PubMed · 92662
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R J Wainwright, D A Brennand-Roper, M N Maisey, E Sowton. 1979-12-08. Cold-pressor test.. https://doi.org/10.1016/s0140-6736(79)92370-5
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The vibrational infrared absorption changes associated with the oxidation of cytochrome b559 (Cyt b559) have been characterized. In photosystem II (PS II) enriched membranes, low-potential (LP) and high-potential (HP) Cyt b559 were investigated by light-induced FTIR difference spectroscopy. The redox transition of isolated Cyt b559 is characterized by protein electrochemistry. On the basis of a model of the assembly of Cyt b559 with the two axial Fe ligands being histidine residues of two distinct polypeptides, each forming a transmembrane alpha-helix [Cramer, W.A., Theg, S.M., & Widger, W.R. (1986) Photosynth. Res. 10, 393-403], the bisimidazole and bismethylimidazole complexes of Fe protoporphyrin IX were electrochemically oxidized and reduced to detect the IR oxidation markers of the heme and its two axial ligands. Major bands at 1674/1553, 1535, and 1240 cm-1 are tentatively assigned to nu 37 (CaCm), nu 38-(CbCb) and delta (CmH) modes, respectively; other bands at 1626, 1613, 1455, 1415, and 1337 cm-1 are assigned to porphyrin skeletal and vinyl modes. Modes at 1103 and 1075/1066 cm-1 are assigned to the 4-methylimidazole and imidazole ligands, respectively. For the isolated Cyt b559, it is shown that both the heme (at 1556-1535, 1337, and 1239 cm-1), the histidine ligands at 1104 cm-1 and the protein (between 1600 and 1700 cm-1 and at 1545 cm-1) are affected by the charge stabilization. The excellent agreement between model compounds and isolated Cyt b559 reinforces the validity of the model of a heme iron coordinated to two histidine residues for Cyt b559. A differential signal at 1656/1641 cm-1 is assigned to peptide C = O mode(s). We speculate that this signal reflects the change in strength of a hydrogen bond formed between the histidine ligand(s) and the polypeptide backbone upon oxidoreduction of the cytochrome. In PS II membranes, the signals characteristic of Cyt b559 photooxidation are found at 1660/1652 and 1625 cm-1, for both the high- and low-potential forms. The differences observed in the amplitude of the 1660/1652-cm-1 band, at 1700 and 1530-1510 cm-1 in the light-induced FTIR difference spectra of Cyt b559 HP and LP, show that the mechanisms of heme oxidation in vivo imply different molecular processes for the two forms Cyt b559 HP and LP.
Effect of the unsaturation of fatty acids in the glycerolipids of thylakoid membranes on low-temperature photoinhibition of photosynthesis was studied by mutation and transformation of the cyanobacterium Synechocystis PCC6803. When grown at 34 degrees C, the wild type contained mono-, di-, and triunsaturated lipids; a mutant, designated Fad6, contained mono- and diunsaturated lipids; and a transformant of Fad6, with a disrupted gene for desaturation and designated Fad6/desA::Kmr, contained only monounsaturated lipids. Fad6/desA::Kmr was the most susceptible among these strains to low-temperature photoinhibition of photosynthesis, whereas Fad6 and the wild type were apparently indistinguishable in terms of sensitivity to photoinhibition. This result suggests that the presence of diunsaturated fatty acids is important in protecting against low-temperature photoinhibition. The photoinhibition at room temperature, although much less significant than that at low temperature, was also affected by the unsaturation of fatty acids. By contrast, the photosynthetic transport of electrons, measured at various temperatures, was not affected by changes in extent of fatty acid unsaturation.
The kinetics of electron transfer from the third highest potential heme (c-552, Em = +20 mV) to the primary donor (P-960) have been measured by flash absorption spectroscopy in isolated reaction centers of Rhodopseudomonas viridis between 300 K and 7 K. The data are analyzed on the basis of three exponential components with a very fast phase (t1/2 = 120 ns) dominating at high temperature and a very slow one (t1/2 = 1.2 ms) at low temperature. This multiphasic behavior is interpreted in terms of the existence of three states with a temperature-dependent population and a very limited effect of the temperature on the kinetics for each state.