Light-induced changes in the structure and accessibility of the cytoplasmic loops of rhodopsin in the activated MII state.

Bovine rhodopsin was specifically labeled on the cytoplasmic surface at cysteine 140 (the first residue of the loop connecting helices III and IV) or at cysteine 316 (in the loop connecting helix VII and the palmitoylation sites) with the fluorescent labels fluorescein and Texas Red. These loops are involved in activation and signal transduction. The time-resolved fluorescence depolarization was measured in the dark state and in the M(II) state, with labeled samples consisting of rhodopsin-octylglucoside micelles or rod outer segment (ROS) membranes. In this way the diffusional dynamics of the flexible loops of rhodopsin were measured for the first time directly on the nanosecond time scale. Control experiments showed that the large number of weak excitation pulses required in these single photon counting experiments leads to <5% bleaching of the sample. Rhodopsin was trapped in the activated M(II) state for the duration of the fluorescence experiments ( approximately 20 min) after illumination at pH 6 and 5 degrees C. For both types of samples and at both labeled positions the dynamics of the label and loop motion as monitored by the time constants of the depolarization were not significantly different in the two states of the receptor. The end-anisotropy increased, however, from 0.09 in the dark to 0.16 in the M(II) state for ROS samples labeled at C140. The corresponding numbers for the C316 position are 0.06 and 0.12. Light-induced activation in M(II) is thus associated with a large increase in the loop steric hindrance due to a changed loop domain structure on the cytoplasmic surface. These results are supported by fluorescence quenching experiments with I(-), which indicate a significant decrease in the collisional quenching constant k(q) and in accessibility in the M(II) state at both positions. The rotational correlation time of the rhodopsin micelles increased from 48 ns in the dark state to 60 ns in M(II). This increase is caused by a change in volume and/or shape and is consistent with a structural change. These results demonstrate that time-resolved fluorescence depolarization is a powerful tool to study the changes in conformation and dynamics of the cytoplasmic loops that accompany the activation of rhodopsin and other G-protein coupled receptors.

Light-induced proton release and proton uptake reactions in the cyanobacterial phytochrome Cph1.

The P(r) to P(fr) transition of recombinant Synechocystis PCC 6803 phytochrome Cph1 and its N-terminal sensor domain Cph1Delta2 is accompanied by net acidification in unbuffered solution. The extent of this net photoreversible proton release was measured with a conventional pH electrode and increased from less than 0.1 proton released per P(fr) formed at pH 9 to between 0.6 (Cph1) and 1.1 (Cph1Delta2) H(+)/P(fr) at pH 6. The kinetics of the proton release were monitored at pH 7 and pH 8 using flash-induced transient absorption measurements with the pH indicator dye fluorescein. Proton release occurs with time constants of approximately 4 and approximately 20 ms that were also observed in parallel measurements of the photocycle (tau(3) and tau(4)). The number of transiently released protons per P(fr) formed is about one. This H(+) release phase is followed by a proton uptake phase of a smaller amplitude that has a time constant of approximately 270 ms (tau(5)) and is synchronous with the formation of P(fr). The acidification observed in the P(r) to P(fr) transition with pH electrodes is the net effect of these two sequential protonation changes. Flash-induced transient absorption measurements were carried out with Cph1 and Cph1Delta2 at pH 7 and pH 8. Global analysis indicated the presence of five kinetic components (tau(1)-tau(5): 5 and 300 micros and 3, 30, and 300 ms). Whereas the time constants were approximately pH independent, the corresponding amplitude spectra (B(1), B(3), and B(5)) showed significant pH dependence. Measurements of the P(r)/P(fr) photoequilibrium indicated that it is pH independent in the range of 6.5-9.0. Analysis of the pH dependence of the absorption spectra from 6.5 to 9.0 suggested that the phycocyanobilin chromophore deprotonates at alkaline pH in both P(r) and P(fr) with an approximate pK(a) of 9.5. The protonation state of the chromophore at neutral pH is therefore the same in both P(r) and P(fr). The light-induced deprotonation and reprotonation of Cph1 at neutral pH are thus due to pK(a) changes in the protein moiety, which are linked to conformational transitions occurring around 4 and 270 ms after photoexcitation. These transient structural changes may be relevant for signal transduction by this cyanobacterial phytochrome.

