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Mitochondrial complex I is a redox-driven proton pump that generates proton-motive force across the inner mitochondrial membrane, powering oxidative phosphorylation and ATP synthesis in eukaryotes. We report the structure of complex I from the thermophilic fungus Chaetomium thermophilum, determined by cryoEM up to 2.4 Å resolution. We show that the complex undergoes a transition between two conformations, which we refer to as form 1 and 2. The conformational switch is manifest in a twisting movement of the peripheral arm relative to the membrane arm, but most notably in substantial rearrangements of the Q-binding cavity and the E-channel, resulting in a continuous aqueous passage from the E-channel to subunit ND5 at the far end of the membrane arm. The conformational changes in the complex interior resemble those reported for mammalian complex I, suggesting a highly conserved, universal mechanism of coupling electron transport to proton pumping.

Na+/H+ antiporters in the CPA1 branch of the cation proton antiporter family drive the electroneutral exchange of H+ against Na+ ions and ensure pH homeostasis in eukaryotic and prokaryotic organisms. Although their transport cycle is overall electroneutral, specific partial reactions are electrogenic. Here, we present an electrophysiological study of the PaNhaP Na+/H+ antiporter from Pyrococcus abyssi reconstituted into liposomes. Positive transient currents were recorded upon addition of Na+ to PaNhaP proteoliposomes, indicating a reaction where positive charge is rapidly displaced into the proteoliposomes with a rate constant of k >200 s−1. We attribute the recorded currents to an electrogenic reaction that includes Na+ binding and possibly occlusion. Subsequently, positive charge is transported out of the cell associated with H+ binding, so that the overall reaction is electroneutral. We show that the differences in pH profile and Na+ affinity of PaNhaP and the related MjNhaP1 from Methanocaldococcus jannaschii can be attributed to an additional negatively charged glutamate residue in PaNhaP. The results are discussed in the context of the physiological function of PaNhaP and other microbial Na+/H+ exchangers. We propose that both, electroneutral and electrogenic Na+/H+ antiporters, represent a carefully tuned self-regulatory system, which drives the cytoplasmic pH back to neutral after any deviation.

Charging of physical phase plates is a problem that has prevented their routine use in transmission electron microscopy of weak-phase objects. In theory, electrostatic phase plates are superior to thin-film phase plates since they do not attenuate the scattered electron beam and allow freely adjustable phase shifts. Electrostatic phase plates consist of multiple layers of conductive and insulating materials, and are thus more prone to charging than thin-film phase plates, which typically consist of only one single layer of amorphous material. We have addressed the origins of charging of Boersch phase plates and show how it can be reduced. In particular, we have performed simulations and experiments to analyze the influence of the insulating Si3N4 layers and surface charges on electrostatic charging. To optimize the performance of electrostatic phase plates, it would be desirable to fabricate electrostatic phase plates, which (i) impart a homogeneous phase shift to the unscattered electrons, (ii) have a low cut-on frequency, (iii) expose as little material to the intense unscattered beam as possible, and (iv) can be additionally polished by a focused ion-beam instrument to eliminate carbon contamination accumulated during exposure to the unscattered electron beam (Walter et al., 2012, Ultramicroscopy, 116, 62–72). We propose a new type of electrostatic phase plate that meets the above requirements and would be superior to a Boersch phase plate. It consists of three free-standing coaxial rods converging in the center of an aperture (3-fold coaxial phase plate). Simulations and preliminary experiments with modified Boersch phase plates indicate that the fabrication of a 3-fold coaxial phase plate is feasible.

