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Dmitry A Cherepanov

Publications and source records attributed to Dmitry A Cherepanov.

9 recordsLinked to original sources

Probing biological interfaces by tracing proton passage across them.

The properties of water at the surface, especially at an electrically charged one, differ essentially from those in the bulk phase. Here we survey the traits of surface water as inferred from proton pulse experiments with membrane enzymes. In such experiments, protons that are ejected (or captured) by light-triggered enzymes are traced on their way between the membrane surface and the bulk aqueous phase. In several laboratories it has been shown that proton exchange between the membrane surface and the bulk aqueous phase takes as much as about 1 ms, but could be accelerated by added mobile pH-buffers. Since the accelerating capacity of the latter decreased with increase in their electric charge, it was suggested that the membrane surface is separated from the bulk aqueous phase by a barrier of electrostatic nature. In terms of ordinary electrostatics, the barrier could be ascribed to dielectric saturation of water at a charged surface. In terms of nonlocal electrostatics, the barrier could result from the dielectric overscreening in the surface water layers. It is discussed how the interfacial potential barrier can affect the reactions at interface, especially those coupled with biological energy conversion and membrane transport.

Ion Transport↗

Protons @ interfaces: implications for biological energy conversion.

The review focuses on the anisotropy of proton transfer at the surface of biological membranes. We consider (i) the data from "pulsed" experiments, where light-triggered enzymes capture or eject protons at the membrane surface, (ii) the electrostatic properties of water at charged interfaces, and (iii) the specific structural attributes of proton-translocating enzymes. The pulsed experiments revealed that proton exchange between the membrane surface and the bulk aqueous phase takes as much as about 1 ms, but could be accelerated by added mobile pH-buffers. Since the accelerating capacity of the latter decreased with the increase in their electric charge, it was concluded that the membrane surface is separated from the bulk aqueous phase by a barrier of electrostatic nature. The barrier could arise owing to the water polarization at the negatively charged membrane surface. The barrier height depends linearly on the charge of penetrating ions; for protons, it has been estimated as about 0.12 eV. While the proton exchange between the surface and the bulk aqueous phase is retarded by the interfacial barrier, the proton diffusion along the membrane, between neighboring enzymes, takes only microseconds. The proton spreading over the membrane is facilitated by the hydrogen-bonded networks at the surface. The membrane-buried layers of these networks can eventually serve as a storage/buffer for protons (proton sponges). As the proton equilibration between the surface and the bulk aqueous phase is slower than the lateral proton diffusion between the "sources" and "sinks", the proton activity at the membrane surface, as sensed by the energy transducing enzymes at steady state, might deviate from that measured in the adjoining water phase. This trait should increase the driving force for ATP synthesis, especially in the case of alkaliphilic bacteria.

Biological Transport↗

Force oscillations and dielectric overscreening of interfacial water.

The anomalous properties of interfacial water, such as the layering of electrolyte solutions confined in nanoscopic films, the rise of hydration repulsion at high ionic strength, and the existence of an interfacial potential barrier, were consistently described by the theory of nonlocal electrostatics using the dielectric function of isotropic water as obtained by molecular dynamics. The layering arises owing to the negative sign of the dielectric function at certain wave vectors ("overscreening") similar to the appearance of charge density waves in high-temperature superconductors.

Journal Article↗

Proton transfer dynamics at the membrane/water interface: dependence on the fixed and mobile pH buffers, on the size and form of membrane particles, and on the interfacial potential barrier.

Crossing the membrane/water interface is an indispensable step in the transmembrane proton transfer. Elsewhere we have shown that the low dielectric permittivity of the surface water gives rise to a potential barrier for ions, so that the surface pH can deviate from that in the bulk water at steady operation of proton pumps. Here we addressed the retardation in the pulsed proton transfer across the interface as observed when light-triggered membrane proton pumps ejected or captured protons. By solving the system of diffusion equations we analyzed how the proton relaxation depends on the concentration of mobile pH buffers, on the surface buffer capacity, on the form and size of membrane particles, and on the height of the potential barrier. The fit of experimental data on proton relaxation in chromatophore vesicles from phototropic bacteria and in bacteriorhodopsin-containing membranes yielded estimates for the interfacial potential barrier for H(+)/OH(-) ions of approximately 120 meV. We analyzed published data on the acceleration of proton equilibration by anionic pH buffers and found that the height of the interfacial barrier correlated with their electric charge ranging from 90 to 120 meV for the singly charged species to >360 meV for the tetra-charged pyranine.

