Interaction of Horse Heart Cytochrome c with Lipid Bilayer Membranes: Effects on Redox Potentials

Cyclic voltammetry has been used to study the effects of interactions between horse cytochrome c and solid-supported planar lipid membranes, comprised of either egg phosphatidylcholine (PC) or PC plus 20 mol.% cardiolipin (CL), on the redox potential and the electrochemical electron transfer rate between the protein and a semiconductor electrode. Experiments were performed over a wide range of cytochrome c concentrations (0–440 M) at low (20 mM) and medium (160 mM) ionic strengths. Three types of electrochemical behavior were observed, which varied as a function of the experimental conditions. At very low cytochrome c concentration (0.1 M), and under conditions where electrostatic forces dominated the protein–lipid membrane interaction (i.e., low ionic strength with membranes containing CL), a redox potential (265 mV) and an electrochemical electron transfer rate constant (0.09s ^–1)were obtained which compare well with those measured in other laboratories using a variety of different chemical modifications of the working electrode. Two other electrochemical signals (not reported with chemically modified electrodes) were also observed to occur at higher cytochrome c concentrations with this membrane system, as well as with two other systems (membranes containing CL under medium ionic strength conditions, and PC only at low ionic strength). These involved positive shifts of the cytochrome c redox potential (by 40 and 60 mV) and large decreases in the electron transfer rate (to 0.03 and 0.003 s^–1). The observations can be rationalized in terms of a structural model of the cytochrome c–membrane interaction, in which association involves both electrostatic and hydrophobic forces and results in varying degrees of insertion of the protein into the hydrophobic interior of the membrane.     

Electron transfer between cytochrome c2 and the tetraheme cytochrome c in Rhodopseudomonas viridis

Kinetics of electron transfer from soluble cytochrome c₂ to the tetraheme cytochrome c have been measured in isolated reaction centers and in membrane fragments of the photosynthetic purple bacterium Rhodopseudomonas viridis by time-resolved flash absorption spectroscopy. Absorbance changes kinetics in the region of cytochrome -bands (540–560 nm) were measured at 21 °C under redox conditions where the two high-potential hemes (c-559 and c-556) of the tetraheme cytochrome were chemically reduced. After flash excitation, the heme c-559 donates an electron to the special pair of bacteriochlorophylls and is then re-reduced by heme c-556. The data show that oxidized heme c-556 is subsequently re-reduced by electron transfer from reduced cytochrome c₂ present in the solution. The rate of this reaction has a non-linear dependence on the concentration of cytochrome c₂, suggesting a (minimal) two-step mechanism involving the f ormation of a complex between cytochrome c₂ and the reaction center, followed by intracomplex electron transfer. To explain the monophasic character of the reaction kinetics, we propose a collisional mechanism where the lifetime of the temporary complex is short compared to electron transfer. The limit of the halftime of the bimolecular process when extrapolated to high concentrations of cytochrome c₂ is 60 ± 20 s. There is a large ionic strength effect on the kinetics of electron transfer from cytochrome c₂ to heme c-556. The pseudofirst-order rate constant decreases from 1.1 × 10⁷ M^-1 s^-1 to 1.3 × 10⁶ M^-1 s^-1 when the ionic strength is increased from 1 to 1000 mM. The maximum rate (1.1 × 10⁷ M^-1 s^-1) was obtained at about 1 mM ionic strength. This dependence of the rate on ionic strength s uggests that attractive electrostatic interactions contribute to the binding of cytochrome c₂ with the tetraheme cytochrome. On the basis of our data and of previous molecular modelling, it is proposed that cytochrome c₂ docks close to the low-potential heme c-554 and reduces heme c-556 via c-554.     

