Deriving reaction mechanisms from kinetic spectroscopy. Application to late rhodopsin intermediates

Parallel photocycle kinetic model of anion channelrhodopsin GtACR1 function

The light-gated anion channelrhodopsin GtACR1 is an important optogenetic tool for neuronal silencing. Its photochemistry, including its photointermediates, is poorly understood. The current mechanistic view presumes BR-like kinetics and assigns the open channel to a blue-absorbing L intermediate. Based on time-resolved absorption and electrophysiological data, we recently proposed a red-absorbing spectral form for the open channel state. Here, we report the results of a comprehensive kinetic analysis of the spectroscopic data combined with channel current information. The time evolutions of the spectral forms derived from the spectroscopic data are inconsistent with the single chain mechanism and are analyzed within the concept of parallel photocycles. The spectral forms partitioned into conductive and nonconductive parallel cycles are assigned to intermediate states. Rejecting reversible connections between conductive and nonconductive channel states leads to kinetic schemes with two independent conductive states corresponding to the fast- and slow-decaying current components. The conductive cycle is discussed in terms of a single cycle and two parallel cycles. The reaction mechanisms and reaction rates for the wild-type protein, the A75E, and the low-conductance D234N and S97E protein variants are derived. The parallel cycles of channelrhodopsin kinetics, its relation to BR photocycle, and the role of the M intermediate in channel closure are discussed.

Isospectral intermediates in the photochemical reaction cycle of anion channelrhodopsin GtACR1

The most effective tested optogenetic tools available for neuronal silencing are the light-gated anion channel proteins found in the cryptophyte alga Guillardia theta (GtACRs). Molecular mechanisms of GtACRs, including the photointermediates responsible for the open channel state, are of great interest for understanding their exceptional conductance. In this study, the photoreactions of GtACR1 and its D234N, A75E, and S97E mutants were investigated using multichannel time-resolved absorption spectroscopy. For each of the proteins, the analysis showed two early microsecond transitions between K-like and L-like forms and two late millisecond recovery steps. Spectral forms associated with potential molecular intermediates of the proteins were derived and their evolutions in time were analyzed. The results indicate the presence of isospectral intermediates in the photocycles and expand the range of potential intermediates responsible for the open channel state.

Styrene-maleic acid copolymer effects on the function of the GPCR rhodopsin in lipid nanoparticles

Styrene-maleic acid (SMA) copolymers solubilize biological membranes to form lipid nanoparticles (SMALPs) that contain membrane proteins surrounded by native lipids, thus enabling the use of a variety of biophysical techniques for structural and functional studies. The question of whether SMALPs provide a truly natural environment or SMA solubilization affects the functional properties of membrane proteins, however, remains open. We address this question by comparing the photoactivation kinetics of rhodopsin, a G-protein-coupled receptor in the disk membranes of rod cells, in native membrane and SMALPs prepared at different molar ratios between SMA(3:1) and rhodopsin. Time-resolved absorption spectroscopy combined with complex kinetic analysis reveals kinetic and mechanistic differences between the native membrane and SMA-stabilized environment. The results suggest a range of molar ratios for nanoparticles suitable for kinetic studies.

The Reactions of O2 and NO with Mixed-Valence ba3 Cytochrome c Oxidase from Thermus thermophilus

Earlier CO flow-flash experiments on the fully reduced Thermus thermophilus ba₃ (Tt ba₃) cytochrome oxidase revealed that O₂ binding was slowed down by a factor of 10 in the presence of CO (Szundi et al., 2010, PNAS 107, 21010-21015). The goal of the current study is to explore whether the long apparent lifetime (∼50 ms) of the Cu_B⁺-CO complex generated upon photolysis of the CO-bound mixed-valence Tt ba₃ (Koutsoupakis et al., 2019, Acc. Chem. Res. 52, 1380-1390) affects O₂ and NO binding and the ability of Cu_B to act as an electron donor during O-O bond splitting. The CO recombination, NO binding, and the reaction of mixed-valence Tt ba₃ with O₂ were investigated by time-resolved optical absorption spectroscopy using the CO flow-flash approach and photolabile O₂ and NO carriers. No electron backflow was detected after photolysis of the mixed-valence CO-bound Tt ba₃. The rate of O₂ and NO binding was two times slower than in the fully reduced enzyme in the presence of CO and 20 times slower than in the absence of CO. The purported long-lived Cu_B⁺-CO complex did not prevent O-O bond splitting and the resulting P_M formation, which was significantly faster (5-10 times) than in the bovine heart enzyme. We propose that O₂ binding to heme a₃ in Tt ba₃ causes CO to dissociate from Cu_B⁺ in a concerted manner through steric and/or electronic effects, thus allowing Cu_B⁺ to act as an electron donor in the mixed-valence enzyme. The significantly faster O₂ binding and O-O bond cleavage in Tt ba₃ compared to analogous steps in the aa₃ oxidases could reflect evolutionary adaptation of the enzyme to the microaerobic conditions of the T. thermophilus HB8 species.

Mechanism of Hormone Peptide Activation of a GPCR: Angiotensin II Activated State of AT1R Initiated by van der Waals Attraction

We present a succession of structural changes involved in hormone peptide activation of a prototypical GPCR. Microsecond molecular dynamics simulation generated conformational ensembles reveal propagation of structural changes through key "microswitches" within human AT₁R bound to native hormone. The endocrine octa-peptide angiotensin II (AngII) activates AT₁R signaling in our bodies which maintains physiological blood pressure, electrolyte balance, and cardiovascular homeostasis. Excessive AT₁R activation is associated with pathogenesis of hypertension and cardiovascular diseases which are treated by sartan drugs. The mechanism of AT₁R inhibition by sartans has been elucidated by 2.8 Å X-ray structures, mutagenesis, and computational analyses. Yet, the mechanism of AT₁R activation by AngII is unclear. The current study delineates an activation scheme initiated by AngII binding. A van der Waals "grasp" interaction between Phe8^AngII with Ile288^7.39 in AT₁R induced mechanical strain pulling Tyr292^7.43 and breakage of critical interhelical H-bonds, first between Tyr292^7.43 and Val108^3.32 and second between Asn111^3.35 and Asn295^7.46. Subsequently changes are observed in conserved microswitches DRY^TM3, Yx7K(R)^TM5, CWxP^TM6, and NPxxY^TM7 in AT₁R. Activating the microswitches in the intracellular region of AT₁R may trigger formation of the G-protein binding pocket as well as exposure of helix-8 to cytoplasm. Thus, the active-like conformation of AT₁R is initiated by the van der Waals interaction of Phe8^AngII with Ile288^7.39, followed by systematic reorganization of critical interhelical H-bonds and activation of microswitches.