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.

Evidence for long range allosteric interactions between the extracellular and cytoplasmic parts of bacteriorhodopsin from the mutant R82A and its second site revertant R82A/G231C.

Evidence is presented for long range interactions between the extracellular and cytoplasmic parts of the heptahelical membrane protein bacteriorhodopsin in the mutant R82A and its second site revertant R82A/G231C. (i) In the double mutants R82A/G72C and R82A/A160C, with the cysteine mutation on the extracellular or cytoplasmic surface, respectively, the photocycle is the same as in the single mutant R82A with an accelerated deprotonation of the Schiff base and a reversed order of proton release and uptake. Proton release and uptake kinetics were measured directly at either surface by using the unique cysteine residue as attachment site for the pH indicator fluorescein. Whereas in wild type proton uptake on the cytoplasmic surface occurs during the M-decay (tau approximately 8 ms), in R82A it occurs already during the first phase of the M-rise (tau < 1 microseconds). (ii) The introduction of a second mutation at the cytoplasmic surface in position 231 (helix G) restores wild type ground state absorption properties, kinetics of photocycle and of proton release, and uptake in the mutant R82A/G231C. In addition, kinetic H/D isotope effects provide evidence that the proton release mechanism in R82A/G231C and in wild type is similar. These results suggest the existence of long range interactions between the cytoplasmic and extracellular surface domains of bacteriorhodopsin mediated by salt bridges and hydrogen-bonded networks between helices C (Arg-82) and G (Asp-212 and Gly-231). Such long range interactions are expected to be of functional significance for activation and signal transduction in heptahelical G-protein-coupled receptors.

The angles between the C(1)-, C(5)-, and C(9)-methyl bonds of the retinylidene chromophore and the membrane normal increase in the M intermediate of bacteriorhodopsin: direct determination with solid-state (2)H NMR.

The orientations of three methyl bonds of the retinylidene chromophore of bacteriorhodopsin were investigated in the M photointermediate using deuterium solid-state NMR ((2)H NMR). In this key intermediate, the chromophore has a 13-cis, 15-anti conformation and a deprotonated Schiff base. Purple membranes containing wild-type or mutant D96A bacteriorhodopsin were regenerated with retinals specifically deuterated in the methyl groups of either carbon C(1) or C(5) of the beta-ionone ring or carbon C(9) of the polyene chain. Oriented hydrated films were formed by drying concentrated suspensions on glass plates at 86% relative humidity. The lifetime of the M state was increased in the wild-type samples by applying a guanidine hydrochloride solution at pH 9.5 and in the D96A sample by raising the pH. (2)H NMR experiments were performed on the dark-adapted ground state (a 2:1 mixture of 13-cis, 15-syn and all-trans, 15-anti chromophores), the cryotrapped light-adapted state (all-trans, 15-anti), and the cryotrapped M intermediate (13-cis, 15-anti) at -50 degrees C. Bacteriorhodopsin was first completely converted to M under steady illumination of the hydrated films at +5 degrees C and then rapidly cooled to -50 degrees C in the dark. From a tilt series of the oriented sample in the magnetic field and an analysis of the (2)H NMR line shapes, the angles between the individual C-CD(3) bonds and the membrane normal could be determined even in the presence of a substantial degree of orientational disorder. While only minor differences were detected between dark- and light-adapted states, all three angles increase in the M state. This is consistent with an upward movement of the C(5)-C(13) part of the polyene chain toward the cytoplasmic surface or with increased torsional strain. The C(9)-CD(3) bond shows the largest orientational change of 7 degrees in M. This reorientation of the chromophore in the binding pocket provides direct structural support for previous suggestions (based on spectroscopic evidence) for a steric interaction in M between the C(9)-methyl group and Trp 182 in helix F.

