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Plants absorb sunlight via photosynthetic pigments and convert light energy intochemical energy in the process of photosynthesis. These pigments are mainly bound to antenna protein complexes that funnel the excitation energy to the photosynthetic reaction centres. The peripheral antenna of plant photosystem II (PSII) consists of the major light-harvesting complex of PSII (LHC-II) and the minor LHCs CP29, CP26 and CP24. Light intensity can change frequently and plants need to adapt to high-light conditions in order to avoid photodamage. When more photons are absorbed than can be utilised by the photosynthetic machinery, excessive excitation energy is dissipated as heat by short-term adaptation processes collectively known as non-photochemical quenching (NPQ). A decrease in PSII antenna chlorophyll (Chl) fluorescence yield and a reduction in the average Chl fluorescence lifetime are associated with NPQ. The main component of NPQ is the so-called energy-dependent quenching (qE), and it is triggered by the rapid drop in thylakoid lumenal pH resulting from the plant’s photosynthetic activity. This process is thought to take place at the PSII antenna complexes, which therefore not only capture and transfer light energy but are also involved in balancing the energy flow. The decrease in lumenal pH acivates the enzyme violaxanthin de-epoxidase (VDE), which converts the xanthophyll violaxanthin (Vio) into zeaxanthin (Zea) in the xanthophyll cycle. In addition, the PSII subunit PsbS was discovered to be essential for qE by screening qE-deficient Arabidopsis thaliana mutants. This membrane protein is considered a member of the LHC superfamily, which also includes LHC-II and the minor LHCs. Previous studies on PsbS isolated either from native source or refolded in vitro have produced inconsistent results on its pigment binding capacity. Interestingly, a pH-dependent change in the quaternary structure of PsbS under high light conditions has been reported. This observed dimer-tomonomer transition very likely follows the protonation of lumenal glutamates upon the drop in pH and is accompanied by a change in PSII supercomplex localisation. PsbS dimers are preferentially found in association with the PSII core, whereas PsbS monomers co-localise with LHC-II.Despite the identification of !pH, Zea and PsbS as key players in qE, both the nature of the quencher(s) as well as the underlying molecular mechanism leading to excess energy dissipation still remain unknown. Several models have been put forward to explain the reversible switch in the antenna from an energy-transmitting to a quenched state. Proposals include a simple pigment exchange of Vio for Zea, and aggregation or an internal conformational change of LHC-II. Charge transfer (CT)quenching in the minor LHCs or quenching by carotenoid dark state (Car S1)-Chl interactions have also been suggested. However, none of these qE models has so far been capable of accommodating all the physiological observations and available experimental data. Most importantly, the function of PsbS remains an enigma. A recent qE model suggested that monomerisation of PsbS enables the protein to transiently bind a carotenoid and form a quenching unit with a Chl of a PSII LHC. In view of the various proposed qE mechanisms, this thesis aimed at understanding the interplay of the different qE components and the contribution of the PSII subunits LHC-II, the minor LHCs and PsbS to qE. The initial approach was to investigate the properties of the PSII subunits in the most simple in vitro model system, namely in detergent solution. For this purpose, LHC-II was isolated either from native source or refolded from recombinantly produced protein. Investigation of the minor LHCs and PsbS required heterologous expression and refolding. In addition, experiments were performed on aggregated LHC-II. Aggregates of LHC-II have been used as a popular model system for qE because they exhibit highly quenched Chl fluorescence. At the final stage of this doctoral work, a more sophisticated model system to approximate the thylakoid membrane was developed by reconstitution of the PSII subunits LHC-II and PsbS into liposomes. This system not only allowed for investigation of these membrane proteins in their native environment, but also for mimicking the xanthophyll cycle by distribution of Zea within the membrane as well as !pH by outside buffer exchange. The role of Zea in qE was first investigated with detergent solubilised antenna proteins. The requirement of this xanthophyll for qE is well-known, but the specific contribution to the molecular quenching mechansim is unclear. Previous work had shown that replacement of Vio for Zea in LHC-II was not sufficient to induce Chl fluorescence quenching in Zea-LHC-II, as suggested by the so-called molecular gearshift mechanism. However, by means of selective two-photon excitation spectroscopy, an increase in electronic interactions between Car S1 and Chls was observed for LHC-II upon lowering the pH of the detergent buffer. Electronic Car S1-Chl coupling became even stronger when Zea-LHC-II was probed. The extent of Car S1-Chl coupling correlated directly with the extent of Chl fluorescence quenching, in a similar way as observed previously in live plants under high-light conditions. However, very similar results were obtained with LHC-II aggregates. This implied that the increase in electronic interactions and fluorescence quenching was independent of Zea and low pH. Further experiments on aggregates of LHC-II Chl mutants indicated that the targeted pigments were also not essential for the observed effects. It is proposed that the same molecular mechanism causes an increase in electronic Car S1-Chl interactions and Chl fluorescence quenching in Zea-LHC-II at low pH as well as in aggregated LHC-II. Most likely, surface exposed pigments form random quenching centres in both cases. On the other hand, it was possible that Zea could act as a direct quencher of excess excitation energy in the minor LHCs. However, enrichment of refolded CP29, CP26 and CP24 with Zea did not lead to a change in the Chl excited state lifetime. Formation of a carotenoid radical cation, previously implied in CT quenching, was also not observed, although artificial generation of such a radical cation was principally possible as shown for CP29. During the course of this work, a study reporting the formation of Zea radical cations in minor LHCs was published. Therefore, Zea-enriched minor LHCs were again investigated on the experimental apparatus used in the reported study. Indeed, the presence of at least one carotenoid radical cation for each minor complex was detected. It is suggested that either the preparation method of incubating the refolded minor LHCs with Zea in