Infrared evidence that the Schiff base of bacteriorhodopsin is protonated: bR570 and K intermediates

Vibrational spectroscopy of bacteriorhodopsin mutants: chromophore isomerization perturbs tryptophan-86

Fourier transform infrared difference spectra have been obtained for the bR----K and bR----M photoreactions of bacteriorhodopsin mutants with Phe replacements for Trp residues 10, 12, 80, 86, 138, 182, and 189 and Cys replacements for Trp residues 137 and 138. None of the tryptophan mutations caused a significant shift in the retinylidene C = C or C-C stretching frequencies of the visible absorption maximum of the chromophore, it is concluded that none of the tryptophan residues are essential for forming a normal bR570 chromophore. However, a 742-cm-1 negative peak attributed previously to the perturbation of a tryptophan residue during the bR----K photoreaction was found to be absent in the bR----K and bR----M difference spectra of the Trp-86 mutant. On this basis, we conclude that the structure or environment of Trp-86 is altered during the bR----K photoreaction. All of the other Trp----Phe mutants exhibited this band, although its frequency was altered in the Trp-189----Phe mutant. In addition, the Trp-182----Phe mutant exhibited much reduced formation of normal photoproducts relative to the other mutants, as well as peaks indicative of the presence of additional chromophore conformations. A model of bR is discussed in which Trp-86, Trp-182, and Trp-189 form part of a retinal binding pocket. One likely function of these tryptophan groups is to provide the structural constraints needed to prevent chromophore photoisomerization other than at the C13 = C14 double bond.

Nuclear magnetic resonance study of the Schiff base in bacteriorhodopsin: counterion effects on the 15N shift anisotropy

High-resolution, solid-state 15N NMR has been used to study the chemical shift anisotropies of the Schiff bases in bacteriorhodopsin (bR) and in an extensive series of model compounds. Using slow-spinning techniques, we are able to obtain sufficient rotational sideband intensity to determine the full 15N chemical shift anisotropy for the Schiff base nitrogen in bR548 and bR568. Comparisons are made between all-trans-bR568 and N-all-trans-retinylidene butylimine salts with halide, phenolate, and carboxylate counterions. It is argued that for the model compounds the variation in 15N chemical shift reflects the variation in (hydrogen) bond strength with the various counterions. The results suggest that carboxylates and tyrosinates may form hydrogen bonds of comparable strength in a hydrophobic environment. Thus, the hydrogen bonding strength of a counterion depends on factors that are not completely reflected in the solution pKa of its conjugate acid. For the model compounds, the two most downfield principal values of the 15N chemical shift tensor, sigma 22 and sigma 33, vary dramatically with different counterions, whereas sigma 11 remains essentially unaffected. In addition, there exists a linear correlation between sigma 22 and sigma 33, which suggests that a single mechanism is responsible for the variation in chemical shifts present in all three classes of model compounds. The data for bR568 follow this trend, but the isotropic shift is 11 ppm further upfield than any of the model compounds. This extreme value suggests an unusually weak hydrogen bond in the protein.

Analysis of the factors that influence the C=N stretching frequency of polyene Schiff bases. Implications for bacteriorhodopsin and rhodopsin

In this study quantum mechanical calculations of force constants and normal mode analysis are used to elucidate the factors that influence the C=C and C=N stretching frequencies in polyenes and in protonated Schiff bases. The C=N stretching frequency is found to depend on both the C=N stretching force constant and the C=N-H bending force constant. Due to the contributions of these two modes, the C=N stretching frequency is particularly sensitive to the magnitude of the Schiff base counterion interactions and to the hydrogen bonding environment of the Schiff base nitrogen. Models for chromophore-protein interactions in the retinal binding site and for the photochemical transformations of bacteriorhodopsin and rhodopsin are evaluated in light of these results.