Kinetics of the light-induced proton translocation associated with the pH-dependent formation of the metarhodopsin I/II equilibrium of bovine rhodopsin.

The kinetics of the formation of the metaII (MII) state of bovine rhodopsin was investigated by time-resolved electrical and absorption measurements with rod outer segment (ROS) fragments. Photoexcitation leads to proton transfer in the direction from the cytosolic to the intradiscal side of the membrane, probably from the Schiff base to the acceptor glutamate 113. Two components of comparable amplitude are required to describe the charge movement with exponential times of 1.1 (45%) and 3.0 ms (55%) (pH 7.8, 22 degreesC, 150 mM KCl). The corresponding activation energies are 86 and 123 kJ/mol, respectively (150 mM KCl). The time constants and amplitudes depend strongly on pH. Between pH 7.1 and 3.8 the kinetics becomes much faster, with the faster and slower components accelerating by factors of about 8 and 2, respectively. Complementary single-flash absorption experiments at 380 nm and 10 degreesC show that the formation of MII also occurs with two components with similar time constants and pH dependence. This suggests that both signals monitor the same molecular events. The pH dependence of the two apparent time constants and amplitudes of the optical data can be described well over the pH range 4-7.5 by two coupled equilibria between MI and two isochromic MII species MIIa and MIIb: MI MIIa(380) MIIb(380), with k0 proportional to the proton concentration. This model implies that deprotonation of the Schiff base and proton uptake are tightly coupled in ROS membranes. Models with k2 proportional to the proton concentration cannot describe the data. Photoreversal of MII by blue flashes (420 nm) leads to proton transfer in a direction opposite to that of the signal associated with MII formation. In this transition the Schiff base is reprotonated, most likely from glutamate 113. At pH 7.3, 150 mM KCl, 22 degreesC, this electrical charge reversal has an exponential time constant of about 30 ms and is about 10 times slower than the forward charge motion.

Chromophore orientation in bacteriorhodopsin determined from the angular dependence of deuterium nuclear magnetic resonance spectra of oriented purple membranes.

The orientation of prosthetic groups in membrane proteins is of considerable importance in understanding their functional role in energy conversion, signal transduction, and ion transport. In this work, the orientation of the retinylidene chromophore of bacteriorhodopsin (bR) was investigated using 2H NMR spectroscopy. Bacteriorhodopsin was regenerated with all-trans-retinal stereospecifically deuterated in one of the geminal methyl groups on C1 of the cyclohexene ring. A highly oriented sample, which is needed to obtain individual bond orientations from 2H NMR, was prepared by forming hydrated lamellar films of purple membranes on glass slides. A Monte Carlo method was developed to accurately simulate the 2H NMR line shape due to the distribution of bond angles and the orientational disorder of the membranes. The number of free parameters in the line shape simulation was reduced by independent measurements of the intrinsic line width (1.6 kHz from T2e experiments) and the effective quadrupolar coupling constant (38. 8-39.8 kHz from analysis of the line shape of a powder-type sample). The angle between the C1-(1R)-1-CD3 bond and the purple membrane normal was determined with high accuracy from the simultaneous analysis of a series of 2H NMR spectra recorded at different inclinations of the uniaxially oriented sample in the magnetic field at 20 and -50 degrees C. The value of 68.7 +/- 2.0 degrees in dark-adapted bR was used, together with the previously determined angle of the C5-CD3 bond, to calculate the possible orientations of the cyclohexene ring in the membrane. The solutions obtained from 2H NMR were then combined with additional constraints from linear dichroism and electron cryomicroscopy to obtain the allowed orientations of retinal in the noncentrosymmetric membrane structure. The combined data indicate that the methyl groups on the polyene chain point toward the cytoplasmic side of the membrane and the N-H bond of the Schiff base to the extracellular side, i.e., toward the side of proton release in the pump pathway.

Structure of the interhelical loops and carboxyl terminus of bacteriorhodopsin by X-ray diffraction using site-directed heavy-atom labeling.