Ionic Strength-Dependent Physicochemical Factors in Cytochrome c3 Regulating the Electron Transfer Rate

The effect of ionic strength on the macroscopic and microscopic redox potentials and the heme environment of cytochrome c₃ from Desulfovibrio vulgaris Miyazaki F have been investigated by NMR and electrochemical methods. The redox potentials of this tetraheme protein are found to be ionic strength-dependent. Especially, the microscopic redox potentials of hemes 2 and 3 at the fourth reduction step increase significantly with increasing ionic strength, which is in contradiction to the theoretical expectation. The coordinated imidazole proton signals are unaffected by ionic strength. However, the methyl and propionate proton signals of hemes 1 and 4 showed significant ionic strength dependencies that are distinct from those for hemes 2 and 3. This heme classification is the same as that found in the ionic strength dependencies of the microscopic redox potentials at the fourth reduction step. Furthermore, the effect of ionic strength on the electrostatic potentials at the heme irons has been examined on the theoretical basis. The electrostatic potential at heme 4 changes up to 1 M ionic strength, which was not expected from the observations reported on cytochromes so far. These results are discussed in connection with the reported anomalous ionic strength dependency of the reduction rate of cytochrome c₃.     

An imidoester spin probe of membrane protein interactions: application to cytochrome c

The synthesis of an imidoester spin label, whose advantages relative to other spin labels include its water solubility, lysine specificity, and retention of positive charge at the reaction site is described. Cytochrome c is spin labeled and shown to exhibit spectral changes upon interacting with lipid vesicles and lipid-rich cytochrome oxidase preparations. Spin labeled cytochrome c in buffer or in the presence of mitochondria at high ionic strength had a correlation time of τ = 0.91 ± 10^?9 s; at low ionic strength the mitochondrial signal was more immobilized, τ = 2.27 ± 0.13 × 10^?9 s; and further immobilization was observed when cytochrome c was bound to the high-affinity site of purified oxidase containing 37% phospholipid (τ = 2.71 ± 0.22 × 10^?9). Cytochrome c-oxidase electron transfer rates were unaltered by spin labeling. The results suggest that this imidoester spin label will be useful for studies of protein-protein and protein-lipid interactions.     

Electrostatic effects on the kinetics of photoinduced electron-transfer reactions of the triplet state of zinc cytochrome c with wild-type and mutant forms of Pseudomonas aeruginosa azurin

We study, by laser flash photolysis, the effects of ionic strength on the kinetics of the reaction ³Zncyt + az(II) → Zncyt⁺ + az(I), i.e., oxidative quenching of the triplet state of zinc cytochrome c by the wild-type form and the following three mutants of cupriazurin: Met44Lys, Met64Glu, and the double mutant Met44Lys/Met64Glu. Mutations in the hydrophobic patch of azurin significantly affect the reactivity of the protein with the triplet state of zinc cytochrome c. Dependence on the ionic strength of the bimolecular rate constant for the aforementioned reaction is analyzed by several electrosatic models. The two transition-state theories, Brønsted-Debye-Hückel and van Leeuwen theories, allow the best approximation to the experimental data when effective charges of the proteins are used. Protein-protein interactions are also analyzed in terms of local charges on the protein surfaces. The rate constants depend little on ionic strength, and the monopolar and dipolar electrostatic interactions between zinc cytochrome c and azurin are not well resolved. Semiquantitative analysis of electrostatic interactions indicates that azurin uses its hydrophobic patch for contact with zinc cytochrome c.     

Cytochrome c-Lipid Interactions: New Insights from Resonance Energy Transfer

Resonance energy transfer (RET) from anthrylvinyl-labeled phosphatidylcholine (AV-PC) or cardiolipin (AV-CL) to cytochrome c (cyt c) heme moiety was employed to assess the molecular-level details of protein interactions with lipid bilayers composed of PC with 2.5 (CL2.5), 5 (CL5), 10 (CL10), or 20 (CL20) mol % CL under conditions of varying ionic strength and lipid/protein molar ratio. Monte Carlo analysis of multiple data sets revealed a subtle interplay between 1), exchange of the neutral and acidic lipid in the protein-lipid interaction zone; 2), CL transition into the extended conformation; and 3), formation of the hexagonal phase. The switch between these states was found to be controlled by CL content and salt concentration. At ionic strengths ≥40 mM, lipid bilayers with CL fraction not exceeding 5 mol % exhibited the tendency to transform from lamellar to hexagonal phase upon cyt c adsorption, whereas at higher contents of CL, transition into the extended conformation seems to become thermodynamically favorable. At lower ionic strengths, deviations from homogeneous lipid distributions were observed only for model membranes containing 2.5 mol % CL, suggesting the existence of a certain surface potential critical for assembly of lipid lateral domains in protein-lipid systems that may subsequently undergo morphological transformations depending on ambient conditions. These characteristics of cyt c-CL interaction are of great interest, not only from the viewpoint of regulating cyt c electron transfer and apoptotic propensities, but also to elucidate the general mechanisms by which membrane functional activities can be modulated by protein-lipid interactions.     