Deprotonation of tyrosines in bacteriorhodopsin as studied by Fourier transform infrared spectroscopy with deuterium and nitrate labeling

Fourier transform infrared (FTIR) difference spectra are presented for bacteriorhodopsin (BR) at low temperature. Previous FTIR measurements have identified several tyrosine residues that change their absorption characteristics between light-adapted BR and dark-adapted BR, or between intermediates K and M [Dollinger, G., Eisenstein, L., Lin, S.-L., Nakanishi, K., Odashima, K., & Termini, J. (1986) Methods Enzymol. 127, 649-662]. These changes were explained by protonation/deprotonation of tyrosine moieties and perturbation of the protein environment surrounding tyrosines. A tyrosine deprotonation was observed to occur between intermediates K and M. The present studies confine the deprotonation to being between intermediates L and M and show that no tyrosines undergo changes between the K and the L states. Evidence is presented that none of the tyrosines undergoing changes at low temperature can be assigned to tyrosine-64. The environmental changes of these tyrosines are discussed in relation to the proton pumping mechanism. Their spatial relation to the chromophore is also discussed. At least two tyrosines are suggested to reside close to the retinal binding site. The reactive groups of the nitrated tyrosine-64 are speculated to be remote from the Schiff base and the active tyrosines but can possibly interact sterically with the ionone ring of the retinal.

Conformational changes in bacteriorhodopsin studied by infrared attenuated total reflection

We report on a new method based on Fourier transform infrared (FTIR)-difference spectroscopy for studying the conformational changes occurring during the photocycle of bacteriorhodopsin. Previous studies have been made by measuring the absorbance of an infrared (IR) beam transmitted through a thin hydrated purple membrane film. In contrast, the present study utilizes the technique of attenuated total reflection (ATR). Purple membrane is fixed on the surface of a germanium internal reflection crystal and immersed in a buffer whose pH and ionic composition can be varied. Measurements of the amide I and II absorbance with light polarized parallel and at 45 degrees to the crystal surface reveals that the membrane is highly oriented. An ATR-FTIR-difference spectrum of the light to dark (bR570 to bR548) transition is similar but not identical to the transmittance FTIR-difference spectrum. This disagreement between the two methods is shown to be due in the ATR case to the absorption of transition moments oriented predominantly out of the membrane plane. Raising the pH of La3+ substituted purple membrane films from 6.8 to 8.0 slows the M-decay rate sufficiently so that a bR570 to M412 difference spectrum can be obtained with steady state illumination at room temperature. A comparison of this difference spectrum with that obtained at -23 degrees C using the transmittance method reveals several changes that cannot be attributed to out-of-plane transition moments. An increase in the intensity of peaks in the amide I and II regions agrees with recent time-resolved kinetic FTIR-difference measurements and indicates that a localized protein conformational change involving the peptide backbone of bR occurs which is not evident at the lower temperature.

Millisecond Fourier-transform infrared difference spectra of bacteriorhodopsin's M412 photoproduct

We have obtained room-temperature transient infrared difference spectra of the M412 photoproduct of bacteriorhodopsin (bR) by using a "rapid-sweep" Fourier-transform infrared (FT-IR) technique that permits the collection of an entire spectrum (extending from 1000 to 2000 cm-1 with 8-cm-1 resolution) in 5 ms. These spectra exhibit less than 10(-4) absorbance unit of noise, even utilizing wet samples containing approximately 10 pmol of bR in the measuring beam. The bR----M transient difference spectrum is similar to FT-IR difference spectra previously obtained under conditions where M decay was blocked (low temperature or low humidity). In particular, the transient spectrum exhibits a set of vibrational difference bands that were previously attributed to protonation changes of several tyrosine residues on the basis of isotopic derivative spectra of M at low temperature. Our rapid-sweep FT-IR spectra demonstrate that these tyrosine/tyrosinate bands are also present under more physiological conditions. Despite the overall similarity to the low-temperature and low-humidity spectra, the room-temperature bR----M transient difference spectrum shows significant additional features in the amide I and amide II regions. These features' presence suggests that a small alteration of the protein backbone accompanies M formation under physiological conditions and that this conformational change is inhibited in the absence of liquid water.

