SP-B(CTERM) is a cationic amphipathic helical peptide and functional fragment composed of residues 63 to 78 of surfactant protein B (SP-B). Static oriented and magic angle spinning solid state NMR, along with molecular dynamics simulation was used to investigate its structure, orientation, and depth in lipid bilayers of several compositions, namely POPC, DPPC, DPPC/POPC/POPG, and bovine lung surfactant extract (BLES). In all lipid environments the peptide was oriented parallel to the membrane surface. While maintaining this approximately planar orientation, SP-B(CTERM) exhibited a flexible topology controlled by subtle variations in lipid composition. SP-B(CTERM)-induced lipid realignment and/or conformational changes at the level of the head group were observed using (31)P solid-state NMR spectroscopy. Measurements of the depth of SP-B(CTERM) indicated the peptide center positions ~8Å more deeply than the phosphate headgroups, a topology that may allow the peptide to promote functional lipid structures without causing micellization upon compression.
Superoxide dismutases (SODs) protect cells against oxidative stress by disproportionating O 2 − to H 2 O 2 and O 2 . The recent finding of a nickel-containing SOD (Ni-SOD) has widened the diversity of SODs in terms of metal contents and SOD catalytic mechanisms. The coordination and geometrical structure of the metal site and the related electronic structure are the keys to understanding the dismutase mechanism of the enzyme. We performed Q-band 14 N, 1/2 H continuous wave (CW) and pulsed electron–nuclear double resonance (ENDOR) and X-band 14 N electron spin echo envelope modulation (ESEEM) on the resting-state Ni-SOD extracted from Streptomyces seoulensis . In-depth analysis of the data obtained from the multifrequency advanced electron paramagnetic resonance techniques detailed the electronic structure of the active site of Ni-SOD. The analysis of the field-dependent Q-band 14 N CW ENDOR yielded the nuclear hyperfine and quadrupole coupling tensors of the axial N δ of the His-1 imidazole ligand. The tensors are coaxial with the g -tensor frame, implying the g -tensor direction is modulated by the imidazole plane. X-band 14 N ESEEM characterized the hyperfine coupling of N ε of His-1 imidazole. The nuclear quadrupole coupling constant of the nitrogen suggests that the hydrogen-bonding between N ε –H and O Glu-17 present for the reduced-state Ni-SOD is weakened or broken upon oxidizing the enzyme. Q-band 1 H CW ENDOR and pulsed 2 H Mims ENDOR showed a strong hyperfine coupling to the protons(s) of the equatorially coordinated His-1 amine and a weak hyperfine coupling to either the proton(s) of a water in the pocket at the side opposite the axial N δ or the proton of a water hydrogen-bonded to the equatorial thiolate ligand.
Nitrogenase reduces dinitrogen (N2) by six electrons and six protons at an active-site metallocluster called FeMo cofactor, to yield two ammonia molecules. Insights into the mechanism of substrate reduction by nitrogenase have come from recent successes in trapping and characterizing intermediates generated during the reduction of protons as well as nitrogenous and alkyne substrates by MoFe proteins with amino acid substitutions. Here, we describe an intermediate generated at a high concentration during reduction of the natural nitrogenase substrate, N2, by wild-type MoFe protein, providing evidence that it contains N2 bound to the active-site FeMo cofactor. When MoFe protein was frozen at 77 K during steady-state turnover with N2, the S = 3/2 EPR signal (g = [4.3, 3.64, 2.00]) arising from the resting state of FeMo cofactor was observed to convert to a rhombic, S = 1/2, signal (g = [2.08, 1.99, 1.97]). The intensity of the N2-dependent EPR signal increased with increasing N2 partial pressure, reaching a maximum intensity of approximately 20% of that of the original FeMo cofactor signal at > or = 0.2 atm N2. An almost complete loss of resting FeMo cofactor signal in this sample implies that the remainder of the enzyme has been reduced to an EPR-silent intermediate state. The N2-dependent EPR signal intensity also varied with the ratio of Fe protein to MoFe protein (electron flux through nitrogenase), with the maximum signal intensity observed with a ratio of 2:1 (1:1 Fe protein:FeMo cofactor) or higher. The pH optimum for the signal was 7.1. The N2-dependent EPR signal intensity exhibited a linear dependence on the square root of the EPR microwave power in contrast to the nonlinear response of signal intensity observed for hydrazine-, diazene-, and methyldiazene-trapped states. 15N ENDOR spectroscopic analysis of MoFe protein captured during turnover with 15N2 revealed a 15N nuclear spin coupled to the FeMo cofactor with a hyperfine tensor A = [0.9, 1.4, 0.45] MHz establishing that an N2-derived species was trapped on the FeMo cofactor. The observation of a single type of 15N-coupled nucleus from the field dependence, along with the absence of an associated exchangeable 1H ENDOR signal, is consistent with an N2 molecule bound end-on to the FeMo cofactor.
