X-ray diffraction studies of bacteriorhodopsin. Determination of the positions of mercury label at several engineered cysteine residues

Structural studies of bacteriorhodopsin in BC era

It marked half a century since the discovery of bacteriorhodopsin two years ago. On this occasion, I have revisited historically important diffraction studies of this membrane protein, based on my recollections. X-ray diffraction and electron diffraction, and electron microscopy, described the low-resolution structure of bacteriorhodopsin within the purple membrane. Neutron diffraction was effective to assign the helical regions in the primary structure with 7 rods revealed by low-resolution structure as well as to describe the retinal position. Substantial conformational changes upon light illumination were clarified by the structures of various photointermediates. Early trials of time-resolved studies were also introduced. Models for the mechanism of light-driven proton pump based on the low-resolution structural studies are also described. Significantly, they are not far from the today's understanding. I believe that the spirit of the early research scientists in this field and the essence of their studies, which constitute the foundations of the field, still actively fertilizes current membrane protein research.

Picometer-scale dynamical observations of individual membrane proteins: the case of bacteriorhodopsin

In vivo measurements of dynamical conformational changes in single biomolecules under functional conditions have had a tremendous impact on molecular and cell biology. However, even single-molecule fluorescent resonance energy transfer cannot easily monitor the intramolecular dynamics in cell systems due to shortcomings in monitoring precision. Here, we report dynamical observations of irreversible intramolecular conformational changes in a single-membrane protein [bacteriorhodopsin (BR)] using diffracted x-ray tracking. The light-driven proton pump BR is the best-characterized membrane protein. The position of BR's 35th amino acid, which is located farthest from retinal, exhibits a momentary positional jump of 0.73+/-0.48 A due to the expression of its function. Following that, we observed Brownian motion without the diffracted spots returning to their initial positions. The average width of this jump is about 14 times larger than that of thermal Brownian motion and agrees with estimated movements from known x-ray crystallography data. This result is an important step toward realizing in vivo observations of single-molecular conformational changes in membrane proteins.

Significance of low-frequency local fluctuation motions in the transmembrane B and C alpha-helices of bacteriorhodopsin, to facilitate efficient proton uptake from the cytoplasmic surface, as revealed by site-directed solid-state 13C NMR

13C NMR spectra of [1-13C]Val- or -Pro-labeled bacteriorhodopsin (bR) and its single or double mutants, including D85N, were recorded at various pH values to reveal conformation and dynamics changes in the transmembrane alpha-helices, in relation to proton release and uptake between bR and the M-like state caused by modified charged states at Asp85 and the Schiff base (SB). It was found that the D85N mutant acquired local fluctuation motion with a frequency of 10(4) Hz in the transmembrane B alpha-helix, concomitant with deprotonation of SB in the M-like state at pH 10, as manifested from a suppressed 13C NMR signal of the [1-13C]-labeled Val49 residue. Nevertheless, local dynamics at Pro50 neighboring with Val49 turned out to be unchanged, irrespective of the charged state of SB as viewed from the 13C NMR of [1-13C]-labeled Pro50. This means that the transmembrane B alpha-helix is able to acquire the fluctuation motion with a frequency of 10(4) Hz beyond the kink at Pro50 in the cytoplasmic side. Concomitantly, fluctuation motion at the C helix with frequency in the order of 10(4) Hz was found to be prominent, due to deprotonation of SB at pH 10, as viewed from the 13C NMR signal of Pro91. Accordingly, we have proposed here a novel mechanism as to proton uptake and transport based on a dynamic aspect that a transient environmental change from a hydrophobic to hydrophilic nature at Asp96 and SB is responsible for the reduced p Ka value which makes proton uptake efficient, as a result of acquisition of the fluctuation motion at the cytoplasmic side of the transmembrane B and C alpha-helices in the M-like state. Further, it is demonstrated that the presence of a van der Waals contact of Val49 with Lys216 at the SB is essential to trigger this sort of dynamic change, as revealed from the 13C NMR data of the D85N/V49A mutant.

Reconciling crystallography and mutagenesis: a synthetic approach to the creation of a comprehensive model for proton pumping by bacteriorhodopsin

As a result of the number of new high-resolution structures of the pigment and some of its photointermediates, a realistic model for the functioning of bacteriorhodopsin seems to be finally emerging. However, lack of structural information for some of the key functional states, and contradictions between some published structural models, argue for the use of the synthetic approach, one that includes use of data from both crystallographic and mutagenesis studies. The role of mutagenesis in this synthetic approach falls into two categories. First, to provide additional structural information, and second, to test the predictions of structural models by studying mutant phenotypes. This review urges critical comparisons of the structural and mutagenesis data, as there are problems with their selective and indiscriminate use.