The positions of single amino acids in the interhelical loop regions and the C-terminal tail of bacteriorhodopsin (bR) were investigated by X-ray diffraction using site-directed heavy-atom labeling. Since wild-type bR does not contain any cysteines, appropriate cysteine mutants were produced with a unique sulfhydryl group at specific positions. These sites were then labeled with mercury using the sulfhydryl specific reagent p-chloromercuribenzoate (p-CMB). The cysteine mutants D96A/V101C, V130C, A160C, and G231C were derivatized with labeling stoichiometries of 0.93 +/- 5%, 0.85 +/- 5%, 0.79 +/- 7%, and 0.77 +/- 8%, respectively (Hg per bR). No incorporation was observed with wild-type bR under the same conditions. All mutants and heavy-atom derivatives were fully active as judged by the kinetics of the photocycle and of the proton release and uptake. Moreover, the unit cell dimensions of the two-dimensional P3 lattice were unchanged by the mutations and the derivatization. This allowed the position of the mercury atoms, projected onto the plane of the membrane, to be calculated from the intensity differences in the X-ray diffraction pattern between labeled and unlabeled samples using Fourier difference methods. The X-ray diffraction data were collected at room temperature from oriented purple membrane films at 100% relative humidity without the use of dehydrating solvents. These native conditions of temperature, humidity, and solvent are expected to preserve the structure of the surface-exposed loops. Sharp maxima corresponding to a single mercury atom were found in the difference density maps for D96A/V101C and V130C. Residues 101 and 130 are in the short loops connecting helices C/D and D/E, respectively. No localized difference density was found for A160C and G231C. Residue 160 is in the longer loop connecting helices E and F, whereas residue 231 is in the C-terminal tail. Residues 160 and 231 are apparently in a more disordered and mobile part of the structure.

Sulfur distribution in bacteriorhodopsin from multiple wavelength anomalous diffraction near the sulfur K-edge with synchrotron x-ray radiation.

Bacteriorhodopsin contains nine sulfur atoms from the nine methionine residues. The distribution of these sulfur atoms in the projected density map was determined from x-ray diffraction experiments using multiple wavelength anomalous diffraction (MAD) at the sulfur K-edge (5.02 A) with synchrotron radiation. The experiments were performed with uniaxial samples of oriented purple membranes at room temperature and 86% relative humidity. For such samples only the real part f' (lambda) of the resonant scattering amplitude of sulfur contributes to the observed scattering intensity. The sulfur density was determined from the difference in diffraction intensities detected at two wavelengths near the sulfur K-edge that were approximately 0.004 A apart. The measured change in f' between these two wavelengths corresponds to 6 electron units. This shows that large anomalous dispersion effects occur near the sulfur K-edge. The in-plane positions of the sulfur atoms of Met32, Met56, and Met209 were determined unambiguously. The difference density from Met20, Met60, Met118, and Met145 is concentrated in the interior of the seven alpha-helical bundle, overlaps strongly in the projected density map, and cannot be resolved at the resolution of these experiments (8.2 A). This method of localizing individual sulfur atoms can be applied to other two-dimensional protein crystals and is promising in conjunction with the site-directed introduction of sulfur atoms by the use of cysteine mutants.

Evidence for the first phase of the reprotonation switch of bacteriorhodopsin from time-resolved photovoltage and flash photolysis experiments on the photoreversal of the M-intermediate.

