Redox potentials of the oriented film of the wild-type,the E194Q-, E204Q- and D96N-mutated bacteriorhodopsins

The redox potentials of the oriented films of the wild-type, the E194Q-, E204Q- and D96N-mutated bacteriorhodopsins (bR), prepared by adsorbing purple membrane (PM) sheets or its mutant on a Pt electrode, have been examined. The redox potentials (V) of the wild-type bR were -470 mV for the 13-cis configuration of the retinal Shiff base in bR and -757 mV for the all-trans configuration in H(2)O, and -433 mV for the 13-cis configuration and -742 mV for the all-trans configuration in D(2)O. The solvent isotope effect (DeltaV=V(D(2)O)-V(H(2)O)), which shifts the redox potential to a higher value, originates from the cooperative rearrangements of the extensively hydrogen-bonded water molecules around the protonated C=N part in the retinal Schiff base. The redox potential of bR was much higher for the 13-cis configuration than that for the all-trans configuration. The redox potentials for the E194Q mutant in the extracellular region were -507 mV for the 13-cis configuration and -788 mV for the all-trans configuration; and for the E204Q mutant they were -491 mV for the 13-cis configuration and -769 mV for the all-trans configuration. Replacement of the Glu(194) or Glu(204) residues by Gln weakened the electron withdrawing interaction to the protonated C=N bond in the retinal Schiff base. The E204 residue is less linked with the hydrogen-bonded network of the proton release pathway compared with E194. The redox potentials of the D96N mutant in the cytoplasmic region were -471 mV for the 13-cis configuration and -760 mV for the all-trans configuration which were virtually the same as those of the wild-type bR, indicating that the D to N point mutation of the 96 residue had no influence on the interaction between the D96 residue and the C=N part in the Schiff base under the light-adapted condition. The results suggest that the redox potential of bR is closely correlated to the hydrogen-bonded network spanning from the retinal Schiff base to the extracellular surface of bR in the proton transfer pathway.     

Increasing protein stability by altering long-range coulombic interactions.

It is difficult to increase protein stability by adding hydrogen bonds or burying nonpolar surface. The results described here show that reversing the charge on a side chain on the surface of a protein is a useful way of increasing stability. Ribonuclease T1 is an acidic protein with a pI approximately 3.5 and a net charge of approximately -6 at pH 7. The side chain of Asp49 is hyperexposed, not hydrogen bonded, and 8 A from the nearest charged group. The stability of Asp49Ala is 0.5 kcal/mol greater than wild-type at pH 7 and 0.4 kcal/mol less at pH 2.5. The stability of Asp49His is 1.1 kcal/mol greater than wild-type at pH 6, where the histidine 49 side chain (pKa = 7.2) is positively charged. Similar results were obtained with ribonuclease Sa where Asp25Lys is 0.9 kcal/mol and Glu74Lys is 1.1 kcal/mol more stable than the wild-type enzyme. These results suggest that protein stability can be increased by improving the coulombic interactions among charged groups on the protein surface. In addition, the stability of RNase T1 decreases as more hydrophobic aromatic residues are substituted for Ala49, indicating a reverse hydrophobic effect.     

Effective light-induced hydroxylamine reactions occur with C13 = C14 nonisomerizable bacteriorhodopsin pigments.

The light-driven proton pump bacteriorhodopsin (bR) undergoes a bleaching reaction with hydroxylamine in the dark, which is markedly catalyzed by light. The reaction involves cleavage of the (protonated) Schiff base bond, which links the retinyl chromophore to the protein. The catalytic light effect is currently attributed to the conformational changes associated with the photocycle of all-trans bR, which is responsible for its proton pump mechanism and is initiated by the all-trans --> 13-cis isomerization. This hypothesis is now being tested in a series of experiments, at various temperatures, using three artificial bR molecules in which the essential C13==C14 bond is locked by a rigid ring structure into an all-trans or 13-cis configuration. In all three cases we observe an enhancement of the reaction by light despite the fact that, because of locking of the C13==C14 bond, these molecules do not exhibit a photocycle, or any proton-pump activity. An analysis of the rate parameters excludes the possibility that the light-catalyzed reaction takes place during the approximately 20-ps excited state lifetimes of the locked pigments. It is concluded that the reaction is associated with a relatively long-lived (micros-ms) light-induced conformational change that is not reflected by changes in the optical spectrum of the retinyl chromophore. It is plausible that analogous changes (coupled to those of the photocycle) are also operative in the cases of native bR and visual pigments. These conclusions are discussed in view of the light-induced conformational changes recently detected in native and artificial bR with an atomic force sensor.     

