Chromophore reorientation during the photocycle of bacteriorhodopsin: experimental methods and functional significance

Light-induced isomerization leads to orientational changes of the retinylidene chromophore of bacteriorhodopsin in its binding pocket. The chromophore reorientation has been characterized by the following methods: polarized absorption spectroscopy in the visible, UV and IR; polarized resonance Raman scattering; solid-state deuterium nuclear magnetic resonance; neutron and X-ray diffraction. Most of these experiments were performed at low temperatures with bacteriorhodopsin trapped in one or a mixture of intermediates. Time-resolved measurements at room temperature with bacteriorhodopsin in aqueous suspension can currently only be carried out with transient polarized absorption spectroscopy in the visible. The results obtained to date for the initial state and the K, L and M intermediates are presented and discussed. The most extensive data are available for the M intermediate, which plays an essential role in the function of bacteriorhodopsin. For this intermediate the various methods lead to a consistent picture: the curved all-trans polyene chain in the initial state straightens out in the M intermediate (13-cis) and the chain segment between C(5) and C(13) tilts upwards in the direction of the cytoplasmic surface. The kink at C(13) allows the positions of beta-ionone ring and Schiff base nitrogen to remain approximately fixed.     

Control of the pump cycle in bacteriorhodopsin: mechanisms elucidated by solid-state NMR of the D85N mutant.

By varying the pH, the D85N mutant of bacteriorhodopsin provides models for several photocycle intermediates of the wild-type protein in which D85 is protonated. At pH 10.8, NMR spectra of [zeta-(15)N]lys-, [12-(13)C]retinal-, and [14,15-(13)C]retinal-labeled D85N samples indicate a deprotonated, 13-cis,15-anti chromophore. On the other hand, at neutral pH, the NMR spectra of D85N show a mixture of protonated Schiff base species similar to that seen in the wild-type protein at low pH, and more complex than the two-state mixture of 13-cis,15-syn, and all-trans isomers found in the dark-adapted wild-type protein. These results lead to several conclusions. First, the reversible titration of order in the D85N chromophore indicates that electrostatic interactions have a major influence on events in the active site. More specifically, whereas a straight chromophore is preferred when the Schiff base and residue 85 are oppositely charged, a bent chromophore is found when both the Schiff base and residue 85 are electrically neutral, even in the dark. Thus a "bent" binding pocket is formed without photoisomerization of the chromophore. On the other hand, when photoisomerization from the straight all-trans,15-anti configuration to the bent 13-cis,15-anti does occur, reciprocal thermodynamic linkage dictates that neutralization of the SB and D85 (by proton transfer from the former to the latter) will result. Second, the similarity between the chromophore chemical shifts in D85N at alkaline pH and those found previously in the M(n) intermediate of the wild-type protein indicate that the latter has a thoroughly relaxed chromophore like the subsequent N intermediate. By comparison, indications of L-like distortion are found for the chromophore of the M(o) state. Thus, chromophore strain is released in the M(o)-->M(n) transition, probably coincident with, and perhaps instrumental to, the change in the connectivity of the Schiff base from the extracellular side of the membrane to the cytoplasmic side. Because the nitrogen chemical shifts of the Schiff base indicate interaction with a hydrogen-bond donor in both M states, it is possible that a water molecule travels with the Schiff base as it switches connectivity. If so, the protein is acting as an inward-driven hydroxyl pump (analogous to halorhodopsin) rather than an outward-driven proton pump. Third, the presence of a significant C [double bond] N syn component in D85N at neutral pH suggests that rapid deprotonation of D85 is necessary at the end of the wild-type photocycle to avoid the generation of nonfunctional C [double bond] N syn species.     

Molecular dynamics study of the 13-cis form (bR548) of bacteriorhodopsin and its photocycle.

