Effect of point mutations on the ultrafast photo-isomerization of Anabaena sensory rhodopsin.

Anabaena sensory rhodopsin (ASR) is a particular microbial retinal protein for which light-adaptation leads to the ability to bind both the all-trans, 15-anti (AT) and the 13-cis, 15-syn (13C) isomers of the protonated Schiff base of retinal (PSBR). In the context of obtaining insight into the mechanisms by which retinal proteins catalyse the PSBR photo-isomerization reaction, ASR is a model system allowing to study, within the same protein, the protein-PSBR interactions for two different PSBR conformers at the same time. A detailed analysis of the vibrational spectra of AT and 13C, and their photo-products in wild-type ASR obtained through femtosecond (pump-) four-wave-mixing is reported for the first time, and compared to bacterio- and channelrhodopsin. As part of an extensive study of ASR mutants with blue-shifted absorption spectra, we present here a detailed computational analysis of the origin of the mutation-induced blue-shift of the absorption spectra, and identify electrostatic interactions as dominating steric effects that would entail a red-shift. The excited state lifetimes and isomerization reaction times (IRT) for the three mutants V112N, W76F, and L83Q are studied experimentally by femtosecond broadband transient absorption spectroscopy. Interestingly, in all three mutants, isomerization is accelerated for AT with respect to wild-type ASR, and this the more, the shorter the wavelength of maximum absorption. On the contrary, the 13C photo-reaction is slightly slowed down, leading to an inversion of the ESLs of AT and 13C, with respect to wt-ASR, in the blue-most absorbing mutant L83Q. Possible mechanisms for these mutation effects, and their steric and electrostatic origins are discussed.

Photoisomerization in rhodopsin.

This article reviews the primary reaction processes in rhodopsin, a photoreceptive pigment for twilight vision. Rhodopsin has an 11-cis retinal as the chromophore, which binds covalently with a lysine residue through a protonated Schiff base linkage. Absorption of a photon by rhodopsin initiates the primary photochemical reaction in the chromophore. Picosecond time-resolved spectroscopy of 11-cis locked rhodopsin analogs revealed that the cis-trans isomerization of the chromophore is the primary reaction in rhodopsin. Then, generation of femtosecond laser pulses in the 1990s made it possible to follow the process of isomerization in real time. Formation of photorhodopsin within 200 fsec was observed by a transient absorption (pump-probe) experiment, which also revealed that the photoisomerization in rhodopsin is a vibrationally coherent process. Femtosecond fluorescence spectroscopy directly captured excited-state dynamics of rhodopsin, so that both coherent reaction process and unreacted excited state were observed. Faster photoreaction of the chromophore in rhodopsin than that in solution implies that the protein environment facilitates the efficient isomerization process. Such contributions of the protein residues have been monitored by infrared spectroscopy of rhodopsin, bathorhodopsin, and isorhodopsin (9-cis rhodopsin) at low temperatures. The crystal structure of bovine rhodopsin recently reported will lead to better understanding of the mechanism in future.

Internal water molecules of pharaonis phoborhodopsin studied by low-temperature infrared spectroscopy.

In the Schiff base region of bacteriorhodopsin (BR), a light-driven proton-pump protein, three internal water molecules are involved in a pentagonal cluster structure. These water molecules constitute a hydrogen-bonding network consisting of two positively charged groups, the Schiff base and Arg82, and two negatively charged groups, Asp85 and Asp212. Previous infrared spectroscopy of BR revealed stretching vibrations of such water molecules under strong hydrogen-bonding conditions using spectral differences in D2O and D2(18O) [Kandori and Shichida (2000) J. Am. Chem. Soc. 122, 11745-11746]. The present study extends the infrared analysis to another archaeal rhodopsin, pharaonis phoborhodopsin (ppR; also called pharaonis sensory rhodopsin-II, psR-II), involved in the negative phototaxis of Natronobacterium pharaonis. Despite functional differences between ppR and BR, similar spectral features of water bands were observed before and after photoisomerization of the retinal chromophore at 77 K. This implies that the structure and the structural changes of internal water molecules are similar between ppR and BR. Higher stretching frequencies of the bridged water in ppR suggest that the water-containing pentagonal cluster structure is considerably distorted in ppR. These observations are consistent with the crystallographic structures of ppR and BR. The water structure and structural changes upon photoisomerization of ppR are discussed here on the basis of their infrared spectra.

