Biomedical subjects

R Needleman

Publications and source records attributed to R Needleman.

At least 73 records · Page 4Linked to original sources

PubMed1995

Photocycle of halorhodopsin from Halobacterium salinarium.

The light-driven chloride pump, halorhodopsin, is a mixture containing all-trans and 13-cis retinal chromophores under both light and dark-adapted conditions and can exist in chloride-free and chloride-binding forms. To describe the photochemical cycle of the all-trans, chloride-binding state that is associated with the transport, and thereby initiate study of the chloride translocation mechanism, one must first dissect the contributions of these species to the measured spectral changes. We resolved the multiple photochemical reactions by determining flash-induced difference spectra and photocycle kinetics in halorhodopsin-containing membranes prepared from Halobacterium salinarium, with light- and dark-adapted samples at various chloride concentrations. The high expression of cloned halorhodopsin made it possible to do these measurements with unfractionated cell envelope membranes in which the chromophore is photostable not only in the presence of NaCl but also in the Na2SO4 solution used for reference. Careful examination of the flash-induced changes at selected wavelengths allowed separating the spectral changes into components and assigning them to the individual photocycles. According to the results, a substantial revision of the photocycle model for H. salinarium halorhodopsin, and its dependence on chloride, is required. The cycle of the all-trans chloride-binding form is described by the scheme, HR-hv-->K<==>L1<==>L2<==>N-->HR, where HR, K, L, and N designate halorhodopsin and its photointermediates. Unlike the earlier models, this is very similar to the photoreaction of bacteriorhodopsin when deprotonation of the Schiff base is prevented (e.g., at low pH or in the D85N mutant). Also unlike in the earlier models, no step in this photocycle was noticeably affected when the chloride concentration was varied between 20 mM and 2 M in an attempt to identify a chloride-binding reaction.

Bacteriorhodopsins↗

PubMed1994

Energy coupling in an ion pump. The reprotonation switch of bacteriorhodopsin.

The active site of an ion pump must communicate alternately with the two opposite membrane surfaces. In the light-driven proton pump, bacteriorhodopsin, the retinal Schiff base is first the proton donor to D85 (with access to the extracellular side), and then it becomes the acceptor of the proton of D96 (with access to the cytoplasmic side). This "reprotonation switch" has been associated with a protein conformation change observed during the photocycle. When D85 is replaced with asparagine, the pKa value of the Schiff base is lowered from above 13 to about 9. We determined the direction of the loss or gain of the Schiff base proton in unphotolyzed and in photoexcited D85N, and the D85N/D96N and D85N/D96A double mutants, in order to understand the intrinsic and the induced connectivities of the Schiff base to the two membrane surfaces. The influence of D96 mutations on proton exchange and on acceleration of proton shuttling to the surface by azide indicated that in either case the access of the Schiff base on D85N mutants is to the cytoplasmic side. In the wild-type protein (but with the pKa of the Schiff base lowered by 13-trifluoromethyl retinal substitution) the results suggested that the Schiff base can communicate also with the extracellular side. Raising the pH without illumination of D85N so as to deprotonate the Schiff base caused the same, or nearly the same, change of X-ray scattering as observed when the Schiff base deprotonates during the wild-type photocycle. The results link the charge state of the active site to the global protein conformation and to the connectivity of the Schiff base proton to the membrane surfaces. Their relationship suggests that the conformation of the unphotolyzed wild-type protein is stabilized by coulombic interaction of the Schiff base with its counter-ion. A proton is translocated across the membrane after light-induced transfer of the Schiff base proton to D85, because the protein assumes an alternative conformation that separates the donor from the acceptor and opens new conduction pathways between the active site and the two membrane surfaces.

Acid-Base Equilibrium↗

PubMed1994

The retinal Schiff base-counterion complex of bacteriorhodopsin: changed geometry during the photocycle is a cause of proton transfer to aspartate 85.