B3LYP/6-311++G** study of alpha- and beta-D-glucopyranose and 1,5-anhydro-D-glucitol: 4C1 and 1C4 chairs, (3,O)B and B(3,O) boats, and skew-boat conformations

Geometry optimization, at the B3LYP/6-311++G** level of theory, was carried out on 4C1 and 1C4 chairs, (3,O)B and B(3,O) boats, and skew-boat conformations of alpha- and beta-D-glucopyranose. Similar calculations on 1,5-anhydro-D-glucitol allowed examination of the effect of removal of the 1-hydroxy group on the energy preference of the hydroxymethyl rotamers. Stable minimum energy boat conformers of glucose were found, as were stable skew boats, all having energies ranging from approximately 4-15 kcal/mol above the global energy 4C1 chair conformation. The 1C4 chair electronic energies were approximately 5-10 kcal/mol higher than the 4C1 chair, with the 1C4 alpha-anomers being lower in energy than the beta-anomers. Zero-point energy, enthalpy, entropy, and relative Gibbs free energies are reported at the harmonic level of theory. The alpha-anomer 4C1 chair conformations were found to be approximately 1 kcal/mol lower in electronic energy than the beta-anomers. The hydroxymethyl gt conformation was of lowest electronic energy for both the alpha- and beta-anomers. The glucose alpha/beta anomer ratio calculated from the relative free energies is 63/37%. From a numerical Hessian calculation, the tg conformations were found to be approximately 0.4-0.7 kcal/mol higher in relative free energy than the gg or gt conformers. Transition-state barriers to rotation about the C-5-C-6 bond were calculated for each glucose anomer with resulting barriers to rotation of approximately 3.7-5.8 kcal/mol. No energy barrier was found for the path between the alpha-gt and alpha-gg B(3,O) boat forms and the equivalent 4C1 chair conformations. The alpha-tg conformation has an energy minimum in the 1S3 twist form. Other boat and skew-boat forms are described. The beta-anomer boats retained their starting conformations, with the exception of the beta-tg-(3,O)B boat that moved to a skew form upon optimization.     

Combined use of molecular dynamics simulations and NMR to explore peptide bond isomerization and multiple intramolecular hydrogen-bonding possibilities in a cyclic pentapeptide, cyclo(Gly-Pro-D-Phe-Gly-Val).

The conformational behavior of a model cyclic pentapeptide--cyclo(Gly-L-Pro-D-Phe-Gly-L-Val)--has been explored through the combined use of in vacuo molecular dynamics simulations and a range of nmr experiments (preceding paper). The molecular dynamics analysis suggests that, despite the conformational constraints imposed by formation of the pentapeptide cycle, this pentapeptide undergoes conformational transitions between various hydrogen-bonded conformations, characterized by low energy barriers. An inverse gamma turn with Pro in position i + 1 and a gamma turn with D-Phe in position i + 1 are two alternatives occurring frequently. Like other DLDDL cyclic pentapeptides, cyclo(Gly-Pro-D-Phe-Gly-Val) is also stabilized by an inverse gamma-turn structure with the beta-branched Val residue in position i + 1, and this hydrogen bond is retained in the different conformational families. The gamma-turn around D-Phe3 and the inverse gamma turn around Val5 are consistent with the nmr observations. 3JNH-CH alpha coupling constants of the all-trans forms were calculated from one of the molecular dynamics trajectories and are comparable to nmr experimental data, suggesting that the conformational states visited during the simulation are representative of the conformational distribution in solution. In addition to the equilibrium among various hydrogen-bonded all-trans conformers, the observation in nmr spectra of two sets of resonances for all peptide protons indicated a slow conformational interconversion of the Gly-Pro peptide bond between trans and cis isomers. The activation energy between these two conformers was determined experimentally by magnetization transfer and was calculated by high temperature constrained molecular dynamics simulation. Both methods yield a free energy of activation of ca. 20 kcal/mol. Furthermore, the free energy of activation is dependent on the direction of rotation of the Gly-Pro peptide bond.     