Structural changes of pharaonis phoborhodopsin upon photoisomerization of the retinal chromophore: infrared spectral comparison with bacteriorhodopsin.

Archaeal rhodopsins possess a retinal molecule as their chromophores, and their light energy and light signal conversions are triggered by all-trans to 13-cis isomerization of the retinal chromophore. Relaxation through structural changes of the protein then leads to functional processes, proton pump in bacteriorhodopsin and transducer activation in sensory rhodopsins. In the present paper, low-temperature Fourier transform infrared spectroscopy is applied to phoborhodopsin from Natronobacterium pharaonis (ppR), a photoreceptor for the negative phototaxis of the bacteria, and infrared spectral changes before and after photoisomerization are compared with those of bacteriorhodopsin (BR) at 77 K. Spectral comparison of the C--C stretching vibrations of the retinal chromophore shows that chromophore conformation of the polyene chain is similar between ppR and BR. This fact implies that the unique chromophore-protein interaction in ppR, such as the blue-shifted absorption spectrum with vibrational fine structure, originates from both ends, the beta-ionone ring and the Schiff base regions. In fact, less planer ring structure and stronger hydrogen bond of the Schiff base were suggested for ppR. Similar frequency changes upon photoisomerization are observed for the C==N stretch of the retinal Schiff base and the stretch of the neighboring threonine side chain (Thr79 in ppR and Thr89 in BR), suggesting that photoisomerization in ppR is driven by the motion of the Schiff base like BR. Nevertheless, the structure of the K state after photoisomerization is different between ppR and BR. In BR, chromophore distortion is localized in the Schiff base region, as shown in its hydrogen out-of-plane vibrations. In contrast, more extended structural changes take place in ppR in view of chromophore distortion and protein structural changes. Such structure of the K intermediate of ppR is probably correlated with its high thermal stability. In fact, almost identical infrared spectra are obtained between 77 and 170 K in ppR. Unique chromophore-protein interaction and photoisomerization processes in ppR are discussed on the basis of the present infrared spectral comparison with BR.

Difference in molecular structure of rod and cone visual pigments studied by Fourier transform infrared spectroscopy.

To investigate the local structure that causes the differences in molecular properties between rod and cone visual pigments, we have measured the difference infrared spectra between chicken green and its photoproduct at 77 K and compared them with those from bovine and chicken rhodopsins. In contrast to the similarity of the vibrational bands of the chromophore, those of the protein part were notably different between chicken green and the rhodopsins. Like the rhodopsins, chicken green has an aspartic acid at position 83 (D83) but exhibited no signals due to the protonated carboxyl of D83 in the C=O stretching region, suggesting that the molecular contact between D83 and G120 through water molecule evidenced in bovine rhodopsin is absent in chicken green. A pair of positive and negative bands due to the peptide backbone (amide I) was prominent in chicken green, while the rhodopsins exhibited only small bands in this region. Furthermore, chicken green exhibited characteristic paired bands around 1480 cm(-1), which were identified as the imide bands of P189 using site-directed mutagenesis. P189, situated in the putative second extracellular loop, is conserved in all the known cone visual pigments but not in rhodopsins. Thus, some region of the second extracellular loop including P189 is situated near the chromophore and changes its environment upon formation of the batho-intermediate. The results noted above indicate that differences in the protein parts between chicken green and the rhodopsins alter the changes seen in the protein upon photoisomerization of the chromophore. Some of these changes appear to be the pathway from the chromophore to cytoplasmic surface of the pigment and thus could affect the activation process of transducin.

Tight Asp-85--Thr-89 association during the pump switch of bacteriorhodopsin.

