Fig. 2 Absorbance changes during reaction of the fully reduced ba3 CytcO with O2. Absorbance changes during reaction of the fully reduced ba3 CytcO with.

Slides:



Advertisements
Similar presentations
Volume 106, Issue 1, Pages (February 2017)
Advertisements

Kinga Turzó, Gábor Laczkó, Zoltán Filus, Péter Maróti 
Volume 91, Issue 8, Pages (October 2006)
Michael J. Reddish, Robert Callender, R. Brian Dyer 
Volume 98, Issue 7, Pages (April 2010)
Volume 111, Issue 7, Pages (October 2016)
Volume 103, Issue 2, Pages (July 2012)
Volume 99, Issue 1, Pages (July 2010)
Low-Temperature Electron Transfer from Cytochrome to the Special Pair in Rhodopseudomonas viridis: Role of the L162 Residue  José M. Ortega, Barbara Dohse,
Fig. 2 Time-resolved THz reflectivity from MAPI after band-edge optical excitation. Time-resolved THz reflectivity from MAPI after band-edge optical excitation.
Fig. 2 Nonlinearities in a cavity-embedded perovskite single crystal.
Comparison of network robustness measures over a larger time window
Fig. 5 In vivo MIP imaging of lipid and protein in C. elegans.
Fig. 4 Estimations of nonlinear functionals of a single-qubit state with the quantum Fredkin gate. Estimations of nonlinear functionals of a single-qubit.
Fig. 1 Reconstitution of DCV membrane fusion.
Fig. 2 Absolute recovery of species richness and relative recovery of species richness and composition in relation to stand age for Neotropical secondary.
Fig. 2 Transport properties of a BP transistor at low temperature.
Fig. 5 Metafluorophores with different photostability.
Fig. 2 The arrangements of metal core and ligands.
Fig. 3 Evolution of absorber with annealing.
Fig. 1 Demographic shifts in knowledge producers.
Fig. 1 Pump-probe signatures of vermilion (red HgS), black HgS, and metallic Hg. Pump-probe signatures of vermilion (red HgS), black HgS, and metallic.
Wei Zhang, John S. Olson, George N. Phillips  Biophysical Journal 
Fig. 4 Reentrant and doubly reentrant transition state analysis.
Fig. 3 Tracing Poynting flux along Polar’s orbit during a period of 28 days, which includes a moderate storm and a major storm. Tracing Poynting flux along.
Fig. 5 Binding dynamics of the noninactivating channel.
Fig. 5 High-speed printing and process performance metrics.
Fig. 3 Saturation velocity of BP FETs.
Fig. 4 Structural details of tRNA binding to Elp123.
Fig. 1 Cryo-EM structure of yeast Elp123 showing its active site.
Fig. 1 The structure of the 3DGraphene foam.
Fig. 2 Full-frame images recording the violation of a Bell inequality in four images. Full-frame images recording the violation of a Bell inequality in.
Fig. 3 Circuits with an INHIBIT logic gate, multiple inputs (fan-in), or multiple outputs (fan-out). Circuits with an INHIBIT logic gate, multiple inputs.
Fig. 2 Mineralization and surface colonization of films of three PBAT [poly(butylene adipate-co-terephthalate)] variants during a 6-week soil incubation.
Fig. 3 Extension of our proposed programmable synthesis to the selective synthesis of a wide variety of liposome/metal hybrids. Extension of our proposed.
Fig. 5 Hydrogenation of activated C═C bonds via direct, light-driven activation of TsOYE using NAD+. Hydrogenation of activated C═C bonds via direct, light-driven.
Fig. 2 NAD+-sensitized reduction of O2and oxidation of H2O.
Fig. 2 2D QWs of different propagation lengths.
Fig. 1 Maximum likelihood tree relating the Denisova 2 mtDNA to other ancient and present-day mtDNAs. Maximum likelihood tree relating the Denisova 2 mtDNA.
Fig. 2 EUV TG signal. EUV TG signal. Black lines in (A), (B), and (C) are the EUV TG signals from Si3N4 membranes at LTG = 110, 85, and 28 nm, respectively,
Fig. 4 EUV TG signal from Si.
