsin in lipid bilayers: insertion, rigid-body motions, and local conformational fluctuations at ambient temperature

We have recorded (13)C NMR spectra of selectively [3-(13)C]Ala-, [1-(13)C]Ala-, or [1-(13)C]Val-labeled synthetic transmembrane peptides of bacteriorhodopsin (bR) and enzymatically cleaved C-2 fragment in the solid and dimyristoylphosphatidylcholine bilayer. It turned out that these transmembrane peptides either in hexafluoroisopropanol or cast from it take an ordinary alpha-helix (alpha(I)-helix) irrespective of their amino acid sequences with reference to the conformation-dependent (13)C chemical shifts of (Ala)(n) taking the alpha-helix form. These transmembrane peptides are not always static in the lipid bilayer as in the solid state but undergo rigid-body motions with various frequencies as estimated from suppressed peaks either by fast isotropic or large-amplitude motions (>10(8) Hz) or intermediate frequencies (10(5) or 10(3) Hz). Further, (13)C chemical shifts of the [3-(13)C]Ala-labeled peptides in the bilayer were displaced downfield by 0.3-1.1 ppm depending upon amino acid sequence with respect to those in the solid state, which were explained in terms of local conformational fluctuation (10(2) Hz) deviated from the torsion angles (alpha(II)-helix) from those of standard alpha-helix, under anisotropic environment in lipid bilayer, in addition to the above-mentioned rigid-body motions. The carbonyl (13)C peaks, on the other hand, are not sensitively displaced by such local anisotropic fluctuations, because they are more sensitive to the manner of hydrogen-bond interactions. The amino acid sequences of these peptides inserted within the bilayer were not always the same as those of intact bR, causing disposition of the transmembrane alpha-helical segment from that of intact bR. Finally, we confirmed that the (13)C NMR peak positions of the random coil form are located at the boundary between the alpha-helix and a turned structure in loop regions.     

Conformation and dynamics of the [3-(13)C]Ala, [1-(13)C]Val-labeled truncated pharaonis transducer, pHtrII(1-159), as revealed by site-directed (13)C solid-state NMR: changes due to association with phoborhodopsin (sensory rhodopsin II)

We have recorded (13)C NMR spectra of the [3-(13)C]Ala, [1-(13)C]Val-labeled pharaonis transducer pHtrII(1-159) in the presence and absence of phoborhodopsin (ppR or sensory rhodopsin II) in egg phosphatidylcholine or dimyristoylphosphatidylcholine bilayers by means of site-directed (amino acid specific) solid-state NMR. Two kinds of (13)C NMR signals of [3-(13)C]Ala-pHtrII complexed with ppR were clearly seen with dipolar decoupled magic angle spinning (DD-MAS) NMR. One of these resonances was at the peak position of the low-field alpha-helical peaks (alpha(II)-helix) and is identified with cytoplasmic alpha-helices protruding from the bilayers; the other was the high-field alpha-helical peak (alpha(I)-helix) and is identified with the transmembrane alpha-helices. The first peaks, however, were almost completely suppressed by cross-polarization magic angle spinning (CP-MAS) regardless of the presence or absence of ppR or by DD-MAS NMR in the absence of ppR. This is caused by an increased fluctuation frequency of the cytoplasmic alpha-helix from 10(5) Hz in the uncomplexed states to >10(6) Hz in the complexed states, leading to the appearance of peaks that were suppressed because of the interference of the fluctuation frequency with the frequency of proton decoupling (10(5) Hz), as viewed from the (13)C NMR spectra of [3-(13)C]Ala-labeled pHtrII. Consistent with this view, the (13)C DD-MAS NMR signals of the cytoplasmic alpha-helices of the complexed [3-(13)C]Ala-pHtrII in the dimyristoylphosphatidylcholine (DMPC) bilayer were partially suppressed at 0 degrees C due to a decreased fluctuation frequency at the low temperature. In contrast, examination of the (13)C CP-MAS spectra of [1-(13)C]Val-labeled complexed pHtrII showed that the (13)C NMR signals of the transmembrane alpha-helix were substantially suppressed. These spectral changes are again interpreted in terms of the increased fluctuation frequency of the transmembrane alpha-helices from 10(3) Hz of the uncomplexed states to 10(4) Hz of the complexed states. These findings substantiate the view that the transducers alone are in an aggregated or clustered state but the ppR-pHtrII complex is not aggregated. We show that (13)C NMR is a very useful tool for achieving a better understanding of membrane proteins which will serve to clarify the molecular mechanism of signal transduction in this system.     