Bacteriorhodopsin contains all-trans-retinal linked via a protonated Schiff base to K216. The proton transport in this pump is initiated by all-trans to 13-cis photoisomerization of the retinal and the ensuing transfer of the Schiff base proton to D85. Changed geometrical relationship of the Schiff base and D85 after the photoisomerization is a possible reason for the proton transfer. We introduced small volume/shape changes with site-specific mutagenesis of residues V49 and A53 that contact the side chain of K216, in order to force the Schiff base into somewhat different positions relative to D85. Earlier [Zimányi, L., Váró, G., Chang, M., Ni, B., Needleman, R., & Lanyi, J. K. (1992) Biochemistry 31, 8535-8543] we had described the kinetics of absorbance changes in the microsecond to millisecond time range after photoexcitation with the scheme L<-->M1<-->M2 + H+ (where the first equilibrium is the internal proton transfer and the second is proton release on the extracellular surface). Testing it at various pH values with mutants, where selected rate constants are changed, now confirms the validity of this scheme. The kinetics of the M state thus allowed examination of the transient equilibrium that develops in the L<-->M1 reaction and represents the redistribution of the proton between the Schiff base and D85. From the structure of the protein, the V49A and V49M residue replacements were both predicted to cause decreased alignment of the Schiff base and D85, and indeed we found that they both changed the equilibrium toward the protonated Schiff base. In contrast, the residue replacements A53V and A53G were predicted to move the Schiff base in opposite directions, away from and closer to alignment with D85, respectively. The former indeed changed the equilibrium toward the protonated Schiff base and the latter toward the deprotonated Schiff base. In addition, the hydroxyl stretch band of a bound water in the L state was affected by all mutations that disfavor proton transfer to D85. We conclude that the geometry of the proton donor and acceptor in the Schiff base-D85 pair, mediated by bound water, is a determinant of the proton transfer equilibrium.

Aspartic Acid↗

PubMed1994

The proton transfers in the cytoplasmic domain of bacteriorhodopsin are facilitated by a cluster of interacting residues.

The stepwise internal proton transfer reactions across the membrane, and the release and uptake at the surface, are the elementary steps that together constitute the transport mechanism in a proton pump. Although the proton donor and acceptor residues can be usually identified, the directionality and the energetics of the proton transfer must be determined to a large extent also by interactions of these with neighboring groups. We have examined the roles of residues D96, T46 and R227 in proton transfers during the photocycle of bacteriorhodopsin near its cytoplasmic surface, and in general the relationship between the reprotonation of the Schiff base and the subsequent proton uptake from the cytoplasmic side. The phenotypes of single and double mutants suggest close functional interaction among D96, T46, R227, and probably internal bound water. Measurements of the free energies of activation indicate that mechanistic interpretation of the rates changed by residue replacements is hindered by a general tendency toward lowered activation enthalpies in the mutated proteins. There is less ambiguity in the free energy levels of the photointermediates. It appears from these that the inhibitory and stimulatory influences of T46 and R227, respectively, on D96 as a proton donor compensate one another and ensure the effective reprotonation of the Schiff base. T46 and D96 mediate, in turn, proton uptake at the cytoplasmic surface. Although ultimately this will reprotonate D96, the observation of proton uptake from the bulk in R82Q without reprotonation of the aspartate residue suggests that the direct proton acceptor is not D96. The results thus indicate that the passage of the proton from the surface to the Schiff base is facilitated by multiple residue and water interactions in the cytoplasmic domain.

Amino Acids↗

PubMed1994

Complete identification of C = O stretching vibrational bands of protonated aspartic acid residues in the difference infrared spectra of M and N intermediates versus bacteriorhodopsin.