The kinetics of the photoreversal reaction of the M-intermediate of bacteriorhodopsin (bR) was investigated by time-resolved optical absorption spectroscopy and photovoltage measurements using double-flash excitation (a green flash (532 nm) followed by a blue flash (400 nm) after a variable delay). The sign of the photovoltage and the 1H/2H kinetic isotope effect indicate that the Schiff base is reprotonated by a group between the Schiff base and the extracellular surface, probably Asp85. Analysis of the kinetic data shows that the charge movement in 150 mM KCl at 12 degrees C is characterized by two components with time constants of approximately 100 ns and approximately 600 ns, respectively, which are independent of the delay time between the flashes and the pH. The amplitudes of the fast and slow components depend on the delay and the pH. The slower component starts to contribute to the charge movement only after delays longer than 100 micros, is absent at low pH, and increases in amplitude with a pKa of approximately 6. Because the proton release group deprotonates after 70-100 micros and has a transient pKa of 5.8, these results suggest the following assignment: the fast and the combination of fast and slow components represent photoreversal from two M states, with the release group protonated and deprotonated, respectively. The slow phase of the photoreversal starts from a state with the release group deprotonated, and with the pK of Asp85 elevated, and is probably due to the restoration of the pK of Asp85 to its initial low value. This provides further evidence for coupling between the pK's of Asp85 and the release group and suggests that proton release is the first step in the reprotonation switch. At alkaline pH the amplitude of the electrical signal from the back photoreaction decreases with an apparent pK of 8, without a corresponding decrease in the amount of M. At neutral pH the movement of the positively charged guanidinium group of Arg82 from a position near the release group on the surface to Asp85 makes a substantial contribution to the electrical photoreversal amplitude. Above the pK of the release group in the unphotolysed state (approximately 8), Arg82 stays near the surface, leading to a corresponding signal reduction.

Proton transport by a bacteriorhodopsin mutant, aspartic acid-85-->asparagine, initiated in the unprotonated Schiff base state.

At alkaline pH the bacteriorhodopsin mutant D85N, with aspartic acid-85 replaced by asparagine, is in a yellow form (lambda max approximately 405 nm) with a deprotonated Schiff base. This state resembles the M intermediate of the wild-type photocycle. We used time-resolved methods to show that this yellow form of D85N, which has an initially unprotonated Schiff base and which lacks the proton acceptor Asp-85, transports protons in the same direction as wild type when excited by 400-nm flashes. Photoexcitation leads in several milliseconds to the formation of blue (630 nm) and purple (580 nm) intermediates with a protonated Schiff base, which decay in tens of seconds to the initial state (400 nm). Experiments with pH indicator dyes show that at pH 7, 8, and 9, proton uptake occurs in about 5-10 ms and precedes the slow release (seconds). Photovoltage measurements reveal that the direction of proton movement is from the cytoplasmic to the extracellular side with major components on the millisecond and second time scales. The slowest electrical component could be observed in the presence of azide, which accelerates the return of the blue intermediate to the initial yellow state. Transport thus occurs in two steps. In the first step (milliseconds), the Schiff base is protonated by proton uptake from the cytoplasmic side, thereby forming the blue state. From the pH dependence of the amplitudes of the electrical and photocycle signals, we conclude that this reaction proceeds in a similar way as in wild type--i.e., via the internal proton donor Asp-96. In the second step (seconds) the Schiff base deprotonates, releasing the proton to the extracellular side.

Intramolecular charge transfer in the bacteriorhodopsin mutants Asp85-->Asn and Asp212-->Asn: effects of pH and anions.

The photovoltage kinetics of the bacteriorhodopsin mutants Asp212-->Asn and Asp85-->Asn after excitation at 580 nm have been investigated in the pH range from 0 to 11. With the mutant Asp85-->Asn (D85N) at pH 7 no net charge translocation is observed and the signal is the same, both in the presence of Cl- (150 mM) and in its absence (75 mM SO4(2-)). Under both conditions the color of the pigment is blue (lambda max = 615 nm). The time course of the photovoltage kinetics is similar to that of the acid-blue form of wild-type, except that an additional transient charge motion occurs with time constants of 60 microseconds and 1.3 ms, indicating the transient deprotonation and reprotonation of an unknown group to and from the extracellular side of the membrane. It is suggested that this is the group XH, which is responsible for proton release in wild-type. At pH 1, the photovoltage signal of D85N changes upon the addition of Cl- from that characteristic for the acid-blue state of wild-type to that characteristic for the acid-purple state. Therefore, the protonation of the group at position at 85 is necessary, but not sufficient for the chloride-binding. At pH 11, well above the pKa of the Schiff base, there is a mixture of "M-like" and "N-like" states. Net proton transport in the same direction as in wild-type is restored in D85N from this N-like state. With the mutant Asp212-->Asn (D212N), time-resolved photovoltage measurements show that in the absence of halide ions the signal is similar to that of the acid-blue form of wild-type and that no net charge translocation occurs in the entire pH range from 0 to 11. Upon addition of Cl- in the pH range from 3.8 to 7.2 the color of the pigment returns to purple and the photovoltage experiments indicate that net proton pumping is restored. However, this Cl(-)-induced activation of net charge-transport in D212N is only partial. Outside this pH range, no net charge transport is observed even in the presence of chloride, and the photovoltage shows the same chloride-dependent features as those accompanying the acid-blue to acid-purple transition of the wild-type.

