Biomedical subjects

Marina Belenky

Publications and source records attributed to Marina Belenky.

11 recordsLinked to original sources

PubMed2006

Structural changes in bacteriorhodopsin following retinal photoisomerization from the 13-cis form.

Bacteriorhodopsin (BR), a light-driven proton pump in Halobacterium salinarum, accommodates two resting forms of the retinylidene chromophore, the all-trans form (AT-BR) and the 13-cis,15-syn form (13C-BR). Both isomers are present in thermal equilibrium in the dark, but only the all-trans form has proton-pump activity. In this study, we applied low-temperature Fourier-transform infrared (FTIR) spectroscopy to 13C-BR at 77 K and compared the local structure around the chromophore before and after photoisomerization with that in AT-BR. Strong hydrogen-out-of-plane (HOOP) vibrations were observed at 964 and 958 cm(-)(1) for the K state of 13C-BR (13C-BR(K)) versus a vibration at 957 cm(-)(1) for the K state of AT-BR (AT-BR(K)). In AT-BR(K), but not in 13C-BR(K), the HOOP modes exhibit isotope shifts upon deuteration of the retinylidene at C15 and at the Schiff base nitrogen. Whereas the HOOP modes of AT-BR(K) were significantly affected by the mutation of Thr89, this was not the case for the HOOP modes of 13C-BR(K). These observations imply that, while the chromophore distortion is localized near the Schiff base in AT-BR(K), it is located elsewhere in 13C-BR(K). By use of [zeta-(15)N]lysine-labeled BR, we identified the N-D stretching vibrations of the 13C-BR Schiff base (in D(2)O) at 2173 and 2056 cm(-)(1), close in frequency to those of AT-BR. These frequencies indicate strong hydrogen bonding of the Schiff base in 13C-BR, presumably with a water molecule as in AT-BR. In contrast, the N-D stretching vibration appears at 2332 and 2276 cm(-)(1) in 13C-BR(K) versus values of 2495 and 2468 cm(-)(1) for AT-BR(K), suggesting that the rupture of the Schiff base hydrogen bond that occurs in AT-BR(K) does not occur in 13C-BR(K). Rotational motion of the Schiff base upon retinal isomerization is probably smaller in magnitude for 13C-BR than for AT-BR. These differences in the primary step are possibly related to the absence of light-driven proton pumping by 13C-BR.

Bacteriorhodopsins↗

PubMed2004

Role of arginine-82 in fast proton release during the bacteriorhodopsin photocycle: a time-resolved FT-IR study of purple membranes containing 15N-labeled arginine.

Arginine-82 has long been recognized as an important residue in bacteriorhodopsin (bR), because its mutation usually results in loss of fast H(+) release, an important step in the normal light-induced H(+) transport mechanism. To help to clarify the structural changes in Arg-82 associated with the H(+)-release step, we have measured time-resolved FT-IR difference spectra of wild-type bR containing either natural-abundance isotopes ((14)N-Arg-bR) or all seven arginines selectively and uniformly labeled with (15)N at the two eta-nitrogens ((15)N-Arg-bR). Comparison of the spectra from the two isotopic variants shows that a 1556 cm(-1) vibrational difference band due to the M photocycle intermediate of (14)N-Arg-bR loses substantial intensity in (15)N-Arg-bR. However, this isotope-sensitive arginine vibrational difference band is only observed at pH 7 and not at pH 4 where fast H(+) release is blocked. These observations support the earlier conclusion, based on site-directed mutagenesis and chemical labeling, that a strong C-N stretch vibration of Arg-82 can be assigned to a highly perturbed frequency near 1555 cm(-1) in the M state of wild-type bR [Hutson et al. (2000) Biochemistry 39, 13189-13200]. Furthermore, alkylguanidine model compound spectra indicate that the unusually low arginine C-N stretch frequency in the M state is consistent with a nearly stoichiometric light-induced deprotonation of an arginine side chain within bR, presumably arginine-82.

Arginine↗

PubMed2004

Altered hydrogen bonding of Arg82 during the proton pump cycle of bacteriorhodopsin: a low-temperature polarized FTIR spectroscopic study.