Mitochondria are the powerhouses of eukaryotic cells and the main site of ATP synthesis in cells performing aerobic respiration. Located on the cristae of the inner mitochondrial membrane, the ATP synthase uses the energy stored in a transmembrane gradient of protons to power the synthesis of ATP while the respiratory chain complexes replenish the gradient. Using the technique of electron cryo-tomography and subtomogram averaging, we are characterizing how the structure and spatial distribution of membrane proteins influence mitochondrial function. So far we have discovered: 1) the structure of the ATP synthase varies dramatically between different eukaryotic lineages, 2) that in all species studied so far, the ATP synthase form rows of dimers along the highly curved edges of the cristae membranes, 3) that the structure of the rows varies between protozoan and multicellular organisms, and 4) the purpose of the rows appears to be the maintenance of organized inner membrane invaginations. In parallel, we have shown that the proteins of the respiratory chain are located in the flat membrane regions of cristae and that they form species specific supercomplexes. Alongside the cryo-ET studies, we have determined a 6.2A structure of the mitochondrial ATP synthase of Polytomella sp. using single particle cryo-EM. Our structure revealed four highly tilted membrane-intrinsic helices (∼20° to the membrane plane) adjacent to the rotor ring which we assign to the elusive a-subunit. Based on this structure, we present a model describing how protons move through the ATP synthase.

The ubiquitous mammalian Na(+)/H(+) exchanger NHE1 has critical functions in regulating intracellular pH, salt concentration, and cellular volume. The regulatory C-terminal domain of NHE1 is linked to the ion-translocating N-terminal membrane domain and acts as a scaffold for signaling complexes. A major interaction partner is calmodulin (CaM), which binds to two neighboring regions of NHE1 in a strongly Ca(2+)-dependent manner. Upon CaM binding, NHE1 is activated by a shift in sensitivity toward alkaline intracellular pH. Here we report the 2.23 Å crystal structure of the NHE1 CaM binding region (NHE1(CaMBR)) in complex with CaM and Ca(2+). The C- and N-lobes of CaM bind the first and second helix of NHE1(CaMBR), respectively. Both the NHE1 helices and the Ca(2+)-bound CaM are elongated, as confirmed by small angle x-ray scattering analysis. Our x-ray structure sheds new light on the molecular mechanisms of the phosphorylation-dependent regulation of NHE1 and enables us to propose a model of how Ca(2+) regulates NHE1 activity.

Channelrhodopsin-2 (ChR2) is the prototype of a new class of light-gated ion channels that is finding widespread applications in optogenetics and biomedical research. We present a 6-Å projection map of ChR2, obtained by cryo-electron microscopy of two-dimensional crystals grown from pure, heterologously expressed protein. The map shows that ChR2 is the same dimer with non-crystallographic 2-fold symmetry in three different membrane crystals. This is consistent with biochemical analysis, which shows a stable dimer in detergent solution. Comparison to the projection map to bacteriorhodopsin indicates a similar structure of seven transmembrane alpha helices. Based on the projection map and sequence alignments, we built a homology model of ChR2 that potentially accounts for light-induced channel gating. Although a monomeric channel is not ruled out, comparison to other membrane channels and transporters suggests that the ChR2 channel is located at the dimer interface on the 2-fold axis, lined by transmembrane helices 3 and 4.

The channel activity of the outer-membrane protein G (OmpG) from Escherichia coli is pH-dependent. To investigate the role of the histidine pair His231/His261 in triggering channel opening and closing, we mutated both histidines to alanines and cysteines. Fourier transform infrared spectra revealed that the OmpG mutants stay—independent of pH—in an open conformation. Temperature ramp experiments indicate that the mutants are as stable as the open state of wild-type OmpG. The X-ray structure of the alanine-substituted OmpG mutant obtained at pH 6.5 confirms the constitutively open conformation. Compared to previous structures of the wild-type protein in the open and closed conformation, the mutant structure shows a difference in the extracellular loop L6 connecting β-strands S12 and S13. A deletion of amino acids 220–228, which are thought to block the channel at low pH in wild-type OmpG, indicates conformational changes, which might be triggered by His231/His261.

A gating mechanism of the beta-barrel-forming outer membrane protein G (OmpG) from Escherichia coli was recently presented. The mechanism was based on X-ray structures revealed from crystals grown from solubilized OmpG at both neutral pH and acidic pH. To investigate whether these conformations represent the naturally occurring gating mechanism, we reconstituted OmpG in native E. coli lipids and applied high-resolution atomic force microscopy. The reconstituted OmpG molecules assembled into both monomers and dimers. Single monomeric and dimeric OmpG molecules showed open channel entrances at pH 7.5 and at room temperature. The extracellular loops connecting the beta-strands that form the transmembrane beta-barrel pore exhibited elevated structural flexibility. Upon lowering the pH to 5.0, the conformation of OmpG molecules changed to close the extracellular entrance of their channel. It appears that one or more of the extracellular loops collapsed onto the channel entrance. This conformational change was fully reversible. Our data confirm that the previously reported gating mechanism of OmpG occurs at physiological conditions in E. coli lipid membranes.

