Carbon-13 nuclear magnetic resonance spectroscopy of high-spin iron(III) prophyrin compounds

¹³C nuclear magnetic resonance spectra have been obtained for variety of high-spin iron(III) porphyrin compounds and corresponding μ-oxo-bridged dimeric species. Large hyperfine shifts and significant line broadening are observed. The monomeric exhibit hyperfine shifts which are downfield with te exception of an upfield shift for the meso-carbon atom. Possible unpaired spin delocalization mechanisms and prospects for observing ¹³C NMR porphyrin resonances in high-spin ferrihemoproteins are discussed. Spectra reported here provide strategy for incorporation of ¹³C labels in hemoproteins either by biosynthetic or chemical means. The vinyl-CH₂ resonances of iron(III) protoporphyrin IX located 260 parts per million downfield from tetramethylsilane are especially attractive from the standpoint of chemical labeling.     

Pressure dependence of side chain <Superscript>13</Superscript>C chemical shifts in model peptides Ac-Gly-Gly-Xxx-Ala-NH<Subscript>2</Subscript>

For evaluating the pressure responses of folded as well as intrinsically unfolded proteins detectable by NMR spectroscopy the availability of data from well-defined model systems is indispensable. In this work we report the pressure dependence of ¹³C chemical shifts of the side chain atoms in the protected tetrapeptides Ac-Gly-Gly-Xxx-Ala-NH₂ (Xxx, one of the 20 canonical amino acids). Contrary to expectation the chemical shifts of a number of nuclei have a nonlinear dependence on pressure in the range from 0.1 to 200 MPa. The size of the polynomial pressure coefficients B ₁ and B ₂ is dependent on the type of atom and amino acid studied. For H^N, N and C^α the first order pressure coefficient B ₁ is also correlated to the chemical shift at atmospheric pressure. The first and second order pressure coefficients of a given type of carbon atom show significant linear correlations suggesting that the NMR observable pressure effects in the different amino acids have at least partly the same physical cause. In line with this observation the magnitude of the second order coefficients of nuclei being direct neighbors in the chemical structure also are weakly correlated. The downfield shifts of the methyl resonances suggest that gauche conformers of the side chains are not preferred with pressure. The valine and leucine methyl groups in the model peptides were assigned using stereospecifically ¹³C enriched amino acids with the pro-R carbons downfield shifted relative to the pro-S carbons.     

Configurational assignments of C-nitromethyl-C-hydroxy branched-chain carbohydrate derivatives by use of a europium shift-reagent in 1 H-N.M.R. spectroscopy

Configurational assignments for the tertiary alcoholic centers of four branched-chain 3-C-nitromethylglycopyranosides, namely, methyl 2-benzamido-4,6-O-benzylidene-2-deoxy-3-C-nitromethyl-α-D-allopyranoside (1), benzyl 2-acetamido-4,6-O-benzylidene-2-deoxy-3-C-nitromethyl-α-D-glucopyranoside (4), benzyl 2-acetamido-4,6-O-benzylidene-2-deoxy-3-C-nitromethyl-α-D-allopyranoside (5), and methyl 4,6-O-benzylidene-3-C-nitromethyl-2-O-p-tolylsulfonyl-α-D-glucopyranoside (8), were made on the basis of the downfield chemical shifts of their identifiable protons per molar equivalent of added Eu(fod)₃, as compared with those of model compounds, of known configuration, having a close structural relationship. In some cases, the assignments were corroborated by the position of the acetyl resonances in the unshifted 60-MHz p.m.r. spectra of the corresponding O-acetyl derivatives.     

Comparison of 13C NMR chemical shifts of 2-aminovaleric acid,L-methionine and DL-selenomethionine and their interactions with aurothiomalate in aqueous solution

The¹³C NMR chemical shifts of DL-selenomethionine were measured and compared with L-methionine and 2-aminovaleric acid in neutral and basic aqueous solutions. The Cγ and Cδ carbons which are directly attached to the sulphur atom of L-methionine experience a shielding effect compared to the Cγ and Cδ of 2-amonivaleric acid resonances. However, shielding effects were observed on Cγ and Cδ resonances when S was substituted by Se, i.e., on going from L-methionine to DL-selenomethionine. The interaction of L-methionine and DL-selenomethionine with aurothiomalate was also studied. The results show that L-methionine does not bind to gold(I) at any pH. However, there is a weak binding observed with DL-selenomethionine in basic aqueous solutions, as seen by ¹³C NMR spectroscopy.     