Contributions of long-range electrostatic interactions to 4-chlorobenzoyl-CoA dehalogenase catalysis: a combined theoretical and experimental study

It is well established that electrostatic interactions play a vital role in enzyme catalysis. In this work, we report theory-guided mutation experiments that identified strong electrostatic contributions of a remote residue, namely, Glu232 located on the adjacent subunit, to 4-chlorobenzoyl-CoA dehalogenase catalysis. The Glu232Asp mutant was found to bind the substrate analogue 4-methylbenzoyl-CoA more tightly than does the wild-type dehalogenase. In contrast, the kcat for 4-chlorobenzoyl-CoA conversion to product was reduced 10000-fold in the mutant. UV difference spectra measured for the respective enzyme-ligand complexes revealed an approximately 3-fold shift in the equilibrium of the two active site conformers away from that inducing strong pi-electron polarization in the ligand benzoyl ring. Increased substrate binding, decreased ring polarization, and decreased catalytic efficiency indicated that the repositioning of the point charge in the Glu232Asp mutant might affect the orientation of the Asp145 carboxylate with respect to the substrate aromatic ring. The time course for formation and reaction of the arylated enzyme intermediate during a single turnover was measured for wild-type and Glu232Asp mutant dehalogenases. The accumulation of arylated enzyme in the wild-type dehalogenase was not observed in the mutant. This indicates that the reduced turnover rate in the mutant is the result of a slow arylation of Asp145, owing to decreased efficiency in substrate nucleophilic attack by Asp145. To rationalize the experimental observations, a theoretical model is proposed, which computes the potential of mean force for the nucleophilic aromatic substitution step using a hybrid quantum mechanical/molecular mechanical method. To this end, the removal or reorientation of the side chain charge of residue 232, modeled respectively by the Glu232Gln and Glu232Asp mutants, is shown to increase the rate-limiting energy barrier. The calculated 23.1 kcal/mol free energy barrier for formation of the Meisenheimer intermediate in the Glu232Asp mutant represents an increase of 6 kcal/mol relative to that of the wild-type enzyme, consistent with the 5.6 kcal/mol increase calculated from the difference in experimentally determined rate constants. On the basis of the combination of the experimental and theoretical evidence, we hypothesize that the Glu232(B) residue contributes to catalysis by providing an electrostatic force that acts on the Asp145 nucleophile.     

Molecular dynamics study of the 13-cis form (bR548) of bacteriorhodopsin and its photocycle.

The structure and the photocycle of bacteriorhodopsin (bR) containing 13-cis,15-syn retinal, so-called bR548, has been studied by means of molecular dynamics simulations performed on the complete protein. The simulated structure of bR548 was obtained through isomerization of in situ retinal around both its C13-C14 and its C15-N bond starting from the simulated structure of bR568 described previously, containing all-trans,15-anti retinal. After a 50-ps equilibration, the resulting structure of bR548 was examined by replacing retinal by analogues with modified beta-ionone rings and comparing with respective observations. The photocycle of bR548 was simulated by inducing a rapid 13-cis,15-anti-->all-trans,15-syn isomerization through a 1-ps application of a potential that destabilizes the 13-cis isomer. The simulation resulted in structures consistent with the J, K, and L intermediates observed in the photocycle of bR548. The results offer an explanation of why an unprotonated retinal Schiff base intermediate, i.e., an M state, is not formed in the bR548 photocycle. The Schiff base nitrogen after photoisomerization of bR548 points to the intracellular rather than to the extracellular site. The simulations suggest also that leakage from the bR548 to the bR568 cycle arises due to an initial 13-cis,15-anti-->all-trans,15-anti photoisomerization.     