Photovoltage kinetics of the acid-blue and acid-purple forms of bacteriorhodopsin: evidence for no net charge transfer.

Time-resolved photovoltage measurements were performed with the acid-blue (bR605A) and acid-purple (bR565A) forms of bacteriorhodopsin (bR) in the time range from 25 ns to 100 s. The bR605A and bR565A pigments were formed by titration with H2SO4 in the absence and presence of 150 mM KCI, respectively. Qualitatively the kinetics of the charge displacement in these two states are similar and consist of two fast phases in one direction (100 ns bandwidth limited and approximately 1 microsecond) followed by a decay in the opposite direction via one component for bR605A (4.4 +/- 0.6 ms) or two components for bR565A (33 +/- 8 microseconds and 3.6 +/- 0.5 ms). The transient photovoltage signal returns exactly to the initial value after several milliseconds, well before the passive discharge of the electrical measuring system at 2 s. We conclude that no net charge transfer occurs in either bR605A or bR565A. The direction of the fast components is opposite that of net proton translocation in bR at pH 7. So, if the charge that moves back and forth is due to a proton, it moves first in the direction of the cytoplasmic side of the membrane (< 1 microsecond) and returns to its initial position via the 4.4 ms (bR605A) or the 33 microseconds and 3.6 ms (bR565A) decay components. The amplitude of the charge motion in both low pH forms is too large to be due to isomerization alone and is comparable to one of the major components in bR at pH 7.2

Time-resolved surface charge change on the cytoplasmic side of bacteriorhodopsin.

The pH-sensitive dye 5-iodoacetamidofluorescein was covalently bound to a single cysteine residue introduced by site-directed mutagenesis in position 101 on the cytoplasmic surface or in position 130 on the extracellular surface of the proton pump bacteriorhodopsin. Using time-resolved absorption spectroscopy at 495 nm a transient increase was observed in the apparent pK of the dye attached at residue 101. At pH 7.3 the rise and decay times of this pK-change (approximately 2 ms and approximately 60 ms) correlate well with decay times observed for the M and O intermediates and with the proton uptake time. Interpreting the pK-increase of +0.18 pH-unit in terms of a transiently more negative surface charge density, we calculate a change of -0.80 elementary charge per bacteriorhodopsin at the cytoplasmic surface. It is likely that this charge change is due to the transient deprotonation of aspartate-96. With the label in position 130 on the extracellular surface no transient pK-shift was detected.

Bacteriorhodopsin: the effect of bilayer thickness on 2D-array formation, and the structural re-alignment of retinal through the photocycle.