Protein Sequence and Membrane Lipid Roles in the Activation Kinetics of Bovine and Human Rhodopsins

Rhodopsin is a G protein-coupled receptor found in the rod outer segments in the retina, which triggers a visual response under dim light conditions. Recently, a study of the late, microsecond-to-millisecond kinetics of photointermediates of the human and bovine rhodopsins in their native membranes revealed a complex, double-square mechanism of rhodopsin activation. In this kinetic scheme, the human rhodopsin exhibited more Schiff base deprotonation than bovine rhodopsin, which could arise from the ∼7% sequence difference between the two proteins, or from the difference between their membrane lipid environments. To differentiate between the effects of membrane and protein structure on the kinetics, the human and bovine rhodopsins were inserted into 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine lipid nanodiscs and the kinetics of activation at 15°C and pH 8.7 was investigated by time-resolved absorption spectroscopy and global kinetic analysis. For both proteins, the kinetics in nanodiscs shows the characteristics observed in the native membranes, and is described by a multisquare model with Schiff base deprotonation at the lumirhodopsin I intermediate stage. The results indicate that the protein sequence controls the extent of Schiff base deprotonation and accumulation of intermediates, and thus plays the main role in the different activation kinetics observed between human and bovine rhodopsins. The membrane lipid does have a minor role by modulating the timing of the kinetics, with the nanodisc environment leading to an earlier Schiff base deprotonation.

Role of Heme Pocket Water in Allosteric Regulation of Ligand Reactivity in Human Hemoglobin

Water molecules can enter the heme pockets of unliganded myoglobins and hemoglobins, hydrogen bond with the distal histidine, and introduce steric barriers to ligand binding. The spectrokinetics of photodissociated CO complexes of human hemoglobin and its isolated α and β chains were analyzed for the effect of heme hydration on ligand rebinding. A strong coupling was observed between heme hydration and quaternary state. This coupling may contribute significantly to the 20-60-fold difference between the R- and T-state bimolecular CO binding rate constants and thus to the modulation of ligand reactivity that is the hallmark of hemoglobin allostery. Heme hydration proceeded over the course of several kinetic phases in the tetramer, including the R to T quaternary transition. An initial 150 ns hydration phase increased the R-state distal pocket water occupancy, nw(R), to a level similar to that of the isolated α (∼60%) and β (∼10%) chains, resulting in a modest barrier to ligand binding. A subsequent phase, concurrent with the first step of the R → T transition, further increased the level of heme hydration, increasing the barrier. The final phase, concurrent with the final step of the allosteric transition, brought the water occupancy of the T-state tetramer, nw(T), even higher and close to full occupancy in both the α and β subunits (∼90%). This hydration level could present an even larger barrier to ligand binding and contribute significantly to the lower iron reactivity of the T state toward CO.

The CO Photodissociation and Recombination Dynamics of the W172Y/F282T Ligand Channel Mutant of Rhodobacter sphaeroides aa3 Cytochrome c Oxidase

In the ligand channel of the cytochrome c oxidase from Rhodobacter sphaeroides (Rs aa3 ) W172 and F282 have been proposed to generate a constriction that may slow ligand access to and from the active site. To explore this issue, the tryptophan and phenylalanine residues in Rs aa3 were mutated to the less bulky tyrosine and threonine residues, respectively, which occupy these sites in Thermus thermophilus (Tt) ba3 cytochrome oxidase. The CO photolysis and recombination dynamics of the reduced wild-type Rs aa3 and the W172Y/F282T mutant were investigated using time-resolved optical absorption spectroscopy. The spectral changes associated with the multiple processes are attributed to different conformers. The major CO recombination process (44 μs) in the W172Y/F282T mutant is ~500 times faster than the predominant CO recombination process in the wild-type enzyme (~23 ms). Classical dynamic simulations of the wild-type enzyme and double mutant showed significant structural changes at the active site in the mutant, including movement of the heme a3 ring-D propionate toward CuB and reduced binuclear center cavity volume. These structural changes effectively close the ligand exit pathway from the binuclear center, providing a basis for the faster CO recombination in the double mutant.

Platymonas subcordiformis Channelrhodopsin-2 Function: I. THE PHOTOCHEMICAL REACTION CYCLE

The photocycle kinetics of Platymonas subcordiformis channelrhodopsin-2 (PsChR2), among the most highly efficient light-gated cation channels and the most blue-shifted channelrhodopsin, was studied by time-resolved absorption spectroscopy in the 340-650-nm range and in the 100-ns to 3-s time window. Global exponential fitting of the time dependence of spectral changes revealed six lifetimes: 0.60 μs, 5.3 μs, 170 μs, 1.4 ms, 6.7 ms, and 1.4 s. The sequential intermediates derived for a single unidirectional cycle scheme based on these lifetimes were found to contain mixtures of K, L, M, O, and P molecular states, named in analogy to photointermediates in the bacteriorhodopsin photocycle. The photochemistry is described by the superposition of two independent parallel photocycles. The analysis revealed that 30% of the photoexcited receptor molecules followed Cycle 1 through the K, M, O, and P states, whereas 70% followed Cycle 2 through the K, L, M, and O states. The recovered state, R, is spectrally close, but not identical, to the dark state on the seconds time scale. The two-cycle model of this high efficiency channelrhodopsin-2 (ChR) opens new perspectives in understanding the mechanism of channelrhodopsin function.

Theory and procedures for finding a correct kinetic model for the bacteriorhodopsin photocycle

In this paper, we present the implementation and results of new methodology based on linear algebra. The theory behind these methods is covered in detail in the Supporting Information, available electronically (Shragerand Hendler). In brief, the methods presented search through all possible forward sequential submodels in order to find candidates that can be used to construct a complete model for the BR-photocycle. The methodology is limited only to forward sequential models. If no such models are compatible with the experimental data,none will be found. The procedures apply objective tests and filters to eliminate possibilities that cannot be correct, thus cutting the total number of candidate sequences to be considered. In the current application,which uses six exponentials, the total sequences were cut from 1950 to 49. The remaining sequences were further screened using known experimental criteria. The approach led to a solution which consists of a pair of sequences, one with 5 exponentials showing BR* f L(f) M(f) N O BR and the other with three exponentials showing BR* L(s) M(s) BR. The deduced complete kinetic model for the BR photocycle is thus either a single photocycle branched at the L intermediate or a pair of two parallel photocycles. Reasons for preferring the parallel photocycles are presented. Synthetic data constructed on the basis of the parallel photocycles were indistinguishable from the experimental data in a number of analytical tests that were applied.