Myosin light chain kinase binding to plastic

Methionine-81 and/or -8 of the transmembrane sialoglycoprotein, glycophorin A, have been specifically alkylated with ¹³CH₃I to produce the sulfonium ion derivatives [S-[¹³C]methylmethionine-8]glycophorin A and [S-[¹³C]methylmethionine-8 and -81]glycophorin A. ¹³C NMR spectra of these species show that the resonances of the methyl groups of the modified glycophorins occur at 26.1 ppm downfield from Me₄Si. A spin-lattice relaxation time of 0.4 was observed for the ¹³C-enriched methyl resonances of the sulfonium ion derivatives of Met-8 and -81, which corresponds to an effective correlation time of < 2× 10^?10 s. Demethylation of the 2 glycophorin A sulfonium ion species with 2-mercaptoethanol produces native glycophorin A which now has the ε-carbon of the methionine residue(s) 45% isotopically enriched. The ε-carbon of Met-8 was found to occur at 15.7 ppm downfield from Me₄Si whereas the ε-carbon of Met-81 exhibited an unusual chemical shift of 2.0 ppm downfield from Me₄Si. The spin-lattice relaxation time of both resonances was found to be ～0.3 s.     

Human Nucleotide Excision Repair Protein XPA: 1H NMR and CD Solution Studies of a Synthetic Peptide Fragment Corresponding to the Zinc-Binding Domain (101–141)

Abstract

A peptide corresponding to residues 101–141 of the human nucleotide excision repair protein XPA was synthesized with an isoleucine substituted for L138 and its solution structure studied by circular dichroism and homonuclear ¹H NMR spectroscopy. The peptide, (XPA-41), contains a C₄?type zinc-binding motif, C105-(X)₂C108-(X)_l7?C126-(X)₂ C129, which XPA requires for damaged-DNA binding activity. The proton resonances of XPA-41without zinc (apoXPA-41) were assigned using homonuclear TOCSY, NOESY and DQF-COSY data and show the apo-zinc peptide is a random coil. The peptide was folded with the addition of 1.2 equivalents of ZnCl₂ in dilute solution at pH 4.0. Electrospray ionization mass spectroscopy illustrated an increase in the molecular weight of XPA-41 by 65 amu. Circular dichroism spectra of the zinc-folded peptide (zXPA-41) showed the acquisition of elements of secondary structure. Such a conclusion was confirmed with'H NMR data collected at 25°C, pH 6.3. Hα-secondary shifts and NOE patterns indicate that regions V102-C105 and G109-F112 form an anti-parallel β-sheet and residues N128-K137 form a nascent α-helix. Rapid exchange of most amide resonances between S115-C126 prohibited unambiguous assignment of all the proton resonances in this region. However, a 1.19 ppm downfield shift of the H^α resonance of T125 relative to the apo-zinc peptide, together with downfield shifted H^α resonances for the adjacent residues (P124 and L123), suggest a second β-sheet is present in the S115-C126 region. On the basis of structural similarities to GATA-1 (Science 267:438–446), a homology generated structure for zXPA-41 was made, using GATA-1 as the template, which satisfied all the observed NOEs. Using the hybrid homology-NMR based zXPA-41 structure and analogy to GATA-1, models for the role played by the zinc-binding core (101–141) of XPA in DNA damage recognition are proposed.     

Carbon-13 nuclear magnetic resonance studies of polyamino acids: the helix-coil transition of poly-L-lysine

The helix-coil transition of poly-l-lysine hydrochloride ((Lys)_n) in aqueous solution has been studied by ¹³C Fourier-transform nuclear magnetic resonance spectroscopy. As reference compounds dodeca-l-lysine hydrobromide ((Lys)^?₁₂, tri-l-lysine hydrochloride ((Lys)₃), and l-lysine hydrochloride (Lys), have been also studied by the same method. It is found that ¹³C spin-lattice relaxation times t₁ of the carbonyl and the side-chain carbons decrease sharply at pD 10.2 which is the midpoint of the transition from the random-coil to the α-helix. Similarly the T₁ values of the carbonyl groups of (Lys)^?₁₂ decrease at this point in a more moderate way, while no change is observed for those of the side-chain carbons. This is interpreted in terms of the reduced α-helicity involved for (Lys)^?₁₂.The variation of ¹³C chemical shifts with pD for (Lys)_n and (Lys)^?₁₂ show the same trend:downfield shifts at higher pD. Furthermore, nonterminal and C-terminal residues of (Lys)₃ show similar behavior. Thus it is concluded that the ¹³C chemical shift changes are caused mainly by the pD changes and not by the conformational transition. Conversion from α-helix to β-structure by elevation of temperature at pD 11.2 results in narrowing and downfield shifts of the ¹³C resonances of (Lys)_n.     

