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Biomedical subjects

Masahide Terazima

Publications and source records attributed to Masahide Terazima.

26 records · Page 2Linked to original sources

Kinetics of intermolecular interaction during protein folding of reduced cytochrome c.

Kinetics of intermolecular interaction between reduced cytochrome c (Cyt c) protein and solvent during the protein-refolding process is studied by monitoring the time dependence of apparent diffusion coefficient (D) using the pulsed-laser-induced transient grating technique. The refolding was triggered by photoinduced reduction of unfolded Fe(III) Cyt c in 3.5 M guanidine hydrochloride (GdnHCl) solution and the change in the diffusion coefficient was monitored in time domain. The relationship between D and the protein conformations under equilibrium condition were investigated at various GdnHCl concentrations using a photolabeling reagent. The time dependence of the observed transient grating signal was analyzed using these data and two models: a continuous change model of the intermolecular interaction and a two-state model. It was found that the TG signals in various time ranges can be consistently reproduced well by the two-state model. The dynamics of D is expressed well by a single exponential function with a rate constant of 22 +/- 7 s(-1) in a whole time range. The folding process of Cyt c is discussed based on these observations.

Carbon Monoxide↗

Time-resolved detection of sensory rhodopsin II-transducer interaction.

The dynamics of protein conformational change of Natronobacterium pharaonis sensory rhodopsin II (NpSRII) and of NpSRII fused to cognate transducer (NpHtrII) truncated at 159 amino acid sequence from the N-terminus (NpSRII-DeltaNpHtrII) are investigated in solution phase at room temperature by the laser flash photolysis and the transient grating methods in real time. The diffusion coefficients of both species indicate that the NpSRII-DeltaNpHtrII exists in the dimeric form in 0.6% dodecyl-beta-maltopyranoside (DM) solution. Rate constants of the reaction processes in the photocycles determined by the transient absorption and grating methods agree quite well. Significant differences were found in the volume change and the molecular energy between NpSRII and NpSRII-DeltaNpHtrII samples. The enthalpy of the second intermediate (L) of NpSRII-DeltaNpHtrII is more stabilized compared with that of NpSRII. This stabilization indicates the influence of the transducer to the NpSRII structure in the early intermediate species by the complex formation. Relatively large molecular volume expansion and contraction were observed in the last two steps for NpSRII. Additional volume expansion and contraction were induced by the presence of DeltaNpHtrII. This volume change, which should reflect the conformational change induced by the transducer protein, suggested that this is the signal transduction process of the NpSRII-DeltaNpHtrII.

Archaeal Proteins↗

A novel method for study of protein folding kinetics by monitoring diffusion coefficient in time domain.

Molecular diffusion process after the photo-induced electron injection to ferric cytochrome c (Fe(III) cyt c) in guanidine hydrochloride (GdnHCl) 3.5 M buffer solution is studied by the time-resolved transient grating technique. Circular dichroism studies have revealed that Fe(III) cyt c is unfolded under this condition but the reduced form, Fe(II) cyt c, is folded. Hence, this pulsed laser-induced reduction should initiate the folding process of cyt c. The observed transient grating signal shows prominent features, which have never been observed before. Based on several characteristic points, we concluded that the apparent diffusion coefficient (D) of Fe(II) cyt c after the reduction is time dependent, which must be associated with the protein folding dynamics. This time-dependent apparent D should reflect either the continuous time development of the hydrodynamic radius or population change of the unfolded and folded states during the folding dynamics. This is the first observation of the time-dependent apparent D during any chemical reaction, and this time-dependent measurement of D should be a unique and powerful way to study the protein folding kinetics from a viewpoint of the protein's shape or the protein-water intermolecular interaction.

Biophysics↗

Photoreaction of caged ATP studied by the time-resolved transient grating method.

The photoreaction of caged ATP, P3-[1-(2-nitrophenyl)ethyl]adenosine-5'-triphosphate, has been investigated using the time-resolved transient grating (TG) method. We found that a feature of the TG signal time profile depends sensitively on the grating wavenumber (q) after the photoexcitation of caged ATP. This q-dependent feature of the TG signal was interpreted based on a model where the ATP release rate is comparable to the molecular diffusion process. We found that the TG signals at various q can be consistently analyzed based on this model and the ATP release rate determined. The enthalpy and volume changes of the reaction have been determined by quantitative measurement of the grating and photoacoustic signals.

Acoustics↗

Structural dynamics of distal histidine replaced mutants of myoglobin accompanied with the photodissociation reaction of the ligand.