Molecular Modeling of the Ternary Complex of Rusticyanin-Cytochrome c4-Cytochrome Oxidase: An Insight to Possible H-Bond Mediated Recognition and Electron Transfer Reaction in T.ferrooxidans

Abstract

The metabolism of Thiobacillus ferrooxidans involves electron transfer from the Fe⁺² ions in the extracellular environment to the terminal oxygen in the bacterial cytoplasm through a series of periplasmic proteins like Rusticyanin (RCy), Cytochrome (Cyt c₄), and Cytochrome oxidase (CcO). The energy minimization and MD studies reveal the stabilization of the three redox proteins in their ternary complex through the direct and water mediated H-bonds and electrostatic interaction. The surface exposed polar residues of the three proteins, i.e., RCy (His 143, Thr 146, Lys 81, Glu 20), Cyt c₄ (Asp 5, 15, 52, Ser 14, Glu 61), and CcO (Asp 135, Glu 126, 140, 142, Thr 177) formed the intermolecular hydrogen bonds and stabilized the ternary complex. The oxygen (O^εl) of Glu 126, 140, and 142 on subunit II of the CcO interact to the exposed side-chain and O^b atoms of the Asp 52 of Cyt c₄ and Glu 20 and Leu 12 of RCy. The Asp 135 of subunit II also forms H-bond with the N^ε atom of Lys 81 of RCy. The O^εl of Glu 61 of Cyt c₄ is also H-bonded to O^γ atom of Thr 177 of CcO. Solvation followed by MD studies of the ternary protein complex revealed the presence of seven water molecules in the interfacial region of the interacting proteins. Three of the seven water molecules (W 79, W 437, and W 606) bridged the three proteins by forming the hydrogen bonded network (with the distances ～ 2.10–2.95 Å) between the Lys 81 (RCy), Glu 61 (Cyt c₄), and Asp 135 (CcO). Another water molecule W 603 was H-bonded to Tyr 122 (CcO) and interconnected the Lys 81 (RCy) and Asp 135 (CcO) through the water molecules W 606 and W 437. The other two water molecules (W 21 and W 455) bridged the RCy to Cyt c₄ through H-bonds, whereas the remaining W 76 interconnected the His 53 (Cytc₄) to Glu 126 (CcO) with distances ～ 2.95–3.0 Å.     

A “parallel plate” electrostatic model for bimolecular rate constants applied to electron transfer proteins

A “parallel plate” model describing the electrostatic potential energy of protein-protein interactions is presented that provides an analytical representation of the effect of ionic strength on a bimolecular rate constant. The model takes into account the asymmetric distribution of charge on the surface of the protein and localized charges at the site of electron transfer that are modeled as elements of a parallel plate condenser. Both monopolar and dipolar interactions are included. Examples of simple (monophasic) and complex (biphasic) ionic strength dependencies obtained from experiments with several electron transfer protein systems are presented, all of which can be accommodated by the model. The simple cases do not require the use of both monopolar and dipolar terms (i.e., they can be fit well by either alone). The biphasic dependencies can be fit only by using dipolar and monopolar terms of opposite sign, which is physically unreasonable for the molecules considered. Alternatively, the high ionic strength portion of the complex dependencies can be fit using either the monopolar term alone or the complete equation; this assumes a model in which such behavior is a consequence of electron transfer mechanisms involving changes in orientation or site of reaction as the ionic strength is varied. Based on these analyses, we conclude that the principal applications of the model presented here are to provide information about the structural properties of intermediate electron transfer complexes and to quantify comparisons between related proteins or site-specific mutants. We also conclude that the relative contributions of monopolar and dipolar effects to protein electron transfer kinetics cannot be evaluated from experimental data by present approximations.     