Unidirectional proton transport in bacteriorhodopsin is enforced by the switching machinery of the active site. Threonine 89 is located in this region, with its O--H group forming a hydrogen bond with Asp-85, the acceptor for proton transfer from the Schiff base of the retinal chromophore. Previous IR spectroscopy of [3-(18)O]threonine-labeled bacteriorhodopsin showed that the hydrogen bond of the O--D group of Thr-89 in D(2)O is strengthened in the K photocycle intermediate. Here, we show that the strength and orientation of this hydrogen bond remains unchanged in the L intermediate and through the M intermediate. Furthermore, a strong interaction between Asp-85 and the O--H (O--D) group of Thr-89 in M is indicated by a shift in the C==O stretching vibration of the former because of (18)O substitution in the latter. Thus, the strong hydrogen bond between Asp-85 and Thr-89 in K persists through M, contrary to structural models based on x-ray crystallography of the photocycle intermediates. We propose that, upon photoisomerization of the chromophore, Thr-89 forms a tight, persistent complex with one of the side-chain oxygens of Asp-85 and is thereby precluded from participating in the switching process. On the other hand, the loss of hydrogen bonding at the other oxygen of Asp-85 in M may be related to the switching event.

Chloride effect on iodopsin studied by low-temperature visible and infrared spectroscopies.

To investigate the chloride effect on the spectral properties of iodopsin, we have prepared an anion-free iodopsin (iodopsin.free) by extensive dialysis of an iodopsin sample against a buffer containing no chloride, and visible and infrared difference spectra between iodopsin.free and its photoproduct at 77 K were recorded. The absorption maximum of iodopsin.free in L-alpha-phosphatidylcholine liposomes was 528 nm, which was almost identical with that of the nitrate-bound form of iodopsin (526 nm, iodopsin.NO(3)), but 43 nm blue-shifted from that of the chloride-bound form of iodopsin (iodopsin.Cl). The iod/batho visible difference spectrum obtained from iodopsin.free was similar in shape to that from iodopsin.NO(3), but not to that from iodopsin.Cl. FTIR spectroscopy revealed that the chromophore vibrational bands and the peptide bonds of the original state in iodopsin.free were identical with those in iodopsin.NO(3) and were also similar to those in iodopsin.Cl except for the ethylenic vibrations of the chromophore. In contrast, those of the batho state in iodopsin.free were similar to those in iodopsin.NO(3) but considerably different from those in iodopsin.Cl. These results suggested that the binding of chloride but not nitrate induces a conformational change in the protein and that the chloride binding site is situated in a position where it directly interacts with the chromophore when the chromophore is photoisomerized. FTIR spectroscopy also revealed that one of the four water bands observed in the batho/iod spectrum of iodospin.Cl is absent in the spectra of iodopsin.free and iodopsin.NO(3). Thus, in contrast to nitrate, a lyotropic anion, chloride would bind to the binding site with water molecule(s) which could form a hydrogen-bonding network with amino acid residue(s) near the chromophore, thereby resulting in the red shift of the absorption maximum of iodopsin.

Role of internal water molecules in bacteriorhodopsin.

Internal water molecules are considered to play a crucial role in the functional processes of proton pump proteins. They may participate in hydrogen-bonding networks inside proteins that constitute proton pathways. In addition, they could participate in the switch reaction by mediating an essential proton transfer at the active site. Nevertheless, little has been known about the structure and function of internal water molecules in such proteins. Recent progress in infrared spectroscopy and X-ray crystallography provided new information on water molecules inside bacteriorhodopsin, the light-driven proton pump. The accumulated knowledge on bacteriorhodopsin in the last decade of the 20th century will lead to a realistic picture of internal water molecules at work in the 21st century. In this review, I describe how the role of water molecules has been studied in bacteriorhodopsin, and what should be known about the role of water molecules in the future.

Relocation of internal bound water in bacteriorhodopsin during the photoreaction of M at low temperatures: an FTIR study.

