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.     

Significance of low-frequency local fluctuation motions in the transmembrane B and C α-helices of bacteriorhodopsin,to facilitate efficient proton uptake from the cytoplasmic surface,as revealed by site-directed solid-state <Superscript>13</Superscript>C NMR

¹³C NMR spectra of [1-¹³C]Val- or -Pro-labeled bacteriorhodopsin (bR) and its single or double mutants, including D85N, were recorded at various pH values to reveal conformation and dynamics changes in the transmembrane -helices, in relation to proton release and uptake between bR and the M-like state caused by modified charged states at Asp85 and the Schiff base (SB). It was found that the D85N mutant acquired local fluctuation motion with a frequency of 10⁴ Hz in the transmembrane B -helix, concomitant with deprotonation of SB in the M-like state at pH 10, as manifested from a suppressed ¹³C NMR signal of the [1-¹³C]-labeled Val49 residue. Nevertheless, local dynamics at Pro50 neighboring with Val49 turned out to be unchanged, irrespective of the charged state of SB as viewed from the ¹³C NMR of [1-¹³C]-labeled Pro50. This means that the transmembrane B -helix is able to acquire the fluctuation motion with a frequency of 10⁴ Hz beyond the kink at Pro50 in the cytoplasmic side. Concomitantly, fluctuation motion at the C helix with frequency in the order of 10⁴ Hz was found to be prominent, due to deprotonation of SB at pH 10, as viewed from the ¹³C NMR signal of Pro91. Accordingly, we have proposed here a novel mechanism as to proton uptake and transport based on a dynamic aspect that a transient environmental change from a hydrophobic to hydrophilic nature at Asp96 and SB is responsible for the reduced pK_a value which makes proton uptake efficient, as a result of acquisition of the fluctuation motion at the cytoplasmic side of the transmembrane B and C -helices in the M-like state. Further, it is demonstrated that the presence of a van der Waals contact of Val49 with Lys216 at the SB is essential to trigger this sort of dynamic change, as revealed from the ¹³C NMR data of the D85N/V49A mutant.     

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.     

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.     

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.     

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 C 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 α-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 α-helices of wild-type were almost completely suppressed at the interface between the surface and inner part (up to 8.7 Å deep from the surface) with reference to those of the similarly suppressed peaks by Mn²⁺-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_α 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].     

Redox potentials of the oriented film of the wild-type, the E194Q-, E204Q- and D96N-mutated bacteriorhodopsins

The redox potentials of the oriented films of the wild-type, the E194Q-, E204Q- and D96N-mutated bacteriorhodopsins (bR), prepared by adsorbing purple membrane (PM) sheets or its mutant on a Pt electrode, have been examined. The redox potentials (V) of the wild-type bR were −470 mV for the 13-cis configuration of the retinal Shiff base in bR and −757 mV for the all-trans configuration in H₂O, and −433 mV for the 13-cis configuration and −742 mV for the all-trans configuration in D₂O. The solvent isotope effect (ΔV=V(D₂O)−V(H₂O)), which shifts the redox potential to a higher value, originates from the cooperative rearrangements of the extensively hydrogen-bonded water molecules around the protonated CN part in the retinal Schiff base. The redox potential of bR was much higher for the 13-cis configuration than that for the all-trans configuration. The redox potentials for the E194Q mutant in the extracellular region were −507 mV for the 13-cis configuration and −788 mV for the all-trans configuration; and for the E204Q mutant they were −491 mV for the 13-cis configuration and −769 mV for the all-trans configuration. Replacement of the Glu¹⁹⁴ or Glu²⁰⁴ residues by Gln weakened the electron withdrawing interaction to the protonated CN bond in the retinal Schiff base. The E204 residue is less linked with the hydrogen-bonded network of the proton release pathway compared with E194. The redox potentials of the D96N mutant in the cytoplasmic region were −471 mV for the 13-cis configuration and −760 mV for the all-trans configuration which were virtually the same as those of the wild-type bR, indicating that the D to N point mutation of the 96 residue had no influence on the interaction between the D96 residue and the CN part in the Schiff base under the light-adapted condition. The results suggest that the redox potential of bR is closely correlated to the hydrogen-bonded network spanning from the retinal Schiff base to the extracellular surface of bR in the proton transfer pathway.     

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.     