Electron transfer between horse heart and Candida krusei cytochromes c in the free and bound states

Electron transfer between horse heart and Candida krusei cytochromes c in the free and phosvitin-bound states was examined by difference spectrum and stopped-flow methods. The difference spectra in the wavelength range of 540–560 nm demonstrated that electrons are exchangeable between the cytochromes c of the two species. The equilibrium constants of the electron transfer reaction for the free and phosvitin-bound forms, estimated from these difference spectra, were close to unity at 20°C in 20 mM Tris-HCl buffer (pH 7.4). The electron transfer rate for free cytochrome c was (2–3) · 10⁴ M^?1 · s^?1 under the same conditions. The transfer rate for the bound form increased with increase in the binding ratio at ratios below half the maximum, and was almost constant at higher ratios up to the maximum. The maximum electron exchange rate was about 2 · 10⁶ M^?1 · s^?1, which is 60–70 times that for the free form at a given concentration of cytochrome c. The activation energy of the reaction for the bound cytochrome c was equal to that for the free form, being about 10 kcal/mol. The dependence of the exchange rate on temperature, cytochrome c concentration and solvent viscosity suggests that enhancement of the electron transfer rate between cytochromes c on binding to phosvitin is due to increase in the collision frequency between cytochromes c concentrated on the phosvitin molecule.     

Is ubiquinone diffusion rate-limiting for electron transfer?

The different possible dispositions of the electron transfer components in electron transfer chains are discussed: (a) random distribution of complexes and ubiquinone with diffusion-controlled collisions of ubiquinone with the complexes, (b) random distribution as above, but with ubiquinone diffusion not rate-limiting, (c) diffusion and collision of protein complexes carrying bound ubiquinone, and (d) solid-state assembly. Discrimination among these possibilities requires knowledge of the mobility of the electron transfer chain components. The collisional frequency of ubiquinone-10 with the fluorescent probe 12-(9-anthroyl)stearate, investigated by fluorescence quenching, is 2.3 × 10⁹ M^–1 sec^–1 corresponding to a diffusion coefficient in the range of 10^–6 cm²/sec (Fato, R., Battino, M., Degli Esposti, M., Parenti Castelli, G., and Lenaz, G.,Biochemistry,25, 3378–3390, 1986); the long-range diffusion of a short-chain polar Q derivative measured by fluorescence photobleaching recovery (FRAP) (Gupte, S., Wu, E. S., Höchli, L., Höchli, M., Jacobson, K., Sowers, A. E., and Hackenbrock, C. R.,Proc. Natl. Acad. Sci. USA 81, 2606–2610, 1984) is 3×10^–9 cm²/sec. The discrepancy between these results is carefully scrutinized, and is mainly ascribed to the differences in diffusion ranges measured by the two techniques; it is proposed that short-range diffusion, measured by fluorescence quenching, is more meaningful for electron transfer than long-range diffusion measured by FRAP, or microcollisions, which are not sensed by either method. Calculation of the distances traveled by random walk of ubiquinone in the membrane allows a large excess of collisions per turnover of the respiratory chain. Moreover, the second-order rate constants of NADH-ubiquinone reductase and ubiquinol-cytochromec reductase are at least three orders of magnitude lower than the second-order collisional constant calculated from the diffusion of ubiquinone. The activation energies of either the above activities or integrated electron transfer (NADH-cytochromec reductase) are well above that for diffusion (found to be ca. 1 kcal/mol). Cholesterol incorporation in liposomes, increasing bilayer viscosity, lowers the diffusion coefficients of ubiquinone but not ubiquinol-cytochromec reductase or succinate-cytochromec reductase activities. The decrease of activity by ubiquinone dilution in the membrane is explained by its concentration falling below theK _m of the partner enzymes. It is calculated that ubiquinone diffusion is not rate-limiting, favoring a random model of the respiratory chain organization. It is not possible, however, to exclude solid-state assemblies if the rate of dissociation and association of ubiquinone is faster than the turnover of electron transfer.     