Changes in the FTIR difference spectra upon photoconversion of the M intermediate to its photoproduct(s) M' were studied in wild-type bacteriorhodopsin and several mutants at low temperatures. The studies aimed at examining whether internally bound water molecules interact with the chromophore and the key residues Asp85 and Asp96 in M, and whether these water molecules participate in the reprotonation of the Schiff base. We have found that three water molecules are perturbed by the isomerization of the chromophore in the M --> M' transition at 80 K. The perturbation of one water molecule, detected as a bilobe at 3567(+)/3550(-) cm(-)(1), relaxed in parallel with the relaxation of an Asp85 perturbation upon increasing temperature from 80 to 100 and 133 K (before the reprotonation of the Schiff base). Two water bands of M at 3588 and 3570 cm(-)(1) shift to 3640 cm(-)(1) upon photoconversion at 173 K. These bands were attributed to water molecules which are located in the vicinity of the Schiff base and Asp85 (Wat85). In the M to M' transition at 80 and 100 K, where the Schiff base remained unprotonated, the Wat85 pair stayed in similar states to those in M. The reprotonation of the Schiff base at 133 K occurred without the restoration of the Wat85 band around 3640 cm(-)(1). This band was restored at higher temperatures. Two water molecules in the region surrounded by Thr46, Asp96, and Phe219 (Wat219) were perturbed in the M to M' transition at 80 K and relaxed in parallel with the relaxation of the perturbation of Asp96 upon increasing the temperature. Mutant studies show that upon photoisomerization of the chromophore at 80 K one of the Wat219 water molecules moves closer to Val49 (located near the lysine side chain attached to retinal, and close to the Schiff base). These data along with our previous results indicate that the water molecules in the cytoplasmic domain participate in the connection of Asp96 with the Schiff base and undergo displacement during photoconversions, presumably shuttling between the Schiff base and a site close to Asp96 in the L to M to N transitions.

Water structural changes involved in the activation process of photoactive yellow protein.

Fourier transform infrared (FTIR) spectroscopy was applied to the blue-light photoreceptor photoactive yellow protein (PYP) to investigate water structural changes possibly involved in the photocycle of PYP. Photointermediates were stabilized at low temperature, and difference IR spectra were obtained between intermediate states and the original state of PYP (pG). Water structural changes were never observed in the >3570 cm(-)(1) region for the intermediates stabilized at 77-250 K, such as the red-shifted pR and blue-shifted pB intermediates. In contrast, a negative band was observed at 3658 cm(-)(1) in the pB minus pG spectrum at 295 K, which shifts to 3648 cm(-)(1) upon hydration with H(2)(18)O. The high frequency of the O-H stretch of water indicates that the water O-H group does not form hydrogen bonds in pG, and newly forms these upon pB formation at 295 K, but not at 250 K. Among 92 water molecules in the crystal structure of PYP, only 1 water molecule, water-200, is present in a hydrophobic core inside the protein. The amide N-H of Gly-7 and the imidazole nitrogen atom of His-108 are its possible hydrogen-bonding partners, indicating that one O-H group of water-200 is free to form an additional hydrogen bond. The water band at 3658 cm(-)(1) was indeed diminished in the H108F protein, which strongly suggests that the water band originates from water-200. Structural changes of amide bands in pB were much greater in the wild-type protein at 295 K than at 250 K or in the H108F protein at 295 K. The position of water-200 is >15 A remote from the chromophore. Virtually no structural changes were reported for regions larger than a few angstroms away from the chromophore, in the time-resolved X-ray crystallography experiments on pB. On the basis of the present results, as well as other spectroscopic observations, we conclude that water-200 (buried in a hydrophobic core in pG) is exposed to the aqueous phase upon formation of pB in solution. In neither crystalline PYP nor at low temperature is this structural transition observed, presumably because of the restrictions on global structural changes in the protein under these conditions.

Local and distant protein structural changes on photoisomerization of the retinal in bacteriorhodopsin.