Conformational heterogeneity of transmembrane residues after the Schiff base reprotonation of bacteriorhodopsin: 15N CPMAS NMR of D85N/T170C membranes

bR, N-like and O-like intermediate states of [15N]methionine-labelled wild type and D85N/T170C bacteriorhodopsin were accumulated in native membranes by controlling the pH of the preparations. 15N cross polarization and magic angle sample spinning (CPMAS) NMR spectroscopy allowed resolution of seven out of nine resonances in the bR-state. It was possible to assign some of the observed resonances by using 13C/15N rotational echo double resonance (REDOR) NMR and Mn2+ quenching as well as D2O exchange, which helps to identify conformational changes after the bacteriorhodopsin Schiff base reprotonation. The significant differences in chemical shifts and linewidths detected for some of the resonances in N- and O-like samples indicate changes in conformation, structural heterogeneity or altered molecular dynamics in parts of the protein.     

Effects of D-glucose upon D-fuctose metabolism in rat hepatocytes: A 13C NMR study

Isolated hepatocytes from fed rats were exposed for 120 min to D-glucose (10 mM) and either D-[1-¹³C]fructose, D-[2-¹³C]fructose or D-[6-¹³C]fructose (also 10 mM) in the presence of D₂O. The identification and quantification of ¹³C-enriched D-fructose and its metabolites (D-glucose, L-lactate, L-alanine) in the incubation medium and the measurement of their deuterated isotopomers indicated, by comparison with a prior study conducted in the absence of exogenous D-glucose, that the major effects of the aldohexose were to increase the recovery of ¹³C-enriched D-fructose, decrease the production of ¹³C-enriched D-glucose, restrict the deuteration of the ¹³C-enriched isotopomers of D-glucose to those generated by cells exposed to D-[2-¹³C]fructose, and to accentuate the lesser deuteration of the C₂ (as compared to C₅) of ¹³C-enriched D-glucose derived from D-[2-¹³C]fructose. The ratio between C2-deuterated and C₂-hydrogenated L-lactate, as well as the relative amounts of the CH₃-, CH₂D-, CHD₂ and CD₃- isotopomers of ¹³C-enriched L-lactate were not significantly different, however, in the absence or presence of exogenous D-glucose. These findings indicate that exogenous D-glucose suppressed the deuteration of the C₁ of D-[1-¹³C]glucose generated by hepatocytes exposed to D-[1-¹³C]fructose or D-[6-¹³C]fructose, as otherwise attributable, in part at least, to gluconeogenesis from fructose-derived [3-¹³C]pyruvate, and apparently favoured the phosphorylation of D-fructose by hexokinase isoenzymes, probably through stimulation of D-fructose phosphorylation by glucokinase.     

Metabolic engineering of a non-allosteric citrate synthase in an Escherichia coli citrate synthase mutant

This study examined the organization of the Krebs tricarboxylic acid (TCA) cycle by metabolic engineering and high-resolution ¹³C NMR. The oxidation of [1,2,3-¹³C]propionate to glutamate via the TCA cycle was measured in wild-type (WT) and a citrate synthase mutant (CS^?) strain of Escherichia coli transformed with allosteric E. coli citrate synthase (ECCS) or non-allosteric pig citrate synthase (PCS). The ¹³C fractional enrichment in glutamate C-2, C-3, and C-4 in ECCS and PCS were similar; although quantitative differences in total citrate synthase activity and total C-4 labeling of glutamate were observed in ECCS and PCS. Allosteric ECCS cells contained 10-fold less total enzyme activity than PCS but only 50% less total labeling in glutamate C-4 and equivalent doubling times. The observed spectra were mathematically fitted using an iterative procedure(TCACALC) and yielded an acetate/succinyl-CoA flux ratio of 10 for both ECCS and PCS, a result that is in agreement with the isotopomer analyses of the ¹³C spectra of cells presented with [3-¹³C] propionate or [2-¹³C]propionate. The results are consistent with the presence of an allosteric citrate synthase in ECCS and a non-allosteric citrate synthase in PCS. The former maintains TCA cycle flux via alternative propionate pathways activated by positive allosteric mechanisms and the latter via elevated enzyme levels.     

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 (T_CH and T_NH) for ¹³C and ¹⁵N nuclei and carbon or nitrogen-resolved, ¹H spin-lattice relaxation times in the rotating flame (¹H T_1ρ) 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 β-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 T_1ρ and cross relaxation times. In addition, breakage of the β-sheet structure in the BC loop was seen in bacterio-opsin (bO) in the absence of 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.     