Cytochrome c peroxidase-cytochrome c complex: locating the second binding domain on cytochrome c peroxidase with site-directed mutagenesis

Cytochrome c peroxidase (CcP) can bind as many as two cytochrome c (Cc) molecules in an electrostatic complex. The location of the two binding domains on CcP has been probed by photoinduced interprotein electron transfer (ET) between zinc-substituted horse cytochrome c (ZnCc) and CcP with surface charge-reversal mutations and by isothermal titration calorimetry (ITC). These results, which are the first experimental evidence for the location of domain 2, indicate that the weak-binding domain includes residues 146-150 on CcP. CcP(E290K) has a charge-reversal mutation in the tight-binding domain, which should weaken binding, and it weakens the 1:1 complex; K(1) decreases 20-fold at 18 mM ionic strength. We have employed two mutations to probe the proposed location for the weak-binding domain on the CcP surface: (i) D148K, a "detrimental" mutation with a net (+2) change in the charge of CcP, and (ii) K149E, a "beneficial" mutation with a net (-2) change in the charge. The interactions between FeCc and CcP(WT and K149E) also have been studied with ITC. The CcP(D148K) mutation causes no substantial change in the 2:1 binding but an increase in the reactivity of the 2:1 complex. The latter can be interpreted as a long-range influence on the heme environment or, more likely, the enhancement of a minority subset of binding conformations with favorable pathways for ET. CcP(K149E) has a charge-reversal mutation in the weak-binding domain that produces a substantial increase in the 2:1 binding constant as measured by both quenching and ITC. For the 1:1 complex of CcP(WT), DeltaG(1) = -8.2 kcal/mol (K(1) = 1.3 x 10(6) M(-)(1)), DeltaH(1) = +2.7 kcal/mol, and DeltaS(1) = +37 cal/K.mol at 293 K; for the second binding stage, K(2) < 5 x 10(3) M(-)(1), but accurate thermodynamic parameters were not obtained. For the 1:1 complex of CcP(K149E), DeltaG(1) = -8.5 kcal/mol (K(1) = 2 x 10(6) M(-)(1)), DeltaH(1) = +2. 0 kcal/mol, and DeltaS(1) = +36 cal/K.mol; for the second stage, DeltaG(2) = -5.5 kcal/mol (K(1) = 1.3 x 10(4) M(-)(1)), DeltaH(2) = +2.9 kcal/mol, and DeltaS(2) = +29 cal/K.mol.     

Kinetics of flash-induced electron transfer between bacterial reaction centres,mitochondrial ubiquinol: Cytochrome c oxidoreductase and cytochrome c

Ascorbate-reduced horse heart cytochrome c reduces photo-oxidized bacterial reaction centres with a second-order rate constant of (5–8) · 10⁸ M^?1 · s^?1 at an ionic strength of 50 mM. In the absence of cytochrome c, the cytochrome c₁ in the ubiquinol:cytochrome c oxidoreductase is oxidized relatively slowly (k = 3.3 · 10⁵ M^?1 · s^?1). Ferrocytochrome c binds specifically to ascorbate-reduced reductase, with a K_d of 0.6 μM, and only the free cytochrome c molecules are involved in the rapid reduction of photo-oxidized reaction centres. The electron transfer between ferricytochrome c and ferrocytochrome c₁ of the reductase is rapid, with a second-order rate constant of 2.1 · 10⁸ M^?1 · s^?1 at an ionic strength of 50 mM. The rate of electron transfer from the Rieske iron-sulphur cluster to cytochrome c₁ is even more rapid. The cytochrome b of the ubiquinol:cytochrome c oxidoreductase can be reduced by electrons from the reaction centres through two pathways: one is sensitive to antimycin and the other to myxothiazol. The amount of cytochrome b reduced in the absence of antimycin is dependent on the redox potential of the system, but in no case tested did it exceed 25% of the amount of photo-oxidized reaction centres.     

