New transients in the electron-transfer dynamics of photolyzed mixed-valence CO-cytochrome c oxidase

Cytochrome c oxidase: chemistry of a molecular machine

The plethora of proposed chemical models attempting to explain the proton pumping reactions catalyzed by the CcO complex, especially the number of recent models, makes it clear that the problem is far from solved. Although we have not discussed all of the models proposed to date, we have described some of the more detailed models in order to illustrate the theoretical concepts introduced at the beginning of this section on proton pumping as well as to illustrate the rich possibilities available for effecting proton pumping. It is clear that proton pumping is effected by conformational changes induced by oxidation/reduction of the various redox centers in the CcO complex. It is for this reason that the CcO complex is called a redox-linked proton pump. The conformational changes of the proton pump cycle are usually envisioned to be some sort of ligand-exchange reaction arising from unstable geometries upon oxidation/reduction of the various redox centers. However, simple geometrical rearrangements, as in the Babcock and Mitchell models are also possible. In any model, however, hydrogen bonds must be broken and reformed due to conformational changes that result from oxidation/reduction of the linkage site during enzyme turnover. Perhaps the most important point emphasized in this discussion, however, is the fact that proton pumping is a directed process and it is electron and proton gating mechanisms that drive the proton pump cycle in the forward direction. Since many of the models discussed above lack effective electron and/or proton gating, it is clear that the major difficulty in developing a viable chemical model is not formulating a cyclic set of protein conformational changes effecting proton pumping (redox linkage) but rather constructing the model with a set of physical constraints so that the proposed cycle proceeds efficiently as postulated. In our discussion of these models, we have not been too concerned about which electron of the catalytic cycle was entering the site of linkage, but merely whether an ET to the binuclear center played a role. However, redox linkage only occurs if ET to the activated binuclear center is coupled to the proton pump. Since all of the models of proton pumping presented here, with the exception of the Rousseau expanded model and the Wikström model, have a maximum stoichiometry of 1 H+/e-, they inadequately explain the 2 H+/e- ratio for the third and fourth electrons of the dioxygen reduction cycle (see Section V.B). One way of interpreting this shortfall of protons is that the remaining protons are pumped by an as yet undefined indirectly coupled mechanism. In this scenario, the site of linkage could be coupled to the pumping of one proton in a direct fashion and one proton in an indirect fashion for a given electron. For a long time, it was assumed that at least some elements of such an indirect mechanism reside in subunit III. While recent evidence argues against the involvement of subunit III in the proton pump, subunit III may still participate in a regulatory and/or structural capacity (Section II.E). Attention has now focused on subunits I and II in the search for residues intimately involved in the proton pump mechanism and/or as part of a proton channel. In particular, the role of some of the highly conserved residues of helix VIII of subunit I are currently being studied by site directed mutagenesis. In our opinion, any model that invokes heme alpha 3 or CuB as the site of linkage must propose a very effective means by which the presumedly fast uncoupling ET to the dioxygen intermediates is prevented. It is difficult to imagine that ET over the short distance from heme alpha 3 or CuB to the dioxygen intermediate requires more than 1 ns. In addition, we expect the conformational changes of the proton pump to require much more than 1 ns (see Section V.B).

Photobiomodulation directly benefits primary neurons functionally inactivated by toxins: role of cytochrome c oxidase

Far red and near infrared (NIR) light promotes wound healing, but the mechanism is poorly understood. Our previous studies using 670 nm light-emitting diode (LED) arrays suggest that cytochrome c oxidase, a photoacceptor in the NIR range, plays an important role in therapeutic photobiomodulation. If this is true, then an irreversible inhibitor of cytochrome c oxidase, potassium cyanide (KCN), should compete with LED and reduce its beneficial effects. This hypothesis was tested on primary cultured neurons. LED treatment partially restored enzyme activity blocked by 10-100 microm KCN. It significantly reduced neuronal cell death induced by 300 microm KCN from 83.6 to 43.5%. However, at 1-100 mm KCN, the protective effects of LED decreased, and neuronal deaths increased. LED significantly restored neuronal ATP content only at 10 microm KCN but not at higher concentrations of KCN tested. Pretreatment with LED enhanced efficacy of LED during exposure to 10 or 100 microm KCN but did not restore enzyme activity to control levels. In contrast, LED was able to completely reverse the detrimental effect of tetrodotoxin, which only indirectly down-regulated enzyme levels. Among the wavelengths tested (670, 728, 770, 830, and 880 nm), the most effective ones (830 nm, 670 nm) paralleled the NIR absorption spectrum of oxidized cytochrome c oxidase, whereas the least effective wavelength, 728 nm, did not. The results are consistent with our hypothesis that the mechanism of photobiomodulation involves the up-regulation of cytochrome c oxidase, leading to increased energy metabolism in neurons functionally inactivated by toxins.