The photoisomerization of the retinal in bacteriorhodopsin is selective and efficient and yields perturbation of the protein structure within femtoseconds. The stored light energy in the primary intermediate is then used for the net translocation of a proton across the membrane in the microsecond to millisecond regime. This study is aimed at identifying how the protein changes on photoisomerization by using the O-H groups of threonines as internal probes. Polarized Fourier-transform IR spectroscopy of [3-(18)O]threonine-labeled and unlabeled bacteriorhodopsin indicates that 3 of the threonines (of a total of 18) change their hydrogen bonding. One is exchangeable in D(2)O, but two are not. A comprehensive mutation study indicates that the residues involved are Thr-89, Thr-17, and Thr-121 (or Thr-90). The perturbation of only three threonine side chains suggests that the structural alteration at this stage of the photocycle is local and specific. Furthermore, the structural change of Thr-17, which is located >11 A from the retinal chromophore, implicates a specific perturbation channel in the protein that accompanies the retinal motion.

Effect of anion binding on iodopsin studied by low-temperature fourier transform infrared spectroscopy.

The effect of anion binding on iodopsin, the chicken red-sensitive cone visual pigment, was studied by measurements of the Fourier transform infrared spectra of chloride- and nitrate-bound forms of iodopsin at 77 K. In addition to the blue shift of the absorption maximum upon substituting nitrate for chloride, the C=C stretching vibrations of iodopsin and its photoproducts were upshifted 5-6 cm(-)(1). The C=NH and C=ND stretching vibrations were the same in wavenumber between the chloride- and nitrate-bound forms, indicating that the binding of either chloride or nitrate has no effect on the interaction between the protonated Schiff base and the counterion. The vibrational bands of iodopsin in the fingerprint and the hydrogen out-of-plane wagging regions were insensitive to anion substitution, suggesting that local chromophore interactions with the anions are not crucial for the absorption spectral shift. In contrast, bathoiodopsin in the chloride-bound form exhibited an intense C(14)H wagging mode, whose intensity was considerably weakened upon substitution of nitrate for chloride. These results suggest that binding of chloride changes the environment near the C(14) position of the chromophore, which could be one of the factors in the thermal reverse reaction of bathoiodopsin to iodopsin in the chloride-bound form.

Availability of sperm examination for male reproductive toxicities in rats treated with boric acid.

Sperm morphological examination, computer-assisted sperm analysis (CASA) and histopathologic examination of the testis and epididymis were performed for male rats treated orally with boric acid for 3 weeks at dosage levels of 50, 150 and 500 mg/kg/day, and treated males were mated with untreated females. None of the males treated with 500 mg/kg/day could impregnate untreated females. The fertility index showed a tendency to decrease in males treated with 150 mg/kg/day. At necropsy, the pre-implantation loss rate in females mated with males treated with 150 mg/kg/day was higher than the control values. Upon epididymal sperm analysis using the CASA system, all parameters including the number of sperm and sperm motions were found to be affected in males treated with 500 mg/kg/day, and the number of sperm, percent motile, velocities and amplitude of lateral head displacement (ALH) were affected in males treated with 150 mg/kg/day. Upon sperm morphological examination, head and tail abnormalities were observed in males treated with 150 and 500 mg/kg/day. In the histopathological examination, atrophy of the seminiferous tubules and multinucleated giant cells in the testes were observed in males treated with 500 mg/kg/day.

Effects of subunit I mutations on redox-linked conformational changes of the Escherichia coli bo-type ubiquinol oxidase revealed by Fourier-transform infrared spectroscopy.