Light-driven proton transport in bacteriorhodopsin (BR) is achieved by dynamic rearrangement of the hydrogen-bonding network inside the membrane protein. Arg82 is located between the Schiff base region and proton release group, and has a major influence on the pK(a) values of these groups. It is believed that Arg82 changes its hydrogen-bonding acceptors during the pump cycle of BR, stages of which are correlated with proton movement along the transport pathway. In this study, we compare low-temperature polarized FTIR spectra of [eta(1,2)-(15)N]arginine-labeled BR in the 2750-2000 cm(-1) region with those of unlabeled BR for the K, L, M, and N intermediates. In the K-minus-BR difference spectra, (15)N-shifted modes were found at 2292 (-)/2266 (+) cm(-1) and at 2579 (-)/2567 (+) cm(-1). The former corresponds to strong hydrogen bonding, while the latter corresponds to very weak hydrogen bonding. Both N-D stretches probably originate from Arg82, the former oriented toward water 406 and the latter toward the extracellular side, and both hydrogen bonds are somewhat strengthened upon retinal photoisomerization. This perturbation of arginine hydrogen bonding is entirely relaxed in the L intermediate where no (15)N-isotope shifts are observed in the difference spectrum. In the M intermediate, the frequency is not significantly altered from that in BR. However, the polarized FTIR spectra strongly suggest that the dipolar orientation of the strongly hydrogen bonded N-D group of Arg82 is changed from perpendicular to parallel to the membrane plane. Such a change is presumably related to the motion of the Arg82 side chain from the Schiff base region to the extracellular proton release group. Additional bands corresponding to weak hydrogen bonding were observed in both the M-minus-BR and N-minus-BR spectra. Changes in hydrogen-bonding structures involving Arg82 are discussed on the basis of these FTIR observations.

Arginine↗

PubMed2004

Subunit structure of gas vesicles: a MALDI-TOF mass spectrometry study.

Many aquatic microorganisms use gas vesicles to regulate their depth in the water column. The molecular basis for the novel physical properties of these floatation organelles remains mysterious due to the inapplicability of either solution or single crystal structural methods. In the present study, some folding constraints for the approximately 7-kDa GvpA building blocks of the vesicles are established via matrix-assisted laser desorption ionization time-of-flight mass spectrometry studies of intact and proteolyzed vesicles from the cyanobacterium Anabaena flos-aquae and the archaea Halobacterium salinarum. The spectra of undigested vesicles show no evidence of posttranslational modification of the GvpA. The extent of carboxypeptidase digestion shows that the alanine rich C-terminal pentapeptide of GvpA is exposed to the surface in both organisms. The bonds that are cleaved by Trypsin and GluC are exclusively in the extended N-terminus of the Anabaena flos-aquae protein and in the extended C-terminus of the Halobacterium salinarum protein. All the potentially cleavable peptide bonds in the central, highly conserved portion of the protein appear to be shielded from protease attack in spite of the fact that some of the corresponding side chains are almost certainly exposed to the aqueous medium.

Amino Acid Sequence↗

PubMed2003

Water-mediated hydrogen-bonded network on the cytoplasmic side of the Schiff base of the L photointermediate of bacteriorhodopsin.

The L intermediate in the proton-motive photocycle of bacteriorhodopsin is the starting state for the first proton transfer, from the Schiff base to Asp85, in the formation of the M intermediate. Previous FTIR studies of L have identified unique vibration bands caused by the perturbation of several polar amino acid side chains and several internal water molecules located on the cytoplasmic side of the retinylidene chromophore. In the present FTIR study we describe spectral features of the L intermediate in D(2)O in the frequency region which includes the N-D stretching vibrations of the backbone amides. We show that a broad band in the 2220-2080 cm(-1) region appears in L. By use of appropriate (15)N labeling and mutants, the lower frequency side of this band in L is assigned to the amides of Lys216 and Gly220. These amides are coupled to each other, and interact with Thr46 and Val49 in helix B and Asp96 in helix C via weakly H-bonding water molecules that exhibit O-D stretching vibrations at 2621 and 2605 cm(-1). These water molecules are part of a hydrogen-bonded network characteristic of L which includes other water molecules located closer to the chromophore that exhibit an O-D stretching vibration at 2589 cm(-1). This structure, extending from the Schiff base to the internal proton donor Asp96, stabilizes L and affects the L-to-M transition.