Protein dynamics observed by the transient grating (TG) method are studied for some site-directed mutants at the distal histidine of myoglobin (H64L, H64Q, H64V). The time profiles of the TG signals are very sensitive to the amino acid residue of the 64 position. It was found that the sensitivity is mostly caused by the different rates of the ligand escape from the protein to solvent and the magnitude of the molecular volume change. Several molecular origins of the volume difference between MbCO and Mb, such as the electrostatic interaction in the distal pocket, movement of helices, and distal water, are proposed. Interestingly, the volume difference between the CO-trapped Mb inside the protein interior and Mb is similar to that of the partial molar volume of CO in organic solvent. The effect of mutation on the nature of the CO trapped site is discussed.

Amino Acid Substitution↗

Themodynamic and transport properties of intermediate states of the photocyclic reaction of photoactive yellow protein.

Themodynamic and transport properties of intermediate states of the photocyclic reaction of photoactive yellow protein (PYP) were studied by a combination of the pulsed laser-induced transient grating (TG), transient lens (TrL), and photoacoustic (PA) spectroscopies from tens of nanoseconds to hundreds of milliseconds. The diffusion coefficients (D) of PYP in the ground state (pG) and of the second intermediate state (pB) were determined by the TG analysis, and it was found that D of pG is about 1.2 times larger than D of pB. At the same time, D at various denatured conditions were measured using guanidine hydrochloride as the denaturant. D of completely unfolded protein is about 0.4 times that of the native form. The enthalpy of pB is estimated to be 60 kJ/mol by the TrL method with an assumption that the volume change of pB is not sensitive to the temperature. Since the enthalpy of the first intermediate state (pR) is as high as 160 kJ/mol, it implies that most of the photon energy is stored as the strain of the protein in pR, and this may be the driving force for the successive reaction to pB. From the temperature dependence of the volume change, the difference in the thermal expansion coefficients between pG and pR was calculated. All of the characteristic features of PYP, the negative volume change, the larger thermal expansion coefficient, and the slower diffusion process, indicate that the intermediate pR and pB are reasonably interpreted in terms of the unfolded (loosened) protein structure.

Bacterial Proteins↗

Structural change of site-directed mutants of PYP: new dynamics during pR state.

The energetics, protein dynamics, and diffusion coefficients of three mutants of photoactive yellow protein, R52Q, P68A, and W119G, were studied by the transient grating and pulsed laser-induced photoacoustic method. We observed a new dynamics with a lifetime of approximately 1 micro s in the transient grating signal, which is silent by the light absorption technique. This fact indicates that, after the structure change around the chromophore is completed (pR(1)), the protein part located far from the chromophore is still moving to finally create another pR (pR(2)) species, which can transform to the next intermediate, pB. Although the kinetics of pR(2)-->pB-->pG are very different depending on the mutants, the enthalpies of the first long-lived (in micro seconds, 100-micro s range) intermediate species (pR(2)) are similar and very high for all mutants. The diffusion coefficients of the parent (pG) and pB species of the mutants are also similar to that of the wild-type photoactive yellow protein. From the temperature dependence of the volume change, the difference in the thermal expansion coefficients taken as indicator of the flexibility of the structure between pG and pR(2) is measured. They are also similar to that of the wild-type photoactive yellow protein. These results suggest that the protein structures of pR(2) and pB in these mutants are globally different from that of pG, and this structural change is not altered so much by the single amino acid residue mutation. This is consistent with the partially unfolded nature of these intermediate species. On the other hand, the volume changes during pR(1)-->pR(2) are sensitive to the mutations, which may suggest that the volume change reflects a rather local character of the structure, such as the chromophore-protein interaction.

Acoustics↗

Energetics and volume changes of the intermediates in the photolysis of octopus rhodopsin at a physiological temperature.

Enthalpy changes (Delta H) of the photointermediates that appear in the photolysis of octopus rhodopsin were measured at physiological temperatures by the laser-induced transient grating method. The enthalpy from the initial state, rhodopsin, to bathorhodopsin, lumirhodopsin, mesorhodopsin, transient acid metarhodopsin, and acid metarhodopsin were 146 +/- 15 kJ/mol, 122 +/- 17 kJ/mol, 38 +/- 8 kJ/mol, 12 +/- 5 kJ/mol, and 12 +/- 5 kJ/mol, respectively. These values, except for lumirhodopsin, are similar to those obtained for the cryogenically trapped intermediate species by direct calorimetric measurements. However, the Delta H of lumirhodopsin at physiological temperatures is quite different from that at low temperature. The reaction volume changes of these processes were determined by the pulsed laser-induced photoacoustic method along with the above Delta H values. Initially, in the transformation between rhodopsin and bathorhodopsin, a large volume expansion of +32 +/- 3 ml/mol was obtained. The volume changes of the subsequent reaction steps were rather small. These results are compared with the structural changes of the chromophore, peptide backbone, and water molecules within the membrane helixes reported previously.

Animals↗