The structure and the photocycle of bacteriorhodopsin (bR) containing 13-cis,15-syn retinal, so-called bR548, has been studied by means of molecular dynamics simulations performed on the complete protein. The simulated structure of bR548 was obtained through isomerization of in situ retinal around both its C13-C14 and its C15-N bond starting from the simulated structure of bR568 described previously, containing all-trans,15-anti retinal. After a 50-ps equilibration, the resulting structure of bR548 was examined by replacing retinal by analogues with modified beta-ionone rings and comparing with respective observations. The photocycle of bR548 was simulated by inducing a rapid 13-cis,15-anti-->all-trans,15-syn isomerization through a 1-ps application of a potential that destabilizes the 13-cis isomer. The simulation resulted in structures consistent with the J, K, and L intermediates observed in the photocycle of bR548. The results offer an explanation of why an unprotonated retinal Schiff base intermediate, i.e., an M state, is not formed in the bR548 photocycle. The Schiff base nitrogen after photoisomerization of bR548 points to the intracellular rather than to the extracellular site. The simulations suggest also that leakage from the bR548 to the bR568 cycle arises due to an initial 13-cis,15-anti-->all-trans,15-anti photoisomerization.     

Isomeric composition of retinal chromophore in dark-adapted bacteriorhodopsin

1. Retinal isomers extracted from the acid-hydrolysate of cetyltrimethylammonium bromide-treated dark-adapted bacteriorhodopsin (bRD) were analyzed in a high performance liquid chromatograph (HPLC) system. The extract from bRD contains almost equal molar amounts of both 13-cis retinal and all-trans retinal isomers. The extent of isomerization and the yield of both isomers during the isolation process were investigated by the application of the same extraction procedure to artificial bacteriorhodopsin reconstituted with 13-cis retinal isomer (13-cis bacteriorhodopsin) and also to light-adapted bacteriorhodopsin (bRL) which has been shown to contain only the all-trans isomer (all-trans bacteriorhodopsin). 2. A reconstituted bacteriorhodopsin, which had been prepared from apo-bacteriorhodopsin and an equimolar mixture of both 13-cis retinal and all-trans retinal isomers, showed an absorption spectrum having the same maximum wavelength as that of bRD even at the beginning of the reconstitution process. 3. Analysis of the photosteady states of bRD at -190 degrees C revealed that it was composed of two different species, one having 13-cis retinal and the other having all-trans retinal isomers in approximately equal molar amounts. These two also gave their respective photoproducts. 4. From these results it can be concluded that bRD contains both 13-cis retinal and all-trans retinal isomers in nearly equal molar amounts as its chromophore.     

Chromophore structure in bacteriorhodopsin's N intermediate: implications for the proton-pumping mechanism

By elevating the pH to 9.5 in 3 M KCl, the concentration of the N intermediate in the bacteriorhodopsin photocycle has been enhanced, and time-resolved resonance Raman spectra of this intermediate have been obtained. Kinetic Raman measurements show that N appears with a half-time of 4 +/- 2 ms, which agrees satisfactorily with our measured decay time of the M412 intermediate (2 +/- 1 ms). This argues that M412 decays directly to N in the light-adapted photocycle. The configuration of the chromophore about the C13 = C14 bond was examined by regenerating the protein with [12,14-2H]retinal. The coupled C12-2H + C14-2H rock at 946 cm-1 demonstrates that the chromophore in N is 13-cis. The shift of the 1642-cm-1 Schiff base stretching mode to 1618 cm-1 in D2O indicates that the Schiff base linkage to the protein is protonated. The insensitivity of the 1168-cm-1 C14-C15 stretching mode to N-deuteriation establishes a C = N anti (trans) Schiff base configuration. The high frequency of the C14-C15 stretching mode as well as the frequency of the 966-cm-1 C14-2H-C15-2H rocking mode shows that the chromophore is 14-s-trans. Thus, N contains a 13-cis, 14-s-trans, 15-anti protonated retinal Schiff base.(ABSTRACT TRUNCATED AT 250 WORDS)     

Light- and dark-adapted bacteriorhodopsin, a time-resolved neutron diffraction study

Recently, neutron diffraction experiments have revealed well-resolved and reversible changes in the protein conformation of bacteriorhodopsin (BR) between the light-adapted ground state and the M-intermediate of the proton pumping photocycle (Dencher, Dresselhaus, Zaccai and Büldt (1989) Proc. Natl. Acad. Sci. USA 86, 7876-7879). These changes are triggered by the light-induced isomerization of the chromophore retinal from the all-trans to the 13-cis configuration. Dark-adapted purple membranes contain a mixture of two pigment species with either the all-trans- or 13-cis-retinal isomer as chromophore. Employing a time-resolved neutron diffraction technique, no changes in protein conformation in the resolution regime of up to 7 A are observed during the transition between the two ground-state species 13-cis-BR and all-trans-BR. This is in line with the fact that the conversion of all-trans BR to 13-cis-BR involves an additional isomerization about the C15 = N Schiff's base bond, which in contrast to M formation minimizes retinal displacement and keeps the Schiff's base in the original protein environment. Furthermore, there is no indication for large-scale redistribution of water molecules in the purple membrane during light-dark adaptation.     