Fourier transform infrared difference spectra were obtained for the M and N intermediates versus light-adapted bacteriorhodopsin (BR) with site-directed mutant proteins in which aspartic acid residues at positions 96 and 115 were replaced by asparagine. The positive and negative bands at 1740 and 1732 cm-1 in the M/BR spectrum are shown to be the superposition of bands due to C = O stretching vibrations of Asp-96 and Asp-115 (a positive band at 1736 cm-1 and a negative band at 1742 cm-1 of Asp-96, and a positive band at 1742 cm-1 and a negative band at 1734 cm-1 of Asp-115). The positive band at 1738 cm-1 and the negative band at 1734 cm-1 in the N/BR spectrum are attributed to Asp-115. On the basis of these results, Asp-115 is protonated in M and N as well as in the ground state. On the other hand, no bands corresponding to Asp-212 were found in the region of protonated carboxylic acid vibration, indicating that Asp-212 remains unprotonated in M and N. The frequencies of the C = O stretching modes of protonated Asp-96 and Asp-115 change in the opposite direction in the BR-to-M conversion relative to the shifts in the BR-to-L conversion, indicating different environmental changes for these residues in L and M.

Asparagine↗

PubMed1994

A covalent link between the chromophore and the protein backbone of bacteriorhodopsin is not required for forming a photochemically active pigment analogous to the wild type.

Bacteriorhodopsin pigments lacking the retinal-Lys-216 covalent bond were prepared by reconstituting the K216G mutant protein with retinal alkylamine Schiff bases. The procedure follows the approach of Zhukovsky et al. [Zhukovsky, E., Robinson, P., & Oprian, D. (1991) Science 251, 558-560] in the case of visual (rhodopsin) pigments. Reconstitution leads to a mixture of three pigments. One of them, bR(K216G)/566a, absorbs (pH = 6.9) at 566 nm. Its absorption is pH-dependent, exhibiting a purple to blue transition. The pigment's laser-induced photocycle patterns are similar to those of wild-type all-trans-bR. A second component, bR(K216G)/566b, exhibits an independent photocycle reminiscent of that of wild-type 13-cis-bR. A third pigment component, bR(K216G)/630, absorbs around 630 nm. Experiments in the presence of a pH dye indicator show that illumination of bR(K216G)/566 produces a detectable proton gradient. It is concluded that a covalent bond between the retinal chromophore and the protein backbone is not a prerequisite for the basic structure and photochemical features of bR or for its proton pump activity.

Bacteriorhodopsins↗

PubMed1994

Interaction of aspartate-85 with a water molecule and the protonated Schiff base in the L intermediate of bacteriorhodopsin: a Fourier-transform infrared spectroscopic study.

Fourier-transform infrared spectra were recorded at 170 K before and after irradiating the Asp85-->Asn mutant of bacteriorhodopsin. The difference spectrum exhibits protein bands such as those due to the perturbations of Asp96 and Asp115 and the N-H stretching vibration of tryptophan, characteristic of the L minus all-trans-bacteriorhodopsin spectrum of the wild-type protein. However, some vibrational bands of the peptide backbone and the chromophore are different from L and more characteristic of N of the wild-type protein. Remarkably, the shift observed for the vibrational band due to an internal water molecule upon L formation [Maeda, Sasaki, Shichida, and Yoshizawa (1992) Biochemistry 31, 462-467] is absent. These changes in the spectrum of the mutant could originate from the destruction of a hydrogen-bonding system consisting of Asp85, the water molecule, and the Schiff base, upon replacement of Asp85 with asparagine. These observations constitute direct evidence for the interaction of water with Asp85 at the time when it is protonated by the Schiff base.

Aspartic Acid↗

PubMed1993

Trimeric mutant bacteriorhodopsin, D85N, shows a monophasic CD spectrum.

The structure of mutant bacteriorhodopsin (bR), D85N, was examined by CD and X-ray diffraction at pH 7. The absorption maximum of D85N at pH 7 is located at 605 nm, which is similar to the acid-blue form of wild-type bR. D85N shows a monophasic CD band, the maximum of which is at 575 nm, although the crystalline arrangement and the trimeric structure is maintained. The acid-blue form of wild-type bR shows a biphasic CD despite the similarity in absorption spectra.