The effect of pH and ionic strength on the pre-steady-state reaction of cytochrome c and cytochrome aa3

(1) In the pH range between 5.0 and 8.0, the rate constants for the reaction of ferrocytochrome c with both the high- and low-affinity sites on cytochrome aa₃ increase by a factor of approx. 2 per pH unit. (2) The pre-steady-state reaction between ferrocytochrome c and cytochrome aa₃ did not cause a change in the pH of an unbuffered medium. Furthermore, it was found that this reaction and the steady-state reaction are equally fast in H₂O and ²H₂O. From these results it was concluded that no protons are directly involved in a rate-determining reaction step. (3) Arrhenius plots show that the reaction between ferrocytochrome c and cytochrome aa₃ requires a higher enthalpy of activation at temperatures below 20°C (15–16 kcal/mol) as compared to that at higher temperature (9 kcal/mol). We found no effect of ionic strength on the activation enthalpy of the pre-steady-state reaction, nor on that of the steady-state reaction. This suggests that ionic strength does not change the character of these reactions, but merely affects the electrostatic interaction between both cytochromes.     

Ionic strength and pH dependence of the reaction between plastocyanin and Photosystem 1. Evidence of a rate-limiting conformational change

The electron-transfer reaction between spinach wild-type plastocyanin (Pc(WT)) two site-directed mutants, Pc(Thr79His) and Pc(Lys81His), and spinach Photosystem 1 particles, has been studied as a function of protein concentration, ionic strength and pH by using laser-flash absorption spectroscopy. The kinetic data are interpreted using the simplest possible three-step model, involving a rate-limiting conformational change preceding intracomplex electron transfer. The three proteins show similar concentration, pH and ionic strength dependencies. The effects of ionic strength and pH on the reaction indicate a strong influence of complementary charges on complex formation and stabilization. Studies with apoprotein support the opinion that the hydrophobic patch is critical for an productive interaction with the reaction center of Photosystem 1. Together with earlier site-directed mutagenesis studies, the absence of a detectable Photosystem 1 reaction in the presence of reduced azurin, stellacyanin, cytochrome c and cytochrome c₅₅₁, demonstrates the existence of a high level of specificity in the protein-protein interface in the formation of an efficient electron-transfer complex.     

Rationalizing 5000-fold differences in receptor-binding rate constants of four cytokines

The four cytokines erythropoietin (EPO), interleukin-4 (IL4), human growth hormone (hGH), and prolactin (PRL) all form four-helix bundles and bind to type I cytokine receptors. However, their receptor-binding rate constants span a 5000-fold range. Here, we quantitatively rationalize these vast differences in rate constants by our transient-complex theory for protein-protein association. In the transient complex, the two proteins have near-native separation and relative orientation, but have yet to form the short-range specific interactions of the native complex. The theory predicts the association rate constant as where k_a0 is the basal rate constant for reaching the transient complex by random diffusion, and the Boltzmann factor captures the rate enhancement due to electrostatic attraction. We found that the vast differences in receptor-binding rate constants of the four cytokines arise mostly from the differences in charge complementarity among the four cytokine-receptor complexes. The basal rate constants (k_a0) of EPO, IL4, hGH, and PRL were similar (5.2 × 10⁵ M⁻¹s⁻¹, 2.4 × 10⁵ M⁻¹s⁻¹, 1.7 × 10⁵ M⁻¹s⁻¹, and 1.7 × 10⁵ M⁻¹s⁻¹, respectively). However, the average electrostatic free energies () were very different (−4.2 kcal/mol, −2.4 kcal/mol, −0.1 kcal/mol, and −0.5 kcal/mol, respectively, at ionic strength = 160 mM). The receptor-binding rate constants predicted without adjusting any parameters, 6.2 × 10⁸ M⁻¹s⁻¹, 1.3 × 10⁷ M⁻¹s⁻¹, 2.0 × 10⁵ M⁻¹s⁻¹, and 7.6 × 10⁴ M⁻¹s⁻¹, respectively, for EPO, IL4, hGH, and PRL agree well with experimental results. We uncover that these diverse rate constants are anticorrelated with the circulation concentrations of the cytokines, with the resulting cytokine-receptor binding rates very close to the limits set by the half-lives of the receptors, suggesting that these binding rates are functionally relevant and perhaps evolutionarily tuned. Our calculations also reproduced well-observed effects of mutations and ionic strength on the rate constants and produced a set of mutations on the complex of hGH with its receptor that putatively enhances the rate constant by nearly 100-fold through increasing charge complementarity. To quantify charge complementarity, we propose a simple index based on the charge distribution within the binding interface, which shows good correlation with . Together these results suggest that protein charges can be manipulated to tune k_a and control biological function.     