From our earlier extensive protein-lipid reconstitution studies, the conditions under which bacteriorhodopsin forms organised 2D arrays in large unilamellar vesicles have been established using freeze-fracture electron microscopy. In a background bilayer matrix of phosphatidylcholine (diC(14:0)), the protein can form arrays only when the anionic purple membrane lipid, phosphatidylglycerol phosphate (or the sulphate derivative) is present. Here we have now extended this work to investigate the effect of bilayer thickness on array formation. Phosphatidylcholines with various chain lengths (diC(12:0), diC(14:0) and diC(16:0)) and which form bilayers of well defined bilayer thickness, have been used as the matrix into which bacteriorhodopsin, together with minimal levels (c. 4-10 lipids per bacteriorhodopsin) of diphytanyl phosphatidyl-glycerol phosphate, has been reconstituted. Arrays are formed in all complexes and bhickness appears only to alter the type of array formed, either as an orthogonal or as an hexagonal array. Secondly, we have previously deduced the entire conformation of retinal within the bacteriorhodopsin binding pocket in oriented purple membrane fragments. Using solid state deuterium NMR of the specifically deutero-methylated retinal labelled at each of the methyl positions in the molecule, the C-CD(3) bond vectors of the chromophore have been resolved to +/- 2 degrees . The ring conformation is 6-S-trans, but the polyene chain is slightly curved when in the protein binding site. Here, we describe studies on the protein in both the ground state and the trapped M(412)-state of the photocycle, to show that the orientation of the central methyl group (C(19)) on the polyene chain, which is at 40 degrees +/- 1 degrees with respect to the membrane normal, only changes its orientation by approximately 4 degrees upon 13-cis-isomerization. Thus, it is the Schiff base end of the chromophore which moves upon light incidence acting as a local switch on the protein in the photocycle, whilst the ring end of the chromophore moves rather less.

Rapid long-range proton diffusion along the surface of the purple membrane and delayed proton transfer into the bulk.

The pH-indicator dye fluorescein was covalently bound to the surface of the purple membrane at position 72 on the extracellular side of bacteriorhopsin and at positions 101, 105, 160, or 231 on the cytoplasmic side by reacting bromomethylfluorescein with the sulfhydryl groups of cysteines introduced by site-directed mutagenesis. At position 72, on the extracellular surface, the light-induced proton release was detected 71 +/- 4 microseconds after the flash (conditions: pH 7.3, 22 degrees C, and 150 mM KCl). On the cytoplasmic side with the dye at positions 101, 105, and 160, the corresponding values were 77, 76, and 74 +/- 5 microseconds, respectively. Under the same conditions, the proton release time in the bulk medium as detected by pyranine was around 880 microseconds--i.e., slower by a factor of more than 10. The fact that the proton that is released on the extracellular side is detected much faster on the cytoplasmic surface than in the aqueous bulk phase demonstrates that it is retained on the surface and migrates along the purple membrane to the other side. These findings have interesting implications for bioenergetics and support models of local proton coupling. From the small difference between the proton detection times by labels on opposite sides of the membrane, we estimate that at 22 degrees C the proton surface diffusion constant is greater than 3 x 10(-5) cm2/s. At 5 degrees C, the proton release detection time at position 72 equals the faster of the two main rise times of the M intermediate (deprotonation of the Schiff base). At higher temperatures this correlation is gradually lost, but the curved Arrhenius plot for the proton release time is tangential to the linear Arrhenius plot for the rise of M at low temperatures. These observations are compatible with kinetic coupling between Schiff base deprotonation and proton release.

Light-induced isomerization causes an increase in the chromophore tilt in the M intermediate of bacteriorhodopsin: a neutron diffraction study.

Bacteriorhodopsin (BR) was regenerated with two selectively deuterated retinals, one with 11 deuterons in the beta-ionone ring (D11) and the other with 5 deuterons (D5) at the end of the polyene chain closest to the Schiff base at carbon atoms C-14, C-15, and C-20. Both label positions (centers of deuteration) were obtained from difference Fourier maps of projections onto the plane of the membrane by neutron diffraction at 90 K, both in the light-adapted ground-state BR568 and in the photocycle intermediate M412. To retard the decay of M412, purple membrane films were soaked in 0.1 M or 1 M guanidine hydrochloride at pH 9.6. M412 was produced by illuminating oriented membrane films at physiological temperature (278 K), followed by rapid cooling to 90 K in the absence of light. The results show that in the projected structure the ring position is unaltered during the transition from BR568 to M412, whereas the position of the D5 label shifts by 1.4 +/- 0.9 A toward the ring. The shortened interlabel distance in the projected structure for the M412 state implies that as a result of the all-trans/13-cis isomerization, the C-5 to C-13 part of the polyene chain tilts out of the plane of the membrane toward the cytoplasm by about 11 degrees +/- 6 degrees. Pairwise comparison of data sets with the same retinal for the two photocycle states M412 and BR568 leads to four difference-density maps for the protein, which are in agreement with previous work. They show changes in the protein density near helices G and F.