Time-resolved optical absorption studies of cytochrome oxidase dynamics

Time-resolved spectroscopic studies in our laboratory of bovine heart cytochrome c oxidase dynamics are summarized. Intramolecular electron transfer was investigated upon photolysis of CO from the mixed-valence enzyme, by pulse radiolysis, and upon light-induced electron injection into the cytochrome c/cytochrome oxidase complex from a novel photoactivatable dye. The reduction of dioxygen to water was monitored by a gated multichannel analyzer using the CO flow-flash method or a synthetic caged dioxygen carrier. The pH dependence of the intermediate spectra suggests a mechanism of dioxygen reduction more complex than the conventional unidirectional sequential scheme. A branched model is proposed, in which one branch produces the P form and the other branch the F form. The rate of exchange between the two branches is pH-dependent. A cross-linked histidine-phenol was synthesized and characterized to explore the role of the cross-linked His-Tyr cofactor in the function of the enzyme. Time-resolved optical absorption spectra, EPR and FTIR spectra of the compound generated after UV photolysis indicated the presence of a radical residing primarily on the phenoxyl ring. The relevance of these results to cytochrome oxidase function is discussed.

Kinetics of intramolecular electron transfer in cytochrome bo3 from Escherichia coli

We have examined the temperature dependence of the intramolecular electron transfer (ET) between heme b and heme o(3) in CO-mixed valence cytochrome bo(3) (Cbo) from Escherichia coli. Upon photolysis of CO-mixed valence Cbo rapid ET occurs between heme o(3) and heme b with a rate constant of 2.2 x 10(5) s(-1) at room temperature. The corresponding rate of CO recombination is found to be 86 s(-1). From Eyring plots the activation energies for these two processes are found to be 3.4 kcal/mol and 6.7 kcal/mol for the ligand binding and ET reactions, respectively. Using variants of the Marcus equation the reorganization energy (lambda), electronic coupling factor (H(AB)), and the ET distance were found to be 1.4 +/- 0.2 eV, (2 +/- 1) x 10(-3) eV, and 9 +/- 1 A, respectively. These values are quite distinct from the analogous values previously obtained for bovine heart cytochrome c oxidase (CcO) (0.76 eV, 9.9 x 10(-5) eV, 13.2 A). The differences in mechanisms/pathways for heme b/heme o(3) and heme a/heme a(3) ET suggested by the Marcus parameters can be attributed to structural changes at the Cu(B) site upon change in oxidation state as well as differences in electronic coupling pathways between Heme b and heme o(3).

Activation volumes for intramolecular electron transfer in Escherichia coli cytochrome bo(3)

In this report we describe the activation volumes associated with the heme-heme electron transfer (ET) and CO rebinding to the binuclear center subsequent to photolysis of the CO-mixed-valence derivative of Escherichia coli cytochrome bo(3) (Cbo). The activation volumes associated with the heme-heme ET (k=1.2 x 10(5) s(-1)), and CO rebinding (k=57 s(-1)) are found to be +27.4 ml/mol and -2.6 ml/mol, respectively. The activation volume associated with the rebinding of CO is consistent with previous Cu X-ray absorption studies of Cbo where a structural change was observed at the Cu(B) site (loss of a histidine ligand) due to a change in the redox state of the binuclear center. In addition, the volume of activation for the heme-heme ET was found to be quite distinct from the activation volumes obtained for heme-heme ET in bovine heart Cytochrome c oxidase. Differences in mechanisms/pathways for heme b/heme o(3) and heme a/heme a(3) ET are suggested based on the associated activation volumes and previously obtained Marcus parameters.

Observation of the equilibrium CuB-CO complex and functional implications of the transient heme a3 propionates in cytochrome ba3-CO from Thermus thermophilus. Fourier transform infrared (FTIR) and time-resolved step-scan FTIR studies

We report the first evidence for the existence of the equilibrium Cu(B)1+-CO species of CO-bound reduced cytochrome ba(3) from Thermus thermophilus at room temperature. The frequency of the C-O stretching mode of Cu(B)1+-CO is located at 2053 cm(-1) and remains unchanged in H(2)O/D(2)O exchanges and, between pD 5.5 and 9.7, indicating that the chemical environment does not alter the protonation state of the Cu(B) histidine ligands. The data and conclusions reported here are in contrast to the changes in protonation state of Cu(B)-His-290, reported recently (Das, T. K., Tomson, F. K., Gennis, R. B., Gordon, M., and Rousseau, D. L. (2001) Biophys. J. 80, 2039-2045 and Das, T. P., Gomes, C. M., Teixeira, M., and Rousseau, D. L. (1999) Proc. Natl. Acad. Sci. U. S. A. 96, 9591-9596). The time-resolved step-scan FTIR difference spectra indicate that the rate of decay of the transient Cu(B)1+-CO complex is 34.5 s(-1) and rebinding to heme a(3) occurs with k(2) = 28.6 s(-1). The rate of decay of the transient Cu(B)1+-CO complex displays a similar time constant as the absorption changes at 1694(+)/1706(-), attributed to perturbation of the heme a(3) propionates (COOH). The nu(C-O) of the transient Cu(B)1+-CO species is the same as that of the equilibrium Cu(B)1+-CO species and remains unchanged in the pD range 5.5-9.7 indicating that no structural change takes place at Cu(B) between these states. The implications of these results with respect to proton pathways in heme-copper oxidases are discussed.

