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Proton transport by halorhodopsin.

In halorhodopsin from Natronobacterium pharaonis, a light-driven chloride pump, the chloride binding site also binds azide. When azide is bound at this location the retinal Schiff base transiently deprotonates after photoexcitation with light > 530 nm, like in the light-driven proton pump bacteriorhodopsin. As in the photocycle of bacteriorhodopsin, pyranine detects the release of protons to the bulk. The subsequent reprotonation of the Schiff base is also dependent on azide, but with different kinetics that suggest a shuttling of protons from the surface as described earlier for halorhodopsin from Halobacterium salinarium. This azide-dependent, bacteriorhodopsin-like photocycle results in active electrogenic proton transport in the cytoplasmic to extracellular direction, detected in cell envelope vesicle suspensions both with a potential-sensitive electrode and by measuring light-dependent pH change. We conclude that in halorhodopsin an azide bound to the extracellular side of the Schiff base, and another azide shuttling between the Schiff base and the cytoplasmic surface, fulfill the functions of Asp-85 and Asp-96, respectively, in bacteriorhodopsin. Thus, although halorhodopsin is normally a chloride ion pump, it evidently contains all structural requirements, except an internal proton acceptor and a donor, of a proton pump. This observation complements our earlier finding that when a chloride binding site was created in bacteriorhodopsin through replacement of Asp-85 with a threonine, that protein became a chloride ion pump.

Azides↗

Control of transmembrane ion fluxes to select halorhodopsin-deficient and other energy-transduction mutants of Halobacterium halobium.

We describe a selection method for mutants altered in the generation and regulation of transmembrane ion flux in Halobacterium halobium. The method is based on experimental control of ion fluxes by a combination of light, ionophore, and external pH to generate an imbalance in the cells' proton circulation through their membranes. The steady-state proton circulation is increased by the introduction of a small inward proton leak with a protonophore. The cells are then illuminated to excite halorhodopsin, which hyperpolarizes the membrane and drives protons into the cells. As a result, wild-type cells suffer cytoplasmic acidification, which causes a dramatic loss of motility and suppresses their growth. These properties can be used to select for mutants that escape cytoplasmic acidification because either they lack halorhodopsin function or they have a greater capacity to eject protons during the illumination. In a popular selected by this method, 97% of the individual cells were demonstrably altered in ion flux properties. Cells were selected with alterations in the halobacterial rhodopsin, specifically with deficiencies in membrane potential generation by halorhodopsin and with increased cellular proton ejection by bacteriorhodopsin. We describe properties of one of the halorhodopsin-deficient strains, Flx37.

Bacteriological Techniques↗

Purification of photochemically active halorhodopsin.

We have developed a procedure for the purification of halorhodopsin in a photochemically active state. Solubilization of membranes from a bacteriorhodopsin-negative Halobacterium strain with octyl glucoside was followed by chromatography on hydroxylapatite and octyl-Sepharose gels. All steps were carried out in high-ionic-strength solutions. The procedure resulted in 270-fold enrichment with a 35% yield. The eluted pigment had an absorption maximum at 575 nm and an A280/A575 ratio of 2. On removal of the detergent by dialysis, the purified halorhodopsin was chemically bleached, regenerated with [3H]retinal, and reduced with cyanoborohydride. Such samples showed one main and one satellite band after staining or fluorography of NaDodSO4/polyacrylamide gels. The apparent molecular weight of the main band was 25,000. Purified halorhodopsin underwent a photocycle after excitation with pulsed laser light and showed a 9-nm blue shift (at neutral pH) on removal of chloride ion. The pigment also underwent a photoreversible shift at alkaline pH to a form absorbing maximally at 410 nm. All three reactions closely resembled those of membrane-bound halorhodopsin.

Bacterial Proteins↗

Effects of anion binding on the deprotonation reactions of halorhodopsin.