Ligand access to the active site in Thermus thermophilus ba(3) and bovine heart aa(3) cytochrome oxidases

Knowledge of the structure and dynamics of the ligand channel(s) in heme-copper oxidases is critical for understanding how the protein environment modulates the functions of these enzymes. Using photolabile NO and O(2) carriers, we recently found that NO and O(2) binding in Thermus thermophilus (Tt) ba(3) is ~10 times faster than in the bovine enzyme, indicating that inherent structural differences affect ligand access in these enzymes. Using X-ray crystallography, time-resolved optical absorption measurements, and theoretical calculations, we investigated ligand access in wild-type Tt ba(3) and the mutants, Y133W, T231F, and Y133W/T231F, in which tyrosine and threonine in the O(2) channel of Tt ba(3) are replaced by the corresponding bulkier tryptophan and phenylalanine, respectively, present in the aa(3) enzymes. NO binding in Y133W and Y133W/T231F was found to be 5 times slower than in wild-type ba(3) and the T231F mutant. The results show that the Tt ba(3) Y133W mutation and the bovine W126 residue physically impede NO access to the binuclear center. In the bovine enzyme, there is a hydrophobic "way station", which may further slow ligand access to the active site. Classical simulations of diffusion of Xe to the active sites in ba(3) and bovine aa(3) show conformational freedom of the bovine F238 and the F231 side chain of the Tt ba(3) Y133W/T231F mutant, with both residues rotating out of the ligand channel, resulting in no effect on ligand access in either enzyme.

Effect of Hofmeister cosolutes on the photocycle of photoactive yellow protein at moderately alkaline pH

The photocycle of photoactive yellow protein was studied by kinetic absorption spectroscopy from below 100ns to seconds, at moderately alkaline pH, in the presence of high concentrations of various salts. Chemometric analysis combined with multiexponential fit of the flash-induced difference spectra provided evidence for five intermediates, including a spectrally silent form before the final recovery of the parent state, but only three with significantly distinct spectra. The calculated intermediate spectra constituted the input for the following spectrotemporal model fit using a sufficiently complex photocycle scheme with reversible transitions. This yielded the rate coefficients of the molecular transitions, the final spectra and the kinetics of the intermediates. Except for the transition between the two red shifted (early) intermediates (pR1 and pR2) and the final photocycle step, all reactions appeared to be reversible. Kosmotropic and chaotropic cosolutes had a systematic effect on the molecular rate coefficients. The largest effect, associated presumably with the exposure of the hydrophobic interior of the protein, accompanies the transition between the second red-shifted and the first blue-shifted intermediate (pR2 and pB1, respectively), i.e. it coincides with the chromophore protonation. The dependence of the rate coefficients on the Hofmeister cosolutes suggests that the conformational change of photoactive yellow protein leading eventually to the most unfolded signaling state takes place in several steps, and starts already with the relaxation after the chromophore isomerization in the microsecond time domain.

Photocycle of the LOV-STAS protein from the pathogen Listeria monocytogenes

Listeria monocytogenes, a food-borne bacterial pathogen causing significant human mortality, propagates by expressing genes in response to environmental signals, such as temperature and pH. Listeria gene (lmo0799) encodes a protein homologous to the Bacillus subtilis YtvA, which has a flavin-light, oxygen or voltage (LOV) domain and a Sulfate Transporters Anti-Sigma factor antagonist (STAS) output domain that regulates transcription-initiation factor Sigma B in the bacterial stress response upon exposure to light. This could be significant for the pathogenesis of listeriosis because Sigma B has been linked to virulence of Listeria, and the Listeria Lmo0799 protein has recently been identified as a virulence factor activated by blue light. We have cloned, expressed heterologously in Escherichia coli and purified the full-length LM-LOV-STAS protein. Although it exhibits photochemical activity similar to that of YtvA, LM-LOV-STAS lacks an almost universally conserved arginine in the flavin-binding site, as well as another positively charged residue, a lysine in YtvA. The absence of these positive charges was found to destabilize retention of the flavin mononucleotide (FMN) chromophore in the LM-LOV-STAS protein, particularly at higher temperatures. The unusual sequence of the LM-LOV-STAS protein alters both spectral features and activation/deactivation kinetics, potentially expanding the sensory capacity of this LOV domain, e.g. to detect light plus cold.

Spectral identification of intermediates generated during the reaction of dioxygen with the wild-type and EQ(I-286) mutant of Rhodobacter sphaeroides cytochrome c oxidase

Cytochrome c oxidase from Rhodobacter sphaeroides is frequently used to model the more complex mitochondrial enzyme. The O(2) reduction in both enzymes is generally described by a unidirectional mechanism involving the sequential formation of the ferrous-oxy complex (compound A), the P(R) state, the oxyferryl F form, and the oxidized state. In this study we investigated the reaction of dioxygen with the wild-type reduced R. sphaeroides cytochrome oxidase and the EQ(I-286) mutant using the CO flow-flash technique. Singular value decomposition and multiexponential fitting of the time-resolved optical absorption difference spectra showed that three apparent lifetimes, 18 μs, 53 μs, and 1.3 ms, are sufficient to fit the kinetics of the O(2) reaction of the wild-type enzyme. A comparison of the experimental intermediate spectra with the corresponding intermediate spectra of the bovine enzyme revealed that P(R) is not present in the reaction mechanism of the wild-type R. sphaeroides aa(3). Transient absorbance changes at 440 and 610 nm support this conclusion. For the EQ(I-286) mutant, in which a key glutamic residue in the D proton pathway is replaced by glutamine, two lifetimes, 16 and 108 μs, were observed. A spectral analysis of the intermediates shows that the O(2) reaction in the EQ(I-286) mutant terminates at the P(R) state, with 70% of heme a becoming oxidized. These results indicate significant differences in the kinetics of O(2) reduction between the bovine and wild-type R. sphaeroides aa(3) oxidases, which may arise from differences in the relative rates of internal electron and proton movements in the two enzymes.