Bacteriorhodopsins↗

PubMed1993

Relationship of proton uptake on the cytoplasmic surface and reisomerization of the retinal in the bacteriorhodopsin photocycle: an attempt to understand the complex kinetics of the pH changes and the N and O intermediates.

In the bacteriorhodopsin photocycle the recovery of the initial BR state from the M intermediate occurs via the N and O intermediates. The molecular events in this process include reprotonation of the Schiff base and the subsequent uptake of a proton from the cytoplasmic side, as well as reisomerization of the retinal from 13-cis to all-trans. We have studied the kinetics of the intermediates and the proton uptake. At moderately low pH little of the N state accumulates, and the O state dominates in the reactions that lead from M to BR. The proton uptake lags behind the formation of O, suggesting the sequence N(0)<==>O(0) + H+ (from the bulk)-->O(+1)-->BR+H+ (to the bulk), where the superscripts indicate the net protonation state of the protein relative to BR. Together with a parallel study of ours at moderately high pH, these results suggest that the sequence of proton uptake and retinal reisomerization depends on pH: at low pH the isomerization occurs first and O accumulates, but at high pH the isomerization is delayed and therefore N accumulates. Although this model contains too many rate constants for rigorous testing, we find that it will generate most of the characteristic pH-dependent kinetic features of the photocycle with few assumptions other than pH dependency for protonation at the proton release and uptake steps.

Amino Acid Sequence↗

PubMed1993

Pathway of proton uptake in the bacteriorhodopsin photocycle.

The time courses of chromophore reactions and proton uptake in the second half of the photocycle of the proton pump bacteriorhodopsin (BR) were examined. At pH > 8.5, the kinetics are simplified by the fact that only the M and N intermediates accumulate. The relaxation kinetics after perturbation of M with a second, blue flash confirm that M<==>N equilibration is the only significant cause of the biphasic M decay. With this feature, the analysis of time-resolved difference spectra yields a scheme which contains two sequential N states connected by a nearly unidirectional reaction. The proton uptake from the bulk, as measured with the pH-indicator dye pyranine, occurs during the decay of the first N rather than the recovery of BR. The results thus suggest the model M2(-1)<==>N(-1) + H+ (from the bulk)<==>N(0)-->BR, where the superscripts indicate the protonation state of the protein relative to BR. M2(-1)-->N(-1) is reprotonation of the Schiff base from D96, N(-1) + H+ (from the bulk)-->N(0) is uptake of proton from the cytoplasmic side, and N(0)-->BR represents 13-cis to all-trans reisomerization of the retinal and other relaxations which regenerate the initial state. R227, a residue near D96, affects the deprotonation of D96 more than the subsequent proton uptake. According to the changed [M2(-1)]/[N(-1)] equilibrium in the R227Q protein, interaction between R227 and D96 is responsible for about 1 pH unit of the decrease in the pKa of D96 during the reprotonation of the Schiff base. According to the pH dependencies of the rate constants in the N(-1)<==>N(0) equilibrium in wild-type and R227Q, interaction with R227 lowers the pKa for proton uptake from the bulk by 0.5 pH unit, to 11. We conclude from the proton uptake kinetics that at physiological pH free energy is converted to proton electrochemical potential in this pump not only as protons are released on the extracellular side [Zimányi, L., Váró. G., Chang, M., Ni, B., Needleman, R., & Lanyi, J. K. (1992) Biochemistry 31, 8535-8543] but also as protons are taken up on the cytoplasmic side.

Bacteriorhodopsins↗

PubMed1993

Photoreaction of the N intermediate of bacteriorhodopsin, and its relationship to the decay kinetics of the M intermediate.