The severity of osteogenesis imperfecta: a comparison to the relative free energy differences of collagen model peptides

Molecular dynamics simulations were carried out to calculate free energy differences between the folded and unfolded states of wild type and mutant collagen model peptides. The calculated stability of the collagen models was compared with the severity of osteogenesis imperfecta. Free energy differences of Gly → Xaa (Xaa: Ser, Cys, Glu, and Asp) mutations between the wild type and the mutants at position 15 of the model peptide were 3.8, 4.2, 5.6, and 8.8 kcal/mol, respectively. The corresponding free energy differences of a second Gly mutation at the same position in different chains were, on average, 1.3, 1.5, 2.9, and 5.4 kcal/mol, respectively. Free energy simulations were also performed to estimate the relative stability between an oxidized form and a reduced form of the mutants containing two Cys residues, which indicated that the mutant of the collagen-like peptide containing an intramolecular disulfide bond was more stable than the mutant containing one Cys residue but less stable than the wild type. The calculated free energy differences between an oxidized and a reduced form of the mutants containing two Cys residues are 0.8 and 2.6 kcal/mol for the disulfide bonds between Chains A and B and between Chains A and C, respectively.     

Femtosecond and picosecond fluorescence of native bacteriorhodopsin and a nonisomerizing analog

The spectrally and temporally resolved fluorescence properties of native bacteriorhodopsin (bR) and bR reconstituted with a nonisomerizing analog of the retinal Schiff base (bR5.12) are examined. The first attempt to experimentally monitor the excited state relaxation processes in both type of pigments using ultrafast fluorescence spectroscopy is reported. The fluorescence is emitted from retinal molecules in an all-trans configuration. Substantial energy relaxation involves very fast intramolecular and intermolecular vibrational modes and these are shown to occur on a time scale faster than isomerization. The possible contribution of dielectric interaction between the retinal Schiff base and the protein environment for the excited state energy relaxation is discussed.     

The effect of protein conformation change from alpha(II) to alpha(I) on the bacteriorhodopsin photocycle

The bacteriorhodopsin (bR) photocycle was followed by use of time-resolved Fourier-transform infrared (FTIR) spectroscopy as a function of temperature (15-85 degrees C) as the alpha(II) --> alpha(I) conformational transition occurs. The photocycle rate increases with increasing temperature, but its efficiency is found to be drastically reduced as the transition takes place. A large shift is observed in the all-trans left arrow over right arrow 13-cis equilibrium due to the increased stability of the 13-cis isomer in alpha(I) form. This, together with the increase in the rate of dark adaptation as the temperature increases, leads to a large increase in the 13-cis isomer concentration in bR in the alpha(I) form. The fact that 13-cis retinal has a much-reduced absorption cross-section and its inability to pump protons leads to an observed large reduction in the concentration of the observed photocycle intermediates, as well as the proton gradient at a given light intensity. These results suggest that nature might have selected the alpha(II) rather than the alpha(I) form as the helical conformation in bR to stabilize the all-trans retinal isomer that is a better light absorber and is capable of pumping protons.     

Positional preference of proline in alpha-helices.

