28 research outputs found
Exploring by pulsed EPR the electronic structure of ubisemiquinone bound at the QH site of cytochrome bo3 from Escherichia coli with in vivo 13C-labeled methyl and methoxy substituents
The cytochrome bo(3) ubiquinol oxidase from Escherichia coli resides in the bacterial cytoplasmic membrane and catalyzes the two-electron oxidation of ubiquinol-8 and four-electron reduction of O(2) to water. The one-electron reduced semiquinone forms transiently during the reaction, and the enzyme has been demonstrated to stabilize the semiquinone. The semiquinone is also formed in the D75E mutant, where the mutation has little influence on the catalytic activity, and in the D75H mutant, which is virtually inactive. In this work, wild-type cytochrome bo(3) as well as the D75E and D75H mutant proteins were prepared with ubiquinone-8 (13)C-labeled selectively at the methyl and two methoxy groups. This was accomplished by expressing the proteins in a methionine auxotroph in the presence of l-methionine with the side chain methyl group (13)C-labeled. The (13)C-labeled quinone isolated from cytochrome bo(3) was also used for the generation of model anion radicals in alcohol. Two-dimensional pulsed EPR and ENDOR were used for the study of the (13)C methyl and methoxy hyperfine couplings in the semiquinone generated in the three proteins indicated above and in the model system. The data were used to characterize the transferred unpaired spin densities on the methyl and methoxy substituents and the conformations of the methoxy groups. In the wild type and D75E mutant, the constraints on the configurations of the methoxy side chains are similar, but the D75H mutant appears to have altered methoxy configurations, which could be related to the perturbed electron distribution in the semiquinone and the loss of enzymatic activity
Interactions of Intermediate Semiquinone with Surrounding Protein Residues at the Q<sub>H</sub> Site of Wild-Type and D75H Mutant Cytochrome <i>bo</i><sub>3</sub> from <i>Escherichia coli</i>
Selective <sup>15</sup>N isotope labeling of the cytochrome <i>bo</i><sub>3</sub> ubiquinol oxidase from <i>Escherichia
coli</i> with auxotrophs was used to characterize the hyperfine
couplings with the side-chain nitrogens from residues R71, H98, and
Q101 and peptide nitrogens from residues R71 and H98 around the semiquinone
(SQ) at the high-affinity Q<sub>H</sub> site. The two-dimensional
ESEEM (HYSCORE) data have directly identified N<sub>Δ</sub> of
R71 as an H-bond donor carrying the largest amount of unpaired spin
density. In addition, weaker hyperfine couplings with the side-chain
nitrogens from all residues around the SQ were determined. These hyperfine
couplings reflect a distribution of the unpaired spin density over
the protein in the SQ state of the Q<sub>H</sub> site and the strength
of interaction with different residues. The approach was extended
to the virtually inactive D75H mutant, where the intermediate SQ is
also stabilized. We found that N<sub>Δ</sub> of a histidine
residue, presumably H75, carries most of the unpaired spin density
instead of N<sub>Δ</sub> of R71, as in wild-type <i>bo</i><sub>3</sub>. However, the detailed characterization of the weakly
coupled <sup>15</sup>N atoms from selective labeling of R71 and Q101
in D75H was precluded by overlap of the <sup>15</sup>N lines with
the much stronger âŒ1.6 MHz line from the quadrupole triplet
of the strongly coupled <sup>14</sup>N<sub>Δ</sub> atom of H75.
Therefore, a reverse labeling approach, in which the enzyme was uniformly
labeled except for selected amino acid types, was applied to probe
the contribution of R71 and Q101 to the <sup>15</sup>N signals. Such
labeling has shown only weak coupling with all nitrogens of R71 and
Q101. We utilize density functional theory-based calculations to model
the available information about <sup>1</sup>H, <sup>15</sup>N, and <sup>13</sup>C hyperfine couplings for the Q<sub>H</sub> site and to describe
the proteinâsubstrate interactions in both enzymes. In particular,
we identify the factors responsible for the asymmetric distribution
of the unpaired spin density and ponder the significance of this asymmetry
to the quinoneâs electron transfer function