Insights from surface enhanced resonance Raman spectroscopy and QM/MM calculations

Understanding the coupling between heme reduction and proton translocation in cytochrome c oxidase (CcO) is still an open problem. The propionic acids of heme a3 have been proposed to act as a proton loading site (PLS) in the proton pumping pathway, yet this proposal could not be verified by experimental data so far. We have set up an experiment where the redox states of the two hemes in CcO can be controlled via external electrical potential. Surface enhanced resonance Raman (SERR) spectroscopy was applied to simultaneously monitor the redox state of the hemes and the protonation state of the heme propionates. Simulated spectra based on QM/MM calculations were used to assign the resonant enhanced CH2 twisting modes of the propionates to the protonation state of the individual heme a and heme a3 propionates respectively. The comparison between calculated and measured H2OD2O difference spectra allowed a sound band assignment. In the fully reduced enzyme at least three of the four heme propionates were found to be protonated whereas in the presence of a reduced heme a and an oxidized heme a3 only protonation of one heme a3 propionates was observed. Our data supports the postulated scenario where the heme a3 propionates are involved in the proton pathway

Protonation State-Dependent Communication in Cytochrome c Oxidase

Proton transfer in cytochrome c oxidase from the cellular inside to the binuclear redox center (BNC) can occur through two distinct pathways, the D- and K-channels. For the protein to function as both a redox enzyme and a proton pump, proton transfer into the protein toward the BNC or toward a proton loading site (and ultimately through the membrane) must be highly regulated. The PR → F transition is the first step in a catalytic cycle that requires proton transfer from the bulk at the N-side to the BNC. Molecular dynamics simulations of the PR → F intermediate of this transition, with 16 different combinations of protonation states of key residues in the D- and K-channel, show the impact of the K-channel on the D-channel to be protonation-state dependent. Strength as well as means of communication, correlations in positions, or communication along the hydrogen-bonded network depends on the protonation state of the K-channel residue K362. The conformational and hydrogen-bond dynamics of the D-channel residue N139 is regulated by an interplay of protonation in the D-channel and K362. N139 thus assumes a gating function by which proton passage through the D-channel toward E286 is likely facilitated for states with protonated K362 and unprotonated E286. In contrast, proton passage through the D-channel is hindered by N139’s preference for a closed conformation in situations with protonated E286

The redox-coupled proton-channel opening in cytochrome c oxidase

Cytochrome c oxidase (CcO), a redox-coupled proton pump, catalyzes the reduction of molecular oxygen to water, thereby establishing the transmembrane proton gradient that fuels ATP synthesis. CcO employs two channels for proton uptake, the D- and the K-channel. In contrast to the D-channel, the K-channel does not constitute a continuous pathway of H-bonds for proton conduction and is only active in the reductive phase rendering its proton transport mechanism enigmatic. Theoretical studies have suggested selective hydration changes within the K-channel to become activated and being essential for vectorial proton transport. Here, we unravel a previously unidentified mechanism for transient proton channel activation by combining computational studies with site-directed nano-environmental probing of protonation, structural changes, and water dynamics. We show that electrostatic changes at the binuclear center lead to long-range conformational changes propagating to the K-channel entrance as evidenced by time-resolved fluorescence depolarization experiments and molecular dynamics (MD) simulations. These redox-induced long-range structural rearrangements affect the H-bond network at the K-channel's protein surface as shown by pKa-shift analysis of a local probe in experiment and simulation. Concomitantly, selective channel hydration at the K-channel entrance was revealed by dipolar relaxation studies to be associated with channel opening. We propose that instead of a singular change, it is the intricate interplay of these individual redox-triggered changes in the cause–effect relationship that defines the mechanism for transient proton conduction of the K-channel

Development of Immune-Specific Interaction Potentials and Their Application in the Multi-Agent-System VaccImm

Peptide vaccination in cancer therapy is a promising alternative to conventional methods. However, the parameters for this personalized treatment are difficult to access experimentally. In this respect, in silico models can help to narrow down the parameter space or to explain certain phenomena at a systems level. Herein, we develop two empirical interaction potentials specific to B-cell and T-cell receptor complexes and validate their applicability in comparison to a more general potential. The interaction potentials are applied to the model VaccImm which simulates the immune response against solid tumors under peptide vaccination therapy. This multi-agent system is derived from another immune system simulator (C-ImmSim) and now includes a module that enables the amino acid sequence of immune receptors and their ligands to be taken into account. The multi-agent approach is combined with approved methods for prediction of major histocompatibility complex (MHC)-binding peptides and the newly developed interaction potentials. In the analysis, we critically assess the impact of the different modules on the simulation with VaccImm and how they influence each other. In addition, we explore the reasons for failures in inducing an immune response by examining the activation states of the immune cell populations in detail

Understanding Selectin Counter-Receptor Binding from Electrostatic Energy Computations and Experimental Binding Studies

Higher organisms defend themselves against invading micro-organisms and harmful substances with their immune system. Key players of the immune system are the white blood cells (WBC), which in case of infection move in an extravasation process from blood vessels toward infected tissue promoting inflammation. This process starts with the attachment of the WBC to the blood vessel wall, mediated by protein pair interactions of selectins and counter-receptors (C-R). Individual selectin C-R binding is weak and varies only moderately between the three selectin types. Multivalency enhances such small differences, rendering selectin-binding type specific. In this work, we study selectin C-R binding, the initial step of extravasation. We performed electrostatic energy computations based on the crystal structure of one selectin type co-crystallized with the ligating part of the C-R. The agreement with measured free energies of binding is satisfactory. Additionally, we modeled selectin mutant structures in order to explain differences in binding of the different selectin types. To verify our modeling procedures, surface plasmon resonance data were measured for several mutants and compared with computed binding affinities. Binding affinities computed with soaked rather than co-crystallized selectin C-R structures do not agree with measured data. Hence, these structures are inappropriate to describe the binding mode. The analysis of selectin/C-R binding unravels the role played by individual molecular components in the binding event. This opens new avenues to prevent immune system malfunction, designing drugs that can control inflammatory processes by moderating selectin C-R binding

Exploring the Possible Role of Glu286 in C<i>c</i>O by Electrostatic Energy Computations Combined with Molecular Dynamics

Cytochrome <i>c</i> oxidase (C<i>c</i>O) is a central enzyme in aerobic life catalyzing the conversion of molecular oxygen to water and utilizing the chemical energy to pump protons and establish an electrochemical gradient. Despite intense research, it is not understood how C<i>c</i>O achieves unidirectional proton transport and avoids short circuiting the proton pump. Within this work, we analyzed the potential role of Glu286 as a proton valve. We performed unconstrained MD simulations of C<i>c</i>O with an explicit membrane for up to 80 ns. Those MD simulations revealed that deprotonated Glu286 (Glu286-) is repelled by the negatively charged propionic acid PRD of heme a₃. Thus, it destabilizes a potential linear chain of waters in the hydrophobic cavity connecting Glu286 with PRD and the binuclear center (BNC). Conversely, protonated Glu286 (Glu286H) may remain in an upward position (oriented toward PRD) and can stabilize the connecting linear water chain in the hydrophobic cavity. We calculated the p<i>K</i>_a of Glu286 under physiological conditions to be above 12, but this value decreases to about 9 under increased water accessibility of Glu286. The latter value is in accordance with experimental measurements. In the time course of MD simulation, we also observed conformations where Glu286 bridges between water molecules located on both sides (the D channel being connected to the N side and the hydrophobic cavity), which might lead to proton backflow