Chromophore configuration of pharaonis phoborhodopsin and its isomerization on photon absorption.

The configuration of the retinylidene chromophore in pharaonis phoborhodopsin (ppR) and its changes during the photoreaction cycle were investigated by means of a chromophore extraction method followed by HPLC analysis. The ppR has an all-trans chromophore, and unlike bacteriorhodopsin, it exhibits no dark isomerization of the chromophore. Irradiation of a ppR sample in the presence of 10 mM hydroxylamine, at which concentration a negligible amount of ppR was bleached, caused the formation of 90% 13-cis- and 10% all-trans-retinal oximes. Because the ppR sample under the continuous irradiation was a mixture containing original ppR, ppRM, and a small amount of ppRO, the above results showed that the chromophores of ppRM and ppRO are in a 13-cis form and an all-trans form, respectively. Therefore, the all-trans chromophore of ppR is isomerized to the 13-cis form on photon absorption, and it is thermally reisomerized to the all-trans form on the conversion process from ppRM to ppRO. The extracted retinal oximes from ppR and ppRO were mainly the 15-syn form, while that from ppRM was mainly the 15-anti form. This fact indicated that the attack of hydroxylamine on the chromophore is stereoselective owing to the unique structure of the chromophore binding site near the Schiff base region of the chromophore.     

Solid-state 2H NMR spectroscopy of retinal proteins in aligned membranes

Solid-state 2H NMR spectroscopy gives a powerful avenue to investigating the structures of ligands and cofactors bound to integral membrane proteins. For bacteriorhodopsin (bR) and rhodopsin, retinal was site-specifically labeled by deuteration of the methyl groups followed by regeneration of the apoprotein. 2H NMR studies of aligned membrane samples were conducted under conditions where rotational and translational diffusion of the protein were absent on the NMR time scale. The theoretical lineshape treatment involved a static axial distribution of rotating C-C2H3 groups about the local membrane frame, together with the static axial distribution of the local normal relative to the average normal. Simulation of solid-state 2H NMR lineshapes gave both the methyl group orientations and the alignment disorder (mosaic spread) of the membrane stack. The methyl bond orientations provided the angular restraints for structural analysis. In the case of bR the retinal chromophore is nearly planar in the dark- and all-trans light-adapted states, as well upon isomerization to 13-cis in the M state. The C13-methyl group at the "business end" of the chromophore changes its orientation to the membrane upon photon absorption, moving towards W182 and thus driving the proton pump in energy conservation. Moreover, rhodopsin was studied as a prototype for G protein-coupled receptors (GPCRs) implicated in many biological responses in humans. In contrast to bR, the retinal chromophore of rhodopsin has an 11-cis conformation and is highly twisted in the dark state. Three sites of interaction affect the torsional deformation of retinal, viz. the protonated Schiff base with its carboxylate counterion; the C9-methyl group of the polyene; and the beta-ionone ring within its hydrophobic pocket. For rhodopsin, the strain energy and dynamics of retinal as established by 2H NMR are implicated in substituent control of activation. Retinal is locked in a conformation that is twisted in the direction of the photoisomerization, which explains the dark stability of rhodopsin and allows for ultra-fast isomerization upon absorption of a photon. Torsional strain is relaxed in the meta I state that precedes subsequent receptor activation. Comparison of the two retinal proteins using solid-state 2H NMR is thus illuminating in terms of their different biological functions.     

Met-145 is a key residue in the dark adaptation of bacteriorhodopsin homologs.