Conformational free energy calculations have been carried out for proline-containing alanine-based pentadecapeptides with the sequence Ac-(Ala)n-Pro-(Ala)m-NHMe, where n + m = 14, to figure out the positional preference of proline in alpha-helices. The relative free energy of each peptide was calculated by subtracting the free energy of the extended conformation from that of the alpha-helical one, which is used here as a measure of preference. The highest propensity is found for the peptide with proline at the N-terminus (i.e., Ncap + 1 position), and the next propensities are found at Ncap, N' (Ncap - 1), and C' (Ccap + 1) positions. These computed results are reasonably consistent with the positional propensities estimated from X-ray structures of proteins. The breaking in hydrogen bonds around proline is found to play a role in destabilizing alpha-helical conformations, which, however, provides the favored hydration of the corresponding N-H and C=O groups. The highest preference of proline at the beginning of alpha-helix appears to be due to the favored electrostatic and nonbonded energies between two residues preceding proline and the intrinsic stability of alpha-helical conformation of the proline residue itself as well as no disturbance in hydrogen bonds of alpha-helix by proline. The average free energy change for the substitution of Ala by Pro in a alpha-helix is computed to be 4.6 kcal/mol, which is in good agreement with the experimental value of approximately 4 kcal/mol estimated for an oligopeptide dimer and proteins of barnase and T4 lysozyme.     

Dissection of the energetic coupling across the Src SH2 domain-tyrosyl phosphopeptide interface

Src Homology (SH2) domains play critical roles in signaling pathways by binding to phosphotyrosine (pTyr)-containing sequences, thereby recruiting SH2 domain-containing proteins to tyrosine-phosphorylated sites on receptor molecules. Investigations of the peptide binding specificity of the SH2 domain of the Src kinase (Src SH2 domain) have defined the EEI motif C-terminal to the phosphotyrosine as the preferential binding sequence. A subsequent study that probed the importance of eight specificity-determining residues of the Src SH2 domain found two residues which when mutated to Ala had significant effects on binding: Tyr beta D5 and Lys beta D3. The mutation of Lys beta D3 to Ala was particularly intriguing, since a Glu to Ala mutation at the first (+1) position of the EEI motif (the residue interacting with Lys beta D3) did not significantly affect binding. Hence, the interaction between Lys beta D3 and +1 Glu is energetically coupled. This study is focused on the dissection of the energetic coupling observed across the SH2 domain-phosphopeptide interface at and around the +1 position of the peptide. It was found that three residues of the SH2 domain, Lys beta D3, Asp beta C8 and AspCD2 (altogether forming the so-called +1 binding region) contribute to the selection of Glu at the +1 position of the ligand. A double (Asp beta C8Ala, AspCD2Ala) mutant does not exhibit energetic coupling between Lys beta D3 and +1 Glu, and binds to the pYEEI sequence 0.3 kcal/mol tighter than the wild-type Src SH2 domain. These results suggest that Lys beta D3 in the double mutant is now free to interact with the +1 Glu and that the role of Lys beta D3 in the wild-type is to neutralize the acidic patch formed by Asp beta C8 and AspCD2 rather than specifically select for a Glu at the +1 position as it had been hypothesized previously. A triple mutant (Lys beta D3Ala, Asp beta C8Ala, AspCD2Ala) has reduced binding affinity compared to the double (Asp beta C8Ala, AspCD2Ala) mutant, yet binds the pYEEI peptide as well as the wild-type Src SH2 domain. The structural basis for such high affinity interaction was investigated crystallographically by determining the structure of the triple (Lys beta D3Ala, Asp beta C8Ala, AspCD2Ala) mutant bound to the octapeptide PQpYEEIPI (where pY indicates a phosphotyrosine). This structure reveals for the first time contacts between the SH2 domain and the -1 and -2 positions of the peptide (i.e. the two residues N-terminal to pY). Thus, unexpectedly, mutations in the +1 binding region affect binding of other regions of the peptide. Such additional contacts may account for the high affinity interaction of the triple mutant for the pYEEI-containing peptide.     

The conserved, buried aspartic acid in oxidized Escherichia coli thioredoxin has a pKa of 7.5. Its titration produces a related shift in global stability.

