Conformational motion in bacteriorhodopsin: the K to L transition

Action spectrum for reorientations in bacteriorhodopsin of purple membrane in suspension

In the present study, the dependency of purple membrane (PM) dielectric responses on the wavelength of light in the range 380-750 nm has showed meaningful changes about the rotation of PM in suspension and about the rotation of bacteriorhodopsin (bR) trimer inside PM, as well. The action spectrum of PM random walk substantiates the existence of two states of bR. One of them (blue edge-state) lies at the blue edge and the other (red edge-state) at the red edge of the visible absorption of bR. The results might bear on correlation of these bands to some bR photocycle intermediates or bR photoproducts. The results implicate the protein-chromophore interactions that eventually underlie protein-lipid interactions. Disrupting the protein-lipid contact during the illumination with light of wavelength in ranges of (410-470 nm) and (610-720 nm) has resulted in emergence of distinct dielectric dispersion at 0.06-0.08 MHz which is comparable to the size of bR trimer or monomer.The work reports on the chromatic adaptation of bR in view of the dielectric spectral parameters of PM. It aimed to explore a correlation seemingly found between the light wavelength and the relaxations of bR trimer inside PM. Changes in rotational diffusion of bR trimer upon blue and red light illumination can influence the three dimensional data storage based on bR, which may implicate bR in bioelectronics.

Analogies between halorhodopsin and bacteriorhodopsin

The light-activated proton-pumping bacteriorhodopsin and chloride ion-pumping halorhodopsin are compared. They belong to the family of retinal proteins, with 25% amino acid sequence homology. Both proteins have seven alpha helices across the membrane, surrounding the retinal binding pocket. Photoexcitation of all-trans retinal leads to ion transporting photocycles, which exhibit great similarities in the two proteins, despite the differences in the ion transported. The spectra of the K, L, N and O intermediates, calculated using time-resolved spectroscopic measurements, are very similar in both proteins. The absorption kinetic measurements reveal that the chloride ion transporting photocycle of halorhodopsin does not have intermediate M characteristic for deprotonated Schiff base, and intermediate L dominates the process. Energetically the photocycle of bacteriorhodopsin is driven mostly by the decrease of the entropic energy, while the photocycle of halorhodopsin is enthalpy-driven. The ion transporting steps were characterized by the electrogenicity of the intermediates, calculated from the photoinduced transient electric signal measurements. The function of both proteins could be described with the 'local access' model developed for bacteriorhodopsin. In the framework of this model it is easy to understand how bacteriorhodopsin can be converted into a chloride pump, and halorhodopsin into a proton pump, by changing the ion specificity with added ions or site-directed mutagenesis.

The photocycle of bacteriorhodopsin at high pH and ionic strength. II. Time-dependent anisotropy studied by partially saturating photoselection

Photoselection measurements with moderate excitation intensity on bacteriorhodopsin (bR) immobilized in a polyacrylamide gel soaked in 3 M KCl in the pH range 8.0-9.5 resulted in an unusual time-dependent anisotropy. In the microsecond region, the anisotropy exhibits a constant level that is considerably less than 2/5 theoretically expected for the vanishing excitation intensity, indicating partial saturation. In the millisecond region, it becomes time-dependent. Theoretical models for such a time-dependent anisotropy are presented. These models include a consideration of: (i) reorientation of the retinal chromophore during or after excitation, (ii) parallel reactions of differently saturated photoselected species of a heterogenous bR population preexisting in the ground state or photochemically induced, (iii) branching in a photochemical step, and (iv) cooperativity of molecules within a trimer. All of these models describe the anisotropy as a ratio of sums of exponentials, where the rate constants correspond to the kinetics of the photocycle. An analysis of the fitted amplitudes of the exponentials favors the models involving parallel processes rather than those invoking chromophore reorientation.

Chromophore reorientations in the early photolysis intermediates of bacteriorhodopsin

The photoselection-induced time-resolved linear dichroism of a bacteriorhodopsin suspension of purple membrane from 350 to 750 nm is measured by a new pseudo-null measurement technique. In combination with time-resolved absorption measurements, these linear dichroism measurements are used to determine the reorientation of the retinal chromophore of bacteriorhodopsin from 50 ns to 50 microseconds after photolysis. This time range covers the times when the K photointermediate decays to form L, as well as the early times during the formation of the M intermediate in the photocycle. An analysis of the photoselection-induced linear dichroism measured directly, along with the absorbance changes polarized parallel to the linearly polarized excitation, shows that the anisotropy is invariant over this time period, implying that the photolyzed chromophore rotates less than 8 degrees C with respect to unphotolyzed chromophores during this part of the photocycle.