Thermal Stability of Cytochrome c 5 of Pressure-Sensitive Shewanella livingstonensis

Cytochrome c ₅ of pressure-sensitive Shewanella livingstonensis (SL cytc ₅) exhibits lower thermal stability than a highly homologous counterpart of pressure-tolerant Shewanella violacea. This stability difference is due to an enthalpic effect that can be attributed to the amino acid residue at position 50 (Leu or Lys). These cytc ₅ proteins are appropriate materials for understanding the protein stability mechanism.     

The reaction between cytochrome C1 and cytochrome C

The kinetics of electron transfer between the isolated enzymes of cytochrome c₁ and cytochrome c have been investigated using the stopped-flow technique. The reaction between ferrocytochrome c₁ and ferricytochrome c is fast; the second-order rate constant (k₁) is 3.0 · 10⁷ M^?1 · s^?1 at low ionic strength (I = 223 mM, 10°C). The value of this rate constant decreases to 1.8 · 10⁵ M^?1 · s^?1 upon increasing the ionic strength to 1.13 M. The ionic strength dependence of the electron transfer between cytochrome c₁ and cytochrome c implies the involvement of electrostatic interactions in the reaction between both cytochromes. In addition to a general influence of ionic strength, specific anion effects are found for phosphate, chloride and morpholinosulphonate. These anions appear to inhibit the reaction between cytochrome c₁ and cytochrome c by binding of these anions to the cytochrome c molecule. Such a phenomenon is not observed for cacodylate. At an ionic strength of 1.02 M, the second-order rate constants for the reaction between ferrocytochrome c₁ and ferricytochrome c and the reverse reaction are k₁ = 2.4 · 10⁵ M^?1 · s^?1 and k_?1 = 3.3 · 10⁵ M^?1 · s^?1, respectively (450 mM potassium phosphate, pH 7.0, 1% Tween 20, 10°C). The ‘equilibrium’ constant calculated from the rate constants (0.73) is equal to the constant determined from equilibrium studies. Moreover, it is shown that at this ionic strength, the concentrations of intermediary complexes are very low and that the value of the equilibrium constant is independent of ionic strength. These data can be fitted into the following simple reaction scheme: cytochrome c²⁺₁ + cytochrome c³⁺ai cytochrome c³⁺₁ + cytochrome c²⁺.     

Interaction of cytochromec with phospholipid monolayers and bilayer membranes

Summary For the study of the interaction between oxidized cytochromec and phosphatidylinositide, two different model systems were used: (1) monolayers which were deposited after the method of Langmuir and Blodgett onto glass plates, and (2) bimolecular (“black”) membranes in aqueous phase. The amount of bound protein was determined with a sensitive spectrophotometer. It was found that at low ionic strength about 10¹³ cytochromec molecules per cm² are bound to the lipid surface, which nearly corresponds to a densely packed monolayer. At high ionic strength (∼ 0.1m) or low pH (pH<3), the adsorbed protein layer becomes unstable. This result indicates that the interaction is mainly electrostatic. In accordance with this conclusion is the observation that the rate of adsorption is diffusion controlled; i.e., almost every protein molecule hitting the surface is bound. The cytochromec monolayer can be reduced by ascorbate. In contrast to ferrocytochromec in solution, the bound ferrocytochrome was found to be autoxidable.     