Schiff base protonation changes in Siberian hamster ultraviolet cone pigment photointermediates

Molecular structure and function studies of vertebrate ultraviolet (UV) cone visual pigments are needed to understand the molecular evolution of these photoreceptors, which uniquely contain unprotonated Schiff base linkages between the 11-cis-retinal chromophore and the opsin proteins. In this study, the Siberian hamster ultraviolet cone pigment (SHUV) was expressed and purified in an n-dodecyl-β-D-maltoside suspension for optical characterization. Time-resolved absorbance measurements, over a spectral range from 300 to 700 nm, were taken for the purified pigment at time delays from 30 ns to 4.64 s after photoexcitation using 7 ns pulses of 355 nm light. The resulting data were fit globally to a sum of exponential functions after noise reduction using singular-value decomposition. Four exponentials best fit the data with lifetimes of 1.4 μs, 210 μs, 47 ms, and 1 s. The first photointermediate species characterized here is an equilibrated mixture similar to the one formed after rhodopsin's Batho intermediate decays into equilibrium with its successor, BSI. The extremely large red shift of the SHUV Batho component relative to the pigment suggests that SHUV Batho has a protonated Schiff base and that the SHUV cone pigment itself has an unprotonated Schiff base. In contrast to SHUV Batho, the portion of the equilibrated mixture's spectrum corresponding to SHUV BSI is well fit by a model spectrum with an unprotonated Schiff base. The spectra of the next two photointermediate species revealed that they both have unprotonated Schiff bases and suggest they are analogous to rhodopsin's Lumi I and Lumi II species. After decay of SHUV Lumi II, the correspondence with rhodopsin photointermediates breaks down and the next photointermediate, presumably including the G protein-activating species, is a mixture of protonated and unprotonated Schiff base photointermediate species.

Quantifying the differential effects of DHA and DPA on the early events in visual signal transduction

A range of evidence from animal, clinical and epidemiological studies indicates that highly polyunsaturated acyl chains play important roles in development, cognition, vision and other aspects of neurological function. In a number of these studies n3 polyunsaturated fatty acids (PUFAs) appear to be more efficacious than n6 PUFAs. In a previous study of retinal rod outer segments obtained from rats raised on either an n3 adequate or deficient diet, we demonstrated that the replacement of 22:6n3 by 22:5n6 in the n3 deficient rats led to functional deficits in each step in the visual signaling process (Niu et al., 2004). In this study, we examined rhodopsin and phosphodiesterase function and acyl chain packing properties in membranes consisting of phosphatidylcholines with sn-1=18:0, and sn-2=22:6n3, 22:5n6, or 22:5n3 in order to determine if differences in function are due to the loss of one double bond or due to differences in double bond location. At 37 °C the n6 lipid shifted the equilibrium between the active metarhodopsin II (MII) state and inactive metarhodopsin I (MI) state towards MI. In addition, 22:5n6 reduced the rates of MII formation and MII-transducin complex formation by 2- and 6-fold, respectively. At a physiologically relevant level of rhodopsin light stimulation, the activity of phosphodiesterase was reduced by 50% in the 22:5n6 membrane, relative to either of the n3 membranes. Activity levels in the two n3 membranes were essentially identical. Ensemble acyl chain order was assessed with time-resolved fluorescence measurements of the membrane probe diphenylhexatriene (DPH). Analysis in terms of the orientational distribution of DPH showed that acyl chain packing in the two n3 membranes is quite similar, while in the 22:5n6 membrane there was considerably less packing disorder in the bilayer midplane. These results demonstrate that the n3 bond configuration uniquely optimizes the early steps in signaling via a mechanism which may involve acyl chain packing deep in the bilayer.

Kinetic studies of the reactions of O(2) and NO with reduced Thermus thermophilus ba(3) and bovine aa(3) using photolabile carriers

The reactions of molecular oxygen (O(2)) and nitric oxide (NO) with reduced Thermus thermophilus (Tt) ba(3) and bovine heart aa(3) were investigated by time-resolved optical absorption spectroscopy to establish possible relationships between the structural diversity of these enzymes and their reaction dynamics. To determine whether the photodissociated carbon monoxide (CO) in the CO flow-flash experiment affects the ligand binding dynamics, we monitored the reactions in the absence and presence of CO using photolabile O(2) and NO complexes. The binding of O(2)/NO to reduced ba(3) in the absence of CO occurs with a second-order rate constant of 1×10(9)M(-1)s(-1). This rate is 10-times faster than for the mammalian enzyme, and which is attributed to structural differences in the ligand channels of the two enzymes. Moreover, the O(2)/NO binding in ba(3) is 10-times slower in the presence of the photodissociated CO while the rates are the same for the bovine enzyme. This indicates that the photodissociated CO directly or indirectly impedes O(2) and NO access to the active site in Tt ba(3), and that traditional CO flow-flash experiments do not accurately reflect the O(2) and NO binding kinetics in ba(3). We suggest that in ba(3) the binding of O(2) (NO) to heme a(3)(2+) causes rapid dissociation of CO from Cu(B)(+) through steric or electronic effects or, alternatively, that the photodissociated CO does not bind to Cu(B)(+). These findings indicate that structural differences between Tt ba(3) and the bovine aa(3) enzyme are tightly linked to mechanistic differences in the functions of these enzymes. This article is part of a Special Issue entitled: Respiratory Oxidases.

CO impedes superfast O2 binding in ba3 cytochrome oxidase from Thermus thermophilus

Kinetic studies of heme-copper terminal oxidases using the CO flow-flash method are potentially compromised by the fate of the photodissociated CO. In this time-resolved optical absorption study, we compared the kinetics of dioxygen reduction by ba(3) cytochrome c oxidase from Thermus thermophilus in the absence and presence of CO using a photolabile O(2)-carrier. A novel double-laser excitation is introduced in which dioxygen is generated by photolyzing the O(2)-carrier with a 355 nm laser pulse and the fully reduced CO-bound ba(3) simultaneously with a second 532-nm laser pulse. A kinetic analysis reveals a sequential mechanism in which O(2) binding to heme a(3) at 90 μM O(2) occurs with lifetimes of 9.3 and 110 μs in the absence and presence of CO, respectively, followed by a faster cleavage of the dioxygen bond (4.8 μs), which generates the P intermediate with the concomitant oxidation of heme b. The second-order rate constant of 1 × 10(9) M(-1) s(-1) for O(2) binding to ba(3) in the absence of CO is 10 times greater than observed in the presence of CO as well as for the bovine heart enzyme. The O(2) bond cleavage in ba(3) of 4.8 μs is also approximately 10 times faster than in the bovine enzyme. These results suggest important structural differences between the accessibility of O(2) to the active site in ba(3) and the bovine enzyme, and they demonstrate that the photodissociated CO impedes access of dioxygen to the heme a(3) site in ba(3), making the CO flow-flash method inapplicable.