Aspartic acid 26 in Escherichia coli thioredoxin is located at the bottom of a hydrophobic cavity, near the redox-active disulfide of the active site. Asp 26 is embedded in the protein except for part of the surface of one carboxyl oxygen. The high degree of evolutionary conversion of Asp 26 suggests that it plays a critical role in thioredoxin function. We have determined the pKa of Asp 26 by a novel electrophoretic method based on the relative electrophoretic mobilities of wild-type thioredoxin and of D26A thioredoxin (with Asp 26 replaced by alanine). The pKa of Asp 26 determined by this technique is 7.5, more than 3 units above the pKa of a solvated carboxyl side chain. The titration of Asp 26 is thermodynamically linked to the stability of thioredoxin. As expected if thioredoxin stability depends on the ionization state of Asp 26, delta Go WT, the free energy of the cooperative denaturation reaction of wild-type thioredoxin by guanidine hydrochloride, varies with pH in a sigmoidal fashion in the vicinity of pH 7.5. Over the same pH range, the free energy for D26A folding, delta Go D26A, is pH independent and D26A is highly stabilized compared to wild type. From the thermodynamic cycle describing the linkage of Asp 26 titration to thioredoxin stability, the difference in free energy between wild-type thioredoxin with protonated Asp 26 and wild-type thioredoxin with deprotonated Asp 26, delta delta Go (COOH----COO-), is calculated to be 4.9 kcal/mol.(ABSTRACT TRUNCATED AT 250 WORDS)     

The coordination of the isomerization of a conserved non-prolyl cis peptide bond with the rate-limiting steps in the folding of dihydrofolate reductase

The propensity for peptide bonds to adopt the trans configuration in native and unfolded proteins, and the relatively slow rates of cis-trans isomerization reactions, imply that the formation of cis peptide bonds in native conformations are likely to limit folding reactions. The role of the conserved cis Gly95-Gly96 peptide bond in dihydrofolate reductase (DHFR) from Escherichia coli was examined by replacing Gly95 with alanine. The introduction of a beta carbon at position 95 is expected to increase the propensity for the trans isomer and perturb the isomerization reaction required to reach the native conformation. Although G95A DHFR is 1.30 kcal mol(-1) less stable than the wild-type protein, it adopts a well-folded structure that can be chemically denatured in a cooperative fashion. The mutant protein also retains the complex refolding kinetic pattern attributed to a parallel-channel mechanism in wild-type DHFR. The spectroscopic response upon refolding monitored by Trp fluorescence and the absence of a Trp/Trp exciton coupling apparent in the far-UV CD spectrum of the wild-type protein, however, indicated that the tertiary structure of the folded state for G95A DHFR is altered. The addition of methotrexate (MTX), a tight-binding inhibitor, to folded G95A DHFR restored the exciton coupling and the fluorescence properties through five slow kinetic events whose relaxation times are independent of the ligand and the denaturant concentrations. The results were interpreted to mean that MTX-binding drives the formation of the cis isomer of the peptide bond between Ala95 and Gly96 in five compact and stable but not wild-type-like conformations that contain the trans isomer. Folding studies in the presence of MTX for both wild-type and G95A DHFR support the notion that the cis peptide bond between Gly95 and Gly96 in the wild-type protein forms during four parallel rate-limiting steps, which are primarily controlled by folding reactions, and lead directly to a set of native, or native-like, conformers. The isomerization of the cis peptide bond is not a source of the parallel channels that characterize the complex folding mechanism for DHFR.     

Catalysis of the retinal subpicosecond photoisomerization process in acid purple bacteriorhodopsin and some bacteriorhodopsin mutants by chloride ions.

The dynamics and the spectra of the excited state of the retinal in bacteriorhodopsin (bR) and its K-intermediate at pH 0 was compared with that of bR and halorhodopsin at pH 6.5. The quantum yield of photoisomerization in acid purple bR was estimated to be at least 0.5. The change of pH from 6.5 to 2 causes a shift of the absorption maximum from 568 to 600 nm (acid blue bR) and decreases the rate of photoisomerization. A further decrease in pH from 2 to 0 shifts the absorption maximum back to 575 nm when HCl is used (acid purple bR). We found that the rate of photoisomerization increases when the pH decreases from 2 to 0. The effect of chloride anions on the dynamics of the retinal photoisomerization of acid bR (pH 2 and 0) and some mutants (D85N, D212N, and R82Q) was also studied. The addition of 1 M HCl (to make acid purple bR, pH 0) or 1 M NaCl to acid blue bR (pH 2) was found to catalyze the rate of the retinal photoisomerization process. Similarly, the addition of 1 M NaCl to the solution of some bR mutants that have a reduced rate of retinal photoisomerization (D85N, D212N, and R82Q) was found to catalyze the rate of their retinal photoisomerization process up to the value observed in wild-type bR. These results are explained by proposing that the bound Cl- compensates for the loss of the negative charges of the COO- groups of Asp85 and/or Asp212 either by neutralization at low pH or by residue replacement in D85N and D212N mutants.     