Constituents of Papaver bracteatum: O-methyl-α-thebaol and 10-n-nonacosanol. Lanthanide-induced chemical shifts in 1H NMR and 13C NMR

Two non-alkaloidal constituents were identified in Papaver bracteatum: O-methyl-α-thebaol and 10-n-nonacosanol. O-Methyl-α-thebaol is a new natural compound. The presence of isothebaine is confirmed. Lanthanide-induced chemical shifts can be used for the assignments of the ₁₃C NMR chemical shifts of isothebaine and phenanthrenes. The use of lanthanide-induced chemical shifts in the identification of methoxyl resonances in ₁H NMR is discussed.     

A NMR experiment for simultaneous correlations of valine and leucine/isoleucine methyls with carbonyl chemical shifts in proteins

A methyl-detected ‘out-and-back’ NMR experiment for obtaining simultaneous correlations of methyl resonances of valine and isoleucine/leucine residues with backbone carbonyl chemical shifts, SIM-HMCM(CGCBCA)CO, is described. The developed pulse-scheme serves the purpose of convenience in recording a single data set for all Ile^δ1, Leu^δ and Val^γ (ILV) methyl positions instead of acquiring two separate spectra selective for valine or leucine/isoleucine residues. The SIM-HMCM(CGCBCA)CO experiment can be used for ILV methyl assignments in moderately sized protein systems (up to ~100 kDa) where the backbone chemical shifts of ¹³C^α, ¹³C_β and ¹³CO are known from prior NMR studies and where some losses in sensitivity can be tolerated for the sake of an overall reduction in NMR acquisition time.     

Carbon-13 NMR studies of C2H5N13C binding to various hemoproteins

The addition of an excess of C₂H₅N¹³C to myoglobin and human adult and fetal hemoglobins, gives three characteristic NMR spectra with new ¹³C resonances respectively at δ = ?10,56 ppm, δ = ?7,03 and ?7,95 ppm and δ = ?6,28 and ?7,95 ppm (CH₃CO₂Na as external standard). These signals correspond to the C₂H₅N¹³C bound to the Fe(II) of the different heme units, according to CO exchange experiments. Characteristic resonances can be assigned to C₂H₅N¹³C bound to α, β and γ subunits. C₂H₅N¹³C appears as a more sensitive probe than ¹³CO for hemoprotein NMR studies.     

Sequential1H-NMR assignments of neurotoxin III from the sea anemoneHeteractis macrodactylus and structural comparison with related toxins

The complete sequence-specific assignment of resonances in the¹H-NMR spectrum of the polypeptide neurotoxin III (Hm III) from the sea anemoneHeteractis macrodactylus is described. Comparison of the chemical shifts and pattern of NOEs for Hm III with those for the related toxin Hp III fromHeteractis paumotensis, which differs only in the substitution of Asn for Tyr at position 11, shows that the overall secondary and tertiary structures are conserved. The largest differences in chemical shift caused by the substitution at position 11 are observed for the NH resonances of Arg-13, Thr-14, Ala-15, Leu-17, and Cys-26. The C^αH resonances influenced most are those of ASP-6, Gly-9, Leu-17, and Glu-42, while the most affected C^βH resonances are from Leu-17, Glu-28, and Lys-32. The absence of long-range NOEs to the aromatic ring of Tyr-11 as well as the lack of significant chemical shift effects on residues outside the loop comprising residues 7–16 confirm that this part of the loop makes no long-lived contacts with the rest of the molecule. The deviations from random coil shifts of Hm III are compared with those of the related anemone toxins Hp II, Hp III, and toxin I fromStichodactyla helianthus (Sh I). The similarity in deviations in chemical shift as a function of sequence position for these four toxins emphasizes the overall structural homology among these polypeptides.     