Kinetics of the electron transfer reaction of Cytochrome <Emphasis Type="Italic">c</Emphasis><Subscript>552</Subscript> adsorbed on biomimetic electrode studied by time-resolved surface-enhanced resonance Raman spectroscopy and electrochemistry

Cytochrome c ₅₅₂ (Cyt-c ₅₅₂) and its redox partner ba ₃ -oxidase from Thermus thermophilus possess structural differences compared with Horse heart cytochrome c (cyt-c)/cytochrome c oxidase (CcO) system, where the recognition between partners and the electron transfer (ET) process is initiated via electrostatic interactions. We demonstrated in a previous study by surface-enhanced resonance Raman (SERR) spectroscopy that roughened silver electrodes coated with uncharged mixed self-assembled monolayers HS–(CH₂) _n –CH₃/HS–(CH₂) _{n + 1}–OH 50/50, n = 5, 10 or 15, was a good model to mimic the Cyt-c ₅₅₂ redox partner. All the adsorbed molecules are well oriented on such biomimetic electrodes and transfer one electron during the redox process. The present work focuses on the kinetic part of the heterogeneous ET process of Cyt-c ₅₅₂ adsorbed onto electrodes coated with such mixed SAMs of different alkyl chain length. For that purpose, two complementary methods were combined. Firstly cyclic voltammetry shows that the ET between the adsorbed Cyt-c ₅₅₂ and the biomimetic electrode is direct and reversible. Furthermore, it allows the estimation of both the density surface coverage of adsorbed Cyt-c ₅₅₂ and the kinetic constants values. Secondly, time-resolved SERR (TR-SERR) spectroscopy showed that the ET process occurs without conformational change of the Cyt-c ₅₅₂ heme group and allows the determination of kinetic constants. Results show that the kinetic constant values obtained by TR-SERR spectroscopy could be compared to those obtained from cyclic voltammetry. They are estimated at 200, 150 and 40 s⁻¹ for the ET of Cyt-c ₅₅₂ adsorbed onto electrodes coated with mixed SAMs HS–(CH₂) _n –CH₃/HS–(CH₂) _{n + 1}–OH 50/50, n = 5, 10 or 15, respectively. Presented at the joint biannual meeting of the SFB-GEIMM-GRIP, Anglet France, 14–19 October, 2006.     

The role of arginine 143 in the electrostatics and mechanism of Cu,Zn superoxide dismutase: Computational and experimental evaluation by mutational analysis

Cu, Zn superoxide dismutase protects cells from oxidative damage by removing superoxide radicals in one of the fastest enzyme reactions known. The redox reaction at the active-site Cu ion is rate-limited by diffusion and enhanced by electrostatic guidance. To quantitatively define the electrostatic and mechanistic contributions of sequence-invariant Arg-143 in human Cu, Zn superoxide dismutase, single-site mutants at this position were investigated experimentally and computationally. Rate constants for several Arg-143 mutants were determined at different pH and ionic strength conditions using pulse radiolytic methods and compared to results from Brownian dynamics simulations. At physiological pH, substitution of Arg-143 by Lys caused a 2-fold drop in rate, neutral substitutions (Ile, Ala) reduced the rate about 10-fold, while charge-reversing substitutions (Asp, Glu) caused a 100-fold decrease. Position 143 mutants showed pH dependencies not seen in other mutants. At low pH, the acidic residue mutations exhibited pro-tonation/deprotonation effects. At high pH, all enzymes showed typical decreases in rate except the Lys mutant in which the rate dropped off at an unusually low pH. Increasing ionic strength at acidic pH decreased the rates of the wild-type enzyme and Lys mutant, while the rate of the Glu mutant was unaffected. Increasing ionic strength at higher pH (>10) increased the rates of the Lys and Glu mutants while the rate of the wild-type enzyme was unaffected. Reaction simulations with Brownian dynamics incorporating electrostatic effects tested computational predictability of ionic strength dependencies of the wild-type enzyme and the Lys, Ile, and Glu mutants. The calculated and experimental ionic strength profiles gave similar slopes in all but the Glu mutant, indicating that the electrostatic attraction of the substrate is accurately modeled. Differences between the calculated and experimental rates for the Glu and Lys mutants reflect the mechanistic contribution of Arg-143. Results from this joint analysis establish that, aside from the Cu ligands, Arg-143 is the single most important residue in Cu, Zn superoxide dismutase both electrostatically and mechanistically, and provide an explanation for the evolutionary selection of arginine at position 143. © 1994 Wiley-Liss, Inc.