Amides↗

PubMed2003

Solid-state NMR investigation of the buried X-proline peptide bonds of bacteriorhodopsin.

The role of proline residues in the photocycle of bacteriorhodopsin (bR) is addressed using solid-state NMR. (13)C and (15)N chemical shifts from X-Pro peptide bonds in bR are assigned from REDOR difference spectra of pairwise labeled samples, and correlations of chemical shifts with structure are explored in a series of X-Pro model compounds. Results for the three membrane-embedded X-Pro bonds of bR indicate only slight changes in the transition from the resting state of the protein to either the early or late M state of the protonmotive photocycle. These results suggest that the buried prolines serve a principally structural role in bR.

Bacteriorhodopsins↗

PubMed2003

Backbone and side chain assignment strategies for multiply labeled membrane peptides and proteins in the solid state.

We demonstrate that the SPECIFIC CP technique can be used to obtain heteronuclear correlation (HETCOR) spectra of peptide backbones with greater efficiency than conventional HETCOR methods. We show that similar design principles can be employed to achieve selective homonuclear polarization transfer mediated through dipolar or scalar couplings. Both approaches are demonstrated in a tripeptide with uniform 15N and 13C labeling, and with uniform 15N labeling and natural abundance 13C. In other applications, the high efficiency of the heteronuclear SPECIFIC CP transfer allows discrimination of single amide signals in the 248-residue membrane protein bacteriorhodopsin (bR). In particular, variations are detected in the ordering of the Ala81-Arg82 peptide bond among the photocycle intermediates of bR and SPECIFIC CP is used to correlate 15N and 13C signals from the three Val-Pro peptide bonds.

Bacteriorhodopsins↗

PubMed2002

Vibrational frequency and dipolar orientation of the protonated Schiff base in bacteriorhodopsin before and after photoisomerization.

Light-driven proton transport in bacteriorhodopsin (BR) is initiated by photoisomerization of the retinylidene chromophore, which perturbs the hydrogen bonding network in the Schiff base region of the active site. This study aimed to identify the frequency and dipolar orientation of the N-D stretching vibrations of the Schiff base before and after photoisomerization, by means of low-temperature polarized FTIR spectroscopy of [zeta-(15)N]lysine-labeled BR in D(2)O. (15)N-shifted modes were found at 2123 and 2173 cm(-1) for BR, and at 2468 and 2495 cm(-1) for the K intermediate. The corresponding N-H stretches are at approximately 2800 cm(-1) for BR and 3350-3310 cm(-1) for the K intermediate. The shift to a 350 cm(-1) higher frequency upon photoisomerization is consistent with loss of the hydrogen bond of the Schiff base. The N-D stretch frequencies of the Schiff base in BR and the K intermediate are close to the O-D stretch frequencies of strongly hydrogen bonded water and Thr89, respectively. The angles of the dipole moments of the N-D stretches to the membrane normal were determined to be 60-65 degrees for BR and approximately 90 degrees for the K intermediate. In the case of BR, the stretch orientation is expected to deviate from the N-D bond orientation due to vibrational mixing in the hydrogen bonding network. In contrast, the data for the K intermediate suggest that the N-D group is not hydrogen bonded and orients along the membrane.

Bacteriorhodopsins↗

PubMed2002

Interaction of internal water molecules with the schiff base in the L intermediate of the bacteriorhodopsin photocycle.

In the photocycle of bacteriorhodopsin (BR), the first proton movement, from the Schiff base to Asp85, occurs after the formation of the L intermediate. In L, the C [double bond] N bond of the Schiff base is strained, and the nitrogen interacts strongly with its counterion. The present study seeks to detect the interaction of internal water molecules with the Schiff base in L using difference FTIR spectroscopy at 170 K. The coupled modes of the hydrogen-out-of plane bending vibrations (HOOPs) of the N-H and C(15)-H of the protonated Schiff base are detected as a broad band centered at 911 cm(-1) for BR. A set of bands at 1073, 1064, and 1056 cm(-1) for L is shown to arise from the coupling of the HOOP with the overtones of interacting water O-H vibrations. Interaction with water was shown by the decreased intensity of the HOOPs of L in H(2)(18)O and by the influence of mutants that have been shown to perturb specific internal water molecules in BR. In contrast, the HOOP band of initial BR was not affected by these mutations. In D85N, the coupled HOOP of BR is depleted, while the coupled HOOPs of L are shifted. The results indicate that the Schiff base interacts with water in the L state but in a different manner than in the BR state. Moreover, the effects of mutations suggest that cytoplasmic water close to Thr46 (Wat46) either interacts stronger with the Schiff base in L or that it is important in stabilizing another water that does.