Calorimetric examination of high-affinity Src SH2 domain-tyrosyl phosphopeptide binding: dissection of the phosphopeptide sequence specificity and coupling energetics

SH2 domains are protein modules which interact with specific tyrosine phosphorylated sequences in target proteins. The SH2 domain of the Src kinase binds with high affinity to a tyrosine phosphorylated peptide containing the amino acids Glu, Glu, and Ile (EEI) at the positions +1, +2, and +3 C-terminal to the phosphotyrosine, respectively. To investigate the degree of selectivity of the Src SH2 domain for each amino acid of the EEI motif, the binding thermodynamics of a panel of substitutions at the +1 (Gln, Asp, Ala, Gly), +2 (Gln, Asp, Ala, Gly), and +3 (Leu, Val, Ala, Gly) positions were examined using titration microcalorimetry. It was revealed that the Src SH2 domain is insensitive (DeltaDeltaG degrees 相似文献   

Effect of 13-cis violaxanthin on organization of light harvesting complex II in monomolecular layers

Lutein, neoxanthin and violaxanthin are the main xanthophyll pigment constituents of the largest light-harvesting pigment-protein complex of photosystem II (LHCII). High performance liquid chromatography analysis revealed photoisomerization of LHCII-bound violaxanthin from the conformation all-trans to the conformation 13-cis and 9-cis. Maximally, the conversion of 15% of all-trans violaxanthin to a cis form could be achieved owing to the light-driven reactions. The reactions were dark-reversible. The all-trans to cis isomerization was found to be driven by blue light, absorbed by chlorophylls and carotenoids, as well as by red light, absorbed exclusively by chlorophyll pigments. This suggests that the photoisomerization is a carotenoid triplet-sensitized reaction. The monomolecular layer technique was applied to study the effect of the 13-cis conformer of violaxanthin and its de-epoxidized form, zeaxanthin, on the organization of LHCII as compared to the all-trans stereoisomers. The specific molecular areas of LHCII in the two-component system composed of protein and exogenous 13-cis violaxanthin or 13-cis zeaxanthin show overadditivity, which is an indication of the xanthophyll-induced disassembly of the aggregated forms of the protein. Such an effect was not observed in the monomolecular layers of LHCII containing all-trans conformers of violaxanthin and zeaxanthin. 77 K chlorophyll a fluorescence emission spectra recorded from the Langmuir-Blodgett (L-B) films deposited to quartz from monomolecular layers formed with LHCII and LHCII in the two-component systems with all-trans and 13-cis isomers of violaxanthin and zeaxanthin revealed opposite effects of both conformers on the aggregation of the protein. The cis isomers of both xanthophylls were found to decrease the aggregation level of LHCII and the all-trans isomers increased the aggregation level. The calculated efficiency of excitation energy transfer to chlorophyll a from violaxanthin assumed to remain in two steric conformations was analyzed on the basis of the chlorophyll a fluorescence excitation spectra and the mean orientation of violaxanthin molecules in LHCII (71 degrees with respect to the normal to the membrane), determined recently in the linear dichroism experiments [Gruszecki et al., Biochim. Biophys. Acta 1412 (1999) 173-183]. The calculated efficiency of excitation energy transfer from the violaxanthin pool assumed to remain in conformation all-trans was found to be almost independent on the orientation angle within a variability range. In contrast the calculated efficiency of energy transfer from the form cis was found to be strongly dependent on the orientation and varied between 1.0 (at 67.48 degrees ) and 0 (at 70.89 degrees ). This is consistent with two essentially different, possible functions of the cis forms of violaxanthin: as a highly efficient excitation donor (and possibly energy transmitter between other chromophores) or purely as a LHCII structure modifier.     