Cytochrome bo is the heme-copper terminal ubiquinol oxidase in the aerobic respiratory chain of Escherichia coli, and functions as a redox-coupled proton pump. As an extension to our mutagenesis and Fourier-transform infrared studies on ion pumps, we examined the effects of subunit I mutations on redox-linked protein structural changes in cytochrome bo. Upon photo-reduction in the presence of riboflavin, Y288F and H333A showed profound effects in their peptide backbone vibrations (amide-I and amide-II), probably due to the loss of CuB or replacement of high-spin heme o with heme B. In the frequency region of protonated carboxylic C=O stretching vibrations, negative 1,743 cm-1 and positive 1,720 cm-1 bands were observed in the wild-type; the former shifted to 1,741 cm-1 in E286D but not in other mutants including D135N. This suggests that Glu286 in the D-channel is protonated in the air-oxidized state and undergoes hydrogen bonding changes upon reduction of the redox metal centers. Two pairs of band shifts at 2,566 (+)/2,574 (-) and 2,546 (+)/2,556 (-) cm-1 in all mutants indicate that two cysteine residues not in the vicinity of the metal centers undergo redox-linked hydrogen bonding changes. Cyanide had no effect on the protein structural changes because of the rigid local protein structure around the binuclear center or the presence of a ligand(s) at the binuclear center, and was released from the binuclear center upon reduction. This study establishes that cytochrome bo undergoes unique redox-linked protein structural changes. Localization and time-resolved analysis of the structural changes during dioxygen reduction will facilitate understanding of the molecular mechanism of redox-coupled proton pumping at the atomic level.

Existence of two L photointermediates of halorhodopsin from Halobacterium salinarium, differing in their protein and water FTIR bands.

FTIR difference spectra were recorded for the photoreactions of halorhodopsin from Halobacterium salinarium at 170 and 250 K. Obvious differences at the two temperatures were noted in neither the visible spectra nor the FTIR bands of the chromophore. However, perturbation of Asp141 is observed in the L intermediate at 250 K but not at 170 K. We named these photoproducts La (at 170 K) and Lb (at 250 K). The spectrum of Lb is distinct from that of La also in the different shifts of water O-H stretching bands, and larger changes in the bands from the protein backbone with different sensitivities to varying the halide. These results suggest that the photocycle of halorhodopsin contains two L states, La and Lb, in which the structure of protein and internal water molecules is different but chloride stays at the same site close to the Schiff base.

Structural change of threonine 89 upon photoisomerization in bacteriorhodopsin as revealed by polarized FTIR spectroscopy.

The all-trans to 13-cis photoisomerization of the retinal chromophore of bacteriorhodopsin occurs selectively, efficiently, and on an ultrafast time scale. The reaction is facilitated by the surrounding protein matrix which undergoes further structural changes during the proton-transporting reaction cycle. Low-temperature polarized Fourier transform infrared difference spectra between bacteriorhodopsin and the K intermediate provide the possibility to investigate such structural changes, by probing O-H and N-H stretching vibrations [Kandori, Kinoshita, Shichida, and Maeda (1998) J. Phys. Chem. B 102, 7899-7905]. The measurements of [3-18O]threonine-labeled bacteriorhodopsin revealed that one of the D2O-sensitive bands (2506 cm(-1) in bacteriorhodopsin and 2466 cm(-1) in the K intermediate, in D2O exhibited 18(O)-induced isotope shift. The O-H stretching vibrations of the threonine side chain correspond to 3378 cm(-1) in bacteriorhodopsin and to 3317 cm(-1) in the K intermediate, indicating that hydrogen bonding becomes stronger after the photoisomerization. The O-H stretch frequency of neat secondary alcohol is 3340-3355 cm(-1). The O-H stretch bands are preserved in the T46V, T90V, T142N, T178N, and T205V mutant proteins, but diminished in T89A and T89C, and slightly shifted in T89S. Thus, the observed O-H stretching vibration originates from Thr89. This is consistent with the atomic structure of this region, and the change of the S-H stretching vibration of the T89C mutant in the K intermediate [Kandori, Kinoshita, Shichida, Maeda, Needleman, and Lanyi (1998) J. Am. Chem. Soc. 120, 5828-5829]. We conclude that all-trans to 13-cis isomerization causes shortening of the hydrogen bond between the OH group of Thr89 and a carboxyl oxygen atom of Asp85.

Fourier-transform infrared studies on conformation changes in bd-type ubiquinol oxidase from Escherichia coli upon photoreduction of the redox metal centers.