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.     

Glutamic acid residues of bacteriorhodopsin at the extracellular surface as determinants for conformation and dynamics as revealed by site-directed solid-state 13C NMR

We recorded (13)C NMR spectra of [3-(13)C]Ala- and [1-(13)C]Val-labeled bacteriorhodopsin (bR) and a variety of its mutants, E9Q, E74Q, E194Q/E204Q (2Glu), E9Q/E194Q/E204Q (3Glu), and E9Q/E74Q/E194Q/E204Q (4Glu), to clarify contributions of the extracellular (EC) Glu residues to the conformation and dynamics of bR. Replacement of Glu-9 or Glu-74 and Glu-194/204 at the EC surface by glutamine(s) induced significant conformational changes in the cytoplasmic (CP) surface structure. These changes occurred in the C-terminal alpha-helix and loops, and also those of the EC surface, as viewed from (13)C NMR spectra of [3-(13)C]Ala- and [1-(13)C]Val-labeled proteins. Additional conformational changes in the transmembrane alpha-helices were induced as modified retinal-protein interactions for multiple mutants involving the E194Q/E204Q pair. Significant dynamic changes were induced for the triple or quadruple mutants, as shown by broadened (13)C NMR peaks of [1-(13)C]Val-labeled proteins. These changes were due to acquired global fluctuation motions of the order of 10(-4)-10(-5) s as a result of disorganized trimeric form. In such mutants (13)C NMR signals from Val residues of [1-(13)C]Val-labeled triple and quadruple mutants near the CP and EC surfaces (including 8.7-A depth from the surface) were substantially suppressed, as shown by comparative (13)C NMR studies with and without 40 micro M Mn(2+) ion. We conclude that these Glu residues at the EC surface play an important role in maintaining the native secondary structure of bR in the purple membrane.     

Interactions of triglycerides with phospholipids: incorporation into the bilayer structure and formation of emulsions

Interactions of carbonyl 13C-enriched triacylglycerols (TG) with phospholipid bilayers [egg phosphatidylcholine (PC), dipalmitoylphosphatidylcholine (DPPC), and an ether-linked phosphatidylcholine] were studied by 13C NMR spectroscopy. Up to 3 mol % triolein (TO) or tripalmitin (TP) was incorporated into DPPC vesicles by cosonication of the TG and DPPC at approximately 50 degrees C. NMR studies were carried out in a temperature range (30-50 degrees C) in which pure TO is a liquid whereas pure TP is a solid. In spectra of DPPC vesicles with TG at 40-50 degrees C, both TO and TP had narrow carbonyl resonances, indicative of rapid motions, and chemical shifts indicative of H bonding of the TG carbonyls with solvent (H2O) at the aqueous interfaces of the vesicle bilayer. Below the phase transition temperature of the DPPC/TG vesicles (approximately 36 degrees C), most phospholipid peaks broadened markedly. In DPPC vesicles with TP, the TP carbonyl peaks broadened beyond detection below the transition, whereas in vesicles with TO, the TO carbonyl peaks showed little change in line width or chemical shift and no change in the integrated intensity. Thus, in the gel phase, TP solidified with DPPC, whereas TO was fluid and remained oriented at the aqueous interfaces. Egg PC vesicles incorporated up to 2 mol % TP at 35 degrees C; the TP carbonyl peaks had line-width and chemical shift values similar to those for TP (or TO) in liquid-crystalline DPPC. TO incorporated into ether-linked PC had properties very similar to TO in ester-linked PC.(ABSTRACT TRUNCATED AT 250 WORDS)     

Irreversible conformational change of bacterio-opsin induced by binding of retinal during its reconstitution to bacteriorhodopsin, as studied by (13)C NMR