The retinal Schiff base of halorhodopsin deprotonates with a pKa of 7.4 in 0.5 M Na2SO4 in the dark. In the presence of various anions, such as chloride or nitrate, etc., the pKa is raised by up to 1.5 units. Analysis of the dependency of the pKa on anion concentration favors the model in which the anions do not bind to the positively charged Schiff base nitrogen, but to a site near it, and exert their effect on the pKa by direct (perhaps electrostatic) interaction. Adding nitrate, or one of several other anions, causes also a small blueshift in the visible absorption band of the chromophore. These effects on the pKa and the absorption band define an anion binding site in halorhodopsin, termed Site I. Chloride and bromide apparently bind in addition to another site, which is associated with a small red-shift of the absorption band and changes in the photocycle. This other anion binding site is termed Site II. Illumination of halorhodopsin samples results in the deprotonation of the Schiff base with a much lowered pKa, but at very low rates probably determined by the generation of a deprotonating photointermediate. Binding of Site I anions increases the pKa of deprotonation in the light also. The similarity of the responses of the apparent pKa in the dark and in the light to anion concentration suggests that anion binding to Site I influences deprotonation of the Schiff base similarly in the photointermediate and in the parent halorhodopsin molecule.

Anions↗

Halorhodopsin is a light-driven chloride pump.

Light-dependent membrane potentials, ionic fluxes, and volume changes were measured in two kinds of Halobacterium halobium cell envelope vesicles: one containing bacteriorhodopsin and another halorhodopsin. Bacteriorhodopsin-containing vesicles extruded protons by a primary electrogenic mechanism and an energized volume decrease was observed. This was shown to be the consequences of sodium extrusion via proton/sodium antiport (which recirculated protons) and the accompanying passive chloride extrusion. Halorhodopsin-containing vesicles, in contrast, exhibited a volume increase during illumination, apparently caused by primary inward transport of chloride, and accompanied by passive cation (sodium or potassium, and proton) uptake. It was demonstrated that the chloride transport will occur against both electrical and concentration gradients across the vesicle membrane. Moreover, chloride was required on the vesicle exterior for the light-dependent generation of membrane potential, pH change, and swelling. These observations are inconsistent with an earlier proposal that halorhodopsin is an outward directed sodium pump, but suggest very strongly that it is an inward directed chloride pump. Quantitative arguments from the present work rule out a significant role of sodium in the functioning of halorhodopsin.

Bacteriorhodopsins↗

Genetic and biochemical resolution of the chromophoric polypeptide of halorhodopsin.

Retinal-binding proteins in bacteriorhodopsin-deficient membranes of Halobacterium halobium have been separated on polyacrylamide gels after labeling with (3H)retinal. Four labeled polypeptides are observed: one at an Mr of 19,000, two distinct bands near 25,000, and one at 94,000. Comparing halorhodopsin-containing and halorhodopsin-deficient mutants and using ion translocation measurements and flash spectroscopy to test for the photoactive retinal pigments, we show that the lower of the two radiolabeled bands at 25,000 is the retinal-binding polypeptide of halorhodopsin. The identities of the other three polypeptides are not known, but one of them, probably the upper of the two 25,000 bands, is likely to be s-rhodopsin.

Bacteriorhodopsins↗

Light-dependent trans to cis isomerization of the retinal in halorhodopsin.

Flash-induced absorption changes in the near UV were determined for bacteriorhodopsin and halorhodopsin on a millisecond time scale. The difference spectrum obtained for bacteriorhodopsin was comparable to model difference spectra of tyrosine (aromatic OH deprotonated vs protonated), as found by others. The flash-induced difference spectrum for halorhodopsin, in contrast, resembled a model spectrum obtained for trans to 13-cis isomerization of retinal in bacteriorhodopsin. A model for chloride translocation by halorhodopsin is presented, in which the retinal isomerization moves positive charges, which in turn modulate the affinity of a site to chloride.

Bacteriorhodopsins↗

Characterization of the proton-transporting photocycle of pharaonis halorhodopsin.

The photocycle of pharaonis halorhodopsin was investigated in the presence of 100 mM NaN(3) and 1 M Na(2)SO(4). Recent observations established that the replacement of the chloride ion with azide transforms the photocycle from a chloride-transporting one into a proton-transporting one. Kinetic analysis proves that the photocycle is very similar to that of bacteriorhodopsin. After K and L, intermediate M appears, which is missing from the chloride-transporting photocycle. In this intermediate the retinal Schiff base deprotonates. The rise of M in halorhodopsin is in the microsecond range, but occurs later than in bacteriorhodopsin, and its decay is more accentuated multiphasic. Intermediate N cannot be detected, but a large amount of O accumulates. The multiphasic character of the last step of the photocycle could be explained by the existence of a HR' state, as in the chloride photocycle. Upon replacement of chloride ion with azide, the fast electric signal changes its sign from positive to negative, and becomes similar to that detected in bacteriorhodopsin. The photocycle is enthalpy-driven, as is the chloride photocycle of halorhodopsin. These observations suggest that, while the basic charge translocation steps become identical to those in bacteriorhodopsin, the storage and utilization of energy during the photocycle remains unchanged by exchanging chloride with azide.