Weakened coupling of conserved arginine to the proteorhodopsin chromophore and its counterion implies structural differences from bacteriorhodopsin

In wild-type proteorhodopsin (pR), titration of the chromophore's counterion Asp(97) occurs with a pK(a) of 8.2+/-0.1. R94C mutation reduces this slightly to 7.0+/-0.2, irrespective of treatment with ethylguanidinium. This contrasts with the homologous archaeal protein bacteriorhodopsin (bR), where R82C mutation was previously shown to elevate the pK(a) of Asp(85) by approximately 5 units, while reconstitution with ethylguanidinium restores it nearly to the wild-type value of 2.5. We conclude there is much weaker electrostatic coupling between Arg(94) and Asp(97) in the unphotolyzed state of pR, in comparison to Arg(82) and Asp(85) in bR. Therefore, while fast light-driven H(+) release may depend on these two residues in pR as in bR, no tightly conserved pre-photolysis configuration of them is required.     

Conformational change in bacterio-opsin on binding to retinal.

The detailed mechanism of retinal binding to bacterio-opsin is important to understanding retinal pigment formation as well as to the process of membrane protein folding. We have measured the temperature dependence of bacteriorhodopsin formation from bacterio-opsin and all-trans retinal. An Arrhenius plot of the apparent second-order rate constants gives an activation energy of 11.6 +/- 0.7 kcal/mol and an activation entropy of -4 +/- 2 cal/mol deg. Comparison of the activation entropy to model compound reactions suggests that chromophore formation in bacteriorhodopsin involves a substantial protein conformational change. Cleavage of the polypeptide chain between residues 71 and 72 has little effect on the activation energy or entropy, indicating that the connecting loop between helices B and C is not involved in this conformational change.     

Asp79 makes a large, unfavorable contribution to the stability of RNase Sa

The two most buried carboxyl groups in ribonuclease Sa (RNase Sa) are Asp33 (99% buried; pK 2.4) and Asp79 (85% buried; pK 7.4). Above these pK values, the stability of the D33A variant is 6kcal/mol less than wild-type RNase Sa, and the stability of the D79A variant is 3.3kcal/mol greater than wild-type RNase Sa. The key structural difference between the carboxyl groups is that Asp33 forms three intramolecular hydrogen bonds, and Asp79 forms no intramolecular hydrogen bond. Here, we focus on Asp79 and describe studies of 11 Asp79 variants. Most of the variants were at least 2kcal/mol more stable than wild-type RNase Sa, and the most interesting was D79F. At pH 3, below the pK of Asp79, RNase Sa is 0.3kcal/mol more stable than the D79F variant. At pH 8.5, above the pK of Asp79, RNase Sa is 3.7kcal/mol less stable than the D79F variant. The unfavorable contribution of Asp79 to the stability appears to result from the Born self-energy of burying the charge and, more importantly, from unfavorable charge-charge interactions. To counteract the effect of the negative charge on Asp79, we prepared the Q94K variant and the crystal structure showed that the amino group of the Lys formed a hydrogen-bonded ion pair (distance, 2.71A; angle, 100 degrees ) with the carboxyl group of Asp79. The stability of the Q94K variant was about the same as the wild-type at pH 3, where Asp79 is uncharged, but 1kcal/mol greater than that of wild-type RNase Sa at pH 8.5, where Asp79 is charged. Differences in hydrophobicity, steric strain, Born self-energy, and electrostatic interactions all appear to contribute to the range of stabilities observed in the variants. When it is possible, replacing buried, non-hydrogen bonded, ionizable side-chains with non-polar side-chains is an excellent means of increasing protein stability.