Bacteriorhodopsins↗

PubMed2002

Tryptophan interactions in bacteriorhodopsin: a heteronuclear solid-state NMR study.

The bulky and amphiphilic nature of tryptophan residues makes them particularly interesting components of proteins. In bacteriorhodopsin, four of the eight tryptophan residues are in the active site, forming parts of the retinal binding pocket. In this work, we use solid-state NMR to study the interactions of the tryptophan residues in wild-type bacteriorhodopsin, in the resting state, and in critical intermediates of the proton-motive photocycle. The range of the chemical shifts of the indole nitrogens suggests that all eight of them are hydrogen bonded. Using difference spectroscopy, we isolate several changes in these hydrogen bonds in the early and late M states. As found earlier for the peptide backbone, some perturbations found in the early M state relax in the transition to the late M state while new perturbations arise. Interestingly, Rotational Echo DOuble Resonance (REDOR) difference spectroscopy of [20-13C]retinal,[indole-15N]Trp-bR shows that indole of Trp182 is not involved in the significant hydrogen bond perturbations. We also use REDOR to measure dipolar interactions in [20-13C]retinal,[indole-15N]Trp-bR, and thereby determine the distance between the C20 of retinal and the indole nitrogen of Trp182. The internuclear distance changes only slightly from the light-adapted state (3.36 +/- 0.2 A) to the early M state (3.16 +/- 0.4 A).

Bacteriorhodopsins↗

PubMed2002

Control of the pump cycle in bacteriorhodopsin: mechanisms elucidated by solid-state NMR of the D85N mutant.

By varying the pH, the D85N mutant of bacteriorhodopsin provides models for several photocycle intermediates of the wild-type protein in which D85 is protonated. At pH 10.8, NMR spectra of [zeta-(15)N]lys-, [12-(13)C]retinal-, and [14,15-(13)C]retinal-labeled D85N samples indicate a deprotonated, 13-cis,15-anti chromophore. On the other hand, at neutral pH, the NMR spectra of D85N show a mixture of protonated Schiff base species similar to that seen in the wild-type protein at low pH, and more complex than the two-state mixture of 13-cis,15-syn, and all-trans isomers found in the dark-adapted wild-type protein. These results lead to several conclusions. First, the reversible titration of order in the D85N chromophore indicates that electrostatic interactions have a major influence on events in the active site. More specifically, whereas a straight chromophore is preferred when the Schiff base and residue 85 are oppositely charged, a bent chromophore is found when both the Schiff base and residue 85 are electrically neutral, even in the dark. Thus a "bent" binding pocket is formed without photoisomerization of the chromophore. On the other hand, when photoisomerization from the straight all-trans,15-anti configuration to the bent 13-cis,15-anti does occur, reciprocal thermodynamic linkage dictates that neutralization of the SB and D85 (by proton transfer from the former to the latter) will result. Second, the similarity between the chromophore chemical shifts in D85N at alkaline pH and those found previously in the M(n) intermediate of the wild-type protein indicate that the latter has a thoroughly relaxed chromophore like the subsequent N intermediate. By comparison, indications of L-like distortion are found for the chromophore of the M(o) state. Thus, chromophore strain is released in the M(o)-->M(n) transition, probably coincident with, and perhaps instrumental to, the change in the connectivity of the Schiff base from the extracellular side of the membrane to the cytoplasmic side. Because the nitrogen chemical shifts of the Schiff base indicate interaction with a hydrogen-bond donor in both M states, it is possible that a water molecule travels with the Schiff base as it switches connectivity. If so, the protein is acting as an inward-driven hydroxyl pump (analogous to halorhodopsin) rather than an outward-driven proton pump. Third, the presence of a significant C [double bond] N syn component in D85N at neutral pH suggests that rapid deprotonation of D85 is necessary at the end of the wild-type photocycle to avoid the generation of nonfunctional C [double bond] N syn species.

Bacteriorhodopsins↗