Because the M photointermediate of recombinant T46V bacteriorhodopsin decays more rapidly and the N intermediate more slowly than in wild-type, the photoreaction of N could be examined without interference from M. We found that between pH 6 and 9 the photoproducts of N included both earlier suggested M-like intermediate and red-shifted R state. However, when the photoexcitation of N was at wavelengths below 500 nm the amount of M-like product decreased with increasing pH, and at pH 9 virtually only R was produced. In the dark, T46V contains an N-like conformer, in increasing amounts with increasing pH like wild-type but in 4-5 times greater concentrations. The photoreaction of this thermally produced state is much like that of the N intermediate. It is associated with the appearance of a slowly decaying M, but we calculate that under most conditions used to follow M in the wild-type photocycle the amount of N-like conformer, and therefore the amplitude of this slow component, will not be significant. The results confirm the suggestion [Fukuda & Kouyama (1992) Biochemistry 31, 11740-11747] that an M-like state is included among the photoproducts of N, but at the same time provide support to photocycle models in which the slow component of the biphasic M decay is attributed not to this secondary photoreaction or to a separate photocycle originating from a heterogeneous initial state, but to thermal equilibration between M and N in a single photocycle.

Bacteriorhodopsins↗

PubMed1993

Proton transfer from Asp-96 to the bacteriorhodopsin Schiff base is caused by a decrease of the pKa of Asp-96 which follows a protein backbone conformational change.

In the bacteriorhodopsin photocycle the transported proton crosses the major part of the hydrophobic barrier during the M to N reaction; in this step the Schiff base near the middle of the protein is reprotonated from D96 located near the cytoplasmic surface. In the recombinant D212N protein at pH > 6, the Schiff base remains protonated throughout the photocycle [Needleman, Chang, Ni, Váró, Fornés, White, & Lanyi (1991) J. Biol. Chem. 266, 11478-11484]. Time-resolved difference spectra in the visible and infrared are described by the kinetic scheme BR-->K<==>L<==>N (-->N')-->BR. As evidenced by the large negative 1742-cm-1 band of the COOH group of the carboxylic acid, deprotonation of D96 in the N state takes place in spite of the absence of the unprotonated Schiff base acceptor group of the M intermediate. Instead of internal proton transfer to the Schiff base, the proton is released to the bulk, and can be detected with the indicator dye pyranine during the accumulation of N'. The D212N/D96N protein has a similar photocycle, but no proton is released. As in wild-type, deprotonation of D96 in the N state is accompanied by a protein backbone conformational change indicated by characteristic amide I and II bands. In D212N the residue D96 can thus deprotonate independent of the Schiff base, but perhaps dependent on the detected protein conformational change. This could occur through increased charge interaction between D96 and R227 and/or increased hydration near D96. We suggest that the proton transfer from D96 to the Schiff base in the wild-type photocycle is driven also by such a decrease in the pKa of D96.

Amino Acid Sequence↗

PubMed1993

Effects of genetic replacements of charged and H-bonding residues in the retinal pocket on Ca2+ binding to deionized bacteriorhodopsin.

Metal cations are known to be required for proton pumping by bacteriorhodopsin (bR). Previous studies found that bR has two high-affinity and four to six low-affinity Ca(2+)-binding sites. In our efforts to find the location of these Ca2+ sites, the effects of replacing charged (Asp-85, Asp-212, and Arg-82) and H-bonding (Tyr-185) residues in the retinal pocket on the color control and binding affinity of Ca2+ ions in Ca(2+)-regenerated bR were examined. The important results are as follows: (i) The removal of Ca2+ from recombinant bR in which charged residues were replaced by neutral ones shifted the retinal absorption to the blue, opposite to that observed in wild-type bR or in recombinant bR in which the H-bonding residue, Tyr-185, was replaced by a non-H-bonding amino acid (Phe). (ii) Similar to the observation in wild-type bR, the binding of Ca2+ to the second site gave the observed color change in the recombinant bR samples in which charged residues were replaced by neutral ones. (iii) The residue replacements had no effect on the affinity constants of the four to six weakly bound Ca2+. (iv) The two high-affinity sites exhibited reduced affinity with substitutions; while the extent of the reduction depended on the specific substitution, each site was reduced by the same factor for each of the charged residue substitutions but by different factors for the mutant where Tyr-185 was replaced with Phe(Y185F). The above results suggest that the two Ca2+ ions in the two high-affinity sites are within interaction distance with one another and with the charged residues in the retinal pocket. The results further suggest that, while the interaction between Tyr-185 and the high-affinity Ca2+ ions is relatively short range and specific (with more coupling to the Ca2+ ion in the second affinity site), between the charged residues and Ca2+ ions it seems to be of the electrostatic (e.g., ion-ion) long range, nonspecific type. Although neither Asp-85, Asp-212, nor Arg-82 is individually directly involved in the binding of Ca2+ in these two sites, they might all participate in it. Together with the protonated Schiff base, the charged residues along with Tyr-185 and one or two Ca2+ ions (and probably a few water molecules) seem to form an electrostatically coupled system that is part of a cavity that controls the color and function of bR.