Composition of retinal isomers in three proton pumps (bacteriorhodopsin, archaerhodopsin-1, and archaerhodopsin-2) was determined by high performance liquid chromatography in their light-adapted and dark-adapted states. In the light-adapted state, more than 95% of the retinal in all three proton pumps were in the all-trans configuration. In the dark-adapted state, there were only two retinal isomers, all-trans and 13-cis, in the ratio of all-trans: 13-cis = 1:2 for bacteriorhodopsin, 1:1 for archaerhodopsin-1, and 3:1 for archaerhodopsin-2. The difference in the final isomer ratios in the dark-adapted bacteriorhodopsin and archaerhodopsin-2 was ascribed to the methionine-145 in bacteriorhodopsin. This is the only amino acid in the retinal pocket that is substituted by phenylalanine in archaerhodopsin-2. The bacteriorhodopsin point-mutated at this position to phenylalanine dramatically altered the final isomer ratio from 1:2 to 3:1 in the dark-adapted state. This point mutation also caused a 10 nm blue-shift of the adsorption spectrum, which is similar to the shift of archaerhodopsin-2 relative to the spectra of bacteriorhodopsin and archaerhodopsin-1.     

Photochromicity of Anabaena sensory rhodopsin, an atypical microbial receptor with a cis-retinal light-adapted form

We characterize changes in isomeric states of the retinylidene chromophore during light-dark adaptation and photochemical reactions of Anabaena (Nostoc) sp. PCC7120 sensory rhodopsin (ASR). The results show that ASR represents a new type of microbial rhodopsin with a number of unusual characteristics. The three most striking are: (i) a primarily all-trans configuration of retinal in the dark-adapted state and (ii) a primarily 13-cis light-adapted state with a blue-shifted and lower extinction absorption spectrum, opposite of the case of bacteriorhodopsin; and (iii) efficient reversible light-induced interconversion between the 13-cis and all-trans unphotolyzed states of the pigment. The relative amount of ASR with cis and trans chromophore forms depends on the wavelength of illumination, providing a mechanism for single-pigment color sensing analogous to that of phytochrome pigments. In addition ASR exhibits unusually slow formation of L-like and M-like intermediates, with a dominant accumulation of M during the photocycle. Co-expression of ASR with its putative cytoplasmic transducer protein shifts the absorption maximum and strongly decreases the rate of dark adaptation of ASR, confirming interaction between the two proteins. Thus ASR, the first non-haloarchaeal sensory rhodopsin characterized, demonstrates the diversity of photochemistry of microbial rhodopsins. Its photochromic properties and the position of its two ground state absorption maxima suggest it as a candidate for controlling differential photosynthetic light-harvesting pigment synthesis (chromatic adaptation) or other color-sensitive physiological responses in Anabaena cells.     

Photoreactions of metarhodopsin III

Meta III is an inactive intermediate thermally formed following light activation of the visual pigment rhodopsin. It is produced from the Meta I/Meta II photoproduct equilibrium of rhodopsin by a thermal isomerization of the protonated Schiff base C=N bond of Meta I, and its chromophore configuration is therefore all-trans 15-syn. In contrast to the dark state of rhodopsin, which catalyzes exclusively the cis to trans isomerization of the C11=C12 bond of its 11-cis 15-anti chromophore, Meta III does not acquire this photoreaction specificity. Instead, it allows for light-dependent syn to anti isomerization of the C15=N bond of the protonated Schiff base, yielding Meta II, and for trans to cis isomerizations of C11=C12 and C9=C10 of the retinal polyene, as shown by FTIR spectroscopy. The 11-cis and 9-cis 15-syn isomers produced by the latter two reactions are not stable, decaying on the time scale of few seconds to dark state rhodopsin and isorhodopsin by thermal C15=N isomerization, as indicated by time-resolved FTIR methods. Flash photolysis of Meta III produces therefore Meta II, dark state rhodopsin, and isorhodopsin. Under continuous illumination, the latter two (or its unstable precursors) are converted as well to Meta II by presumably two different mechanisms.     

On the photocycle and light adaptation of dark-adapted bacteriorhodopsin.

