Interaction of Natronobacterium pharaonis phoborhodopsin (sensory rhodopsin II) with its cognate transducer probed by increase in the thermal stability

Pharaonis phoborhodopsin (ppR, also called Natronobacterium pharaonis sensory rhodopsin II) and its transducer protein, pharaonis halobacterial transducer of ppR (pHtrII), form a signaling complex, and light signals are transmitted from the sensor to the transducer by the protein-protein interaction. A truncated pHtrII(1-159) consisting of intramembrane helices (expressing amino acid residues from the first to the 159th position) and ppR form the complex in a solution containing 0.1% n-dodecyl-beta-D-maltoside. At 75-85 degrees C, the time-dependent color loss of ppR was caused by denaturation. We found that pHtrII(1-159) retarded the denaturation rate of ppR. This increase in the thermal stability was used as a probe for the binding ability in the dark. Tyr199 of ppR and Asn74 of pHtrII(1-114) were proposed as amino acid residues interacting with each other through hydrogen bonding. Then,ppR and pHtrII(1-159) mutants at these positions were prepared to examine the effect on the binding in the dark. The wild-type and Y199F mutant can bind pHtrII(1-159), suggesting that the hydrogen bonding between these specific amino acid residues may not be the only cause of the binding, but the hydrophobic interaction via phenyl ring of ppR may contribute dominantly.     

Dynamics change of phoborhodopsin and transducer by activation: study using D75N mutant of the receptor by site-directed solid-state 13C NMR

Pharaonis phoborhodopsin (ppR or sensory rhodopsin II) is a negative phototaxis receptor of Natronomonas pharaonis, and forms a complex, which transmits the photosignal into cytoplasm, with its cognate transducer (pHtrII). We examined a possible local dynamics change of ppR and its D75N mutant complexed with pHtrII, using solid-state (13)C NMR of [3-(13)C]Ala- and [1-(13)C]Val-labeled preparations. We distinguished Ala C(beta) (13)C signals of relatively static stem (Ala221) in the C-terminus of the receptors from those of flexible tip (Ala228, 234, 236 and 238), utilizing a mutant with truncated C-terminus. The local fluctuation frequency at the C-terminal tip was appreciably decreased when ppR was bound to pHtrII, while it was increased when D75N, that mimics the signaling state because of disrupted salt bridge between C and G helices prerequisite for the signal transfer, was bound to pHtrII. This signal change may be considered with the larger dissociation constant of the complex between pHtrII and M-state of ppR. At the same time, it turned out that fluctuation frequency of cytoplasmic portion of pHtrII is lowered when ppR is replaced by D75N in the complex with pHtrII. This means that the C-terminal tip partly participates in binding with the linker region of pHtrII in the dark, but this portion might be released at the signaling state leading to mutual association of the two transducers in the cytoplasmic regions within the ppR/pHtrII complex.     

Pharaonis phoborhodopsin binds to its cognate truncated transducer even in the presence of a detergent with a 1:1 stoichiometry

Pharaonis phoborhodopsin (ppR) (also pharaonis sensory rhodopsin II) is a receptor of the negative phototaxis of Natronobacterium pharaonis. ppR forms a complex with its pharaonis halobacterial transducer (pHtrII), and this complex transmits the light signal to the sensory system in the cytoplasm. The expressed C-terminal-His tagged ppR and C-terminal-His tagged truncated pHtrII (t-Htr) in Escherichia coli (His means the 6x histidine tag) form a complex even in the presence of 0.1% of n-dodecyl-beta-D-maltoside, and the M-decay of the complex became about twice slower than that of ppR alone. The photocycling rates under varying concentration ratios of ppR to t-Htr in the presence of detergent were measured. The data were analyzed on the following assumptions: (1) the M-decay of both ppR alone and the complex followed a single exponential decay with different time constants; and (2) the M-decay under varying concentration ratios of ppR to t-Htr, therefore, followed a biexponential decay function which combined the decay of the free ppR and that of the complex as photoreactive species. From these analyses we estimated the dissociation constant (15.2 +/- 1.8 microM) and the number of binding sites (1.2 +/- 0.08).     