The lung surfactant protein B (SP-B) is essential for life and plays a critical role in reducing surface tension in the lungs during breathing. An amphipathic helical fragment of SP-B composed of the 16 C-terminal residues, termed SP-BCTERM or SP-B63-78, has a charge of +3 and retains significant bioactivity compared to native SP-B. We have used 31P-, 2H-, 13C-, and 15N- solid state NMR to investigate the insertion of SP-BCTERM into lipid bilayers composed of model lipids, as well as bovine lung extracted surfactant (BLES). When the external magnetic field is parallel to the normal of the oriented lipid bilayers, the 15N chemical shift of the peptide backbone is at ∼ 98 ppm, which corresponds to a helical axis alignment of approximately 70° relative to the lipid bilayer normal. The depth of peptide insertion in vesicles was investigated by 13C{31P} REDOR, as well as by measuring the 13C relaxation time in the absence and presence of the paramagnetic probe Mn2+.
The structure of Peptide T was determined by solution NMR spectroscopy, under strong structure‐inducing conditions: 40% hexafluoro‐2‐propanol aqueous solution at 5 °C. Under these conditions it was possible to detect medium‐range NOEs for the first time for this peptide. This allowed a much better‐defined structure to be determined for Peptide T in comparison with earlier NMR and computational studies. Peptide structures consistent with the experimental restraints were generated using a restrained MD simulation with a full empirical force field. Residues 4–8 of Peptide T take on a well‐defined structure with a heavy atom RMSD of 0.78 Å. The structure is stabilized by hydrogen bonding to side‐chain oxygen atoms of Thr 4 and Thr 8, as well as backbone hydrogen bonding between residues 5 and 7 that forms this region into a classic γ‐turn. Copyright © 2009 European Peptide Society and John Wiley & Sons, Ltd.
A high-resolution (1.16 A) X-ray structure of the nitrogenase molybdenum-iron (MoFe) protein revealed electron density from a single N, O, or C atom (denoted X) inside the central iron prismane ([6Fe]) of the [MoFe7S9:homocitrate] FeMo-cofactor (FeMo-co). We here extend earlier efforts to determine the identity of X through detailed tests of whether X = N or C by interlocking and mutually supportive 9 GHz electron spin echo envelope modulation (ESEEM) and 35 GHz electron-nuclear double resonance (ENDOR) measurements on 14/15N and 12/13C isotopomers of FeMo-co in three environments: (i) incorporated into the native MoFe protein environment; (ii) extracted into N-methyl formamide solution; and (iii) incorporated into the NifX protein, which acts as a chaperone during FeMo-co biosynthesis. These measurements provide powerful evidence that X not equal N/C, unless X in effect is magnetically decoupled from the S = 3/2 electron spin system of resting FeMo-co. They reveal no signals from FeMo-co in any of the three environments that can be assigned to X from either 14/15N or 13C: If X were either element, its maximum observed hyperfine coupling at all fields of measurement is estimated to be A(14/15NX) < 0.07/0.1 MHz, A(13CX) < 0.1 MHz, corresponding to intrinsic couplings of about half these values. In parallel, we have explicitly calculated the hyperfine tensors for X = 14/15N/13C/17O, nuclear quadrupole coupling constant e2qQ for X = 14N, and hyperfine constants for the Fe sites of S = 3/2 FeMo-co using density functional theory (DFT) in conjunction with the broken-symmetry (BS) approach for spin coupling. If X = C/N, then the decoupling required by experiment strongly supports the "BS7" spin coupling of the FeMo-co iron sites, in which a small X hyperfine coupling is the result of a precise balance of spin density contributions from three spin-up and three spin-down (3 upward arrow:3 downward arrow) iron atoms of the [6Fe] prismane "waist" of FeMo-co; this would rule out the "BS6" assignment (4 upward arrow:2 downward arrow for [6Fe]) suggested in earlier calculations. However, even with the BS7 scheme, the hyperfine couplings that would be observed for X near g2 are sufficiently large that they should have been detected: we suggest that the experimental results are compatible with X = N only if aiso(14/15NX) < 0.03-0.07/0.05-0.1 MHz and aiso(13CX) < 0.05-0.1 MHz, compared with calculated values of aiso(14/15NX) = 0.3/0.4 MHz and aiso(13CX) = 1 MHz. However, the DFT uncertainties are large enough that the very small hyperfine couplings required by experiment do not necessarily rule out X = N/C.
