Coupling of the reisomerization of the retinal, proton uptake, and reprotonation of Asp-96 in the N photointermediate of bacteriorhodopsin

In the N to O reaction of the bacteriorhodopsin photocycle, Asp-96 is protonated from the cytoplasmic surface, and coupled to this, the retinal isomerizes from 13-cis,15-anti back to the initial all-trans configuration. To dissect the two steps, and to better understand how and why they occur, we describe the properties of two groups of site-specific mutants in which the N intermediate has greatly increased lifetime. In the first group, with the mutations near the retinal, an unusual N state is produced in which the retinal is 13-cis,15-anti but Asp-96 has a protonated carboxyl group. The apparent pK(a) for the protonation is 7.5, as in the wild-type. It is likely that here the interference with N decay is the result of steric conflict of side-chains with the retinal or with the side-chain of Lys-216 connected to the retinal, which delays the reisomerization after protonation of Asp-96. In the second group, with the mutations located near Asp-96 or between Asp-96 and the cytoplasmic surface, reprotonation of Asp-96 is strongly perturbed. The reisomerization of the retinal occurs only after recovery from a long-living protein conformation in which reprotonation of Asp-96 is either entirely blocked or blocked at low pH.     

Secondary and tertiary structure of bacteriorhodopsin in the SDS denatured state

We characterized the structure of partially unfolded bacteriorhodopsin in sodium dodecyl sulfate (SDS) micelles and compared it with its in vitro refolded structure after reconstitution with dimyristoylphosphatidylcholine/3-[(3-cholamidopropyl)dimethylammonio]-1-propanesulfonate (DMPC/CHAPS). Intrahelical and interhelical distances were mapped in the protein using strategically located spin-label pairs at helical ends, assayed by pulsed electron paramagnetic resonance spectroscopy (double electron-electron spin resonance, DEER). We find that in SDS the intrahelical end-to-end distances exhibit broad distributions, suggesting a heterogeneous ensemble of conformations with differing secondary structures. Nevertheless, a majority of the denatured population retains end-to-end distances similar to those in the native state. In contrast, the observed greatly increased interhelical distances, in addition to their very broad distributions, suggest that in the SDS micelles very little of the native tertiary structure remains.     

Structure Changes upon Deprotonation of the Proton Release Group in the Bacteriorhodopsin Photocycle

In the photocycle of bacteriorhodopsin at pH 7, a proton is ejected to the extracellular medium during the protonation of Asp-85 upon formation of the M intermediate. The group that releases the ejected proton does not become reprotonated until the prephotolysis state is restored from the N and O intermediates. In contrast, at acidic pH, this proton release group remains protonated to the end of the cycle. Time-resolved Fourier transform infrared measurements obtained at pH 5 and 7 were fitted to obtain spectra of kinetic intermediates, from which the spectra of M and N/O versus unphotolyzed state were calculated. Vibrational features that appear in both M and N/O spectra at pH 7, but not at pH 5, are attributable to deprotonation from the proton release group and resulting structural alterations. Our results agree with the earlier conclusion that this group is a protonated internal water cluster, and provide a stronger experimental basis for this assignment. A decrease in local polarity at the N-C bond of the side chain of Lys-216 resulting from deprotonation of this water cluster may be responsible for the increase in the proton affinity of Asp-85 through M and N/O, which is crucial for maintaining the directionality of proton pumping.     

Molecular dynamics simulation of the unfolding of individual bacteriorhodopsin helices in sodium dodecyl sulfate micelles

We report molecular dynamics simulations of the trends in the changes in secondary structure of the seven individual helices of bacteriorhodopsin when inserted into sodium dodecyl sulfate (SDS) micelles, and their dependence on the amino acid sequence. The results indicate that the partitioning of the helices in the micelles and their stability are dependent on the hydrophobicity of the transmembrane segments. Helices A, B, and E are stable and retain their initial secondary structure throughout the 100 ns simulation time. In contrast, helices C, D, F, and G show structural perturbations within the first 10 ns. The instabilities are localized near charged residues within the transmembrane segments. The overall structural instability of the helix is correlated with its partitioning to the surface of the micelle and its interaction with polar groups there. The in silico experiments were performed to complement the in vitro experiments that examined the partial denaturation of bacteriorhodopsin in SDS described in the preceding article (DOI 10.1021/bi201769z ). The simulations are consistent with the trends revealed by the experimental results but strongly underestimate the extent of helix to extended coil transformation. The reason may be either that the sampling time was not sufficiently long or, more interestingly, that interhelix residue interactions play a role in the unfolding of the helices.     