Nonphotochemical quenching (NPQ) is a fundamental mechanism in photosynthesis by which plants protect themselves against excess excitation energy and which is thus of crucial importance for plant survival and fitness. Recently, carotenoid radical cation (Car(*+)) formation has been discovered to be a key step in the feedback deexcitation quenching component (qE) of NPQ, whose molecular mechanism and location remains elusive. A recent model for qE suggests that the replacement of violaxanthin (Vio) by zeaxanthin (Zea) in photosynthetic pigment binding pockets can in principle result in qE via the so-called "gear-shift" or electron transfer quenching mechanisms. We performed pump-probe measurements on individual antenna complexes of photosystem II (CP24, CP26 and CP29) upon excitation of the chlorophylls (Chl) into their first excited Q(y) state at 660 nm when either Vio or Zea was bound to those complexes. The Chl lifetime was then probed by measuring the decay kinetics of the Chl excited state absorption (ESA) at 900 nm. The charge-transfer quenching mechanism, which is characterized by a spectral signature of the transiently formed Zea radical cation (Zea(*+)) in the near-IR, has also been addressed, both in solution and in light-harvesting complexes of photosystem II (LHC-II). Applying resonant two-photon two-color ionization (R2P2CI) spectroscopy we show here the formation of beta-Car(*+) in solution, which occurs on a femtosecond time-scale by direct electron transfer to the solvent. The beta-Car(*+) maxima strongly depend on the solvent polarity. Moreover, our two-color two-photon spectroscopy on CP29 reveals the spectral position of Zea(*+) in the near-IR region at 980 nm.

In this study, structural, functional, and mechanistic properties of the Na(+)/H(+) antiporter MjNhaP1 from Methanococcus jannaschii were analyzed by infrared spectroscopic techniques. Na(+)/H(+) antiporters are generally responsible for the regulation of cytoplasmic pH and Na(+) concentration. MjNhaP1 is active in the pH range between pH 6 and pH 6.5; below and above it is inactive. The secondary structure analysis on the basis of ATR-IR spectra provides the first insights into the structural changes between inactive (pH 8) and active (pH 6) state of MjNhaP1. It results in decreased ordered structural elements with increasing the pH-value i.e. with inactivation of the protein. Analysis of temperature-dependent FTIR spectra indicates that MjNhaP1 in the active state exhibits a much higher unfolding temperature in the spectral region assigned to alpha-helical segments. In contrast, the temperature-induced structural changes for beta-sheet structure are similar for inactive and active state. Consequently, this structure element is not the part of the activation region of the protein. The surface accessibility of the protein was analyzed by following the extent of H/D exchange. Due to higher content of unordered structural elements a higher accessibility for amide protons is observed for the inactive as compared to the active state of MjNhaP1. Altogether, the results present the active state of MjNhaP1 as the state with ordered structural elements which exhibit high thermal stability and increased hydrophobicity.

Bacteria, mitochondria and chloroplasts harbour factors that facilitate the insertion, folding and assembly of membrane proteins. In Escherichia coli, yidC is required for membrane insertion, acting in both a Sec-dependent and a Sec-independent manner. There is an expanding volume of biochemical work on its role in this process, but none so far on its structure. We present the first of this class of membrane proteins determined by electron cryomicroscopy in the near-nativelike state of the membrane. yidC forms dimers in the membrane and each monomer has an area of low density that may be part of the path transmembrane segments follow during their insertion. Upon consideration of the structures of yidC and SecYEG, we speculate on the nature of the interfaces that facilitate the alternative pathways (Sec-dependent and -independent) of membrane protein insertion.