Fourier transform infrared difference spectroscopy of bacteriorhodopsin and its photoproducts regenerated with deuterated tyrosine

Fourier transform infrared (FTIR) difference spectroscopy has been used to detect the vibrational modes due to tyrosine residues in the protein that change in position or intensity between light-adapted bacteriorhodopsin (LA) and other species, namely, the K and M intermediates and dark-adapted bacteriorhodopsin (DA). To aid in the identification of the bands that change in these various species, the FTIR spectra of the free amino acids Tyr-d0, Tyr-d2 (2H at positions ortho to OH), and Tyr-d4 (2H at positions ortho and meta to OH) were measured in H2O and D2O at low and high pH. The characteristic frequencies of the Tyr species obtained in this manner were then used to identify the changes in protonation state of the tyrosine residues in the various bacteriorhodopsin species. The two diagnostically most useful bands were the approximately 1480-cm-1 band of Tyr(OH)-d2 and the approximately 1277-cm-1 band of Tyr(O-)-d0. Mainly by observing the appearance or disappearance of these bands in the difference spectra of pigments incorporating the tyrosine isotopes, it was possible to identify the following: in LA, one tyrosine and one tyrosinate; in the K intermediate, two tyrosines; in the M intermediate, one tyrosine and one tyrosinate; and in DA, two tyrosines. Since these residues were observed in the difference spectra K/LA, M/LA, and DA/LA, they represent the tyrosine or tyrosinate groups that most likely undergo changes in protonation state due to the conversions. These changes are most likely linked to the proton translocation process of bacteriorhodopsin.

Order of proton uptake and release by bacteriorhodopsin at low pH

The order of proton uptake and release in an aqueous suspension of purple membrane in response to a light flash has been investigated at lowered pH. pH indicator dyes and a flash spectrophotometer were used for the study. At pH 6.6 it was found that the release of protons from the purple membrane precedes uptake, as reported by other investigators. At pH 5.9, 4.9, and 4.1 it was also found that release precedes uptake. These results are not in agreement with those of previous investigators.

Evidence for a tyrosine protonation change during the primary phototransition of bacteriorhodopsin at low temperature

Isotopically labeled tyrosines have been selectively incorporated into bacteriorhodopsin (bR). A comparison of the low-temperature bR570 to K Fourier transform infrared-difference spectra of these samples and normal bR provides information about the role of tyrosine in the primary phototransition. Several tyrosine contributions to the difference spectrum are found. These results and comparison with the spectra of model compounds suggest that a tyrosinate group protonates during the bR570 to K transition. This conclusion is strongly supported by the results of UV difference spectroscopy.

Solid-state 13C NMR detection of a perturbed 6-s-trans chromophore in bacteriorhodopsin

Solid-state 13C magic angle sample spinning NMR spectroscopy has been used to study the ionone ring portion of the chromophore of bacteriorhodopsin. Spectra were obtained from fully hydrated samples regenerated with retinals 13C labeled at positions C-5, C-6, C-7, C-8, and C-18 and from lyophilized samples regenerated with retinals labeled at C-9 and C-13. C-15-labeled samples were studied in both lyophilized and hydrated forms. Three independent NMR parameters (the downfield element of the C-5 chemical shift tensor, the C-8 isotropic chemical shift, and the C-18 longitudinal relaxation time) indicate that the chromophore has a 6-s-trans conformation in the protein, in contrast to the 6-s-cis conformation that is energetically favored for retinoids in solution. We also observe an additional 27 ppm downfield shift in the middle element of the C-5 shift tensor, which provides support for the existence of a negatively charged protein residue near C-5. Evidence for a positive charge near C-7, possibly the counterion for the negative charge, is also discussed. On the basis of these results, we present a new model for the retinal binding site, which has important implications for the mechanism of the "opsin shift" observed in bacteriorhodopsin.