Structures of photointermediates and their implications for the proton pump mechanism

It is widely accepted that bacteriorhodopsin undergoes global conformational changes during its photocycle. In this review, the structural properties of the M and N intermediates are described in detail. Based on the clarified global conformational change, we propose a model for the molecular mechanism of the proton pump. The global structural change is suggested to be a key component in establishing vectorial proton transport.

Coupling photoisomerization of retinal to directional transport in bacteriorhodopsin

In order to understand how isomerization of the retinal drives unidirectional transmembrane ion transport in bacteriorhodopsin, we determined the atomic structures of the BR state and M photointermediate of the E204Q mutant, to 1.7 and 1.8 A resolution, respectively. Comparison of this M, in which proton release to the extracellular surface is blocked, with the previously determined M in the D96N mutant indicates that the changes in the extracellular region are initiated by changes in the electrostatic interactions of the retinal Schiff base with Asp85 and Asp212, but those on the cytoplasmic side originate from steric conflict of the 13-methyl retinal group with Trp182 and distortion of the pi-bulge of helix G. The structural changes suggest that protonation of Asp85 initiates a cascade of atomic displacements in the extracellular region that cause release of a proton to the surface. The progressive relaxation of the strained 13-cis retinal chain with deprotonated Schiff base, in turn, initiates atomic displacements in the cytoplasmic region that cause the intercalation of a hydrogen-bonded water molecule between Thr46 and Asp96. This accounts for the lowering of the pK(a) of Asp96, which then reprotonates the Schiff base via a newly formed chain of water molecules that is extending toward the Schiff base.

Recollections of the electron crystallographic heavy atom derivative search of purple membrane: the quest for EM structure determination

The use of multiple isomorphous replacement in protein electron crystallography for phase determination has been systematically studied only for purple membrane, even though the use of heavy atoms or heavy atom clusters has been used on many occasions in electron microscopy for locating domains or subunits in protein assemblies. The background behind the structure determination of bacteriorhodopsin, the protein component of purple membranes, is summarized and an evaluation of the strengths and weaknesses of using isomorphous replacement in electron crystallography is discussed.

Bacteriorhodopsin

Bacteriorhodopsin is a seven-transmembrane helical protein that contains all-trans retinal. In this light-driven pump, a reaction cycle initiated by photoisomerization to 13-cis causes translocation of a proton across the membrane. Local changes in the geometry of the protonated Schiff base and the proton acceptor Asp85, and the proton conductivities of the half channels that lead from this active site to the two membrane surfaces, interact so as to allow timely proton transfers that result in proton release on the extracellular side and proton uptake on the cytoplasmic one. The details of the steps in this photocycle, and the underlying principles that ensure unidirectionality of the movement of a proton across the protein, provide strong clues to how ion pumps function.

Conformational change of helix G in the bacteriorhodopsin photocycle: investigation with heavy atom labeling and x-ray diffraction

According to the current structural model of bacteriorhodopsin, Ile222 is located at the cytoplasmic end of helix G. We labeled the single cysteine of the site-directed mutant Ile222 --> Cys with p-chloromercuribenzoic acid and determined the position of the labeled mercury by x-ray diffraction in the unphotolyzed state, and in the MN photointermediate accumulated in the presence of guanidine hydrochloride at pH 9.5. According to the difference Fourier maps between the MN intermediate and the unphotolyzed state, the structural change in the MN intermediate was not affected by mercury labeling. The difference Fourier map between the labeled and the unlabeled I222C gave the position of the mercury label. This information was obtained for both the unphotolyzed state and the MN intermediate. We found that the position of the mercury at residue 222 is shifted by 2.1 +/- 0.8 A in the MN intermediate. This agrees with earlier results that suggested a structural change in the G helix. The movement of the mercury label is so large that it must originate from a cooperative conformational change in the helix G at its cytoplasmic end, rather than from displacement of residue 222. Because Ile222 is located at the same level on the z coordinate as Asp96, the structural change in the G helix could have the functional role of perturbing the environment and therefore the pKa of this functionally important aspartate.