Temperature dependence of the lumirhodopsin I-lumirhodopsin II equilibrium

Time-resolved absorbance measurements, over a spectral range from 300 to 700 nm, were made at delays from 1 micros to 2 ms after photoexcitation of bovine rhodopsin in hypotonically washed membrane suspensions over a range of temperature from 10 to 35 degrees C. The purpose was to better understand the reversibility of the Lumi I-Lumi II process that immediately precedes Schiff base deprotonation in the activation of rhodopsin under physiological conditions. To prevent artifacts due to rotation of rhodopsin and its photoproducts in the membrane, probe light in the time-resolved absorbance studies was polarized at the magic angle (54.7 degrees) relative to the excitation laser polarization axis. The difference spectrum associated with the Lumi I to Lumi II reaction was found to have larger amplitude at 10 degrees C compared to higher temperatures, suggesting that a significant back-reaction exists for this process and that an equilibrated mixture forms. The equilibrium favors Lumi I entropically, and van't Hoff plot curvature shows the reaction enthalpy depends on temperature. The results suggest that Lumi II changes its interaction with the membrane in a temperature-dependent way, possibly binding a membrane lipid more strongly at lower temperatures (compared to its precursor). To elucidate the origin of the time-resolved absorbance changes, linear dichroism measurements were also made at 20 degrees C. The time constant for protein rotation in the membrane was found to be identical to the time constant for the Lumi I-Lumi II process, which is consistent with a common microscopic origin. We conclude that Lumi II (the last protonated Schiff base photointermediate under physiological conditions) is the first photointermediate whose properties depend on the protein-lipid environment.

Sequential rearrangement of interhelical networks upon rhodopsin activation in membranes: the Meta II(a) conformational substate

Photon absorption by rhodopsin is proposed to lead to an activation pathway that is described by the extended reaction scheme Meta I <==>Meta II(a) <==> Meta II(b) <==> Meta II(b)H(+), where Meta II(b)H(+) is thought to be the conformational substate that activates the G protein transducin. Here we test this extended scheme for rhodopsin in a membrane bilayer environment by investigating lipid perturbation of the activation mechanism. We found that symmetric membrane lipids having two unsaturated acyl chains, such as 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC), selectively stabilize the Meta II(a) substate in the above mechanism. By combining FTIR and UV-visible difference spectroscopy, we characterized the structural and functional changes involved in the transition to the Meta II(a) intermediate, which links the inactive Meta I intermediate with the Meta II(b) states formed by helix rearrangement. Besides the opening of the Schiff base ionic lock, the Meta II(a) substate is characterized by an activation switch in a conserved water-mediated hydrogen-bonded network involving transmembrane helices H1/H2/H7, which is sensed by its key residue Asp83. On the other hand, movement of retinal toward H5 and its interaction with another interhelical H3/H5 network mediated by His211 and Glu122 is absent in Meta II(a). The latter rearrangement takes place only in the subsequent transition to Meta II(b), which has been previously associated with movement of H6. Our results imply that activating structural changes in the H1/H2/H7 network are triggered by disruption of the Schiff base salt bridge and occur prior to other chromophore-induced changes in the H3/H5 network and the outward tilt of H6 in the activation process.

Structural changes due to the deprotonation of the proton release group in the M-photointermediate of bacteriorhodopsin as revealed by time-resolved FTIR spectroscopy

One of the steps in the proton pumping cycle of bacteriorhodopsin (BR) is the release of a proton from the proton-release group (PRG) on the extracellular side of the Schiff base. This proton release takes place shortly after deprotonation of the Schiff base (L-to-M transition) and results in an increase in the pKa of Asp85, which is a crucial mechanistic step for one-way proton transfer for the entire photocycle. Deprotonation of the PRG can also be brought about without photoactivation, by raising the pH of the enzyme (pKa of PRG; approximately 9). Thus, comparison of the FTIR difference spectrum for formation of the M intermediate (M minus initial unphotolyzed BR state) at pH 7 to the corresponding spectrum generated at pH 10 may reveal structural changes specifically associated with deprotonation of the PRG. Vibrational bands of BR that change upon M formation are distributed across a broad region between 2120 and 1685 cm(-1). This broad band is made up of two parts. The band above 1780 cm(-1), which is insensitive to C15-deuteration of the retinal, may be due to a proton delocalized in the PRG. The band between 1725 and 1685 cm(-1), on the lower frequency side of the broad band, is sensitive to C15-deuteration. This band may arise from transition dipole coupling of the vibrations of backbone carbonyl groups in helix G with the side chain of Tyr57 and with the C15H of the Schiff base. In M, these broad bands are abolished, and the 3657 cm(-1) band, which is due to the disruption of the hydrogen bonding of a water molecule, probably with Arg82, appears. Loss of the interaction of the backbone carbonyl groups in helix G with Tyr57 and the Schiff base, and separation of Tyr57 from Arg82, may be causes of these spectral changes, leading to the stabilization of the protonated Asp85 in M.

Lumi I --> Lumi II: the last detergent independent process in rhodopsin photoexcitationt

Time-resolved absorbance difference spectra were collected at delays from 1 to 128 micros after photolysis of membrane and detergent suspensions of rhodopsin at 20 degrees C. Fitting both sets of data with two exponential decays plus a constant showed a similar fast process (lifetime 11 micros in membrane, 12 micros in 5% dodecyl maltoside) with a small but similar spectral change. This demonstrates that the Lumi I - Lumi II process, previously characterized in detergent suspensions, has similar properties in membrane without significant effect of detergent. The slower exponential process detected in the data is quite different in membrane compared to detergent solubilized samples, showing that the pronounced effect of detergent on the later rhodopsin photointermediates begins fairly abruptly near 20 micros. Besides affecting the late processes, the data collected here shows that detergent induces a small blue shift in the 1 micros difference spectrum (the Lumi I minus rhodopsin difference spectrum). The blue shift is similar to one induced by chloride ion in the E181Q rhodopsin mutant and may indicate that the ionization state of Glu181 in rhodopsin is affected by detergent.

Bayesian maximum entropy (two-dimensional) lifetime distribution reconstruction from time-resolved spectroscopic data

Time-resolved spectroscopy is often used to monitor the relaxation processes (or reactions) of physical, chemical, and biochemical systems after some fast physical or chemical perturbation. Time-resolved spectra contain information about the relaxation kinetics, in the form of macroscopic time constants of decay and their decay associated spectra. In the present paper we show how the Bayesian maximum entropy inversion of the Laplace transform (MaxEnt-iLT) can provide a lifetime distribution without sign-restrictions (or two-dimensional (2D)-lifetime distribution), representing the most probable inference given the data. From the reconstructed (2D) lifetime distribution it is possible to obtain the number of exponentials decays, macroscopic rate constants, and exponential amplitudes (or their decay associated spectra) present in the data. More importantly, the obtained (2D) lifetime distribution is obtained free from pre-conditioned ideas about the number of exponential decays present in the data. In contrast to the standard regularized maximum entropy method, the Bayesian MaxEnt approach automatically estimates the regularization parameter, providing an unsupervised and more objective analysis. We also show that the regularization parameter can be automatically determined by the L-curve and generalized cross-validation methods, providing (2D) lifetime reconstructions relatively close to the Bayesian best inference. Finally, we propose the use of MaxEnt-iLT for a more objective discrimination between data-supported and data-unsupported quantitative kinetic models, which takes both the data and the analysis limitations into account. All these aspects are illustrated with realistic time-resolved Fourier transform infrared (FT-IR) synthetic spectra of the bacteriorhodopsin photocycle.