Global fold of human cannabinoid type 2 receptor probed by solid‐state 13C‐, 15N‐MAS NMR and molecular dynamics simulations

The global fold of human cannabinoid type 2 (CB₂) receptor in the agonist‐bound active state in lipid bilayers was investigated by solid‐state ¹³C‐ and ¹⁵N magic‐angle spinning (MAS) NMR, in combination with chemical‐shift prediction from a structural model of the receptor obtained by microsecond‐long molecular dynamics (MD) simulations. Uniformly ¹³C‐ and ¹⁵N‐labeled CB₂ receptor was expressed in milligram quantities by bacterial fermentation, purified, and functionally reconstituted into liposomes. ¹³C MAS NMR spectra were recorded without sensitivity enhancement for direct comparison of C_α, C_β, and C?O bands of superimposed resonances with predictions from protein structures generated by MD. The experimental NMR spectra matched the calculated spectra reasonably well indicating agreement of the global fold of the protein between experiment and simulations. In particular, the ¹³C chemical shift distribution of C_α resonances was shown to be very sensitive to both the primary amino acid sequence and the secondary structure of CB₂. Thus the shape of the C_α band can be used as an indicator of CB₂ global fold. The prediction from MD simulations indicated that upon receptor activation a rather limited number of amino acid residues, mainly located in the extracellular Loop 2 and the second half of intracellular Loop 3, change their chemical shifts significantly (≥1.5 ppm for carbons and ≥5.0 ppm for nitrogens). Simulated two‐dimensional ¹³C_α(i)? ¹³C?O(i) and ¹³C?O(i)? ¹⁵NH(i + 1) dipolar‐interaction correlation spectra provide guidance for selective amino acid labeling and signal assignment schemes to study the molecular mechanism of activation of CB₂ by solid‐state MAS NMR. Proteins 2014; 82:452–465. © 2013 Wiley Periodicals, Inc.     

13C-nuclear magnetic resonance studies of 85% 13C-enriched amino acids and small peptides: pH effects on the chemical shifts,coupling constants,kinetics of cis-trans isomerisation and conformation aspects

The ¹³C chemical shifts of several 85% ¹³C-enriched amino acids and small peptides were studied as a function of pH. The results show that the chemical shifts of carbon atoms of ionizable groups vary significantly within the zone of their pK. Generally with the pH going from 7 to 1 all the δC are shifted more or less upfield with the exception of the carbonyl group of the second last residue which is shifted slightly downfield. This suggests the formation of an hydrogen bond at acid pH involving in a seven-membered ring the C=O in question and the COOH terminal.The percentage of cis and trans conformers of glycyl-l-proline and glycyl-l-prolylglycine were studied as a function of pH. The trans form is always preponderant whatever the pH. The accessibility of the carbonyl group to protonation of the proline residue strongly influences the cis-trans equilibrium. Thus, with the pH varying from 7 to 1, the trans isomer changes from 61 to 85% for glycyl-l-proline and only from 77 to 80% for glycyl-l-prolylglycine.The proton NMR studies underline the important differences existing between the two molecular forms of glycyl-l-proline. The cis conformation is characterized with regard to the trans form by the non-equivalence of the α-protons of the glycine residue, by a lower pK₁ and by a larger ΔδH_α of the proline residue as a function of pH. These results could suggest an end-to-end interaction in the cis form of the glycyl-l-proline molecule.The ¹³C-¹³C coupling constants were also studied as a function of pH. The results show that J_Co-Cα of a C-terminal residue, varying from 5 to 6 Hz and reflecting the pK of the carboxylate group, is a linear function of δ_Co and δ_Cα as in the case of the amino acids. The total variation of the electron density of those two carbons in an amino acid is approximately 40% weaker than in a C-terminal residue. The charge distribution along the C_α−C_o bond, however, is practically the same in both cases.Finally the ratios of the conversion rate constants of the two isomers cis-trans of glycyl-proline were calculated at different pH values; the relations between the isomer percentages and δ_Co, δ_Cα on the one hand and the J_Co-Cα on the other were established.     

Reduced dimensionality (4,3)D-hnCOCANH experiment: an efficient backbone assignment tool for NMR studies of proteins