Covalently bound pH-indicator dyes at selected extracellular or cytoplasmic sites in bacteriorhodopsin. 1. Proton migration along the surface of bacteriorhodopsin micelles and its delayed transfer from surface to bulk.

The kinetics of the light-induced release and uptake of protons was monitored with the optical pH-indicator fluorescein covalently bound to various sites on the extracellular and cytoplasmic surfaces of bacteriorhodopsin. Selective labeling was achieved by reacting (iodoacetamido)fluorescein with the single cysteine residues in bacteriorhodopsin introduced at the desired positions by site-directed mutagenesis. All measurements were performed with bacteriorhodopsin micelles in phospholipid/detergent mixtures in 150 mM KCl at 22 degrees C, pH 7.3. Neither the replacements by cysteine nor the subsequent labeling affected the absorption spectrum of bacteriorhodopsin and the rise times of the M intermediate. Only the decay of M was altered for some bacteriorhodopsin mutants with cysteine residues on the cytoplasmic side. The proton release time detected with fluorescein attached to the extracellular surface (the proton release side) at position 72 (in the loop connecting helices B and C) or 130 (DE loop) was 22 +/- 4 microseconds, clearly faster than that measured with pyranine in the aqueous bulk phase (125 +/- 10 microseconds for wild-type and all mutants studied). For bacteriorhodopsin mutants labeled at positions 35, 101, 160, 229, and 231 in the cytoplasmic loop region (the proton uptake side), the released proton was observed with a time of 61 +/- 4 microseconds. This was about 3-fold slower than the release time on the extracellular side, but still significantly faster than that measured with pyranine in the bulk phase. These results suggest that the released protons are retained on the micellar surface and move more rapidly along this surface to the cytoplasmic side than from the surface to the bulk medium.(ABSTRACT TRUNCATED AT 250 WORDS)

Covalently bound pH-indicator dyes at selected extracellular or cytoplasmic sites in bacteriorhodopsin. 2. Rotational orientation of helices D and E and kinetic correlation between M formation and proton release in bacteriorhodopsin micelles.

The kinetics of the light-induced proton release in bacteriorhodopsin/lipid/detergent micelles was monitored with the optical pH-indicator fluorescein bound covalently to positions 127-134 (helices D and E and the DE loop) on the extracellular side of the protein (the proton release side). Single cysteine residues were introduced in these positions by site-directed mutagenesis, and fluorescein was attached to the sulfhydryl group by reaction with (iodoacetamido)fluorescein. Two characteristic proton release times (approximately 20 and 70 microseconds) were observed. The faster time constant was recorded when fluorescein was attached to positions 127, 130, 131, 132, and 134, while the slower time was observed with the indicator bound to positions 128, 129, and 133. The results are rationalized by assuming specific helical wheel orientations for helics D and E and by making a choice for the residues in the DE loop: (i) The fast time constants occur with fluorescein either attached to residues 130, 131, and 132 that form the DE loop or when pointing toward the interior of the protein with its aqueous proton channel [residues 127 (helix D) and 134 (helix E)]. (ii) The slower time constants are detected with fluorescein exposed to the exterior lipid/detergent phase when bound to residues 128, 129 (both helix D), and 133 (helix E). This interpretation is supported by measurements of the polarity of the label environment which indicate for fluorescein in group i a more hydrophilic environment and for group ii a more hydrophobic environment. The fastest proton release time (10 microseconds) was observed with fluorescein bound to position 127.(ABSTRACT TRUNCATED AT 250 WORDS)