The glutamate transporter GLT-1 from Rattus norvegicus was expressed at high level in baby hamster kidney (BHK-21) cells by the Semliki Forest Virus expression system. We examined the expressed GLT-1 in the plasma membrane and found that the transporter accumulates in detergent-insoluble lipid-protein assemblies. Freeze-fracture, immunogold labeling, and electron microscopy revealed that GLT-1 forms ∼200-nm protein-rich islands in the plasma membrane. Cholesterol depletion in living cells resulted in a dispersion of the GLT-1 islands, indicating that they are the result of lipid-protein rather than protein-protein interactions. Disruption of GLT-1 islands and dispersion of GLT-1 goes along with a reduction of the glutamate transport activity. Our direct visualization of lipid-protein islands in the plasma membrane of tissue culture cells suggests that the reported clustering of glutamate transporters and their cholesterol-dependent transport activity in cells is likewise connected to their association with cholesterol-rich microdomains in the plasma membrane.

The Sec complex forms the core of a conserved machinery transporting proteins across or into membranes. In Escherichia coli SecYEG is active as an oligomer, but the structure predicts that the protein-conducting channel is formed by the monomer. A homology model of the E.coli complex was built using the atomic structure of Methanococcus jannaschii SecYEbeta. Another structure of the membrane-bound dimer was then determined by fitting the homology model to an 8A map of SecYEG determined by electron microscopy. We found that the substrate-binding site of the dimer has opened slightly and the plug domain moved toward the outside. This new position retains the channel in a closed state. These differences partially reflect the movements that have been proposed to occur during channel gating. Further opening of the substrate-binding pocket to bind and release bound substrate and displacement of the plug during secretion, presumably rely on the action of the partner proteins. The contacts arising at the dimer interface in the environment of the lipid bilayer may have activated the assembly.

The major light-harvesting complex (LHC-II) of higher plants plays a crucial role in capturing light energy for photosynthesis and in regulating the flow of energy within the photosynthetic apparatus. Native LHC-II isolated from plant tissue consists of three isoforms, Lhcb1, Lhcb2, and Lhcb3, which form homo- and heterotrimers. All three isoforms are highly conserved among different species, suggesting distinct functional roles. We produced the three LHC-II isoforms by heterologous expression of the polypeptide in Escherichia coli and in vitro refolding with purified pigments. Although Lhcb1 and Lhcb2 are very similar in polypeptide sequence and pigment content, Lhcb3 is clearly different because it lacks an N-terminal phosphorylation site and has a higher chlorophyll a/b ratio, suggesting the absence of one chlorophyll b. Low temperature absorption and fluorescence emission spectra of the pure isoforms revealed small but significant differences in pigment organization. The oligomeric state of the pure isoforms and of their permutations was investigated by native gel electrophoresis, sucrose density gradient centrifugation, and SDS-PAGE. Lhcb1 and Lhcb2 formed trimeric complexes by themselves and with one another, but Lhcb3 was able to do so only in combination with one or both of the other isoforms. We conclude that the main role of Lhcb1 and Lhcb2 is in the adaptation of photosynthesis to different light regimes. The most likely role of Lhcb3 is as an intermediary in light energy transfer from the main Lhcb1/Lhcb2 antenna to the photosystem II core.

The twin-arginine translocation (Tat) system transports folded proteins across bacterial plasma membranes and the chloroplast thylakoid membrane. Here, we investigate the composition and structural organization of three different purified Tat complexes from Escherichia coli, Salmonella typhimurium and Agrobacterium tumefaciens. First, we demonstrate the functional activity of these Tat systems in vivo, since expression of the tatABC operons from S. typhimurium or A. tumefaciens in an E. coli tat null mutant strain resulted in efficient Tat-dependent export of an E. coli cofactor-containing substrate, TMAO reductase. The three isolated, affinity-tagged Tat complexes comprised TatA, TatB and TatC in each case, demonstrating a strong interaction between these three subunits. Single-particle electron microscopy studies of all three complexes revealed approximately oval-shaped, asymmetric particles with maximal dimensions up to 13 nm. A common feature is a number of stain-excluding densities surrounding more or less central pools of stain, suggesting protein-lined pores or cavities. The characteristics of size variation among the particles suggest a modular form of assembly and/or the recruitment of varying numbers of TatBC/TatA units. Despite low levels of sequence homology, the combined data indicate structural and functional conservation in the Tat systems of these three bacterial species.