Bacteriorhodopsins↗

Flash-induced voltage changes in halorhodopsin from Natronobacterium pharaonis.

The flash-induced voltage response of halorhodopsin at high NaCl concentration comprises two main kinetic components. The first component with tau approximately 1 micros does not exceed 4% of the overall response amplitude and is probably associated with the formation of the L (hR520) intermediate. The second main component with tau approximately 1-2.5 ms which is independent of Cl- concentration can be ascribed to the transmembrane Cl- translocation during the L intermediate decay. The photoelectric response in the absence of Cl- has the opposite polarity and does not exceed 6% of the overall response amplitude at high NaCl concentration. A pH decrease results in substitution of the Cl(-)-dependent components by the photoresponse which is similar to that in the absence of Cl-. Thus, the difference between photoresponses of chloride-binding and chloride-free halorhodopsin forms resembles that of bacteriorhodopsin purple neutral and blue acid forms, respectively. The photovoltage data obtained can hardly be explained within the framework of the photocycle scheme suggested by Varo et al. [Biochemistry 34 (1995), 14490-14499]. We suppose that the O-type intermediate belongs to some form of halorhodopsin incapable of Cl- transport.

Bacterial Proteins↗

Mechanism of base-catalyzed Schiff base deprotonation in halorhodopsin.

It has been shown earlier that the deprotonation of the Schiff base of illuminated halorhodopsin proceeds with a much lower pKa than that of the unilluminated pigment and the reversible protonation change is catalyzed by azide and cyanate [Hegemann, P., Oesterhelt, D., & Steiner, M. (1985) EMBO J. 4, 2347-2350]. We have studied the kinetics of the proton-transfer events with flash spectroscopy and compared a variety of anionic bases with different pKa with regard to their apparent binding constants and their catalytic activities. The results suggest a general base catalysis mechanism in which the anionic bases bind with apparently low affinity to halorhodopsin, although with some degree of size- and/or shape-dependent specificity. The locus of the catalysis is accessible from the cytoplasmic side of the membrane and is not at site I, where various anions bind and shift the pKa of the deprotonation. Neither is it at site II, where a few specific anions (like chloride) bind to the all-trans pigment. It may be concluded that while the all-trans pigment loses its Schiff base proton very rapidly at its pKa, there is a kinetic barrier to this deprotonation in the 13-cis photointermediate that can be partially overcome by the reversible protonation of an extrinsic anionic base, which shuttles protons between the interior of the protein and the aqueous medium. The need for an extrinsic proton acceptor for efficient deprotonation of the Schiff base of halorhodopsin is one of the main differences between this pigment and the analogous retinal protein, bacteriorhodopsin.

Bacteriorhodopsins↗

Anion uptake in halorhodopsin from Natromonas pharaonis studied by FTIR spectroscopy: consequences for the anion transport mechanism.

The uptake of chloride, bromide, iodide, nitrate, and azide by anion-depleted blue halorhodopsin from Natronobacterium pharaonis has been followed by FTIR difference spectroscopy using an ATR sampling device. The spectra are compared with the spectrum of the O intermediate obtained by time-resolved FTIR studies of the photocycle. It is demonstrated that anion-free blue halorhodopsin can be identified with the O intermediate and, thus, that the decay of O is due to the passive uptake of the anion. The great similarity of the anion-binding spectra and their identity in the case of the monoatomic anions indicate a rather unspecific binding site for the different anions dominated by electrostatic interactions. Comparing spectra obtained with 15N nitrate and unlabeled nitrate, the NO-stretching bands could be identified. The small splitting and the small IR intensity of those bands indicate a rather nonpolar binding site with a rather isotropic influence on the nitrate, in contrast to aqueous nitrate. In further experiments on the photocycle of blue halorhodopsin, the all-trans --> 13-cis isomerization can be clearly identified. Up to 100 micros, the isomerization-induced structural changes deduced from amide I changes are similar to those occurring during the anion-transporting photocycle. Compared to these, the molecular changes involved in the release and their reversion during the uptake of anions are considerably larger. They can be reached via two pathways: (1) by reducing the anion concentration and (2) transiently during the anion-transporting photocycle with the formation of the precursor of O with O conformation. Consequences of the anion transport mechanism are discussed.