Time-resolved rapid-scan Fourier transform infrared difference spectroscopy on a noncyclic photosystem: rhodopsin photointermediates from Lumi to Meta II

The visual pigment rhodopsin has been extensively studied for the kinetics of its photointermediates by various spectroscopic methods. Unlike such archaeal retinal proteins as bacteriorhodopsin, visual rhodopsin does not thermally recover its dark state after photoexcitation, which precludes repeated excitation of a single sample and thereby complicates time-resolved experiments. Kinetic data on the late rhodopsin photointermediates have so far been available mainly from time-resolved ultraviolet (UV)-visible spectroscopy, but not from Fourier transform infrared (FTIR) spectroscopy. The latter has the advantage of being informative of structural changes of both chromophore and protein, but does not allow the highly reproducible, automated sample exchange procedures available to UV-visible spectroscopy. Using rapid-scan FTIR difference spectroscopy, we obtained time-resolved data sets that were analyzed by a maximum entropy inverse Laplace-transform. Covering the time range from 8 ms to 15 s at temperatures of 0 and -7 degrees C, the transitions from the Lumi to the Meta I and from the Meta I to the Meta II photoproduct states could be resolved. In the transition from Meta I to Meta II, our data reveal a partial deprotonation of the retinal Schiff base preceding the conformational change of the receptor protein to Meta II. The technique and the results are discussed in regard to its advantages as well as its limitations.

Proton movement and photointermediate kinetics in rhodopsin mutants

The role of ionizable amino acid side chains in the bovine rhodopsin activation mechanism was studied in mutants E134Q, E134R/R135E, H211F, and E122Q. All mutants exhibited bathorhodopsin stability on the 30 ns to 1 micros time scale similar to that of the wild type. Lumirhodopsin decay was also similar to that of the wild type except for the H211F mutant where early decay (20 micros) to a second form of lumirhodopsin was seen, followed by formation of an extremely long-lived Meta I(480) product (34 ms), an intermediate which forms to a much reduced extent, if at all, in dodecyl maltoside suspensions of wild-type rhodopsin. A smaller amount of a similar long-lived Meta I(480) product was seen after photolysis of E122Q, but E134Q and E134R/R135Q displayed kinetics much more similar to those of the wild type under these conditions (i.e., no Meta I(480) product). These results support the idea that specific interaction of His211 and Glu122 plays a significant role in deprotonation of the retinylidene Schiff base and receptor activation. Proton uptake measurements using bromcresol purple showed that E122Q was qualitatively similar to wild-type rhodopsin, with at least one proton being released during lumirhodopsin decay per Meta I(380) intermediate formed, followed by uptake of at least two protons per rhodopsin bleached on a time scale of tens of milliseconds. Different results were obtained for H211F, E134Q, and E134R/R135E, which all released approximately two protons per rhodopsin bleached. These results show that several ionizable groups besides the Schiff base imine are affected by the structural changes involved in rhodopsin activation. At least two proton uptake groups and probably at least one proton release group in addition to the Schiff base are present in rhodopsin.

Rhodopsin photointermediates in two-dimensional crystals at physiological temperatures

Bovine rhodopsin photointermediates formed in two-dimensional (2D) rhodopsin crystal suspensions were studied by measuring the time-dependent absorbance changes produced after excitation with 7 ns laser pulses at 15, 25, and 35 degrees C. The crystalline environment favored the Meta I(480) photointermediate, with its formation from Lumi beginning faster than it does in rhodopsin membrane suspensions at 35 degrees C and its decay to a 380 nm absorbing species being less complete than it is in the native membrane at all temperatures. Measurements performed at pH 5.5 in 2D crystals showed that the 380 nm absorbing product of Meta I(480) decay did not display the anomalous pH dependence characteristic of classical Meta II in the native disk membrane. Crystal suspensions bleached at 35 degrees C and quenched to 19 degrees C showed that a rapid equilibrium existed on the approximately 1 s time scale, which suggests that the unprotonated predecessor of Meta II in the native membrane environment (sometimes called MII(a)) forms in 2D rhodopsin crystals but that the non-Schiff base proton uptake completing classical Meta II formation is blocked there. Thus, the 380 nm absorbance arises from an on-pathway intermediate in GPCR activation and does not result from early Schiff base hydrolysis. Kinetic modeling of the time-resolved absorbance data of the 2D crystals was generally consistent with such a mechanism, but details of kinetic spectral changes and the fact that the residuals of exponential fits were not as good as are obtained for rhodopsin in the native membrane suggested the photoexcited samples were heterogeneous. Variable fractional bleach due to the random orientation of linearly dichroic crystals relative to the linearly polarized laser was explored as a cause of heterogeneity but was found unlikely to fully account for it. The fact that the 380 nm product of photoexcitation of rhodopsin 2D crystals is on the physiological pathway of receptor activation suggests that determination of its structure would be of interest.

Bacteriorhodopsin photocycle kinetics analyzed by the maximum entropy method

A maximum entropy method (MEM) was developed for the study of the bacteriorhodopsin photocycle kinetics. The method can be applied directly to experimental kinetic absorption data without any assumption for the number of the intermediate states taking part in the photocycle. Though this method does not give a specific kinetics, its result is very useful for selection between possible photocycle kinetics. Using simulated data, it is shown that MEM gives correct results for the number of the intermediate states and the amplitude distributions around the characteristic lifetimes. Analyzing experimental absorption data at five different wavelengths, MEM gives seven or eight characteristic lifetimes, which means that at least so many distinct intermediate states exist during the photocycle. Many possible photocycle kinetic models were studied and compared with the MEM result. The best agreement was found with a branching photocycle model of eight intermediate states (K, L, M(1), M(2), M(3), M(4), N, O). The branching occurs at the L intermediate state (M(1) and M(2) being in one branch and M(3) and M(4) in the other branch), but at high pH it occurs already at the K state.