Electric-field effects in dry films of D85N and D85,96N mutant bacteriorhodopsin

In the D85N mutant of the protein bacteriorhodopsin (BR), the Schiff base, by which the retinal chromophore is bound to the protein, exhibits an abnormally low proton affinity (pKa approximately 8.9). Recent experiments on thin films of this protein have shown that this causes the protonation state of the Schiff base, and thus the visible absorption spectrum, to be sensitive to external electric fields. In this paper, we explore the dependence of this effect on parameters such as pH, humidity, and film thickness. The results of these experiments point to the importance of water molecules bound in the acceptor part of the proton channel as sources and donors in field-induced proton-transfer reactions. We describe additional results obtained with the D85,96N mutant, which also exhibits a low Schiff-base pK. The similar behavior of the two mutants under applied electric fields at high pH implies that the residue Asp-96 plays no role in field-induced Schiff-base protonation.     

Assembly of the covalent linkage between lipoic acid and its cognate enzymes

Lipoic acid is synthesized from octanoic acid by insertion of sulfur atoms at carbons 6 and 8 and is covalently attached to a pyruvate dehydrogenase (PDH) subunit. We show that sulfur atoms can be inserted into octanoyl moieties attached to a PDH subunit or a derived domain. Escherichia coli lipB mutants grew well when supplemented with octanoate in place of lipoate. Octanoate growth required both lipoate protein ligase (LplA) and LipA, the sulfur insertion protein, suggesting that LplA attached octanoate to the dehydrogenase and LipA then converted the octanoate to lipoate. This pathway was tested by labeling a PDH domain with deuterated octanoate in an E. coli strain devoid of LipA activity. The labeled octanoyl domain was converted to lipoylated domain upon restoration of LipA. Moreover, octanoyl domain and octanoyl-PDH were substrates for sulfur insertion in vitro.     

Electric signals of light excited bacteriorhodopsin mutant D96N.

The study of mutant D96N played an important role in understanding proton translocation by light driven bacteriorhodopsin. Our measurement of photoelectric current for single and double flash illumination revealed new details of the photocycle of this mutant. With double flash excitation we found an intermediate absorbing near the wavelength of the ground state of bacteriorhodopsin (bR) but pumping in the opposite direction. This intermediate has the same lifetime as the species described by Zimányi et al. [Proc. Natl. Acad. Sci. USA 96 (1999) 4414-4419] and was assigned to early recovery of a fraction of the ground state after excitation. Because the electric response does not reconcile with that of the ground state, we tentatively assign it to the L intermediate or to an intermediate similar in absorption to bR (bR').     

Participation of the surface structure of Pharaonis phoborhodopsin, ppR and its A149S and A149V mutants, consisting of the C-terminal alpha-helix and E-F loop, in the complex-formation with the cognate transducer pHtrII, as revealed by site-directed 13C solid-state NMR

We have recorded 13C solid state NMR spectra of [3-13C]Ala-labeled pharaonis phoborhodopsin (ppR) and its mutants, A149S and A149V, complexed with the cognate transducer pharaonis halobacterial transducer II protein (pHtrII) (1-159), to gain insight into a possible role of their cytoplasmic surface structure including the C-terminal alpha-helix and E-F loop for stabilization of the 2:2 complex, by both cross-polarization magic angle spinning (CP-MAS) and dipolar decoupled (DD)-MAS NMR techniques. We found that 13C CP-MAS NMR spectra of [3-13C]Ala-ppR, A149S and A149V complexed with the transducer pHtrII are very similar, reflecting their conformation and dynamics changes caused by mutual interactions through the transmembrane alpha-helical surfaces. In contrast, their DD-MAS NMR spectral features are quite different between [3-13C]Ala-A149S and A149V in the complexes with pHtrII: 13C DD-MAS NMR spectrum of [3-13C]Ala-A149S complex is rather similar to that of the uncomplexed form, while the corresponding spectral feature of A149V complex is similar to that of ppR complex in the C-terminal tip region. This is because more flexible surface structure detected by the DD-MAS NMR spectra are more directly influenced by the dynamics changes than the CP-MAS NMR. It turned out, therefore, that an altered surface structure of A149S resulted in destabilized complex as viewed from the 13C NMR spectrum of the surface areas, probably because of modified conformation at the corner of the helix E in addition to the change of hydropathy. It is, therefore, concluded that the surface structure of ppR including the C-terminal alpha-helix and the E-F loops is directly involved in the stabilization of the complex through conformational stability of the helix E.     