The Escherichia coli porin OmpG, which acts as an efficient unspecific channel for mono-, di- and trisaccharides, has been purified and crystallized in two dimensions. Projection maps of two different crystal forms of OmpG at 6 A resolution show that the protein has a beta-barrel structure characteristic for outer membrane proteins, and that it does not form trimers, unlike most other porins such as OmpF and OmpC, but appears in monomeric form. The size of the barrel is approximately 2.5 nm, indicating that OmpG may consist of 14 beta-strands. The projection map suggests that the channel is restricted by internal loops.

Electron cryo-microscopy has yielded a wealth of detailed new information on structures of biological macromolecules ranging from alphabeta-tubulin at 3.7 A resolution to hepatitis B virus at 7.4 A resolution, as well as a number of membrane proteins at 6-8 A resolution. Much of this progress was made possible by recent advances in instrumentation and image processing techniques.

Background: Structures have recently been solved at 8 a resolution for both Ca 2+ -ATPase from rabbit sarcoplasmic reticulum and H + -ATPase from Neurospora crassa . These cation pumps are two distantly related members of the family of P-type ATPases, which are thought to use similar mechanisms to generate ATP-dependent ion gradients across a variety of cellular membranes. We have undertaken a detailed comparison of the two structures in order to describe their similarities and differences as they bear on their mechanism of active transport. Results: Our first important finding was that the arrangement of 10 transmembrane helices was remarkably similar in the two molecules. This structural homology strongly supports the notion that these pumps use the same basic mechanism to transport their respective ions. Despite this similarity in the membrane-spanning region, the cytoplasmic regions of the two molecules were very different, both in their disposition relative to the membrane and in the juxtaposition of their various subdomains. Conclusions: On the basis of the crystallization conditions, we propose that these two crystal structures represent different intermediates in the transport cycle, distinguished by whether cations are bound to their transport sites. Furthermore, we propose that the corresponding conformational change (E 2 to E 1 ) has two components: the first is an inclination of the main cytoplasmic mass by 20° relative to the membrane-spanning domain; the second is a rearrangement of the domains comprising the cytoplasmic part of the molecules. Accordingly, we present a rough model for this important conformational change, which relays the effects of cation binding within the membrane-spanning domain to the nucleotide-binding site, thus initiating the transport cycle.

Electron cryocrystallography of precipitant-induced two-dimensional surface crystals of the neurospora plasma membrane H+-ATPase and tubular crystals of the sarcoplasmic reticulum Ca2+-ATPase has recently yielded structure maps for these ion transporters at a resolution of about 8 A. The membrane-embedded regions of these closely related enzymes are similar, but the cytoplasmic regions appear to be significantly different.

Electron cryo-microscopy of two-dimensional crystals of the major light-harvesting complex from pea chloroplasts has revealed the structure at 3A A resolution. The atomic model provides insights into the molecular architecture, function and assembly of this key component of the photosynthetic membrane and will enable us to understand how energy is transferred to the photosynthetic reaction centres.

Ultrathin carbon nanomembranes (CNM) comprising crosslinked biphenyl precursors have been tested as support films for energy-filtered transmission electron microscopy (EFTEM) of biological specimens. Due to their high transparency CNM are ideal substrates for electron energy loss spectroscopy (EELS) and electron spectroscopic imaging (ESI) of stained and unstained biological samples. Virtually background-free elemental maps of tobacco mosaic virus (TMV) and ferritin have been obtained from samples supported by ~ 1 nm thin CNM. Furthermore, we have tested conductive carbon nanomembranes (cCNM) comprising nanocrystalline graphene, obtained by thermal treatment of CNM, as supports for cryoEM of ice-embedded biological samples. We imaged ice-embedded TMV on cCNM and compared the results with images of ice-embedded TMV on conventional carbon film (CC), thus analyzing the gain in contrast for TMV on cCNM in a quantitative manner. In addition we have developed a method for the preparation of vitrified specimens, suspended over the holes of a conventional holey carbon film, while backed by ultrathin cCNM.