We compared (13)C NMR spectra of [3-(13)C]Ala- and [1-(13)C]Val-labeled bacterio-opsin (bO), produced either by bleaching bR with hydroxylamine or from a retinal-deficient strain, with those of bacteriorhodopsin (bR), in order to gain insight into the conformational changes of the protein backbone that lead to correct folding after retinal is added to bO. The observed (13)C NMR spectrum of bO produced by bleaching is not greatly different from that of bR, except for the presence of suppressed or decreased peak-intensities. From careful evaluation of the intensity differences between cross polarization magic angle spinning (CP-MAS) and dipolar decoupled-magic angle spinning (DD-MAS) spectra, it appears that the reduced peak-intensities arise from reduced efficiency of cross polarization or interference of internal motions with proton decoupling frequencies. In particular, the E-F and F-G loops and some transmembrane helices of the bleached bO have acquired internal motions whose frequencies interfere with proton decoupling frequencies. In contrast, the protein backbone of the bO from the retinal-negative cells is incompletely folded. Although it contains mainly a-helices, its very broad (13)C NMR signals indicate that its tertiary structure is different from bR. Importantly, this changed structure is identical in form to that of bleached bO from wild-type bR after it was regenerated with retinal in vitro, and bleached with hydroxylamine. We conclude that the binding of retinal is essential for the correct folding of bR after it is inserted in vitro into the lipid bilayer, and the final folded state does not revert to the partially folded form upon removal of the retinal.     

Solid state NMR study of [epsilon-13C]Lys-bacteriorhodopsin: Schiff base photoisomerization.

Previous solid state 13C-NMR studies of bacteriorhodopsin (bR) have inferred the C = N configuration of the retinal-lysine Schiff base linkage from the [14-13C]retinal chemical shift (1-3). Here we verify the interpretation of the [14-13C]-retinal data using the [epsilon-13C]lysine 216 resonance. The epsilon-Lys-216 chemical shifts in bR555 (48 ppm) and bR568 (53 ppm) are consistent with a C = N isomerization from syn in bR555 to anti in bR568. The M photointermediate was trapped at pH 10.0 and low temperatures by illumination of samples containing either 0.5 M guanidine-HCl or 0.1 M NaCl. In both preparations, the [epsilon-13C]Lys-216 resonance of M is 6 ppm downfield from that of bR568. This shift is attributed to deprotonation of the Schiff base nitrogen and is consistent with the idea that the M intermediate contains a C = N anti chromophore. M is the only intermediate trapped in the presence of 0.5 M guanidine-HCl, whereas a second species, X, is trapped in the presence of 0.1 M NaCl. The [epsilon-13C]Lys-216 resonance of X is coincident with the signal for bR568, indicating that X is either C = N anti and protonated or C = N syn and deprotonated.     

Alteration of conformation and dynamics of bacteriorhodopsin induced by protonation of Asp 85 and deprotonation of Schiff base as studied by 13C NMR

According to previous X-ray diffraction studies, the D85N mutant of bacteriorhodopsin (bR) with unprotonated Schiff base assumes a protein conformation similar to that in the M photointermediate. We recorded (13)C NMR spectra of [3-(13)C]Ala- and [1-(13)C]Val-labeled D85N and D85N/D96N mutants at ambient temperature to examine how conformation and dynamics of the protein backbone are altered when the Schiff base is protonated (at pH 7) and unprotonated (at pH 10). Most notably, we found that the peak intensities of three to four [3-(13)C]Ala-labeled residues from the transmembrane alpha-helices, including Ala 39, 51, and 53 (helix B) and 215 (helix G), were suppressed in D85N and D85N/D96N both from CP-MAS (cross polarization-magic angle spinning) and DD-MAS (dipolar decoupled-magic angle spinning) spectra, irrespective of the pH. This is due to conformational change and subsequent acquisition of intermediate time-range motions, with correlation times in the order of 10(-)(5) or 10(-)(4) s, which interferes with proton decoupling frequency or frequency of magic angle spinning, respectively, essential for an attempted peak-narrowing to achieve high-resolution NMR signals. Greater changes were achieved, however, at pH 10, which indicate large-amplitude motions of transmembrane helices upon deprotonation of Schiff base and the formation of the M-like state in the absence of illumination. The spectra detected more rapid motions in the extracellular and/or cytoplasmic loops, with correlation times increasing from 10(-)(4) to 10(-)(5) s. Conformational changes in the transmembrane helices were located at helices B, G, and D as viewed from the above-mentioned spectral changes, as well as at 1-(13)C-labeled Val 49 (helix B), 69 (B-C loop), and [3-(13)C]Ala-labeled Ala 126 (D-helix) signals, in addition to the cytoplasmic and extracellular loops. Further, we found that in the M-like state the charged state of Asp 96 at the cytoplasmic side substantially modulated the conformation and dynamics of the extracellular region through long-distance interaction.     