Quantum and molecular mechanical study of the first proton transfer in the catalytic cycle of cytochrome P450cam and its mutant D251N

In the catalytic cycle of cytochrome P450cam, the hydroperoxo intermediate (Cpd 0) is formed by proton transfer from a reduced oxyheme complex (S5). This process is drastically slowed down when Asp251 is mutated to Asn (D251N). We report quantum mechanical/molecular mechanical (QM/MM) calculations that address this proton delivery in the doublet state through a hydrogen-bond network in the Asp251 channel, both for the wild-type enzyme and the D251N mutant, using four different active-site models. For the wild-type, we find a facile concerted mechanism for proton transfer from protonated Asp251 via Wat901 and Thr252 to the FeOO moiety, with a barrier of about 1 kcal/mol and a high exothermicity of more than 20 kcal/mol. In the D251N mutant with a neutral Asn251 residue, the proton transfer is almost thermoneutral or slightly exothermic in the three models considered. It is still very facile when the Asn251 residue adopts a conformation analogous to Asp251 in the wild-type enzyme, but the barrier increases significantly when the Asn251 side chain flips (as indicated by classical molecular dynamics simulations). This flip disrupts the hydrogen-bond network and hence the proton-transfer pathway, which causes a longer lifetime of S5 in the D251N mutant (consistent with experimental observations). The entry of an additional water molecule into the active site of D251N with flipped Asn251 regenerates the hydrogen-bond network and provides a viable mechanism for proton delivery in the mutant, with a moderate barrier of about 7 kcal/mol.     

Interaction of the halobacterial transducer to a halorhodopsin mutant engineered so as to bind the transducer: Cl- circulation within the extracellular channel

An alkali-halophilic archaeum, Natronomonas pharaonis, contains two rhodopsins that are halorhodopsin (phR), a light-driven inward Cl- pump and phoborhodopsin (ppR), the receptor of negative phototaxis functioning by forming a signaling complex with a transducer, pHtrII (Sudo Y. et al., J. Mol. Biol. 357 [2006] 1274). Previously, we reported that the phR double mutant, P240T/F250Y(phR), can bind with pHtrII. This mutant itself can transport Cl-, while the net transport was stopped upon formation of the complex. The flash-photolysis data were analyzed by a scheme in which phR --> 4 P1 --> P2 --> 4 P3 --> P4 --> phR. The P3 of the wild-type and the double mutant contained two components, X- and O-intermediates. After the complex formation, however, the P3 of the double mutant lacked the X-intermediate. These observations imply that the X-intermediate (probably the N-intermediate) is the state having Cl- in the cytoplasmic binding site and that the complex undergoes an extracellular Cl- circulation because of the inhibition of formation of the X-intermediate.     

Photoinduced surface potential change of bacteriorhodopsin mutant D96N measured by scanning surface potential microscopy

We report the direct measurement of photoinduced surface potential differences of wild-type (WT) and mutant D96N bacteriorhodopsin (BR) membranes at pH 7 and 10.5. Atomic force microscopy (AFM) and scanning surface potential microscopy (SSPM) were used to measure the BR membrane with the extracellular side facing up. We present AFM and SSPM images of WT and mutant D96N in which the light-dark transition occurred in the mid-scan of a single BR membrane. Photosteady-state populations of the M state were generated to facilitate measurement in each sample. The photoinduced surface potential of D96N is 63 mV (peak to valley) at pH 10.5 and is 48 mV at pH 7. The photoinduced surface potential of WT is 37 mV at pH 10.5 and approximately 0 at pH 7. Signal magnitudes are proportional to the amount of M produced at each pH. The results indicated that the surface potentials were generated by photoformation of surface charges on the extracellular side of the membrane. Higher surface potential correlated with a longer lifetime of the charges. A mechanistic basis for these signals is proposed, and it is concluded that they represent a steady-state measurement of the B2 photovoltage.     