Bacterial Chromatophores↗

Rotary F1-ATPase. Is the C-terminus of subunit gamma fixed or mobile?

F-ATP synthase synthesizes ATP at the expense of ion motive force by a rotary coupling mechanism. A central shaft, subunit gamma, functionally connects the ion-driven rotary motor, F(O), with the rotary chemical reactor, F(1). Using polarized spectrophotometry we have demonstrated previously the functional rotation of the C-terminal alpha-helical portion of gamma in the supposed 'hydrophobic bearing' formed by the (alpha beta)(3) hexagon. In apparent contradiction with these spectroscopic results, an engineered disulfide bridge between the alpha-helix of gamma and subunit alpha did not impair enzyme activity. Molecular dynamics simulations revealed the possibility of a 'functional unwinding' of the alpha-helix to form a swivel joint. Furthermore, they suggested a firm clamping of that part of gamma even without the engineered cross-link, i.e. in the wild-type enzyme. Here, we rechecked the rotational mobility of the C-terminal portion of gamma relative to (alpha beta)(3). Non-fluorescent, engineered F(1) (alpha P280C/gamma A285C) was oxidized to form a (nonfluorescent) alpha gamma heterodimer. In a second mutant, containing just the point mutation within alpha, all subunits were labelled with a fluorescent dye. Following disassembly and reassembly of the combined preparations and cystine reduction, the enzyme was exposed to ATP or 5'-adenylyl-imidodiphosphate (AMP-PNP). After reoxidation, we found fluorescent alpha gamma dimers in all cases in accordance with rotary motion of the entire gamma subunit under these conditions. Molecular dynamics simulations covering a time range of nanoseconds therefore do not necessarily account for motional freedom in microseconds. The rotation of gamma within hours is compatible with the spectroscopically detected blockade of rotation in the AMP-PNP-inhibited enzyme in the time-range of seconds.

Adenosine Triphosphate↗

The proton-driven rotor of ATP synthase: ohmic conductance (10 fS), and absence of voltage gating.

The membrane portion of F(0)F(1)-ATP synthase, F(0), translocates protons by a rotary mechanism. Proton conduction by F(0) was studied in chromatophores of the photosynthetic bacterium Rhodobacter capsulatus. The discharge of a light-induced voltage jump was monitored by electrochromic absorption transients to yield the unitary conductance of F(0). The current-voltage relationship of F(0) was linear from 7 to 70 mV. The current was extremely proton-specific (>10(7)) and varied only slightly ( approximately threefold) from pH 6 to 10. The maximum conductance was approximately 10 fS at pH 8, equivalent to 6240 H(+) s(-1) at 100-mV driving force, which is an order-of-magnitude greater than of coupled F(0)F(1). There was no voltage-gating of F(0) even at low voltage, and proton translocation could be driven by deltapH alone, without voltage. The reported voltage gating in F(0)F(1) is thus attributable to the interaction of F(0) with F(1) but not to F(0) proper. We simulated proton conduction by a minimal rotary model including the rotating c-ring and two relay groups mediating proton exchange between the ring and the respective membrane surface. The data fit attributed pK values of approximately 6 and approximately 10 to these relays, and placed them close to the membrane/electrolyte interface.

ATP Synthetase Complexes↗

Survival of the fittest before the beginning of life: selection of the first oligonucleotide-like polymers by UV light.