Cerebral metabolism of [1,2-13C2]acetate as detected by in vivo and in vitro 13C NMR

The metabolism of [1,2-13C2]acetate in rat brain was studied by in vivo and in vitro 13C NMR spectroscopy, in particular by taking advantage of the homonuclear 13C-13C spin coupling patterns. Well nourished rats were infused with [1,2-13C2]acetate or [1-13C]acetate in the jugular vein, and the in situ kinetics of 13C labeling during the infusion period was followed by 13C NMR techniques. The in vivo 13C NMR spectra showed signals from (i) the C-1 carbon of [1,2-13C2] acetate or [1-13C]acetate, (ii) 13CO3H-, and (iii) the natural abundance 13C carbons of sufficiently mobile fatty acids. Methanol/HCl/perchloric acid extracts of the brains were prepared and were further analyzed by high resolution 13C NMR. The homonuclear 13C-13C spin coupling patterns after infusion of [1,2-13C2]acetate showed very different isotopomer populations in glutamate, glutamine, and gamma-aminobutyric acid. Analyzing the relative proportions of these isotopomers revealed (i) two different glutamate compartments in the rat brain characterized by the presence and absence, respectively, of glutamine synthase activity, (ii) two different tricarboxylic acid cycles, one preferentially metabolizing [(1,2-13C2]acetate, the other mainly using unlabeled acetyl-coenzyme A, (iii) a hitherto unknown cerebral pyruvate recycling system associated with the tricarboxylic acid cycle, metabolizing primarily unlabeled acetyl-coenzyme A, and (iv) a predominant production of gamma-aminobutyric acid in the glutamate compartment lacking glutamine synthase.     

Stability of the two-dimensional lattice of bacteriorhodopsin reconstituted in partially fluorinated phosphatidylcholine bilayers

This study aims to investigate bacteriorhodopsin (bR) molecules reconstituted in lipid bilayers composed of di(nonafluorotetradecanoyl)-phosphatidylcholine (F4-DMPC), a partially fluorinated analogue of dimyristoyl-phosphatidylcholine (DMPC) to clarify the effects of partially fluorinated hydrophobic chains of lipids on protein's stability. Calorimetry measurements showed that the chain-melting transition of F4-DMPC/bR systems occurs at 3.5 °C, whereas visible circular dichroism (CD) and X-ray diffraction measurements showed that a two-dimensional (2D) hexagonal lattice formed by bR trimers in F4-DMPC bilayers remains intact even above 30 °C, similar to bR in a native purple membrane. Complete dissociation of the trimers into the monomers detected by visible CD almost coincides with the complete melting of 2D lattice observed by X-ray diffraction, in which both take place at around 65 °C (10 °C lower than that for bR in a native purple membrane). However, it is extremely high in comparison with the bR reconstituted in DMPC bilayers in which the dissociation of bR trimer in DMPC bilayers occurs near the chain-melting transition temperature of DMPC bilayers at approximately 18 °C. In order to explore the rationale behind the difference in stability, a further investigation of the detailed structural features of pure F4-DMPC bilayers was performed by analyzing the lamellar diffraction data using simple electron density models. The results suggested that the perfluoroalkyl groups do not exhibit any conformation change even if the chain-melting transition occurs, which is likely to contribute to the stability of the 2D hexagonal lattice formed by the bR trimers.     

Long-distance effects of site-directed mutations on backbone conformation in bacteriorhodopsin from solid state NMR of [1-13C]Val-labeled proteins.