Nitrogenase catalyzes the sequential addition of six electrons and six protons to a N2 that is bound to the active site metal cluster FeMo-cofactor, yielding two ammonia molecules. The nature of the intermediates bound to FeMo-cofactor along this reduction pathway remains unknown, although it has been suggested that there are intermediates at the level of reduction of diazene (HN=NH, also called diimide) and hydrazine (H2N-NH2). Through in situ generation of diazene during nitrogenase turnover, we show that diazene is a substrate for the wild-type nitrogenase and is reduced to NH3. Diazene reduction, like N2 reduction, is inhibited by H2. This contrasts with the absence of H2 inhibition when nitrogenase reduces hydrazine. These results support the existence of an intermediate early in the N2 reduction pathway at the level of reduction of diazene. Freeze-quenching a MoFe protein variant with alpha-195His substituted by Gln and alpha-70Val substituted by Ala during steady-state turnover with diazene resulted in conversion of the S = 3/2 resting state FeMo-cofactor to a novel S = 1/2 state with g1 = 2.09, g2 = 2.01, and g3 approximately 1.98. 15N- and 1H-ENDOR establish that this state consists of a diazene-derived [-NHx] moiety bound to FeMo-cofactor. This moiety is indistinguishable from the hydrazine-derived [-NHx] moiety bound to FeMo-cofactor when the same MoFe protein is trapped during turnover with hydrazine. These observations suggest that diazene joins the normal N2-reduction pathway, and that the diazene- and hydrazine-trapped turnover states represent the same intermediate in the normal reduction of N2 by nitrogenase. Implications of these findings for the mechanism of N2 reduction by nitrogenase are discussed.
Superoxide reductase (SOR) and P450 enzymes contain similar [Fe(N)4(SCys)] active sites and, although they catalyze very different reactions, are proposed to involve analogous low-spin (hydro)peroxo-Fe(III) intermediates in their respective mechanisms that can be modeled by cyanide binding. The equatorial FeN4 ligation by four histidine ligands in CN-SOR and the heme in CN-P450cam is directly compared by 14N ENDOR, while the axial Fe-CN and Fe-S bonding is probed by 13C ENDOR of the cyanide ligand and 1Hbeta ENDOR measurements to determine the spin density delocalization onto the cysteine sulfur. There are small, but notable, differences in the bonding between Fe(III) and its ligands in the two enzymes. The ENDOR measurements are complemented by DFT computations that support the semiempirical equation used to compute spin densities on metal-coordinated cysteinyl and shed light on bonding changes as the Fe-C-N linkage bends. They further indicate that H bonds to the cysteinyl thiolate sulfur ligand reduce the spin density on the sulfur in both active sites to a degree that exceeds the difference induced by the alternative sets of "in-plane" nitrogen ligands.
Methyldiazene (HN N CH 3 ) isotopomers labeled with 15 N at the terminal or internal nitrogens or with 13 C or 2 H were used as substrates for the nitrogenase α-195 Gln -substituted MoFe protein. Freeze quenching under turnover traps an S = ½ state that has been characterized by EPR and 1 H-, 15 N-, and 13 C-electron nuclear double resonance spectroscopies. These studies disclosed the following: ( i ) a methyldiazene-derived species is bound to the active-site FeMo cofactor; ( ii ) this species binds through an [-NH x ] fragment whose N derives from the methyldiazene terminal N; and ( iii ) the internal N from methyldiazene probably does not bind to FeMo cofactor. These results constrain possible mechanisms for reduction of methyldiazene. In the Chatt–Schrock mechanism for N 2 reduction, H atoms sequentially add to the distal N before N-N bond cleavage ( d -mechanism). In a d -mechanism for methyldiazene reduction, a bound [-NH x ] fragment only occurs after reduction by three electrons, which leads to N-N bond cleavage and the release of the first NH 3 . Thus, the appearance of bound [-NH x ] is compatible with the d -mechanism only if it represents a late stage in the reduction process. In contrast are mechanisms where H atoms add alternately to distal and proximal nitrogens before N-N cleavage ( a -mechanism) and release of the first NH 3 after reduction by five electrons. An [-NH x ] fragment would be bound at every stage of methyldiazene reduction in an a -mechanism. Although current information does not rule out the d -mechanism, the a -mechanism is more attractive because proton delivery to substrate has been specifically compromised in α-195 Gln -substituted MoFe protein.
We extend earlier studies of the effects of relaxation on the intensities of pulsed ENDOR signals by introducing a Davies/Hahn (D/H) pulsed ENDOR multi-sequence that corresponds to a series of Davies sequences with the preparation pulse 'turned off'. In this pulse train, the Hahn [pi/2, pi] detection pulse pair of sequence n-1 both generates the echo detected for that sequence and acts as the preparation portion of sequence n, in effect replacing the pi preparation pulse of the Davies sequence. We show both theoretically, through a master-equation approach, and with both (1)H(I=1/2) and (14)N(I=1) ENDOR experiments on the non-heme Fe enzymes, superoxide reductase (SOR) (S=1/2) and AntDO (S=3/2), that under conditions of high electron-spin polarization (high microwave frequency/low temperature) the D/H multi-sequence allows simplification of ENDOR spectra by suppression of nuclear transitions associated with the m(S)=+1/2 (alpha) manifold. As such suppression depends on the sign of A, it allows determination of this sign. The suppression as a function of the time between individual sequences is found to exhibit behaviors that can be classified into three regimes of the ratio of cross-relaxation to spin-lattice relaxation rates: strong cross-relaxation (X-case); comparable rates (XL); negligible cross relaxation (L). Interestingly, the ENDOR behavior of the S=1/2 SOR center indicates it is an L case, while the S=3/2 AntDO is an L case. Overall, the D/H protocol appears to be a robust and general tool for using relaxation effects to manipulate ENDOR spectra.