Time-resolved absorption and photothermal measurements with sensory rhodopsin I from Halobacterium salinarum.
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An expansion accompanying the formation of the first intermediate in the photocycle of transducer-free sensory rhodopsin I (SRI) was determined by means of time-resolved laser-induced optoacoustic spectroscopy. For the native protein (SRI-WT), the absolute value of the expansion is approximately 5.5 mL and for the mutant SRI-D76N, approximately 1.5 mL per mol of phototransformed species (in 0.5 M NaCl), calculated by using the formation quantum yield for the first intermediate (S610) of Phi610 = 0.4 +/- 0.05 for SRI-WT and 0.5 +/- 0.05 for SRI-D76N, measured by laser-induced optoacoustic spectroscopy and by laser flash photolysis. The similarity in Phi610 and in the determined value of the energy level of S610, E610 = (142 +/- 12) kJ/mol for SRI-WT and SRI-D76N indicates that Asp76 is not directly involved in the first step of the phototransformation. The increase with pH of the magnitude of the structural volume change for the formation of S610 in SRI-WT and in SRI-D76N upon excitation with 580 nm indicates also that amino acids other than Asp76, and other than those related to the Schiff base, are involved in the process. The difference in structural volume changes as well as differences in the activation parameters for the S610 decay should be attributed to differences in the rigidity of the cavity surrounding the chromophore. Except for the decay of the first intermediate, which is faster than in the SRI-transducer complex, the rate constants of the photocycle for transducer-free SRI in detergent suspension are strongly retarded with respect to wild-type membranes (this comparison should be done with great care because the preparation of both samples is very different). (+info)
Proton circulation during the photocycle of sensory rhodopsin II.
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Sensory rhodopsin II (SRII) in Halobacterium salinarum membranes is a phototaxis receptor that signals through its bound transducer HtrII for avoidance of blue-green light. In the present study we investigated the proton movements during the photocycle of SRII in the HtrII-free and HtrII-complexed form. We monitored sustained light-induced pH changes with a pH electrode, and laser flash-induced pH changes with the pH indicator pyranine using sealed membrane vesicles and open sheets containing the free or the complexed receptor. The results demonstrated that SRII takes up a proton in M-to-O conversion and releases it during O-decay. The uptake and release are from and to the extracellular side, and therefore SRII does not transport the proton across the membrane. The pH dependence of the SRII photocycle indicated the presence of a protonatable group (pK(a) approximately 7.5) in the extracellular proton-conducting path, which plays a role in proton uptake by the Schiff base in the M-to-O conversion. The extracellular proton circulation produced by SRII was not blocked by HtrII complexation, unlike the cytoplasmic proton conduction in SRI that was found in the same series of measurements to be blocked by its transducer, HtrI. The implications of this finding for current models of SRI and SRII signaling are discussed. (+info)
Time-resolved absorption and photothermal measurements with recombinant sensory rhodopsin II from Natronobacterium pharaonis.
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Purified wild-type sensory rhodopsin II from Natronobacterium pharaonis (pSRII-WT) and its histidine-tagged analog (pSRII-His) were studied by laser-induced optoacoustic spectroscopy (LIOAS) and flash photolysis with optical detection. The samples were either dissolved in detergent or reconstituted into polar lipids from purple membrane (PML). The quantum yield for the formation of the long-lived state M(400) was determined as Phi(M) = 0.5 +/- 0.06 for both proteins. The structural volume change accompanying the production of K(510) as determined with LIOAS was DeltaV(R,1) /= Phi(M), indicating that the His tag does not influence this early step of the photocycle. The medium has no influence on DeltaV(R,1), which is the largest so far measured for a retinal protein in this time range (<10 ns). This confirms the occurrence of conformational movements in pSRII for this step, as previously suggested by Fourier transform infrared spectroscopy. On the contrary, the decay of K(510) is an expansion in the detergent-dissolved sample and a contraction in PML. Assuming an efficiency of 1.0, DeltaV(R,2) = -3 ml/mol for pSRII-WT and -4.6 ml/mol for pSRII-His were calculated in PML, indicative of a small structural difference between the two proteins. The energy content of K(510) is also affected by the tag. It is E(K) = (88 +/- 13) for pSRII-WT and (134 +/- 11) kJ/mol for pSRII-His. A slight difference in the activation parameters for K(510) decay confirms an influence of the C-terminal His on this step. At variance with DeltaV(R,1), the opposite sign of DeltaV(R,2) in detergent and PML suggests the occurrence of solvation effects on the decay of K(510), which are probably due to a different interaction of the active site with the two dissolving media. (+info)
Functional expression of His-tagged sensory rhodopsin I in Escherichia coli.
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Sensory rhodopsin I (SRI) from Halobacterium salinarum was functionally expressed in Escherichia coli and subsequently purified to homogeneity using a C-terminal His-tag anchor. Yields of 3-4 mg SRI/l cell culture can be obtained. The absorption and photocycle properties of SRI were similar if not indistinguishable from those of the homologously expressed SRI. A global fit analysis of the photocycle data and the calculation of the spectra of states provided strong evidence for the existence of an N-like intermediate. (+info)
Charge motions during the photocycle of pharaonis halorhodopsin.