Amino Acid Sequence↗

PubMed1993

Estimated acid dissociation constants of the Schiff base, Asp-85, and Arg-82 during the bacteriorhodopsin photocycle.

The pK(a) values of D85 in the wild-type and R82Q, as well as R82A recombinant bacteriorhodopsins, and the Schiff base in the D85N, D85T, and D85N/R82Q proteins, have been determined by spectroscopic titrations in the dark. They are used to estimate the coulombic interaction energies and the pK(a) values of the Schiff base, D85, and R82 during proton transfer from the Schiff base to D85, and the subsequent proton release to the bulk in the initial part of the photocycle. The pK(a) of the Schiff base before photoexcitation is calculated to be in effect only 5.3-5.7 pH units higher than that of D85; overcoming this to allow proton transfer to D85 requires about two thirds of the estimated excess free energy retained after absorption of a photon. The proton release on the extracellular surface is from an unidentified residue whose pK(a) is lowered to about 6 after deprotonation of the Schiff base (Zimanyi, L., G. Varo, M. Chang, B. Ni, R. Needleman, and J.K. Lanyi, 1992. Biochemistry. 31:8535-8543). We calculate that the pK(a) of the R82 is 13.8 before photoexcitation, and it is lowered after proton exchange between the Schiff base and D85 only by 1.5-2.3 pH units. Therefore, coulombic interactions alone do not appear to change the pK(a) of R82 as much and D85 only by 1.5-2.3 pH units. Therefore, coulombic interactions alone do not appear to change the pK(a) of R82 as much as required if it were the proton release group.

Arginine↗

PubMed1992

Pathways of proton release in the bacteriorhodopsin photocycle.

The pH dependencies of the rate constants in the photocycles of recombinant D96N and D115N/D96N bacteriorhodopsins were determined from time-resolved difference spectra between 70 ns and 420 ms after photoexcitation. The results were consistent with the model suggested earlier for proteins containing D96N substitution: BR hv----K----L----M1----M2----BR. Only the M2----M1 back-reaction was pH-dependent: its rate increased with increasing [H+] between pH 5 and 8. We conclude from quantitative analysis of this pH dependency that its reverse, the M1----M2 reaction, is linked to the release of a proton from a group with a pKa = 5.8. This suggests a model for wild-type bacteriorhodopsin in which at pH greater than 5.8 the transported proton is released on the extracellular side from this as yet unknown group and on the 100-microseconds time scale, but at pH less than 5.8, the proton release occurs from another residue and later in the photocycle most likely directly from D85 during the O----BR reaction. We postulate, on the other hand, that proton uptake on the cytoplasmic side will be by D96 and during the N----O reaction regardless of pH. The proton kinetics as measured with indicator dyes confirmed the unique prediction of this model: at pH greater than 6, proton release preceded proton uptake, but at pH less than 6, the release was delayed until after the uptake. The results indicated further that the overall M1----M2 reaction includes a second kinetic step in addition to proton release; this is probably the earlier postulated extracellular-to-cytoplasmic reorientation switch in the proton pump.