Reorientations in the bacteriorhodopsin photocycle

Reversible photoinduced reorientations of bacteriorhodopsin have been detected in suspensions of the purple membrane of Halobacterium salinarium. The anisotropy in bacteriorhodopsin during the nanosecond through millisecond stages of the photocycle was measured by time-resolved linear dichroism and transient absorption measurements. From these measurements the anisotropies of the K, L, M, and O intermediates were determined and related to the chromophore orientation with respect to the initially selected orientation. The anisotropies of the K and L states are 0.38 +/- 0.01 and 0.35 +/- 0.01, respectively. Further anisotropy decay after formation of the M intermediate in about 0.5 ms is evidence of orientational motion at this stage in the photocycle. A constant anisotropy with a value of 0.39 +/- 0.02 in the O intermediate demonstrates a recovery of the initial protein orientation with the formation of the O state. These results demonstrate that reorientations in BR are photoinduced and reversible. Similar measurements for L and M were carried out for purple membrane in polyacrylamide gels, where the anisotropies in the L and M states are 0.38 +/- 0.014 and 0.36 +/- 0.01, respectively. These results show that reorientations also occur in BR immobilized in gels. Anisotropy decay in the M state after formation of the M intermediate was not detected in the gels, in contrast to the M intermediate in suspensions. Orientational changes are observed for BR in purple membrane suspensions in the K state, during the K-->L step, in the M state possibly related to an M1-->M2 transition, and in the O state, where an almost complete return to the original orientation occurs.(ABSTRACT TRUNCATED AT 250 WORDS)

Light-induced reorientation in the purple membrane

Reorientation of bacteriorhodopsin in the native purple membrane was studied by time-resolved linear dichroism spectroscopy (TRLD) over the millisecond time regime. The time responses observed in TRLD are distinctly different from the isotropic transient absorption (TA) at wavelengths in the range 550-590 nm, where the bacteriorhodopsin ground state absorbs. In contrast, the TA and TRLD responses have nearly identical time dependence at 410 and 690 nm, where the intermediates M and O, respectively, principally contribute. These results demonstrate ground-state bacteriorhodopsin reorientation triggered by the photocycle. The TRLD and TA data are analyzed to test models for reorientational motion. Rotational diffusion of ground-state bacteriorhodopsin cannot account for the details of the data. Rather, the results are shown to be consistent with a reversible reorientation of "spectator" (nonexcited) members of the bacteriorhodopsin trimer in the purple membrane in response to the photocycling member of the trimer. This response may be associated with cooperativity in the trimer.

1H-15N-NMR studies of bacteriorhodopsin Halobacterium halobium. Conformational dynamics of the four-helical bundle

Series of uniformly and selectively 15N-labeled bacteriorhodopsins of Halobacterium halobium (strain ET 1001) were obtained and a 1H-15N-NMR study was performed in methanol/chloroform (1:1) and 0.1 M NH4CHOO, medium which mimics that in the membrane in vivo. Less than half of the cross-peaks expected from the amino acid sequence of uniformly 15N-labeled bacteriorhodopsin were observed, using heteronuclear 1H-15N coherence spectroscopy. In order to assign the observed cross-peaks, a selective 15N-labeling of amino acid residues (Tyr, Phe, Trp, Lys, Gly, Leu, Val or Ile) was carried out and 1H-15N-NMR spectra of bacteriorhodopsin and its fragments C1 (residues (72-231), C2 (residues 1-71), B1 (residues 1-155) and BP2 (residues 163-231) were investigated. By this procedure, all observed 1H-15N cross-peaks of the entire bacteriorhodopsin were found to belong to the transmembrane segments A, B and G. The cross-peaks from four (C, D, E and F) helical bundles (79-189 residues) were missed. These results clearly indicate that dynamic processes occur in the four helice bundle. The significance of this, in respect to bacteriorhodopsin functioning, is discussed.

Glycine and beta-branched residues support and modulate peptide helicity in membrane environments

Transmembrane (TM) segments of integral membrane proteins are putatively alpha-helical in conformation once inserted into the membrane, yet consist of primary sequences rich in residues known in soluble proteins as helix-breakers (Gly) and beta-sheet promoters (Ile, Val, Thr). To examine the specific 2 degrees structure propensities of such residues in membrane environments, we have designed and synthesized a series of 20-residue peptides with 'guest' hydrophobic segments--expected to provide three turns of incipient alpha-helix content--embedded in 'host' hydrophilic (Lys-Ser) matrices. Circular dichroism (CD) spectra of the model peptides in water showed that significant helical content was observed only for peptides with high Ala content; others behaved as 'random coils'. However, in the membrane-mimetic environment of sodium dodecylsulfate (SDS) micelles, it was found that Gly can be accommodated as readily as Ala, and Ile or Val as readily as Leu, in hydrophobic alpha-helices. Further subtleties of structural preferences could be observed in electrically-neutral lyso-phosphatidylcholine (LPC) micelles, where helical propensity decreased in the order Ala-Leu-rich > Gly-Leu-rich > Gly-Ile(Val)-rich hydrophobic segments. The results conjure a role of environment-dependent helix-modulation for Gly, Ile, and Val residues--and suggest that these residues may provide, in part, the structural basis for conformational transitions within or adjacent to membrane domains, such as those accompanying membrane insertion and/or required for transport or signalling functions.