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Oriented gel samples were prepared from halorhodopsin-containing membranes from Natronobacterium pharaonis, and their photoelectric responses to laser flash excitation were measured at different chloride concentrations. The fast component of the current signal displayed a characteristic dependency on chloride concentration, and could be interpreted as a sum of two signals that correspond to the responses at high-chloride and no-chloride, but high-sulfate, concentration. The chloride concentration-dependent transition between the two signals followed the titration curve determined earlier from spectroscopic titration. The voltage signal was very similar to that reported by another group (Kalaidzidis, I. V., Y. L. Kalaidzidis, and A. D. Kaulen. 1998. FEBS Lett. 427:59-63). The absorption kinetics, measured at four wavelengths, fit the kinetic model we had proposed earlier. The calculated time-dependent concentrations of the intermediates were used to fit the voltage signal. Although no negative electric signal was observed at high chloride concentration, the calculated electrogenicity of the K intermediate was negative, and very similar to that of bacteriorhodopsin. The late photocycle intermediates (O, HR', and HR) had almost equal electrogenicities, explaining why no chloride-dependent time constant was identified earlier by Kalaidzidis et al. The calculated electrogenicities, and the spectroscopic information for the chloride release and uptake steps of the photocycle, suggest a mechanism for the chloride-translocation process in this pump. (+info)
The three-dimensional structure of halorhodopsin to 5 A by electron crystallography: A new unbending procedure for two-dimensional crystals by using a global reference structure.
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Electron microscopy does not, in principle, require highly ordered crystals to determine a high-resolution structure. Nevertheless, crystals of any type help to constrain the molecules into a more limited range of orientations and positions, from which it is easier to carry out structure determination. We describe an improved procedure for determination of crystalline disorder, which we have applied to poorly ordered two-dimensional crystals of the chloride pump halorhodopsin from Halobacterium salinarum. The new image analysis procedure involves the use of a reference projection calculated from a global three-dimensional map to carry out the initial cross-correlation analysis. Coupled with a greater number of images taken with field emission gun microscopes, this has allowed us to calculate a three-dimensional structure for halorhodopsin, in which the seven transmembrane helices and certain molecular features, such as the beta-ionone ring of retinal, are now resolved. (+info)
Aspartate 75 mutation in sensory rhodopsin II from Natronobacterium pharaonis does not influence the production of the K-like intermediate, but strongly affects its relaxation pathway.
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The early steps in the photocycle of the aspartate 75-mutated sensory rhodopsin II from Natrobacterium pharaonis (pSRII-D75N) were studied by time-resolved laser-induced optoacoustic spectroscopy combined with quantum yield determinations by flash photolysis with optical detection. Similar to the case of pSRII-WT, excitation of pSRII-D75N produces in subnanosecond time a K-like intermediate. Different to the case of K in pSRII-WT, in pSRII-D75N there are two K states. K(E) decays into K(L) with a lifetime of 400 ns (independent of temperature in the range 6.5-52 degrees C) which is optically silent under the experimental conditions of our transient absorption experiments. This decay is concomitant with an expansion of 6.5 ml/mol of produced intermediate. This indicates a protein relaxation not affecting the chromophore absorption. For pSRII-D75N reconstituted into polar lipids from purple membrane, the mutation of Asp-75 by the neutral residue Asn affects neither the K(E) production yield (PhiK(e) 0.51 +/- 0.05) nor the energy stored by this intermediate (E(E)K(E) = 91 +/- 11 kJ/mol), nor the expansion upon its production (DeltaV(R,1) = 10 +/- 0.3 ml/mol). All these values are very similar to those previously determined for K with pSRII-WT in the same medium. The millisecond transient species is attributed to K(L) with a lifetime corresponding to that determined by electronic absorption spectroscopy for K(565). The determined energy content of the intermediates as well as the structural volume changes for the various steps afford the calculation of the free energy profile of the phototransformation during the pSRII-D75N photocycle. These data offer insights regarding the photocycle in pSRII-WT. Detergent solubilization of pSRII-D75N affects the sample properties to a larger extent than in the case of pSRII-WT. (+info)
Resonance Raman spectroscopy of sensory rhodopsin II from Natronobacterium pharaonis.
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Sensory rhodopsin II (pSRII), the photophobic receptor from Natronobacterium pharaonis, has been studied by time-resolved resonance Raman (RR) spectroscopy using the rotating cell technique. Upon excitation with low laser power, the RR spectra largely reflect the parent state pSRII(500) whereas an increase of the laser power leads to a substantial accumulation of long-lived intermediates contributing to the RR spectra. All RR spectra could consistently be analysed in terms of four component spectra which were assigned to the parent state pSRII(500) and the long-lived intermediates M(400), N(485) and O(535) based on the correlation between the C = C stretching frequency and the absorption maximum. The parent state and the intermediates N(485) and O(535) exhibit a protonated Schiff base. The C = N stretching frequencies and the H/D isotopic shifts indicate strong hydrogen bonding interactions of the Schiff base in pSRII(500) and O(535) whereas these interactions are most likely very weak in N(485). (+info)