Cytochrome bd is a two-subunit ubiquinol oxidase in the aerobic respiratory chain of Escherichia coli that does not belong to the heme-copper terminal oxidase superfamily. To explore unique protein structural changes associated with the reduction of the redox metal centers, we carried out Fourier-transform infrared and visible spectroscopic studies on cytochrome bd. For infrared measurements of a partially dehydrated thin sample solution, the air-oxidized enzyme was fully reduced by the intermolecular electron transfer of photo-excited riboflavin in the absence and presence of KCN, and redox difference spectra were calculated. Upon reduction, the bound cyanide was released from the heme b595-heme d binuclear center but remained in a protein pocket as a deprotonated form. Reduction of heme b558, heme b595, and heme d resulted in large changes in amide-I and protonated carboxylic CO-stretching vibrations and also a small change in the cysteine SH-stretching vibration. The location of the redox metal centers and the effects of cyanide suggest that these protein structural changes occur at the heme-binding pockets near the protein surface. Systematic site-directed mutagenesis and time-resolved FTIR studies on cytochrome bd will facilitate an understanding of the unique molecular mechanisms for dioxygen reduction and delivery of chemical protons to the active center at the atomic level.

The hydrogen-bonding network of water molecules and the peptide backbone in the region connecting Asp83, Gly120, and Glu113 in bovine rhodopsin.

Difference Fourier transform infrared spectra were recorded between mutants of rhodopsin and their batho products. The pigments studied were single and combined mutants of intramembrane residues of bovine rhodopsin: Asp83, Glu113, Gly120, Gly121, and Glu122. Previous studies [Nagata, T., Terakita, A., Kandori, H., Kojima, D., Shichida, Y., and Maeda, A. (1997) Biochemistry 36, 6164-6170] showed that one of the water molecules which undergoes structural changes in this process forms hydrogen bonds with Glu113 and the Schiff base, and that another water molecule is linked to this structure through the peptide backbone. The present results show that this water molecule is located at the place that is affected by the replacements of Asp83 and Gly120 but only slightly by Gly121 and not at all by Glu122. Asp83 and Gly120 are close to each other, in view of the observations that the carboxylic C=O stretching vibration of Asp83 is affected by the G120A replacement and that each replacement affects the common peptide carbonyl groups. Our results suggest that these residues in the middle of helices B and C are linked-through a hydrogen-bonding network composed of water and the peptide backbone-with the region around Glu113.

Interaction between photoactivated rhodopsin and the C-terminal peptide of transducin alpha-subunit studied by FTIR spectroscopy.

Structural changes in the complex formed between photolyzed bovine rhodopsin and a synthetic 11-mer peptide corresponding to the C-terminal region of the transducin alpha-subunit (Gtalpha) were analyzed by means of Fourier transform infrared spectroscopy. A complex with a protonated Schiff base appears at the beginning, accompanying the formation of an alpha-helix. This complex evolves into another which abolishes the original structure but retains the protonated Schiff base. This complex exhibits the same spectral shape as that of the final stable complex with an unprotonated Schiff base. The Fourier transform infrared spectrum for the formation of this final complex was compared to that with transducin [Nishimura, S., Sasaki, J., Kandori, H., Matsuda, T., Fukada, Y., and Maeda, A. (1996) Biochemistry 35, 13267-13271]. A large part of the frequency shifts of the peptide carbonyl vibrations which form upon complex formation with transducin but are absent with the synthetic 11-mer peptide must be structural changes in other sites, such as the nucleotide binding site in Gtalpha. The peptide, like transducin, shows the perturbation of a carboxylic acid in an extremely apolar environment. Some of the changes in the peptide backbone remain in the complex formed with the peptide. These are due to sites where rhodopsin interacts with the C-terminal region of Gtalpha. Specifically, the labeling of the peptide amide corresponding to Leu349 of transducin by 15N reveals weakening of the hydrogen bond of the peptide N-H of Leu349 and/or distortion of a peptide bond between Gly348 and Leu349 upon complex formation.