Fig. 6 WPS imaging of different chemical components in living cells.
Fig. 3 ET dynamics on the control and treatment watersheds during the pretreatment and treatment periods. ET dynamics on the control and treatment watersheds.
Fig. 2 Assignment of back-exchanged deuterated NaK2K.
Fig. 4 Experimental outputs.
Fig. 4 OER performance of ACoO3 (A = Ca, Sr) in alkaline solutions with different pH. OER performance of ACoO3 (A = Ca, Sr) in alkaline solutions with.
Fig. 2 Results of the learning and testing phases.
Fig. 4 SPICE simulation of stochasticity.
Fig. 4 Randomized benchmarking measurement.
Fig. 2 Sampling. Sampling. (A) Extant stratigraphic section. Zenithal (B) and frontal (C) views of the flowstone capping the excavated deposit. The rectangle.
Fig. 2 Electrical properties of CNT array FETs and influence of postdeposition treatment on conductance. Electrical properties of CNT array FETs and influence.
Fig. 4 Theoretical analysis of the FeN4/GN structure and the catalytic reaction process by DFT calculations. Theoretical analysis of the FeN4/GN structure.
Fig. 2 NP characterization.
Fig. 7 Global change in the collective mass for wild mammals, humans, cattle, and all livestock for the years 1900–2050. Global change in the collective.
Fig. 1 Fractional coverage of the mapping method used in this study.
Fig. 4 Superconductivity gap and specific heat jump.
by Mark T. Edmonds, James L
Fig. 5 Potential-energy energy profiles of 1-HAQ.
Fig. 2 Comparison of the observed DRs and the estimates by the VR model and FL. Comparison of the observed DRs and the estimates by the VR model and FL.
Fig. 3 Ultrafast PM spectroscopy of PEPI film excited at 3.1 eV.
Volume 99, Issue 1, Pages (July 2010)
Fig. 19 Comparisons between sky brightness NPS CCD observations and atlas predictions. Comparisons between sky brightness NPS CCD observations and atlas.
Fig. 5 Fabrication of origami structures by two-side illuminations.
Fig. 2 OH formation and speciation in the PAA – Fe(II) system.
Fig. 2 Supraballs and films from binary SPs.
The combined signal spectra of PSD for protons and helium nuclei
Fig. 3 Characterization of the luminescence temporal time traces.
Fig. 4 Scaling laws distinguish biochemical networks from random networks across levels of organization. Scaling laws distinguish biochemical networks.
Fig. 4 Evolution of rate constants over varying interaction strengths.
Fig. 1 X-ray structures of the ScoI·Cu2+ and CoxB·CuA holo-proteins, and formation of the ScoI·Cu2+·CoxB complex. X-ray structures of the ScoI·Cu2+ and.
Presentation transcript:

Fig. 2 Absorbance changes during reaction of the fully reduced ba3 CytcO with O2. Absorbance changes during reaction of the fully reduced ba3 CytcO with O2. (A and B) pH 7 at 10° and 45°C, respectively. (C and D) pH 10 at 10° and 45°C, respectively. At 610 and 560 nm, the absorbance changes are mainly attributed to redox changes at heme a3 and heme b, respectively. The black lines are fits of the data with a model that is described by a sum of three exponential functions. The rate constants obtained from the fit are given in the text and in Table 1. The difference between the fit and the data (that is, the residuals) is shown below each panel. In addition, in (A), we show the residuals of a fit with a single rate constant (5 × 104 s−1) for electron transfer from heme b to the catalytic site and PR formation (gray lines). Experimental conditions after mixing: 0.6 to 0.8 μM CytcO (scaled to 1 μM), 0.05% DDM, 90 mM Hepes (pH 7) or 90 mM CAPS (pH 10), and ~1 mM O2. The cuvette path length was 1.00 cm. The 560-nm traces are shifted up by 1.7 × 10−3 units for clarity. Federica Poiana et al. Sci Adv 2017;3:e1700279 Copyright © 2017, The Authors