Pulsed Nd laser (25 ns, 530 nm) photolysis experiments were carried out at room temperature in aqueous suspensions of dark- and light-adapted fragments of the purple membrane of Halobacterium halobium. It is shown that the (50%) 13-cis isomeric component (BR13-cis) of dark-adapted bacteriorhodopsin (BRDA) undergoes a photocycle involving a characteristic transient absorbing in the neighborhood of 610 nm. At relatively high excitation intensities BR13-cis is converted to the same 410 nm (M) transient that characterized the photocycle of the all-trans isomer (BRtrans) of light-adapted bacteriorhodopsin (BRLA). This process, which competes with the generation of the "610" species, is attributed to the photo-induced conversion, during the pulse, of BR13-cis (or of its primary photoproduct "X") to a species in the BRtrans photocyte. The relationship between these observations and the mechanism of BRDA hv leads to BRLA adaptation at low excitation intensities (for which a quantum yield limit, 0 less than or equal to (3.5 +/- 0.7) X 10(-2) , is established) is discussed.     

Solid-state NMR analysis of ligand--receptor interactions reveals an induced misfit in the binding site of isorhodopsin

Rhodopsin is the photosensitive protein of the rod photoreceptor in the vertebrate retina and is a paradigm for the superfamily of G-protein-coupled receptors (GPCRs). Natural rhodopsin contains an 11-cis-retinylidene chromophore. We have prepared the 9-cis analogue isorhodopsin in a natural membrane environment using uniformly (13)C-enriched 9-cis retinal. Subsequently, we have determined the complete (1)H and (13)C assignments with ultra-high field solid-state magic angle spinning NMR. The 9-cis substrate conforms to the opsin binding pocket in isorhodopsin in a manner very similar to that of the 11-cis form in rhodopsin, but the NMR data reveal an improper fit of the 9-cis chromophore in this binding site. We introduce the term "induced misfit" to describe this event. Downfield proton NMR ligation shifts (Deltasigma(lig)(H) > 1 ppm) are observed for the 16,17,19-H and nearby protons of the ionone ring and for the 9-methyl protons. They provide converging evidence for global, nonspecific steric interactions between the chromophore and protein, and contrast with the specific interactions over the entire ionone ring and its substituents detected for rhodopsin. The Deltasigma(lig)(C) pattern of the polyene chain confirms the positive charge delocalization in the polyene associated with the protonation of the Schiff base nitrogen. In line with the misalignment of the ionone ring, an additional and anomalous perturbation of the (13)C response is detected in the region of the 9-cis bond. This provides evidence for strain in the isomerization region of the polyene and supports the hypothesis that perturbation of the conjugation around the cis bond induced by the protein environment assists the selective photoisomerization.     

Vibrational spectroscopy of bacteriorhodopsin mutants. Evidence for the interaction of aspartic acid 212 with tyrosine 185 and possible role in the proton pump mechanism

The role of Asp-212 in the proton pumping mechanism of bacteriorhodopsin (bR) has been studied by a combination of site-directed mutagenesis and Fourier transform infrared difference spectroscopy. Difference spectra were recorded at low temperature for the bR----K and bR----M photoreactions of the mutants Asp-212----Glu, Asp-212----Asn, and Asp-212----Ala. Despite an increased proportion of the 13-cis form of bR (normally associated with dark adaptation), all of the mutants exhibited a light-adapted form containing as a principal component the normal all-trans retinal chromophore. The absence of a shift in the retinal C = C stretching frequency in these mutants indicates that Asp-212 is not a major determinant of the visible absorption wavelength maximum in light-adapted bR. It is unlikely that Asp-212 is the acceptor group for the Schiff base proton since both the Asp-212----Glu and Asp-212----Ala mutants formed an M intermediate. All of the Asp-212 mutants were missing a Fourier transform infrared difference band that had been assigned previously to protonation changes of Tyr-185. These results are discussed in terms of a model in which Tyr-185 and Asp-212 form a polarizable hydrogen bond and are positioned near the C13-Schiff base portion of the chromophore. These 2 residues may be involved in stabilizing the relative orientation of the F and G helices and isomerizing the retinal in a regioselective manner about the C13 = C14 double bond.     