Azides↗

Reconstitution of purified halorhodopsin.

Asolectin lipid vesicles containing halorhodopsin show light-induced acidification in the presence of proton ionophores. This effect is abolished by triphenyltin chloride, a chloride/hydroxyl antiporter, and is greatly diminished by valinomycin in the presence of potassium ions, which collapse the membrane potential. This indicates that halorhodopsin orients in the lipid vesicles preferentially inside out, pumping chloride into the extravesicular compartment. The absorption maximum of halorhodopsin in asolectin vesicles in 3 M NaCl is at 567 nm, and the action spectrum for the light-induced pH changes followed closely the absorption spectrum. Replacement of chloride by acetate or sulfate causes a shift in the absorption maximum to approximately equal to 559 nm and renders the pump inactive. The different photocycles of the two forms were used to show that 80% of the molecules have the extracellular side exposed to the vesicle interior and that the halide-binding site(s) associated with the spectral transition is accessible from the extracellular side of the molecule. The data presented demonstrate that the purified chromoprotein is the light-driven chloride pump in Halobacterium halobium.

Bacteriorhodopsins↗

Time-resolved measurements of photovoltage generation by bacteriorhodopsin and halorhodopsin adsorbed on a thin polymer film.

We constructed a time-resolved photovoltage measurement system and examined the photovoltage kinetics of wild-type bacteriorhodopsin, its D96N mutant, and halorhodopsins from Halobacterium salinarum and Natronobacterium pharaonis. Upon illumination with a laser flash, wild-type bacteriorhodopsin showed photovoltage generation with fast (10-100 micros range) and slow (ms range) components while D96N lacked the latter, as reported previously [Holz, M., Drachev, L.A., Mogi, T., Otto, H., Kaulen, A.D., Heyn, M.P., Skulachev, V.P., and Khorana, H.G. (1989) Proc. Natl. Acad. Sci. USA 86, 2167-2171]. In contrast, photovoltage generation in halorhodopsins from H. salinarum and N. pharaonis was significant only in the ms time range. On the basis of the photovoltage kinetics and photocycle, we conclude that major charge (chloride) movements within halorhodopsin occur during the formation and decay of the N intermediate in the ms range. These observations are discussed in terms of the "Energization-Relaxation Channel Model" [Muneyuki, E., Ikematsu, M., and Yoshida, M. (1996) J. Phys. Chem. 100, 19687-19691].

Bacteriorhodopsins↗

Light-induced reaction of halorhodopsin prepared under low salt conditions.

1. Membrane fraction containing halorhodopsin was prepared from the lysate of a mutant strain of Halobacterium halobium, Y1, which is defective in bacteriorhodopsin synthesis. 2. Irradiation of the membrane with red light at 0 degrees C decreased the absorbance intensities over the whole range of 500--600 nm and a new absorption peak appeared at about 400 nm. This process was reversed either by irradiation with blue light or simply by incubation in the dark. The wavelength at which the red light-induced absorbance decrease became maximum was 566 nm in the absence of NaCl and moved to 576 nm upon addition of NaCl. The midpoint for the conversion was at about 0.1 M NaCl. 3. Even though the membrane containing halorhodopsin was prepared in the absence of NaCl, this pigment was photochemically active in the sense that it could form a bathochromic photoproduct, a batho-intermediate, at -196 degrees C. 4. Retinal isomer composition during irradiation with red light at 0 degrees C was determined. Unirradiated halorhodopsin had predominantly all-trans retinal. With the increase of the blue-shifted product on irradiation, 13-cis content increased.

Bacteriorhodopsins↗

Structure of the light-driven chloride pump halorhodopsin at 1.8 A resolution.