miR-15b and miR-16 regulate TNF mediated hepatocyte apoptosis via BCL2 in acute liver failure

Acute liver failure (ALF) still has an unacceptable high mortality rate, despite substantial improvements with multidisciplinary care. The precise underlying mechanism of ALF remains to be explored. It has been reported that microRNAs (miRNAs) are novel regulators in a number of liver diseases, but the role of miRNAs in the development of ALF is not fully understood. An ALF murine model was generated by ip injection of D: -GalN/LPS, which was confirmed with histopathology and biochemistry. The hepatic miRNA expression profile in ALF was determined by microarray and verified by qRT-PCR. The functions and signal pathways of the targeted genes of these deregulated miRNAs were predicted, using bioinformatics analysis. The possible underlying mechanism was investigated by exploring the relationship between miRNA modification and hepatocyte apoptosis. There were a total of 95 significantly changed miRNAs in ALF compared to mock-treated (P < 0.01). Among these 95 miRNAs, 20 were up-regulated and 26 were down-regulated at both 5 and 7 h time points. Bioinformatics analysis predicted that some of these 46 miRNAs were involved in apoptosis. Among the up-regulated miRNAs involved in apoptosis, miR-15b and miR-16 showed the highest enrichment and targeted the common anti-apoptotic gene, BCL2. Our in vitro data demonstrated that miR-15b and/or miR-16 regulated BCL2 at the protein level. Inhibition of miR-15b and/or miR-16 reduced hepatic apoptosis and TNF production. These data suggest that miR-15b and miR-16 regulate TNF mediated hepatic apoptosis via BCL2 during ALF, and may shed light on the development of a therapeutic strategy for treatment of ALF.     

Effects of arginine modification on the photocycle of halorhodopsin

Exhaustive reaction with phenylglyoxal removed 9 of the 12 arginine and 1 of the 2 lysine residues in detergent-solubilized halorhodopsin, without affecting the chromophore. The consequences of this extensive removal of positive charges on various chloride-binding equilibria and the photochemistry were evaluated. No significant effects were seen on the affinity of Site I to chloride and on the increase in the pKa of Schiff-base deprotonation, which is caused by the chloride binding at this site. No significant effects were seen on the affinity of Site II to chloride, either. However, the photocycle of the pigment was affected. Kinetic modeling of the observed changes in flash-induced absorption changes suggests that the modification increases the affinity of the main halorhodopsin photointermediate to chloride by about fourfold. If chloride translocation involves release of chloride from this intermediate during the transport cycle, the result might explain the observed partial inhibitory effects on chloride transport. Plausible models of chloride translocation include reversible binding of the anion by positively charged groups, strategically arranged in the protein. The results indicate that two of the three spectroscopically observable chloride-dependent equilibria do not depend on a large number of positively charged residues in the protein. To the extent that the unaffected equilibria represent association and dissociation which occur during chloride translocation, at least part of the chloride translocation might be accomplished with the participation of only a few positively charged residues.     

Water is required for proton transfer from aspartate-96 to the bacteriorhodopsin Schiff base.

During the M in equilibrium with N----BR reaction sequence in the bacteriorhodopsin photocycle, proton is exchanged between D96 and the Schiff base, and D96 is reprotonated from the cytoplasmic surface. We probed these and the other photocycle reactions with osmotically active solutes and perturbants and found that the M in equilibrium with N reaction is specifically inhibited by withdrawing water from the protein. The N----BR reaction in the wild-type protein and the direct reprotonation of the Schiff base from the cytoplasmic surface in the site-specific mutant D96N are much less affected. Thus, it appears that water is required inside the protein for reactions where a proton is separated from a buried electronegative group, but not for those where the rate-limiting step is the capture of a proton at the protein surface. In the wild type, the largest part of the barrier to Schiff base reprotonation is the enthalpy of separating the proton from D96, which amounts to about 40 kJ/mol. We suggest that in spite of this D96 confers an overall kinetic advantage because when this residue becomes anionic in the N state its electric field near the cytoplasmic surface lowers the free energy barrier of the capture of a proton in the next step. In the D96N protein, the barrier to the M----BR reaction is 20 kJ/mol higher than what would be expected from the rates of the M----N and N----BR partial reactions in the wild type, presumably because this mechanism is not available.