Two different thylakoid lipids are specifically associated with the light-harvesting complex of photosystem II (LHC-II). Digalactosyl diacyl glycerol (DGDG) binds to the isolated complex but can be removed by mild detergent treatment and anion-exchange chromatography. Removal of this lipid renders the complex unable to form two-dimensional or three-dimensional crystals. The ability to crystallize is completely restored by addition of pure DGDG, at a ratio of about four molecules per polypeptide for three dimensional crystals, suggesting several binding sites at the periphery of the trimeric complex. Two-dimensional crystals of purified protein grown in the presence of DGDG are more highly ordered than those obtained from the unfractionated complex. The other lipid, phosphatidyl glycerol (PG), binds more firmly and cannot be removed with non-ionic detergent. Complete delipidation of LHC-H can be achieved either with phospholipase or by proteolytic cleavage of 49 amino acid residues at the N terminus. Both treatments dissociate the native, trimeric complex into monomers. This indicates that PG is directly involved in the formation of trimers, which are a prerequisite for two dimensional and three-dimensional crystallization. Both lipids are therefore present in two dimensional and three-dimensional crystals and have distinct roles in the structure of the complex.

The surface roughness of carbon films, which are used as a specimen support in high-resolution electron microscopy, has been investigated by atomic force microscopy. Carbon films were prepared by evaporating carbon onto mica. We found that the carbon surface that had been in contact with the mica was between 3 and 9 times smoother than the surface which had faced the carbon source. Surfaces of carbon films prepared by multiple evaporation were smoother than films evaporated in a single step. The surface roughness on the mica side of these films was close to that of mica. Two-dimensional crystals of plant light-harvesting complex yielded isotropically sharp high-resolution electron diffraction patterns at high tilt angles only when supported on the smoothest carbon films, produced by multiple evaporation.

Corrigendum to “Structural Asymmetry in a Trimeric Na/Betaine Symporter, BetP, from Corynebacterium glutamicum” [J. Mol. Biol. 407/3 (2011) 368–381] Ching-Ju Tsai, Kamil Khafizov, Jonna Hakulinen, Lucy R. Forrest⁎, Reinhard Kramer, Werner Kuhlbrandt and Christine Ziegler⁎ Department of Structural Biology, Max Planck Institute of Biophysics, 60438 Frankfurt am Main, Germany Computational Structural Biology Group, Max Planck Institute of Biophysics, 60438 Frankfurt am Main, Germany Institut of Biochemistry, University of Cologne, Zulpicher Str. 47, 50674 Koln, Germany

The structure of the light-harvesting chlorophyll a b - protein complex has been determined at 3.7 A resolution in projection by electron diffraction, electron microscopy and image analysis. Diffraction patterns and high-resolution spotscan images of two-dimensional crystals stabilized with tannin were recorded at low temperature. Phases of structure factors were obtained directly by image processing, after correction of the images for lattice distortions, defocus and beam tilt. Amplitudes were measured by electron diffraction. The projection map shows the detailed structure of the trimeric complex, suggesting the positions of two domains of potential structural and functional homology, of one membrane-spanning α-helix approximately perpendicular to the membrane plane and of several tightly bound lipid molecules.

A contrast variation method is described by which protein and nucleic acid components of nucleoprotein assemblies can be distinguished in the electron microscope. Using contrasting media of variable electron scattering density, the contribution to image contrast of protein or nucleic acid can be matched out. The protein and DNA components of T4 bacteriophages were visualized separately in this way. The distribution of RNA and protein in ribosomes was studied by processing images of crystalline sheets of ribosomes embedded in a range of contrasting media. Projection maps of crystalline ribosomes suggest that the ribosomal RNA is located predominantly in the central region of the particle.