BACKGROUND: A key event in the origin of life on this planet has been formation of self-replicating RNA-type molecules, which were complex enough to undergo a Darwinian-type evolution (origin of the "RNA world"). However, so far there has been no explanation of how the first RNA-like biopolymers could originate and survive on the primordial Earth. RESULTS: As condensation of sugar phosphates and nitrogenous bases is thermodynamically unfavorable, these compounds, if ever formed, should have undergone rapid hydrolysis. Thus, formation of oligonucleotide-like structures could have happened only if and when these structures had some selective advantage over simpler compounds. It is well known that nitrogenous bases are powerful quenchers of UV quanta and effectively protect the pentose-phosphate backbones of RNA and DNA from UV cleavage. To check if such a protection could play a role in abiogenic evolution on the primordial Earth (in the absence of the UV-protecting ozone layer), we simulated, by using Monte Carlo approach, the formation of the first oligonucleotides under continuous UV illumination. The simulations confirmed that UV irradiation could have worked as a selective factor leading to a relative enrichment of the system in longer sugar-phosphate polymers carrying nitrogenous bases as UV-protectors. Partial funneling of the UV energy into the condensation reactions could provide a further boost for the oligomerization. CONCLUSION: These results suggest that accumulation of the first polynucleotides could be explained by their abiogenic selection as the most UV-resistant biopolymers.

Biopolymers↗

Low dielectric permittivity of water at the membrane interface: effect on the energy coupling mechanism in biological membranes.

Protonmotive force (the transmembrane difference in electrochemical potential of protons, ) drives ATP synthesis in bacteria, mitochondria, and chloroplasts. It has remained unsettled whether the entropic (chemical) component of relates to the difference in the proton activity between two bulk water phases (deltapH(B)) or between two membrane surfaces (deltapH(S)). To scrutinize whether deltapH(S) can deviate from deltapH(B), we modeled the behavior of protons at the membrane/water interface. We made use of the surprisingly low dielectric permittivity of interfacial water as determined by O. Teschke, G. Ceotto, and E. F. de Souza (O. Teschke, G. Ceotto, and E. F. de Sousa, 2001, PHYS: Rev. E. 64:011605). Electrostatic calculations revealed a potential barrier in the water phase some 0.5-1 nm away from the membrane surface. The barrier was higher for monovalent anions moving toward the surface (0.2-0.3 eV) than for monovalent cations (0.1-0.15 eV). By solving the Smoluchowski equation for protons spreading away from proton "pumps" at the surface, we found that the barrier could cause an elevation of the proton concentration at the interface. Taking typical values for the density of proton pumps and for their turnover rate, we calculated that a potential barrier of 0.12 eV yielded a steady-state pH(S) of approximately 6.0; the value of pH(S) was independent of pH in the bulk water phase under neutral and alkaline conditions. These results provide a rationale to solve the long-lasting problem of the seemingly insufficient protonmotive force in mesophilic and alkaliphilic bacteria.

Cell Membrane↗

Chromatophore vesicles of Rhodobacter capsulatus contain on average one F(O)F(1)-ATP synthase each.

ATP synthase is a unique rotary machine that uses the transmembrane electrochemical potential difference of proton (Delta(H(+))) to synthesize ATP from ADP and inorganic phosphate. Charge translocation by the enzyme can be most conveniently followed in chromatophores of phototrophic bacteria (vesicles derived from invaginations of the cytoplasmic membrane). Excitation of chromatophores by a short flash of light generates a step of the proton-motive force, and the charge transfer, which is coupled to ATP synthesis, can be spectrophotometrically monitored by electrochromic absorption transients of intrinsic carotenoids in the coupling membrane. We assessed the average number of functional enzyme molecules per chromatophore vesicle. Kinetic analysis of the electrochromic transients plus/minus specific ATP synthase inhibitors (efrapeptin and venturicidin) showed that the extent of the enzyme-related proton transfer dropped as a function of the inhibitor concentration, whereas the time constant of the proton transfer changed only marginally. Statistical analysis of the kinetic data revealed that the average number of proton-conducting F(O)F(1)-molecules per chromatophore was approximately one. Thereby chromatophores of Rhodobacter capsulatus provide a system where the coupling of proton transfer to ATP synthesis can be studied in a single enzyme/single vesicle mode.

Adenosine Diphosphate↗