C75N+位置异构体的电子结构和光谱研究

杂原子的介入可改变纯碳笼的电子结构, 使其在超导、光电子器件及有机铁磁体等方面得到应用, 还可改善其氧化还原性能, 提高反应活性, 因而引起人们的研究兴趣[1～3]. Averdung[1]研究了C59N+与H的反应, 用质谱检测到C59NH和C59NH+2, 并用AM1方法优化其结构; Lamparth[2]以双氮杂富勒烯为前体, 合成了C59N+和C69N+, 测定中间体的 1H NMR谱、 UV谱及产物的FAB质谱, 并用 15N标记法证实了最强的碎片峰是N原子进入母体碳笼骨架所致. Diederich[3]观察到C76氮化物的FAB质谱信号, 但未给出进一步信息. 本文用INDO系列方法对氮杂富勒烯C75N+位置异构体的结构和稳定性进行理论研究, 找出最稳定的异构体, 计算其电子吸收光谱, 为实验室合成分离提供理论依据.     

Hyperfine coupling constants of the azafullerenes C19N, C59N, C69N, and C75N

The isomers of the nitrogen-substituted fullerenes (azafullerenes) C19N, C59N, C69N, and C75N are examined using all-electron Gaussian atomic orbital basis density functional theory, to determine the doublet radical geometries and hyperfine coupling constants. We find that the inaccuracy of previously calculated hyperfine coupling constants of C59N resulted from a poor treatment of the geometry optimization. We find that UB3LYP minimization of the radical geometry in the 6-31G basis, followed by single-point evaluation of the hyperfine constants in which an expanded basis is used on the atomic sites of interest, forms an efficient compromise between computational cost and accuracy with respect to experimental hyperfine constants. Using this approach, we assign the hyperfine signals observed in experiments on the C69N radical by calculating the hyperfine coupling constants for all five of the isomers and examine the electron spin density distribution. Finally, we present predicted hyperfine coupling constants for the isomers of C19N and C75N for use in the interpretation of future experiments.     

Direct observation of enhanced translocation of a homeodomain between DNA cognate sites by NMR exchange spectroscopy

A novel approach is presented for studying the kinetics of specific protein-DNA interactions by NMR exchange spectroscopy. The experimental design involves the direct observation of translocation of a homeodomain between cognate sites on two oligonucleotide duplexes, differing by only a single base pair at the edge of the DNA recognition sequence. The single base-pair change perturbs the 1H-15N correlation spectrum of a number of residues, while leaving the affinity for the DNA unchanged. The exchange process has apparent rate constants in the 5-20 s-1 range which are linearly dependent upon the concentration of free DNA. These rates are about 3 orders of magnitude larger than the dissociation rate constant determined by gel shift assays at nanomolar DNA concentrations. The complete NMR exchange data set, comprising auto- and cross-peak intensities as a function of mixing time at five concentrations of free DNA, can be fit simultaneously to a simple model in which protein translocation between DNA duplexes occurs via a second-order process (with rate constants of approximately 6 x 104 M-1 s-1) involving direct collision of a protein-DNA complex with free DNA. This is akin to intersegmental transfer, and a physical model for the process is discussed. Rapid translocation at high concentrations of free DNA observed directly by NMR exchange spectroscopy reconciles the long half-lives of protein-DNA complexes measured by biochemical analysis in vitro with the highly dynamic behavior of such complexes observed in vivo. The relevance of this mechanism to the kinetics of protein-DNA interactions within the cell is discussed.     