FTIR study of the photoisomerization processes in the 13-cis and all-trans forms of Anabaena sensory rhodopsin at 77 K

Archaeal-type rhodopsins can accommodate either all-trans- or 13-cis,15-syn-retinal in their chromophore binding site in the dark, but only the former isomer is functionally important. In contrast, Anabaena sensory rhodopsin (ASR), an archaeal-type rhodopsin found in eubacteria, exhibits a photochromic interconversion of both forms, suggesting that ASR functions as a photosensor which interacts with its 14 kDa soluble transducer differently in the all-trans and 13-cis,15-syn forms. In this study, we applied low-temperature Fourier transform infrared (FTIR) spectroscopy to the 13-cis,15-syn form of ASR (13C-ASR) at 77 K and compared the local structure around the chromophore and its structural changes upon retinal photoisomerization with those of the all-trans form (AT-ASR) [Furutani, Y., Kawanabe, A., Jung, K. H., and Kandori, H. (2005) Biochemistry 44, 12287-12296]. By use of [zeta-15N]lysine-labeled ASR, we identified the N-D stretching vibrations of the Schiff base (in D2O) at 2165 cm(-1) for 13C-ASR and at 2163 and 2125 cm(-1) for AT-ASR. The frequencies indicate strong hydrogen bonds of the Schiff base with a water molecule for both 13C-ASR and AT-ASR. In contrast, the N-D stretching vibration appears at 2351 cm(-1) and at 2483 cm(-1) for the K states of 13C-ASR (13C-ASR(K)) and AT-ASR (AT-ASR(K)), respectively, indicating that the Schiff base still forms a hydrogen bond in 13C-ASR(K). Rotational motion of the Schiff base upon retinal isomerization is probably smaller for 13C-ASR than for AT-ASR, the latter altering hydrogen bonding of the Schiff base similar to bacteriorhodopsin (BR), a light-driven proton pump. Appearance of several hydrogen-out-of-plane vibrations and amide I vibrations in 13C-ASR(K), but not in AT-ASR(K), suggests that structural changes are distributed widely along the polyene chain for 13C-ASR. On the other hand, retinal photoisomerization in AT-ASR breaks the hydrogen bond of the Schiff base, and localized structural changes in the Schiff base region are induced.     

Coupling of the reisomerization of the retinal, proton uptake, and reprotonation of Asp-96 in the N photointermediate of bacteriorhodopsin

In the N to O reaction of the bacteriorhodopsin photocycle, Asp-96 is protonated from the cytoplasmic surface, and coupled to this, the retinal isomerizes from 13-cis,15-anti back to the initial all-trans configuration. To dissect the two steps, and to better understand how and why they occur, we describe the properties of two groups of site-specific mutants in which the N intermediate has greatly increased lifetime. In the first group, with the mutations near the retinal, an unusual N state is produced in which the retinal is 13-cis,15-anti but Asp-96 has a protonated carboxyl group. The apparent pK(a) for the protonation is 7.5, as in the wild-type. It is likely that here the interference with N decay is the result of steric conflict of side-chains with the retinal or with the side-chain of Lys-216 connected to the retinal, which delays the reisomerization after protonation of Asp-96. In the second group, with the mutations located near Asp-96 or between Asp-96 and the cytoplasmic surface, reprotonation of Asp-96 is strongly perturbed. The reisomerization of the retinal occurs only after recovery from a long-living protein conformation in which reprotonation of Asp-96 is either entirely blocked or blocked at low pH.     

Orientation of the bacteriorhodopsin chromophore probed by polarized Fourier transform infrared difference spectroscopy

Polarized, low-temperature Fourier transform infrared (FTIR) difference spectroscopy has been used to investigate the structure of bacteriorhodopsin (bR) as it undergoes phototransitions from the light-adapted state, bR570, to the K630 and M412 intermediates. The orientations of specific retinal chromophore and protein groups relative to the membrane plane were calculated from the linear dichroism of the infrared bands, which correspond to the vibrational modes of those groups. The linear dichroism of the chromophore C=C and C-C stretching modes indicates that the long axis of the polyene chain is oriented at 20-25 degrees from the membrane plane at 250 K and that it orients more in-plane when the temperature is reduced to 81 K. The polyene plane is found to be approximately perpendicular to the membrane plane from the linear dichroism calculations of the HOOP (hydrogen out-of-plane) wags. The orientation of the transition dipole moments of chromophore vibrations in the K630 and M412 intermediates has been probed, and the dipole moment direction of the C=O bond of an aspartic acid that is protonated in the bR570----M412 transition has been measured.     