Halorhodopsin, an archaeal rhodopsin ubiquitous in Haloarchaea, uses light energy to pump chloride through biological membranes. Halorhodopsin crystals were grown in a cubic lipidic phase, which allowed the x-ray structure determination of this anion pump at 1.8 angstrom resolution. Halorhodopsin assembles to trimers around a central patch consisting of palmitic acid. Next to the protonated Schiff base between Lys(242) and the isomerizable retinal chromophore, a single chloride ion occupies the transport site. Energetic calculations on chloride binding reveal a combination of ion-ion and ion-dipole interactions for stabilizing the anion 18 angstroms below the membrane surface. Ion dragging across the protonated Schiff base explains why chloride and proton translocation modes are mechanistically equivalent in archaeal rhodopsins.

Bacteriorhodopsins↗

Photochromism of halorhodopsin. cis/trans isomerization of the retinal around the 13-14 double bond.

The isomeric composition of retinal in membrane-bound and in purified but detergent-free, dark-adapted halorhodopsin was found to be about 70% 13-cis and 30% all-trans. Any illumination increased the all-trans content relative to the dark-adapted state, but blue illumination shifted the isomeric composition more toward all-trans while red illumination of blue-adapted samples shifted it more toward 13-cis. In the presence of chloride this photoisomerization caused the kind of photochromic behavior reported earlier in Smith, S. O., Marvin, M. J., Bogomolni, R. A., and Mathies, R. A. (1984) J. Biol. Chem. 259, 12326-12329, i.e. blue light caused the absorption maximum to move toward longer wavelengths and red light reversed the shift. Only the all-trans chromophore exhibited the complete photocycle described earlier in detergent-solubilized halorhodopsin, and this was the form that could be associated with light-driven chloride transport activity in cell envelope vesicles. In the absence of chloride the spectroscopic changes caused by illumination were much smaller. Reconstitution of bleached preparations with 13-cis- and all-trans-retinal, in the presence and absence of chloride, confirmed that the difference between the absorption maxima of the two isomeric forms of the chromophore is affected by chloride: 13-cis-halorhodopsin absorbs at about 567-568 nm with and without chloride, and the all-trans pigment absorbs near 568 nm in the absence of chloride, but at 578 nm in its presence. The simplest explanation of this finding is that most of the red-shift which accompanies the 13-cis----all-trans transition originates from electrostatic interaction of the retinal with chloride bound in its vicinity.

Bacteriorhodopsins↗

Biochemical characterization of halorhodopsin in native membranes.

Procedures are described for selectively radiolabeling the protein moiety (haloopsin) or the chromophoric prosthestic group (retinal) of the light-driven chloride pump halorhodopsin in intact cells of Halobacterium halobium. By sodium dodecyl sulfate-polyacrylamide gel electrophoresis and autofluorography, two retinal-binding polypeptides are observed to band near the known molecular weight of the halorhodopsin chromophoric polypeptide (25,000). Synthesis of one of these polypeptides is controlled by retinal and is sufficient for generation of complete halorhodopsin function. The other is constitutively produced by the cells and differs chemically from the haloopsin protein as indicated by differences in their V8 protease digestion patterns. V8 protease cleavage of haloopsin in its native membrane is compared with that of the protein in denaturing and nondenaturing detergents. Protease cleavage sites available in the denatured haloopsin molecule are hidden in its native membrane-integrated conformation and in nondenaturing detergent micelles. Treatment with a variety of proteases indicates susceptibility of a short terminal region of the haloopsin chain in its native conformation.

Bacteriorhodopsins↗

Structure of the retinal chromophore in the hR578 form of halorhodopsin.

Halorhodopsin is a retinal-containing pigment that is thought to function as a light-driven chloride ion pump in the cell membrane of Halobacterium halobium. To address the role of the retinal chromophore in chloride ion transport, resonance Raman spectra have been obtained of the hR578 form of chromatographically purified halorhodopsin (hR). The close similarity of the frequencies and intensities of the hR578 Raman bands with those of light-adapted bacteriorhodopsin (bR568) shows that the chromophore in hR578 has an all-trans configuration and that the protein environment around the chromophore in these two pigments is very similar. In addition, hR578 exhibits a Raman line at 1633 cm-1 which is assigned as the stretching vibration of a protonated Schiff base linkage to the protein based on its shift to 1627 cm-1 in D2O. The reduced frequency of the Schiff base stretching vibration compared with bR568 (1640 cm-1) is shown to result from a reduction of its coupling with the NH in-plane rock. This may be due to a reduction in hydrogen-bonding between the Schiff base proton and an electronegative counterion in halorhodopsin.

Bacteriorhodopsins↗