Sequence specific resonance assignment of proteins forms the basis for variety of structural and functional proteomics studies by NMR. In this context, an efficient standalone method for rapid assignment of backbone (¹H, ¹⁵N, ¹³C^α and ¹³C′) resonances of proteins has been presented here. Compared to currently available strategies used for the purpose, the method employs only a single reduced dimensionality experiment—(4,3)D-hnCOCANH and exploits the linear combinations of backbone (¹³C^α and ¹³C′) chemical shifts to achieve a dispersion relatively better compared to those of individual chemical shifts (see the text). The resulted increased dispersion of peaks—which is different in sum (CA + CO) and difference (CA ? CO) frequency regions—greatly facilitates the analysis of the spectrum by resolving the problems (associated with routine assignment strategies) arising because of degenerate amide ¹⁵N and backbone ¹³C chemical shifts. Further, the spectrum provides direct distinction between intra- and inter-residue correlations because of their opposite peak signs. The other beneficial feature of the spectrum is that it provides: (a) multiple unidirectional sequential (i→i + 1) ¹⁵N and ¹³C correlations and (b) facile identification of certain specific triplet sequences which serve as check points for mapping the stretches of sequentially connected HSQC cross peaks on to the primary sequence for assigning the resonances sequence specifically. On top of all this, the F ₂–F ₃ planes of the spectrum corresponding to sum (CA + CO) and difference (CA ? CO) chemical shifts enable rapid and unambiguous identification of sequential HSQC peaks through matching their coordinates in these two planes (see the text). Overall, the experiment presented here will serve as an important backbone assignment tool for variety of structural and functional proteomics and drug discovery research programs by NMR involving well behaved small folded proteins (MW < 15 kDa) or a range of intrinsically disordered proteins.      

Accurate measurements of the effects of deuteration at backbone amide positions on the chemical shifts of 15N, 13Cα, 13Cβ, 13CO and 1Hα nuclei in proteins

An approach towards accurate NMR measurements of deuterium isotope effects on the chemical shifts of all backbone nuclei in proteins (¹⁵N, ¹³C_α, ¹³CO, ¹H_α) and ¹³C_β nuclei arising from ¹H-to-D substitutions at amide nitrogen positions is described. Isolation of molecular species with a defined protonation/deuteration pattern at successive backbone nitrogen positions in the polypeptide chain allows quantifying all deuterium isotope shifts of these nuclei from the first to the fourth order. Some of the deuterium isotope shifts measured in the proteins ubiquitin and GB1 can be interpreted in terms of backbone geometry via empirical relationships describing their dependence on (φ; ψ) backbone dihedral angles. Because of their relatively large variability and notable dependence on the protein secondary structure, the two- and three-bond ¹³C_α isotope shifts, ²ΔC_α(N_iD) and ³ΔC_α(N_i+1D), and three-bond ¹³C_β isotope shifts, ³ΔC_β(N_iD), are useful reporters of the local geometry of the protein backbone.     

Effects of carbohydrate-structure changes on induced shifts in differential isotope-shift 13C-N.M.R.

Deuterium-induced, ¹³C-isotope shifts are shown to vary considerably from the initially predicted values calculated for ordinary pyranose and furanose sugars, when minor structural changes are introduced into the carbohydrate ring. Both substitution of C-OH groups or reduction of C-OH to CH₂ permitted the evaluation of γ effects of OD without the contribution of β-OD-induced shifting. The observed γ-shift values for these modified structures were twice as large as those previously noted. This difference is most probably due to favored salvation. Substitution of OH at C-6 led to the predicted loss of differential isotope-shift (d.i.s.) at C-6 because of its isolation from all β and γ OD groups. The ³¹P resonances of d-glucose 6-phosphate show downfield deuterium shifts. Based on d.i.s. values, new ¹³C-shift assignments are proposed for isomaltose and 2-amino-2-deoxy-α-d-glucose. A study of acidic carbohydrates has demonstrated that isotope shifts are somewhat larger for sp²-hybridized carbon atoms whose OH groups are acidic. Relaxation times for sp² carbon atoms isolated from dipolar interaction with protons were very long in D₂O relative to their relaxation time in the H₂O environment.     

Hydrogen-bonding of the ester carbonyls in phosphatidycholine bilayers.

From the behavior of the ¹³C nmr resonances of the carbonyl carbons of phosphatidylcholine vesicles upon the addition of Yb³⁺, Ho³⁺, or Gd³⁺ lanthanide ions it is concluded that of the two peaks the larger downfield one should be assigned to the outside and the smaller upfield one to the inside of the vesicles. The downfield chemical shifts of the α and β carbonyl carbon peaks in vesicles as compared to CCl₄ suggest that the carbonyl oxygens are hydrogen bonded to water in the vesicles. The β-carbonyl oxygen appears more exposed to water in vesicles. Addition of cholesterol to the vesicles produces little chemical shift change suggesting substitution of cholesterol for water in hydrogen bonding to a carbonyl oxygen; the α-carbonyl oxygen is suggested as the more likely acceptor.     