The structure of thin three-dimensional crystals of the light-harvesting chlorophyll a b protein complex, an integral membrane protein from the photosynthetic membrane of chloroplasts, has been determined at 7 A (1 A = 0.1 nm) resolution in projection. The structure analysis was carried out by image processing of low-dose electron micrographs, and electron diffraction of thin three-dimensional crystals preserved in tannin. The three-dimensional crystals appeared to be stacks of two-dimensional crystals having p321 symmetry. Results of the image analysis indicated that the crystals were disordered, due to random translational displacement of stacked layers. This was established by a translation search routine that used the low-resolution projection of a single layer as a reference. The reference map was derived from the symmetrized average of two images that showed features consistent with the projected structure of negatively stained two-dimensional crystals. The phase shift resulting from the displacement of each layer was corrected. Phase shifts were then refined by minimizing the phase residual, bringing all layers to the same phase origin. Refined phases from different images were in agreement and reliable to 7 A resolution. A projection map was generated from the averaged phases and electron diffraction amplitudes. The map showed that the complex was a trimer composed of three protein monomers related by 3-fold symmetry. The projected density within the protein monomer suggested membrane-spanning α-helices roughly perpendicular to the crystal plane. The density in the centre and on the periphery of the trimeric complex was lower than that of the protein, indicating that this region contained low-density matter, such as lipids and antenna chlorophylls.

Steady-state and picosecond time-resolved fluorescence techniques in conjunction with circular dichroism have been used to study the light-harvesting chlorophyll-a/b protein complex (LHC) isolated from pea chloroplasts. In particular, the effect of changing the detergent / chlorophyll ratio on the state of the LHC has been investigated. Our results have been interpreted in light of the known protein geometry of the LHC in 2-dimensional crystals (Kuhlbrandt, W. (1984) Nature 307, 478–479). The fluorescence lifetime data reveals 1 / e-lifetimes of 3.53 (±0.04) ns and 1.10 (±0.01) ns for a stable, efficiently energy-transferring state of the LHC. Subnanosecond lifetimes are observed under conditions leading to aggregation, while a long component of 5.50 (±0.16) ns corresponding to free Chl a is found when the detergent / chlorophyll ratio is high. The circular dichroism shows a major Chl-b exciton, a Chl-a / b exciton and a further ‘quenching’ Chl-b exciton. These have been attributed to: a C3 symmetric Chl-b interaction for which the intact C3 protein trimer geometry is a prerequisite; a dimeric Chl-a / b interaction, the presence of which is critically dependent on the detergent type; and a further Chl-b interaction which arises from the presence of aggregated trimers, respectively. We have found that the degree of heterogeneity with respect to the oligomeric state of the pigment-protein trimers is dependent upon the detergent / chlorophyll ratio used. Low detergent / chlorophyll ratios result in extensive aggregation of the trimers with a geometry similar to that found in 2-dimensional crystals of the LHC. Moderate detergent conditions yield predominantly non-aggregated trimers. Excess detergent conditions result in considerable chromophore heterogeneity and loss of the main Chl-b exciton consistent with protein denaturation through an initial break up of the trimer geometry. From these results we believe that in vitro the minimum stable functional unit corresponds to a C3 symmetric protein trimer.

Two forms of three-dimensional crystals of the light-harvesting chlorophyll a b protein complex from pea have been obtained. Crystals of one form grew as hexagonal plates measuring up to 150 μm across and 2 to 3 μm in thickness. Electron diffraction patterns of thin hexagonal plates showed sharp reflections to a resolution of 3.7 A on a hexagonal reciprocal lattice. The unit cell in projection ( a = 127.0 A ) and the symmetry of the diffraction pattern (6 mm) suggested that the hexagonal plates were highly ordered stacks of two-dimensional crystals suitable for structure analysis by electron microscopy and image processing. Crystals of a second form grew as dark green octahedra measuring roughly 0.5 mm across. Low-resolution X-ray diffraction patterns suggested a large cubic unit cell ( a = 390 A ). SDS/polyacrylamide gel electrophoresis of single octahedral crystals showed the same polypeptide composition as the starting solution, one major band at 24,000 apparent molecular weight and two satellite bands of 23,000 and 23,500 apparent molecular weight.