Reduction and protonation of the secondary quinone acceptor of Rhodobacter sphaeroides photosynthetic reaction center: kinetic model based on a comparison of wild-type chromatophores with mutants carrying Arg -> Ile substitution at sites 207 and 217 in the L-subunit

Autor(en): Cherepanov, DA
Bibikov, SI
Bibikova, MV
Bloch, DA
Drachev, LA
Gopta, OA
Oesterhelt, D
Semenov, AY
Mulkidjanian, AY
Stichwörter: BACTERIAL REACTION CENTERS; BINDING-SITE; Biochemistry & Molecular Biology; Biophysics; CYTOCHROME-C-OXIDASE; DIRECTED MUTANTS; electrogenesis; electron transfer; ELECTRON-TRANSFER; H+ BINDING; membrane potential; photosynthetic reaction center; PROTEIN; protein electrostatics; proton transfer; PURPLE BACTERIA; Q(B) SITE; Rhodobacter sphaeroides; Rhodopseudomonas viridis; RHODOPSEUDOMONAS-VIRIDIS; ubiquinone
Erscheinungsdatum: 2000
Herausgeber: ELSEVIER SCIENCE BV
Journal: BIOCHIMICA ET BIOPHYSICA ACTA-BIOENERGETICS
Volumen: 1459
Ausgabe: 1
Startseite: 10
Seitenende: 34
Zusammenfassung: 
After the light-induced charge separation in the photosynthetic reaction center (RC) of Rhodobacter sphaeroides, the electron reaches, via the tightly bound ubiquinone Q(A), the loosely bound ubiquinone Q(B). After two subsequent flashes of light, Q(B) is reduced to ubiquinol Q(B)H(2). With a semiquinone anion Q(B)(-) formed as an intermediate after the first flash. We studied Q(B)H(2) formation in chromatophores from Rb. sphaeroides mutants that carried Arg --> Ile substitution at sites 207 and 217 in the L-subunit. While Arg-L207 is 17 Angstrom away from Q(B), Arg-L217 is closer (9 Angstrom) and contacts the Q(B)-binding pocket. From the pH dependence of the charge recombination in the RC after the first flash, we estimated Delta G(AB), the free energy difference between the Q(A)(-)Q(B) and Q(A)Q(B)(-) states, and pK(212), the apparent pK of Glu-L212, a residue that is only 4 Angstrom away from Q(B). As expected, the replacement of positively charged arginines by neutral isoleucines destabilized the Q(B)(-) state in the L217RI mutant to a larger extent than in the L207RI one. Also as expected, pK(212) increased by similar to 0.4 pH units in the L207RI mutant. The value of pK(212) in the L217RI mutant decreased by 0.3 pH units, contrary to expectations. The rate of the Q(A)(-)Q(B)(-) --> Q(A)Q(B)H(2) transition upon the second flash, as monitored by electrometry via the accompanying changes in the membrane potential, was two times faster in the L207RI mutant than in the wild-type, but remained essentially unchanged in the L217RI mutant. To rationalize these findings, we developed and analyzed a kinetic model of the Q(A)(-)Q(B)(-) --> Q(A)Q(B)H(2) transition. The model properly described the available experimental data and provided a set of quantitative kinetic and thermodynamic parameters of the Q(B) turnover. The non-electrostatic, `chemical' affinity of the Q(B) Site to protons proved to be as important for the attracting protons from the bulk, as the appropriate electrostatic potential. The mutation-caused changes in the chemical proton affinity could be estimated from the difference between the experimentally established pK(212) shifts and the expected changes in the electrostatic potential at Glu-L212, calculable from the X-ray structure of the RC. Based on functional studies, structural data and kinetic modeling, we suggest a mechanistic scheme of the Q(B) turnover. The detachment of the formed ubiquinol from its proximal position next to Glu-L212 is considered as the rate-limiting step of the reaction cycle. (C) 2000 Elsevier Science B.V. All rights reserved.
ISSN: 00052728
DOI: 10.1016/S0005-2728(00)00110-9

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