P(M) and P(R) forms of cytochrome c oxidase have different spectral properties

The reaction between bovine heart cytochrome c oxidase and dioxygen was monitored at room temperature in the visible and Soret regions following photolysis of the mixed-valence CO-bound enzyme. Time-resolved optical absorption difference spectra were collected between 50 ns and 1.7 ms by a gated multichannel analyzer. Singular value decomposition and global exponential fitting resolved three processes with apparent lifetimes of 2.2+/-0.5, 17+/-4 and 160+/-30 micros. The spectra of the intermediates were extracted based on a sequential kinetic mechanism and compared to the corresponding intermediate spectra observed during the reaction of the fully reduced enzyme with dioxygen. The first process is associated with a conformational change at heme a(3) upon dissociation of CO from Cu(B)(+) and concomitant back-electron transfer from heme a(3) to heme a. This is followed by O(2) binding to heme a(3) forming compound A (A(M)), with a spectrum identical to that observed upon O(2) binding to heme a(3) in the fully reduced enzyme (A(R)). Intermediate A(M) decays into P(M), the spectrum of which is equivalent to that of the 607 nm form, generated upon addition of H(2)O(2) to the oxidized enzyme at alkaline pH values (P(H)). However, the spectrum of P(M) is significantly different from the corresponding intermediate observed upon the reaction of dioxygen with the fully reduced enzyme (P(R)). The spectral differences between P(M) and P(R) may arise from the different number of redox equivalents at the binuclear site, with a tyrosine radical in the P(M) state, and tyrosine or tyrosinate in P(R), or may be the consequence of a more complex reaction mechanism in the case of the fully reduced enzyme.

Time-resolved optical absorption studies of intramolecular electron transfer in cytochrome c oxidase

Intramolecular electron transfer and conformational changes in cytochrome c oxidase were studied at room temperature following the photodissociation of CO bound to mixed-valence enzyme (cytochrome a3(2+)-CO CuB+ cytochrome a3+ CuA2+) and fully reduced enzyme. Time-resolved optical absorption difference spectra were collected in the Soret region on time scales of nanoseconds to milliseconds using a gated optical spectrometric multichannel analyzer. A global exponential fitting procedure combined with a singular value decomposition method was used to analyze the transient difference spectra at various times following CO photolysis. The analysis shows that at least two processes, with apparent lifetimes of 1.4 microseconds and 11.1 ms, are present following the photodissociation of CO bound to the fully reduced enzyme. These are attributed to a conformational change and CO recombination at the cytochrome a3 site, respectively. Global analysis of the mixed-valence CO complex transient difference spectra showed the presence of five intermediates with apparent lifetimes of 1.0 microseconds, 5.2 microseconds, 83.7 microseconds, 10.5 ms, and 25.3 ms. The data on a microsecond time scale are consistent with a mechanism involving a conformational change at cytochrome a3, followed by electron transfer from cytochrome a3 to cytochrome a with subsequent electron transfer to CuA. One of the two processes on a millisecond time scale is attributed to CO recombination and the other to a structural rearrangement or heme-heme electron transfer. On the basis of this mechanism, the kinetics and the absorption spectra of the intermediates involved in the conformational and electron transfer dynamics of the mixed-valence enzyme were determined.

Light-induced structural changes in cytochrome c oxidase. Measurements of electrogenic events and absorbance changes

We have investigated flash-induced electrogenic events and absorbance changes in cytochrome c oxidase in the absence of dioxygen and carbon monoxide. Electrogenic events were studied using a Teflon-bound layer of cytochrome c oxidase oriented in a phospholipid monolayer. Absorbance changes were observed exclusively in partly reduced cytochrome c oxidase; the largest changes were found in the one-electron-reduced species. Electrogenic events were detected in all reduction states of the enzyme. Both types of experiments displayed a rapid (< 0.5 microseconds) event followed by a biphasic relaxation. The time constants of the relaxation were 6 +/- 2 microseconds and 70 +/- 10 microseconds in the electrogenicity, and 9 +/- 3 microseconds in the absorbance changes (at approximately 22 degrees C). The kinetic absorbance difference spectrum was consistent with that of reduced minus oxidized haem. The experimental results are discussed in terms of structural changes in the vicinity of cytochrome a3. These changes may play an important role in all studies that involve flash photolysis of cytochrome c oxidase-ligand complexes.