We have recorded 13C cross-polarization-magic angle spinning and dipolar decoupled-magic angle spinning NMR spectra of [1-13C]Val-labeled wild-type bacteriorhodopsin (bR), and the V49A, V199A, T46V, T46V/V49A, D96N, and D85N mutants, in order to study conformational changes of the backbone caused by site-directed mutations along the extracellular surface and the cytoplasmic half channel. On the basis of spectral changes in the V49A and V199A mutants, and upon specific cleavage by chymotrypsin, we assigned the three well-resolved 13C signals observed at 172.93, 172.00, and 171. 11 ppm to [1-13C]Val 69, Val 49, and Val 199, respectively. The local conformations of the backbone at these residues are revealed by the conformation-dependent 13C chemical shifts. We find that at the ambient temperature of these measurements Val 69 is not in a beta-sheet, in spite of previous observations by electron microscopy and x-ray diffraction at cryogenic temperatures, but in a flexible turn structure that undergoes conformational fluctuation. Results with the T46V mutant suggest that there is a long-distance effect on backbone conformation between Thr 46 and Val 49. From the spectra of the D85N and E204Q mutants there also appears to be coupling between Val 49 and Asp 85 and between Asp 85 and Glu 204, respectively. In addition, the T2 measurement indicates conformational interaction between Asp 96 and extracellular surface. The protonation of Asp 85 in the photocycle therefore might induce changes in conformation or dynamics, or both, throughout the protein, from the extracellular surface to the side chain of Asp 96.     

Dynamics and orientation of transmembrane peptide from bacteriorhodopsin incorporated into lipid bilayer as revealed by solid state (31)P and (13)C NMR spectroscopy.

13C and (31)P NMR spectra of a transmembrane peptide, [1-(13)C]Ala(14)-labeled A(6-34), of bacteriorhodopsin incorporated into dimyristoylphosphatidylcholine (DMPC) bilayer were recorded to clarify its dynamics and orientation in the lipid bilayer. This peptide is shown to take an alpha-helical form both in liquid crystalline and gel phases, as viewed from the conformation dependent (13)C chemical shifts. In addition, this peptide undergoes rapid rigid-body rotation about the helical axis at ambient temperature as viewed from the axially symmetric (13)C chemical shift anisotropy, whereas this symmetric anisotropy is changed to an asymmetric pattern at temperatures below 10 degrees C. We further incorporated the peptide into the spontaneously aligned DMPC bilayer to applied magnetic field, induced by dynorphin (dynorphin:DMPC =1:10), a heptadeca-opioid peptide with very high affinity to opioid receptor, in order to gain insight into its orientation in the bilayer. This magnetically aligned system turned out to be persistent even at 0 degrees C as viewed from (31)P NMR spectra of the lipid bilayer, after this peptide was incorporated into this system [A(6-34): dynorphin: DMPC = 4:10:100]. It was found from the (13)C NMR spectra of [1-(13)C]Ala(14) A(6-34) that the helical axis of A(6-34) is oriented parallel to the bilayer normal irrespective of the presence or absence of reorientation motion about the helical axis at a temperature above the lowered gel to liquid crystalline phase transition.     

Partition of malathion in synthetic and native membranes

Partition coefficients of [14C]malathion in model and native membranes are affected by temperature, cholesterol content, and lipid chain length. Partition in egg phosphatidylcholine bilayers decreases linearly with temperature, over a range (10-40 degrees C) at which the lipid is in the liquid-crystalline state. Addition of 50 mol% cholesterol severely decreases partition and practically abolishes the temperature dependence. First-order phase transitions of dimyristoyl-, dipalmitoyl- and distearoylphosphatidylcholines (DMPC, DPPC and DSPC) are accompanied by a sharp increase in malathion partition. Apparently, the insecticide is easily accommodated in bilayers of short-aliphatic-chain lipids, since the partitions were 225, 135 and 48 in DMPC, DPPC and DSPC, respectively, at temperatures 10 Cdeg below the midpoint of their transitions. Partition values in native membranes decrease sequentially as follows: sarcoplasmic reticulum, mitochondria, brain microsomes, myelin and erythrocytes. This dependence parallels the relative content of cholesterol and is similar in liposomes of total extracted lipids, although the absolute partitions showed decreased values.