Fourier-transform infrared difference spectroscopy of rhodopsin and its photoproducts at low temperature

Fourier-transform infrared difference spectroscopy has been used to detect the vibrational modes in the chromophore and protein that change in position or intensity between rhodopsin and the photoproducts formed at low temperature (70 K), bathorhodopsin and isorhodopsin. A method has been developed to obtain infrared difference spectra between rhodopsin and bathorhodopsin, bathorhodopsin and isorhodopsin, and rhodopsin and isorhodopsin. To aid in the identification of the vibrational modes, we performed experiments on deuterated and hydrated films of native rod outer segments and rod outer segments regenerated with either retinal containing 13C at carbon 15 or 15-deuterioretinal. Our infrared measurements provide independent verification of the resonance Raman result that the retinal in bathorhodopsin is distorted all-trans. The positions of the C = N stretch in the deuterated pigment and the deuterated pigments regenerated with 11-cis-15-deuterioretinal or 11-cis-retinal containing 13C at carbon 15 are indicative that the Schiff-base linkage is protonated in rhodopsin, bathorhodopsin, and isorhodopsin. Furthermore, the C = N stretching frequency occurs at the same position in all three species. The data indicate that the protonated Schiff base has a C = N trans conformation in all three species. Finally, we present evidence that, even in these early stages of the rhodopsin photosequence, changes are occurring in the opsin and perhaps the associated lipids.

Determination of retinal chromophore structure in bacteriorhodopsin with resonance Raman spectroscopy

The analysis of the vibrational spectrum of the retinal chromophore in bacteriorhodopsin with isotopic derivatives provides a powerful "structural dictionary" for the translation of vibrational frequencies and intensities into structural information. Of importance for the proton-pumping mechanism is the unambiguous determination of the configuration about the C13=C14 and C=N bonds, and the protonation state of the Schiff base nitrogen. Vibrational studies have shown that in light-adapted BR568 the Schiff base nitrogen is protonated and both the C13=C14 and C=N bonds are in a trans geometry. The formation of K625 involves the photochemical isomerization about only the C13=C14 bond which displaces the Schiff base proton into a different protein environment. Subsequent Schiff base deprotonation produces the M412 intermediate. Thermal reisomerization of the C13=C14 bond and reprotonation of the Schiff base occur in the M412------O640 transition, resetting the proton-pumping mechanism. The vibrational spectra can also be used to examine the conformation about the C--C single bonds. The frequency of the C14--C15 stretching vibration in BR568, K625, L550 and O640 argues that the C14--C15 conformation in these intermediates is s-trans. Conformational distortions of the chromophore have been identified in K625 and O640 through the observation of intense hydrogen out-of-plane wagging vibrations in the Raman spectra (see Fig. 2). These two intermediates are the direct products of chromophore isomerization. Thus it appears that following isomerization in a tight protein binding pocket, the chromophore cannot easily relax to a planar geometry. The analogous observation of intense hydrogen out-of-plane modes in the primary photoproduct in vision (Eyring et al., 1982) suggests that this may be a general phenomenon in protein-bound isomerizations. Future resonance Raman studies should provide even more details on how bacterio-opsin and retinal act in concert to produce an efficient light-energy convertor. Important unresolved questions involve the mechanism by which the protein catalyzes deprotonation of the L550 intermediate and the mechanism of the thermal conversion of M412 back to BR568. Also, it has been shown that under conditions of high ionic strength and/or low light intensity two protons are pumped per photocycle (Kuschmitz & Hess, 1981). How might this be accomplished?(ABSTRACT TRUNCATED AT 400 WORDS)

New biophysical techniques and their application to the study of membranes

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Modification of pK values caused by change in H-bond geometry