The coordination chemistry of bidentate tellurium ligands. I. Complexes of palladium,platinum, and mercury with large chelate rings

Complexes formed from the reaction of palladium(II) and platinum(II) halides with (p-EtO·C₆H₄)Te(CH₂)_nTe(C₆H₄OEt-p) (Lⁿ, n = 6, 7, 8, 9, 10) are reported together with data for some mercury(II) complexes, [HgLⁿCl₂] which are used for comparative purposes. The compounds [MLⁿX₂] (M  Pd, Pt; n = 7, 8 (Pt only), 9, 10; X  Cl, Br) have molecular weights in molten naphthalene which fluctuate about the monomer value. [ML⁶X₂] (M  Pd, Pt; X  Cl, Br) are totally insoluble and are believed to be polymeric. The palladium(II) complexes have trans dichloro groups whereas the platinum compounds show cis dichloro groups in the solid state.¹³C NMR spectra are valuable to confirm the coordination of the ligand; the methylene resonance of the TeCH₂ group undergoes a 19–20 ppm downfield shift on coordination. ¹²⁵Te NMR spectra of the Pd(II) and Pt(II) complexes show two broad resonances the chemical shifts of which imply the presence of cis and trans isomers in CDCl₃ solution. A more detailed variable temperature high field study of [PtL⁸Cl₂] (¹²⁵Te and ¹⁹⁵Pt NMR) reveals a complex solution chemistry involving at least two cis and two trans species. The temperature range over which the solution is stable (−10 to 70 °C) is insufficient to allow a totally unambiguous interpretation but a model based on monomer ⇍ dimer equilibria provides a self consistent interpretation.     

NMR and NQR parameters of the SiC-doped on the (4,4) <Emphasis Type="Italic">armchair</Emphasis> single-walled BPNT: a computational study

The structural properties, NMR and NQR parameters in the pristine and silicon carbide (SiC) doped boron phosphide nanotubes (BPNTs) were calculated using DFT methods (BLYP, B3LYP/6-31G*) in order to evaluate the influence of SiC-doped on the (4,4) armchair BPNTs. Nuclear magnetic resonance (NMR) parameters including isotropic (CS^I) and anisotropic (CS^A) chemical shielding parameters for the sites of various ¹³C, ²⁹Si, ¹¹B, and ³¹P atoms and quadrupole coupling constant (C _Q ), and asymmetry parameter (η _Q ) at the sites of various ¹¹B nuclei were calculated in pristine and SiC- doped (4,4) armchair boron phosphide nanotubes models. The calculations indicated that doping of ¹¹B and ³¹P atoms by C and Si atoms had a more significant influence on the calculated NMR and NQR parameters than did doping of the B and P atoms by Si and C atoms. In comparison with the pristine model, the SiC- doping in Si_PC_B model of the (4,4) armchair BPNTs reduces the energy gaps of the nanotubes and increases their electrical conductance. The NMR results showed that the B and P atoms which are directly bonded to the C atoms in the SiC-doped BPNTs have significant changes in the NMR parameters with respect to the B and P atoms which are directly bonded to the Si atoms in the SiC-doped BPNTs. The NQR results showed that in BPNTs, the B atoms at the edges of nanotubes play dominant roles in determining the electronic behaviors of BPNTs. Also, the NMR and NQR results detect that the Fig. 1b (Si_PC_B) model is a more reactive material than the pristine and the Fig. 1a (Si_BC_p) models of the (4,4) armchair BPNTs.     

1H NMR studies of a two-iron: two-sulfur ferredoxin from halobacterium of the dead sea

Ferredoxin isolated from Halobacterium of the Dead Sea (HFd) was found to be stable and retain its conformation in 4–0.5 M salt solutions. Reconstitution of the denatured protein to the oxidized form in ²H₂O indicated that the resonances shifted to the 8–10 ppm region, which include 18 protons, are nonexchangeable -NH protons. The C₂H and C₄H resonances of His-119 were assigned in both oxidized and reduced HFd. pH titration curves of these resonances yielded a pK_a for this His of 6.57 ± 0.1 and 6.65 ± 0.1 in oxidized and reduced HFd, respectively. pH titration curves, T₁ relaxation times, and the temperature dependence of the chemical shift were obtained for resonances between 6 and 10 ppm of oxidized HFd. In oxidized HFd a paramagnetically shifted resonance was observed at 15 ppm with 1 H intensity, and an anti-Curie temperature dependence. In reduced HFd eight resonances each with 1 H intensity were shifted downfield by 10–50 ppm and one resonance with 1 H intensity was shifted upfield to ?6.8 ppm. Four of these resonances exhibited an anti-Curie temperature dependence, two exhibited a moderate Curie dependence, and three were temperature independent.