Retinal isomer ratio in dark-adapted purple membrane and bacteriorhodopsin monomers

On the basis of data obtained by spectroscopic analysis and chromatography of retinal extracts, a consensus has been adopted that dark-adapted purple membrane (pm) contains 13-cis- and all-trans-retinal in equal amounts, whereas the light-adapted membrane contains all-trans-retinal only. We have developed an improved extraction technique which extracts up to 70% of the retinal in pm within 4 min. In the extracts from dark-adapted pm at room temperature, we consistently find 66-67% 13-cis-retinal and 33-34% all-trans-retinal, and more than 98.5% all-trans isomer in light-adapted samples. The spectrum obtained by reconstitution of bacterioopsin with 13-cis-retinal at 2 degrees C (to minimize isomerization) shows an absorbance maximum at 554 nm and agrees well with the spectrum for the 13-cis component calculated from the dark-adapted and light-adapted bR spectra with our extraction data. The ratio of 13-cis:all-trans isomer in dark-adapted pm is 2:1 and nearly constant between 0 and 38 degrees C but begins to decrease distinctly above 40 degrees C, and more rapidly near 70 degrees C, reaching 0.75 at 90 degrees C. The van't Hoff plot of the isomer ratio shows a nonlinear temperature dependence above 40 degrees C, indicating a more complex system than a simple thermal 13-cis/all-trans isomer equilibrium. We attribute the broadening, absorbance decrease, and blut shift of the visible absorption band with increasing temperature to the appearance of at least one and possibly two or three new chromophores which contain, mainly or exclusively, the all-trans isomer.(ABSTRACT TRUNCATED AT 250 WORDS)     

Photoconversion from the light-adapted to the dark-adapted state of bacteriorhodopsin.

Dark and light adaptation of bacteriorhodopsin in purple membrane multilayers at less than 100% relative humidity differs from that seen in suspensions. Equilibrium between the two bacteriorhodopsin isomers (bR cis 550 and bR trans 570) in the light-adapted state becomes dependent on the wavelength of actinic light. Excitation at the red edge of the visible absorption band causes dark adaptation in a light-adapted sample. Using polarized actinic and measuring light, we show that acceleration of the dark adaptation through heating by actinic light cannot explain this observation. A light-driven bR trans 570 to bR cis 550 reaction that competes with the well-known 13 cis-to-all-trans light adaptation reaction must exist under our experimental conditions. Trans-to-cis conversion is a one-photon process distinct from the two photon process observed by others in purple membrane suspensions (Sperling, W., C. N. Rafferty, K. D. Kohl, and N. A. Dencher, 1978, FEBS (Fed. Eur. Biochem. Soc.) Lett. 97:129-132). Its quantum efficiency increases monotonously on reducing the hydration level, and is paralleled by an increase in the lifetime of the M410 intermediate of the trans photocycle. We suggest that at this point a branch leads from the all-trans into the 13-cis photocycle. It is probably the same reaction that causes the reduced light adaptation in monomeric bacteriorhodopsin (Casadio, R., H. Gutowitz, P. Mowery, M. Taylor, and W. Stoeckenius, 1980, Biochim. Biophys. Acta. 590:13-23; Casadio, R., and W. Stoeckenius, 1980, Biochemistry. 19:3374-3381).     

The effect of protein conformation change from alpha(II) to alpha(I) on the bacteriorhodopsin photocycle

The bacteriorhodopsin (bR) photocycle was followed by use of time-resolved Fourier-transform infrared (FTIR) spectroscopy as a function of temperature (15-85 degrees C) as the alpha(II) --> alpha(I) conformational transition occurs. The photocycle rate increases with increasing temperature, but its efficiency is found to be drastically reduced as the transition takes place. A large shift is observed in the all-trans left arrow over right arrow 13-cis equilibrium due to the increased stability of the 13-cis isomer in alpha(I) form. This, together with the increase in the rate of dark adaptation as the temperature increases, leads to a large increase in the 13-cis isomer concentration in bR in the alpha(I) form. The fact that 13-cis retinal has a much-reduced absorption cross-section and its inability to pump protons leads to an observed large reduction in the concentration of the observed photocycle intermediates, as well as the proton gradient at a given light intensity. These results suggest that nature might have selected the alpha(II) rather than the alpha(I) form as the helical conformation in bR to stabilize the all-trans retinal isomer that is a better light absorber and is capable of pumping protons.