The competition between various groups for a proton is studied by ab initio molecular orbital methods. It is found that reorientations of the two groups involved in a H-bond can reverse the equilibrium position of the proton shared between them. Specifically, the carbonyl and hydroxyl groups were modeled by H2CO and HOH. In the H-bond between these two groups, association of the proton with the carbonyl (H2COH...OH2)+ is favored over the hydroxyl (H2CO...HOH2)+ when the latter group is situated along a lone pair of the carbonyl oxygen. However, displacement of the water to the C = O axis between the two carbonyl lone pairs reverses the situation and (H2CO...HOH2)+ is more stable. A similar reversal of stability is observed in the H-bond involving a Schiff base (modeled by CH2NH) and amine (NH3). In one arrangement where the lone pairs of the two groups point toward one another, the proton prefers the Schiff base to the amine--i.e., (H2CHNH...NH3)+ is more stable than (H2CHN...HNH3)+. On the other hand, rotation of the lone pair of the amine away from the Schiff base nitrogen results in proton transfer across to the amine. These shifts in stability correspond to reversal of relative pK of the groups involved. A fundamental principle emerging from the calculations is that ion-dipole electrostatic interactions favor transfer of a proton to the group that is positioned as closely as possible to the negative end of the dipole moment vector of the other. The ideas developed here suggest a number of means by which conformational changes may be utilized to shift protons from residue to residue within a protein molecule such as an enzyme or bacteriorhodopsin.

Trans/13-cis isomerization is essential for both the photocycle and proton pumping of bacteriorhodopsin

We studied an analogue of bacteriorhodopsin whose chromophore is based on all-trans retinal. A five-membered ring was built around the 13-14 double bond so as to prohibit trans to 13-cis isomerization. No light-induced photochemical changes were seen, other than those due to a small amount (approximately 5%) of unbleached bacteriorhodopsin remaining in the apomembrane used for regeneration. The techniques used included flash photolysis at room and liquid nitrogen temperatures and Fourier-transform infrared difference spectroscopy. When the trans-fixed pigment was incorporated into phospholipid vesicles, no evidence of light-initiated proton pumping could be found. The results indicate that trans to 13-cis isomerization is essential for the photochemical transformation and function of bacteriorhodopsin.

Light-driven protonation changes of internal aspartic acids of bacteriorhodopsin: an investigation by static and time-resolved infrared difference spectroscopy using [4-13C]aspartic acid labeled purple membrane

The molecular events during the photocycle of bacteriorhodopsin have been studied by the method of time-resolved and static infrared difference spectroscopy. Characteristic spectral changes involving the C=O stretching vibration of protonated carboxylic groups were detected. To identify the corresponding groups with either glutamic or aspartic acid, BR was selectively labeled with [4-13C]aspartic acid. An incorporation of ca. 70% was obtained. The comparison of the difference spectra in the region of the CO2- stretching vibrations of labeled and unlabeled BR indicates that ionized aspartic acids are influenced during the photocycle, the earliest effect being observed already at the K610 intermediate. Taken together, the results provide evidence that four internal aspartic acids undergo protonation changes and that one glutamic acid, remaining protonated, is disturbed. The results are discussed in relation to the various aspects of the proton pumping mechanism, such as retinal isomerization, charge separation, pK changes, and proton pathway.

Solid-state 13C NMR studies of retinal in bacteriorhodopsin

Solid-state 13C magic-angle sample spinning (MASS) NMR has been used to study lyophilized dark-adapted purple membrane containing 13C-labeled retinals. C-10-, C-11-, and C-12-labeled derivatives each showed two lines, assigned to the coexisting 13-cis and all-trans isomers. The isotropic chemical shifts, particularly of C-11, indicate that the Schiff base is protonated. Shift anisotropies are also similar to those of model compounds, indicating that this part of the chromophore is rigid and immobile and possesses the same degree of in-plane bending as crystalline retinal derivatives. Purple membrane samples labeled on the C-19- and C-20-methyl groups both give single lines from the retinal, upfield shifted by 2.1 and 1.0 ppm, respectively, from model compounds. In all cases, high-quality spectra were obtained from approximately 50-mg samples in modest signal-averaging times. These results suggest that it is now practical to exploit the enormous potential of MASS NMR for structural studies of 13C-labeled membrane proteins.