Bacteriorhodopsins↗

PubMed1992

Structures of aspartic acid-96 in the L and N intermediates of bacteriorhodopsin: analysis by Fourier transform infrared spectroscopy.

The light-induced difference Fourier transform infrared spectrum between the L or N intermediate minus light-adapted bacteriorhodopsin (BR) was measured in order to examine the protonated states and the changes in the interactions of carboxylic acids of Asp-96 and Asp-115 in these intermediates. Vibrational bands due to the protonated and unprotonated carboxylic acid were identified by isotope shift and band depletion upon substitution of Asp-96 or -115 by asparagine. While the signal due to the deprotonation of Asp-96 was clearly observed in the N intermediate, this residue remained protonated in L. Asp-115 was partially deprotonated in L. The C = O stretching vibration of protonated Asp-96 of L showed almost no shift upon 2H2O substitution, in contrast to the corresponding band of Asp-96 or Asp-115 of BR, which shifted by 9-12 cm-1 under the same conditions. In the model system of acetic acid in organic solvents, such an absence of the shift of the C = O stretching vibration of the protonated carboxylic acid upon 2H2O substitution was seen only when the O-H of acetic acid is hydrogen-bonded. The non-hydrogen-bonded monomer showed the 2H2O-dependent shift. Thus, the O-H bond of Asp-96 enters into hydrogen bonding upon conversion of BR to L. Its increased hydrogen bonding in L is consistent with the observed downshift of the O-H stretching vibration of the carboxylic acid of Asp-96.

Acetates↗

PubMed1992

A residue substitution near the beta-ionone ring of the retinal affects the M substates of bacteriorhodopsin.

The switch in the bacteriorhodopsin photocycle, which reorients access of the retinal Schiff base from the extracellular to the cytoplasmic side, was suggested to be an M1----M2 reaction (Váró and Lanyi. 1991. Biochemistry. 30:5008-5015, 5016-5022). Thus, in this light-driven proton pump it is the interconversion of proposed M substates that gives direction to the transport. We find that in monomeric, although not purple membrane-lattice immobilized, D115N bacteriorhodopsin, the absorption maximum of M changes during the photocycle: in the time domain between its rise and decay it shifts 15 nm to the blue relative to the spectrum at earlier times. This large shift strongly supports the existence of two M substates. Since D115 is located near the beta-ionone ring of the retinal, the result raises questions about the possible involvement of the retinal chain or protein residues as far away as 10 A from the Schiff base in the mechanism of the switching reaction.

Bacteriorhodopsins↗

PubMed1992

The back photoreaction of the M intermediate in the photocycle of bacteriorhodopsin: mechanism and evidence for two M species.

The back photoreaction of the M intermediate in the photocycle of bacteriorhodopsin is investigated both for the native pigment and its D96N mutant. The experimental setup is based on creating the M intermediate by a first pulse, followed by a (blue) laser pulse which drives the back photoreaction of M. Experiments are carried out varying the delay between the two pulses, as well as the temperature over the -25 degrees C-20 degrees C range. It is found that the kinetic patterns of the M back photoreaction change with time after the generation of this intermediate. The data provide independent evidence for the suggestion of a photocycle mechanism based on two distinct M intermediates. They are thus in keeping with the consecutive model of Varo and Lanyi (Biochemistry 30, 5016-5022; 1991), although they cannot exclude other models such as those based on branched or parallel cycles. More generally, we offer a "photochemical" approach to discriminating between intermediate stages in the photocycle which does not depend on spectroscopic and/or kinetic data. While markedly affecting the rate of the M --> N transition in the photocycle, the rate of the thermal step in back photoreaction of M, at both room and low temperatures, is not significantly affected by the D96N mutation. It is proposed that while Asp 96 is the Schiff-base protonating moiety in the M --> N transition, another residue (most probably Asp 85) reprotonates the Schiff base following light absorption by M.

Bacteriorhodopsins↗