Fractional <Superscript>13</Superscript>C enrichment of isolated carbons using [1-<Superscript>13</Superscript>C]- or [2-<Superscript>13</Superscript>C]-glucose facilitates the accurate measurement of dynamics at backbone C<Superscript>α</Superscript> and side-chain methyl positions in proteins

A simple labeling approach is presented based on protein expression in [1-¹³C]- or [2-¹³C]-glucose containing media that produces molecules enriched at methyl carbon positions or backbone C^α sites, respectively. All of the methyl groups, with the exception of Thr and Ile(δ1) are produced with isolated ¹³C spins (i.e., no ¹³C–¹³C one bond couplings), facilitating studies of dynamics through the use of spin-spin relaxation experiments without artifacts introduced by evolution due to large homonuclear scalar couplings. Carbon-α sites are labeled without concomitant labeling at C^β positions for 17 of the common 20 amino acids and there are no cases for which ¹³C^α−¹³CO spin pairs are observed. A large number of probes are thus available for the study of protein dynamics with the results obtained complimenting those from more traditional backbone ¹⁵N studies. The utility of the labeling is established by recording ¹³C R _1ρ and CPMG-based experiments on a number of different protein systems.     

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 ¹³C NMR spectra of [3-¹³C]Ala-, [1-¹³C]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-β-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 ¹³C 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 (10⁴ or 10⁵ Hz, respectively). In gel phase lipids, however, up to six distinct ¹³C NMR peaks were well-resolved due to lowered fluctuation frequencies (<10⁵ Hz) for the transmembrane region, the amphipathic α-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.     

Characterization of S-layers from mesophilic bacillaceae and studies on their protective role towards muramidases

High resolution ¹³C NMR combined with chemical analysis were used to study the formation of metabolites from [1-¹³C]-labelled glucose by the salt-tolerant yeast Debaryomyces hansenii after transfer to media containing 8% NaCl. Time course spectroscopy of an aerobic cell suspension showed [1,3-¹³C]glycerol as the predominant end product. Perchloric acid extracts revealed additional less prominent incorporation of label into arabinitol, trehalose, glutamic acid, and alanine. The incorporation into trehalose and arabinitol showed a transient increase after shift to the high salinity medium. It is concluded that glycerol and arabinitol are the major organic solutes in D. hansenii, the production of glycerol being strongly induced by high salinity. Analysis of labelled extracts of D. hansenii after transfer to 8% NaCl media containing [1-¹³C]- or [6-¹³C]glucose, demonstrated that glucose is dissimilated via a combination of the Embden-Meyerhof-Parnas pathway and the pentose phosphate pathway, with the former playing a major role in glycerol formation and the latter in arabinitol production. The almost exclusive labelling of C5 of arabinitol from [6-¹³C]glucose indicates that the pathway to arabinitol proceeds via reduction of ribulose-5-phosphate.Abbreviations used NMR nuclear magnetic resonance - EMP Emden-Meyerhof-Parnas - PP pentose phosphate - GAP glyceraldehyde phosphate - DHAP dihydroxyacetone phosphate - ppm parts per million     

Control of the pump cycle in bacteriorhodopsin: mechanisms elucidated by solid-state NMR of the D85N mutant.

By varying the pH, the D85N mutant of bacteriorhodopsin provides models for several photocycle intermediates of the wild-type protein in which D85 is protonated. At pH 10.8, NMR spectra of [zeta-(15)N]lys-, [12-(13)C]retinal-, and [14,15-(13)C]retinal-labeled D85N samples indicate a deprotonated, 13-cis,15-anti chromophore. On the other hand, at neutral pH, the NMR spectra of D85N show a mixture of protonated Schiff base species similar to that seen in the wild-type protein at low pH, and more complex than the two-state mixture of 13-cis,15-syn, and all-trans isomers found in the dark-adapted wild-type protein. These results lead to several conclusions. First, the reversible titration of order in the D85N chromophore indicates that electrostatic interactions have a major influence on events in the active site. More specifically, whereas a straight chromophore is preferred when the Schiff base and residue 85 are oppositely charged, a bent chromophore is found when both the Schiff base and residue 85 are electrically neutral, even in the dark. Thus a "bent" binding pocket is formed without photoisomerization of the chromophore. On the other hand, when photoisomerization from the straight all-trans,15-anti configuration to the bent 13-cis,15-anti does occur, reciprocal thermodynamic linkage dictates that neutralization of the SB and D85 (by proton transfer from the former to the latter) will result. Second, the similarity between the chromophore chemical shifts in D85N at alkaline pH and those found previously in the M(n) intermediate of the wild-type protein indicate that the latter has a thoroughly relaxed chromophore like the subsequent N intermediate. By comparison, indications of L-like distortion are found for the chromophore of the M(o) state. Thus, chromophore strain is released in the M(o)-->M(n) transition, probably coincident with, and perhaps instrumental to, the change in the connectivity of the Schiff base from the extracellular side of the membrane to the cytoplasmic side. Because the nitrogen chemical shifts of the Schiff base indicate interaction with a hydrogen-bond donor in both M states, it is possible that a water molecule travels with the Schiff base as it switches connectivity. If so, the protein is acting as an inward-driven hydroxyl pump (analogous to halorhodopsin) rather than an outward-driven proton pump. Third, the presence of a significant C [double bond] N syn component in D85N at neutral pH suggests that rapid deprotonation of D85 is necessary at the end of the wild-type photocycle to avoid the generation of nonfunctional C [double bond] N syn species.     