Fourier-transform infrared spectroscopy applied to rhodopsin. The problem of the protonation state of the retinylidene Schiff base re-investigated

By measuring the rhodopsin--bathorhodopsin, isorhodopsin--bathorhodopsin, rhodopsin--isorhodopsin and rhodopsin--meta-II difference spectra with the method of Fourier-transform infrared spectroscopy we have identified the C = N stretching vibration of the protonated retinylidene Schiff base of rhodopsin, isorhodopsin and bathorhodopsin. In contrast to resonance Raman spectroscopy additional strong bands were observed between 1700 cm-1 and 1620 cm-1. Most of them depend on the isomeric state of the chromophore. The origin of these bands will be discussed. In the fingerprint region isorhodopsin and bathorhodopsin are quite similar but no similarities with infrared spectra of model compounds of any isomeric composition are observed. Therefore, no conclusions on the isomeric state of the retinal in bathorhodopsin can be drawn. We provide evidence for the modification of one or two carboxylic group(s) during the rhodopsin--bathorhodopsin and isorhodopsin--bathorhodopsin transition.

Proton currents and protein motion in membranes

A mechanism is proposed whereby a proton gradient along a membrane-spanning alpha-helix is coupled to small changes in the torsional angles around the alpha-helix peptide bonds. Small concerted changes in the torsional angles are coupled to a change in the unit twist of the alpha-helix; a change in the unit twist is coupled to a change in the crossing angle between neighbouring alpha-helices; and a change in the crossing angle is coupled to a change in the size and shape of an assembly of alpha-helices. Following this logical linkage in one direction shows how a proton gradient could induce a pumping motion in an assembly of alpha-helices; following it in the other direction shows how motion in an assembly of alpha-helices could pump protons.

Biological applications of picosecond spectroscopy

Technological advances in picosecond spectroscopy have permitted the mechanisms of various chemical, physical and biological processes to be elucidated and understood to a greater degree than ever before. By means of picosecond emission, absorption and Raman spectroscopy, one can probe and measure directly the transient intermediates and kinetics of primary events in complex biological processes. A description of two current types of laser systems--solid-state and synchronously pumped dye lasers--and their application to determining the primary events in the biological processes of dissociation of oxy- and carboxymyoglobin, excited-state relaxation of porphyrins and visual transduction, illustrate the power of picosecond spectroscopy.

Investigation of the primary photochemistry of bacteriorhodopsin by low-temperature Fourier-transform infrared spectroscopy

The method of Fourier-transform infrared difference spectroscopy was applied to investigate the transition at 77K of bacteriorhodopsin in its light-adapted form to K6(10), the first intermediate which is stable at low temperature. In addition to unmodified bacteriorhodopsin, bacteriorhodopsin in 2H2O and bacteriorhodopsin containing [15-2H]retinal was used. The results show that major rearrangements occur in the Schiff base in this transition. It is not possible to identify a C = N stretching vibration of the Schiff base in K6(10). The identification of an N-H bending vibration in K6(10) shows that the nitrogen of the previous Schiff base still has a proton attached. The fingerprint region exhibits very unusual features for K6(10) and bears no similarity to protonated retinylidene Schiff base model compounds of any isomeric composition. Therefore, no conclusions on the isomeric state of the retinal in K6(10) can be drawn. The spectra show that the terminal part of the retinal is predominantly reflected in the difference spectra. This indicates that the most polar part of the retinal is located near the Schiff base. We have evidence for protein molecular changes occurring in this transition at 77K.