Global and target analysis of time-resolved spectra

In biological/bioenergetics research the response of a complex system to an externally applied perturbation is often studied. Spectroscopic measurements at multiple wavelengths are used to monitor the kinetics. These time-resolved spectra are considered as an example of multiway data. In this paper, the methodology for global and target analysis of time-resolved spectra is reviewed. To fully extract the information from the overwhelming amount of data, a model-based analysis is mandatory. This analysis is based upon assumptions regarding the measurement process and upon a physicochemical model for the complex system. This model is composed of building blocks representing scientific knowledge and assumptions. Building blocks are the instrument response function (IRF), the components of the system connected in a kinetic scheme, and anisotropy properties of the components. The combination of a model for the kinetics and for the spectra of the components results in a more powerful spectrotemporal model. The model parameters, like rate constants and spectra, can be estimated from the data, thus providing a concise description of the complex system dynamics. This spectrotemporal modeling approach is illustrated with an elaborate case study of the ultrafast dynamics of the photoactive yellow protein.

pH dependence of the reduction of dioxygen to water by cytochrome c oxidase. 1. The P(R) state is a pH-dependent mixture of three intermediates, A, P, and F

Recent studies on cytochrome oxidase have indicated that the putative "peroxy" intermediate in the catalytic cycle (P(R)) is a mixture of intermediates, including P and F [Sucheta, A., et al. (1998) Biochemistry 37, 17905-17914], and the bench-made P and F forms appear to have the same redox state (Fe(a3)(4+)=O(2-)), but a different protonation state [Fabian, M., and Palmer, G. (2001) Biochemistry 40, 1867-1874]. To explore the possibility that the putative P(R) state is a pH-dependent mixture of intermediates, we investigated the reduction of dioxygen to water by the fully reduced cytochrome oxidase at pH 6.2, 7.5, and 8.5 in the visible and Soret regions (350-800 nm) using the CO flow-flash technique. Singular value decomposition and global exponential fitting of the time-resolved absorption difference spectra resolved five apparent lifetimes. The fastest three (1.5, 13, and 34 micros) were independent of pH, while the two slowest rates (80-240 micros and 1.1-2.4 ms) decreased by a factor of 2-3 as the pH increased. When the time-resolved spectra were analyzed using a unidirectional sequential model, the spectra of the reduced enzyme and the dioxygen-bound intermediate, compound A, were found to be pH-independent. However, the putative P(R) intermediate was best represented by a pH-dependent mixture of compound A, P, and F. The ferryl form was favored at low pH. The subsequent intermediate is a ferryl with a pH-dependent electron transfer equilibrium between heme a and Cu(A), the reduced heme a being favored at low pH. These results suggest a pH-dependent reaction mechanism of the reduction of dioxygen to water by the fully reduced enzyme that is more complex than previously proposed.

Two intermediates appear on the lumirhodopsin time scale after rhodopsin photoexcitation

Absorbance difference spectra were recorded at 20 degrees C with a dense sequence of delay times from 1 to 128 micros after photolysis of lauryl maltoside suspensions of rhodopsin prepared from hypotonically washed bovine rod outer segments. Data were best fit by two-exponential components with a small, fast component (tau = 12 micros) occurring during the period that lumirhodopsin has been presumed to be stable. The shape of the spectral change corresponds to an approximately 2 nm red shift of the lumirhodopsin spectrum. Measurements with linearly polarized light verified that no absorbance changes associated with rotational diffusion were present in these preparations on this time scale, and experiments designed to enhance isorhodopsin production during photolysis showed no effect on the relative amplitude of the fast process. A similar process was previously observed in membrane suspensions of rhodopsin, but there the similarity of the change to rotational diffusion artifacts made conclusive identification of a second lumirhodopsin difficult. However, reexamination of polarized light measurements on rhodopsin in membrane supports the fact that the fast process seen here in detergent also takes place there. The new absorbance process occurs when time-resolved resonance Raman experiments have shown that the protonated Schiff base is moving from one hydrogen bond acceptor to another. The results are discussed in the context of possibly related processes on the same time scale that have been observed recently in artificial visual pigments with synthetic retinylidene chromophores and in a related rhodopsin mutant. The details of lumirhodopsin behavior are important because it is the last protonated Schiff base intermediate that occurs under physiological conditions.

pH dependence of the reduction of dioxygen to water by cytochrome c oxidase. 2. Branched electron transfer pathways linked by proton transfer

Recent time-resolved optical absorption studies in our laboratory have indicated that the putative peroxy intermediate formed during the reduction of dioxygen to water by cytochrome oxidase (P(R)) is a pH-dependent mixture of compound A, P, and F [Van Eps, N., et al. (2003) Biochemistry 42, 5065-5073]. This conclusion is based on a kinetic analysis of flow-flash time-resolved data using a unidirectional sequential scheme with five apparent lifetimes. To account for this observation, we propose a more complex kinetic model that consists of branched pathways, one branch producing the 607 nm P form and the other the 580 nm F form. The two pathways are interconnected, and the rate of exchange between the two is pH-dependent. The kinetic analysis and testing of the new model involves a novel algebraic approach which transforms the intermediates of the complex branched scheme into intermediates comparable to those derived on the basis of a sequential model. The branched model reproduces the experimental data very well and is consistent with a variety of experimental observations. The two branches may arise from two structurally different CO or O(2) conformers or protein conformers, which could lead to different accessibilities of proton donors to the binuclear center.

Bleaching kinetics of artificial visual pigments with modifications near the ring-polyene chain connection

Absorbance difference spectra were recorded at 20 degrees C from 30 ns to milliseconds after photolysis of lauryl maltoside suspensions of artificial visual pigments derived from 9-cis isomers of 5-ethylretinal, 8,16-methanoretinal (a 6-s-trans-bicyclic analogue), or 5-demethyl-8-methylretinal. In all three pigments, the earliest intermediate that was detected had the characteristics of a mixture of bathorhodopsin and a blue-shifted intermediate, BSI, which is the first decay product of bathorhodopsin in bovine rhodopsin. The first decays resolved on the nanosecond time scale were the formation of the lumirhodopsin analogues. Subsequent decays were able to be fit with a mechanistic scheme which has been shown to apply to both membrane and detergent suspensions of rhodopsin. Large increases were seen in the amount of metarhodopsin I which appeared after photolysis of 5-ethylisorhodopsin and the bicyclic isorhodopsin analogue, while 5-demethyl-8-methylisorhodopsin more closely followed native rhodopsin in decaying through meta I380, a 380 nm absorbing precursor to metarhodopsin II. In addition to forming more metarhodopsin I, the bicyclic analogue stabilized the metarhodopsin I-metarhodopsin II equilibrium similarly to what has been previously reported for 9-demethylrhodopsin in detergent, introducing the possibility that the bicyclic analogue could similarly be defective in transducin activation. These observations support the idea that long after initial photolysis, structural details of the retinylidene chromophore continue to play a decisive role in processes leading to the activated form, metarhodopsin II.