Protein-protein interaction of a Pharaonis halorhodopsin mutant forming a complex with Pharaonis halobacterial transducer protein II detected by Fourier-transform infrared spectroscopy

Pharaonis halorhodopsin (pHR) functions as a light-driven inward chloride ion pump in Natoronomonas pharaonis, while pharaonis phoborhodopsin (ppR; also called pharaonis sensory rhodopsin II, pSRII), is a light sensor for negative phototaxis. ppR forms a 2:2 complex with its cognate transducer protein (pHtrII) through intramembranous hydrogen bonds: Tyr199(ppR)-Asn74(pHtrII) and Thr189(ppR)-Glu43 (pHtrII), Ser62(pHtrII). It was reported that a pHR mutant (P240T/F250Y), which possesses the hydrogen-bonding sites, impairs its pumping activity upon complexation with pHtrII. In this study, effect of the complexation with pHtrII on the structural changes upon formation of the K, L(1) and L(2) intermediates of pHR was investigated by use of Fourier-transform infrared spectroscopy. The vibrational changes of Tyr250(pHR) and Asn74(pHtrII) were detected for the L(1) and L(2) intermediates, supporting that Tyr250(pHR) forms a hydrogen bond with Asn74(pHtrII) as similarly to Tyr199(ppR). The conformational changes of the retinal chromophore were never affected by complexation with pHtrII, but amide-I vibrations were clearly different in the absence and presence of pHtrII. The molecular environment around Asp156(pHR) in helix D is also slightly affected. These additional structural changes are probably related to blocking of translocation of a chloride ion from the extracellular to the cytoplasmic side during the photocycle.     

Dynamics of a myoglobin mutant enzyme: 2D IR vibrational echo experiments and simulations

Myoglobin (Mb) double mutant T67R/S92D displays peroxidase enzymatic activity in contrast to the wild type protein. The CO adduct of T67R/S92D shows two CO absorption bands corresponding to the A(1) and A(3) substates. The equilibrium protein dynamics for the two distinct substates of the Mb double mutant are investigated by using two-dimensional infrared (2D IR) vibrational echo spectroscopy and molecular dynamics (MD) simulations. The time-dependent changes in the 2D IR vibrational echo line shapes for both of the substates are analyzed using the center line slope (CLS) method to obtain the frequency-frequency correlation function (FFCF). The results for the double mutant are compared to those from the wild type Mb. The experimentally determined FFCF is compared to the FFCF obtained from molecular dynamics simulations, thereby testing the capacity of a force field to determine the amplitudes and time scales of protein structural fluctuations on fast time scales. The results provide insights into the nature of the energy landscape around the free energy minimum of the folded protein structure.     

Rate coefficient measurements for reactions between uracil and N(2D0) atoms

Rate coefficients of the reactions between uracil molecules and excited nitrogen atoms (N(²D₀)) have been measured at room temperature using the dynamic flowing afterglow method. The measured rate coefficients are 3.3 and 2.7 × 10⁻¹⁰ cm³ s⁻¹.     

Crystal Structure of a Supramolecular Complex Formed between 1-bromo-2-iodo-tetrafluoroethane and N,N,N′,N′-tetramethyl-ethylenediamine

X-ray analysis has revealed that N,N,N′,N′-tetramethyl-ethylenediamine 1 form donor–acceptor complex 3 with 1-bromo-2-iodo-tetrafluoroethane 2, in which the N X (X = Br, I) distances are longer than the average covalent bond length between X and N, but are also definitively shorter than the sum of the corresponding van der Waals radii of X and N, thus that indicating weak interactions between the nitrogen and bromine or iodine atoms. In our experimental section, a valuable method for recrystallization and collect X-ray data from crystals that easily exhibit decay and can be cracked is reported.     

Influence of Isotope Effects on Product Polarizations of N(2D)+D2, N(2D)+H2 and N(2D)+HD Reactive Systems

To figure out the influence of isotope effect on product polarizations of the N(²D)+D₂ reactive system and its isotope variants, quasi-classical trajectory(QCT) calculation was performed on Ho’s potential energy surface(PES) of ²A″ state. Product polarizations such as product distributions of P(θ_r), P(φ_r) and P(θ_r,φ_r), as well as the generalized polarization-dependent differential cross sections(PDDCSs) were discussed and compared in detail among the four product channels of the title reactions. Both the intermolecular and intramolecular isotope effects were proved to be influential on product polarizations.