13C-NMR Study of propionate metabolism by sludges from bioreactors treating sulfate and sulfide rich wastewater

Applications of nuclear magnetic resonance (NMR) to study a variety of physiological and biochemical aspects of bacteria with a role in the sulfur cycle are reviewed. Then, a case-study of high resolution¹³ C-NMR spectroscopy on sludges from bioreactors used for treating sulfate and sulfide rich wastewaters is presented.¹³ C-NMR was used to study the effect of sulfate and butyrate on propionate conversion by mesophilic anaerobic (methanogenic and sulfate reducing) granular sludge and microaerobic (sulfide oxidizing) flocculant sludge. In the presence of sulfate, propionate was degraded via the randomising pathway in all sludge types investigated. This was evidenced by scrambling of [3-¹³C]propionate into [2-¹³C]propionate and the formation of acetate equally labeled in the C₁ and C₂ position. In the absence of sulfate, [3-¹³C]propionate scrambled to a lesser extend without being degraded further. Anaerobic sludges converted [2,3-¹³C]propionate partly into the higher fatty acid 2-methyl[2,3-¹³C]butyrate during the simultaneous degradation of [2,3-¹³C]propionate and butyrate. [4,5-¹³C]valerate was also formed in the methanogenic sludges. Up to 10% of the propionate present was converted via these alternative degradation routes. Labeled butyrate was not detected in the incubations, suggesting that reductive carboxylation of propionate does not occur in the sludges.     

Combined effects of an oxidative enzyme and dissolved humic substances on 13C-labelled 2,4-D herbicide as revealed by high-resolution 13C NMR spectroscopy

Phenoxyalkanoic acids are a widely used class of herbicides. This work employed high-resolution ¹³C NMR to study the structural changes induced by humic substances and horseradish perodixase on 2,4-dichorophenoxyacetic acid (2,4-D) ¹³C-labelled in the side chain. NMR spectra showed that humic substances chemically catalyze abiotic splitting of [¹³C]2,4-D into 2,4-dichlorophenol and [¹³C]acetic acid at pH 7 but not at pH 4.7. Peroxidase did not catalyze the oxidative degradation of [¹³C]2,4-D at any pH tested and inhibited the effect of humic substances. Catalytic degradation by humic substances was attributed to free-radical reactions enhanced by the stereochemical contribution of large conformational structures formed by heterogeneous humic molecules at neutral pHs. Inhibition of 2,4-D degradation when humic substances were combined with peroxidase was explained by modification of both chemical and conformational humic structure due to peroxidase-promoted oxidative cross-coupling among humic molecules. Our findings show for the first time that the abiotic degradation of 2,4-D is catalyzed by dissolved humic substances at neutral pH. Journal of Industrial Microbiology & Biotechnology (2001) 26, 70–76. Received 09 February 2000/ Accepted in revised form 22 May 2000     

Catalysis of the retinal subpicosecond photoisomerization process in acid purple bacteriorhodopsin and some bacteriorhodopsin mutants by chloride ions.

The dynamics and the spectra of the excited state of the retinal in bacteriorhodopsin (bR) and its K-intermediate at pH 0 was compared with that of bR and halorhodopsin at pH 6.5. The quantum yield of photoisomerization in acid purple bR was estimated to be at least 0.5. The change of pH from 6.5 to 2 causes a shift of the absorption maximum from 568 to 600 nm (acid blue bR) and decreases the rate of photoisomerization. A further decrease in pH from 2 to 0 shifts the absorption maximum back to 575 nm when HCl is used (acid purple bR). We found that the rate of photoisomerization increases when the pH decreases from 2 to 0. The effect of chloride anions on the dynamics of the retinal photoisomerization of acid bR (pH 2 and 0) and some mutants (D85N, D212N, and R82Q) was also studied. The addition of 1 M HCl (to make acid purple bR, pH 0) or 1 M NaCl to acid blue bR (pH 2) was found to catalyze the rate of the retinal photoisomerization process. Similarly, the addition of 1 M NaCl to the solution of some bR mutants that have a reduced rate of retinal photoisomerization (D85N, D212N, and R82Q) was found to catalyze the rate of their retinal photoisomerization process up to the value observed in wild-type bR. These results are explained by proposing that the bound Cl- compensates for the loss of the negative charges of the COO- groups of Asp85 and/or Asp212 either by neutralization at low pH or by residue replacement in D85N and D212N mutants.