Effect of NADPH on formation and decay of human metarhodopsin III at physiological temperatures

Difference absorption spectra were recorded during the formation and decay of metarhodopsin III after sonicated membrane suspensions of rhodopsin were bleached at 37 degrees C. The data were analyzed using SVD, spectral decomposition and global exponential fitting. By comparison of the results in the presence or absence of 70 microM NADPH and those for bovine or human rhodopsin, a single comprehensive scheme was fit to all the data, including reduction of retinal to retinol by the intrinsic retinol dehydrogenase. On the time scale studied the mechanism involves two 382 nm absorbing species and two 468 nm, absorbing species, supporting the notion that human metarhodopsin III is not a homogeneous species. The results confirm that metarhodopsin III forms and persists sufficiently long in the human retina under physiological conditions that it could undergo secondary photoisomerization.

Multicolored protein conformation states in the photocycle of transducer-free sensory rhodopsin-I

Sensory rhodopsin-I (SRI), a phototaxis receptor of archaebacteria, is a retinal-binding protein that exists in the cell membrane intimately associated with a signal-transducing protein (HtrI) homologous to eubacterial chemotaxis receptors. Transducer-free sensory rhodopsin-I (fSRI), from cells devoid of HtrI, undergoes a photochemical cycle kinetically different from that of native SRI. We report here on the measurement and analysis of the photochemical kinetics of fSRI reactions in the 350-750-nm spectral range and in a 10(-7) s to 1 s time window. The lack of specific intermolecular interactions between SRI and HtrI results in early return of the ground form via distinct branching reactions in fSRI, not evident in the photocycle of native SRI. The chromophore transitions are loosely coupled to protein structural transitions. The coexistence of multiple spectral forms within kinetic intermediates is interpreted within the concept of multicolored protein conformational states.

New photointermediates in the two photon signaling pathway of sensory rhodopsin-I

Sensory rhodopsin-I (SRI) functions as a color discriminating receptor in halobacterial phototaxis. SRI exists in the membrane as a molecular complex with a signal transducer protein. Excitation of its thermally stable form, SRI(587), generates a long-lived photointermediate of its photocycle, S(373), and an attractant phototactic response. S(373) decays thermally in a few seconds into SRI(587.) However, when S(373) is excited by UV-blue light, it photoconverts into SRI(587) in less than a second, generating a repellent phototactic response. Only one intermediate of this back-photoreaction, S(b)(510), is known. We studied the back-photoreaction in both native SRI and its transducer free form fSRI by measuring laser flash induced absorption changes of S(373) photoproducts from 100 ns to 1 s in the 350-750 nm range. Using global exponential fitting, we determined the spectra and kinetics of the photointermediates. S(373) and fS(373) when pumped with 355 nm laser light generate in less than 100 ns two intermediate species: a previously undetected species that absorbs maximally at about 410 nm, S(b)(410), and the previously described S(b)(510). These two intermediates appear to be in a rapid equilibrium, which probably entails protonation change of the Schiff base chromophore. At pH 6 this system relaxes to SRI(587) via another intermediate absorbing maximally around 550 nm, which thermally decays back to the ground state. The same intermediates are seen in the presence and absence of transducer; however, the kinetics are affected by binding of the transducer.

Structural constraints imposed by a non-native disulfide cause reversible changes in rhodopsin photointermediate kinetics

Suspensions of bovine rhodopsin in 2% lauryl maltoside detergent were treated with Cu(phen)(3)(2+) to form a disulfide bridge between cysteines 140 and 222 which occur naturally in the bovine rhodopsin sequence. Absorption difference spectra were collected after excitation with a pulse of 477 nm light on the time scale from 1 micros to 690 ms, and the results were analyzed using global exponential fitting. Only two exponentials could be fit to data from the Cu(phen)(3)(2+)-treated rhodopsin, while three exponentials were needed to fit data either from untreated rhodopsin or from Cu(phen)(3)(2+)-oxidized rhodopsin after further dithiothreitol reduction. Dithiothreitol treatment of rhodopsin which had not been previously oxidized with Cu(phen)(3)(2+) had no effect on the observed kinetics. Since the 140-222 disulfide has previously been shown to block transducin activation, its effects on rhodopsin activation are of considerable interest. Cu(phen)(3)(2+) treatment favors formation of the meta I(380) intermediate relative to meta I(480) and slows formation of meta II from meta I(380). This suggests that the protein change involved in meta I(380) formation is similar to the structural constraint introduced by the 140-222 disulfide. These results show that formation of disulfides in rhodopsin has potential as a tool for discriminating between the three isochromic, 380 nm absorbing intermediates involved in rhodopsin activation and for gaining insight into how their structures differ.

pH dependence of photolysis intermediates in the photoactivation of rhodopsin mutant E113Q

Glutamic acid at position 113 in bovine rhodopsin ionizes to form the counterion to the protonated Schiff base (PSB), which links the 11-cis-retinylidene chromophore to opsin. Photoactivation of rhodopsin requires both Schiff base deprotonation and neutralization of Glu-113. To better understand the role of electrostatic interactions in receptor photoactivation, absorbance difference spectra were collected at time delays from 30 ns to 690 ms after photolysis of rhodopsin mutant E113Q solubilized in dodecyl maltoside at different pH values at 20 degrees C. The PSB form (pH 5. 5, lambda(max) = 496 nm) and the unprotonated Schiff base form (pH 8. 2, lambda(max) = 384 nm) of E113Q rhodopsin were excited using 477 nm or 355 nm light, respectively. Early photointermediates of both forms of E113Q were qualitatively similar to those of wild-type rhodopsin. In particular, early photoproducts with spectral shifts to longer wavelengths analogous to wild-type bathorhodopsin were seen. In the case of the basic form of E113Q, the absorption maximum of this intermediate was at 408 nm. These results suggest that steric interaction between the retinylidene chromophore and opsin, rather than charge separation, plays the dominant role in energy storage in bathorhodopsin. After lumirhodopsin, instead of deprotonating to form metarhodopsin I(380) on the submillisecond time scale as is the case for wild type, the acidic form of E113Q produced metarhodopsin I(480), which decayed very slowly (exponential lifetime = 12 ms). These results show that Glu-113 must be present for efficient deprotonation of the Schiff base and rapid visual transduction in vertebrate visual pigments.