contrast to refolding the complexes with only Zea and lutein causes the observed differences or that the observed spectral radical cation signatures are due to experimental artifacts. While the experiments with LHC-II and the minor LHCs gave useful insights into the putative qE mechanism, the quencher site and the mode of action of Zea could still not be unambiguously identified. Most importantly, these studies could not explain the function of the qE keyplayer PsbS. Therefore, the focus of the work was shifted to PsbS protein production, purification and characterisation. In view of inconsistent reports on the pigment binding capacity of this PSII subunit, refolding trials with and without photosynthetic pigments were conducted. The formation of a specific pigmentprotein complex typical for other LHCs was not observed and neither was the earlier reported “activation” of Zea for qE by binding to this protein. Nevertheless, PsbS refolded without pigments displayed secondary structure content in agreement with previous studies, indicating pigment-independent folding. Reconstitution of pigmentfree, refolded PsbS into liposomes confirmed that the protein is stable in the absence of pigments. Zea distributed in PsbS-containing liposomes also showed no spectral alteration that would indicate its “activation”. With the ability to reconstitute PsbS, it was then possible to proceed to modelling qE in a proteoliposome system. For this purpose, PsbS was co-reconstituted with LHC-II, which has been reported to interact with PsbS. One-photon excitation (OPE) and two-photon excitation (TPE) spectroscopy measurements were performed on LHC-II- and LHC-II/PsbS-containing liposomes. This enabled both quantification of Chl fluorescence quenching as well as determination of the extent of electronic Car S1-Chl interactions. The effect of Zea was investigated by incorporating it in the proteoliposome membrane. It was shown that Zea alone was not able to induce significant Chl fluorescence quenching when only LHC-II was present. However, when LHC-II and PsbS were co-reconstituted, pronounced Chl fluorescence quenching and an increase in electronic Car S1-Chl interactions were observed and both effects were enhanced when Zea was present. Western blot analysis indicated the presence of a LHC-II/PsbS-heterodimer in these proteoliposomes. In addition to the OPE and TPE measurements, the average Chl fluorescence lifetime was determined in detergent-free buffer at neutral pH and directly after buffer exchange to low pH. No significant changes in the average lifetime were observed for LHC-II proteoliposomes when either Zea was present or after exchange for low pH buffer. This indicated that Zea alone cannot act as a direct quencher, which concurs with the OPE measurements. Moreover, the complex was also properly reconstituted as no aggregation or significant Chl fluorescence quenching were observed. The average lifetime was not significantly affected in LHC-II/PsbS-proteoliposomes, independent of Zea or pH. However, a shortlived component in the presence of a long-lived component was not resolvable with the time resolution of the fluorescence lifetime apparatus.
Implications for qE model systems and the in vivo quenching mechanism are discussed based on the experiments in detergent solution, on LHC-II aggregates and with the proteoliposome model system.
Channelrhodopsin-2 (ChR2) is a light-gated cation selective channel from the unicellular alga Chlamydomonas reinhardtii, which is involved in phototaxis and photophobic responses. As other rhodopsins, ChR2 comprises a seven-transmembrane helix (TMH) motif and a retinal as the light-sensitive chromophore. The chromophore is covalently attached via a protonated Schiff base to the conserved lysine residue Lys257 located in TMH7. Based on its primary sequence and the all-trans configuration of the retinal in the ground state, ChR2 is assigned to the type I rhodopsins, also referred to as microbial-type rhodopsins. Upon light activation, the retinal isomerizes from the all-trans to the 13-cis form. This photoisomerization, which is accompanied by conformational changes of the protein, eventually leads to the opening of the channel and cation translocation. Cation flux during the conductive state leads to depolarization of the cell membrane and subsequent triggering of action potentials when expressed in neurons. Therefore, ChR2 has become the most versatile optogenetic tool, enabling a non-invasive investigation of neural circuits at high spatial and temporal resolution. With the rapidly increasing importance of ChR2 as a tool in neurobiology and cell biology, structural information is the prerequisite to an unambiguous understanding of the molecular mechanisms of this unique light-activated ion channel. The coupling between isomerization and structural alterations is well understood for other microbial-type rhodopsins, like bacteriorhodopsin (bR), halorhodopsin (HR) and sensory rhodopsin II (SRII). In case of ChR2, the first data on light-induced conformational changes came from spectroscopic studies and structural information is still missing. However, in order to fully understand the mechanism of light transduction by ChR2, it is necessary to determine the changes in the protein structure at specific steps in the photocycle.
By the time I started my PhD thesis, there was no structural information of ChR2 available. Therefore, the objective of this thesis was to obtain structural information of the transmembrane domain containing the first 315 amino acids of ChR2 by cryo electron crystallography. Besides revealing the structure of membrane proteins, cryo-EM of two-dimensional (2D) crystals is ideal for investigating conformational changes in membrane proteins induced by different stimuli. Therefore, the second objective of my thesis was the investigation of light-induced conformational changes in the slow C128T ChR2 mutant. The ~1,000 times longer lifetime of the open state of the C128T mutant compared to the wild-type allowed to trap different intermediates that accumulate during the photocycle.
In 2012, the X-ray structure of a channelrhodopsin-1/channelrhodopsin-2 chimaera (C1C2) at 2.3 Å resolution in the closed dark-adapted state was published (Kato et al., 2012). The structure revealed the essential molecular architecture of C1C2, including the retinal-binding pocket and the putative cation conduction pathway. Together with biochemical, spectroscopic, mutagenesis experiments, and the high-resolution model, some functionally important residues of ChR2 have been identified. However, unambiguous explanation of the molecular determinants that contribute to activation (gating) and transport were still mostly unknown.
RESULTS AND CONCLUSIONS
The first half of my theses dealt with 2D crystallization of ChR2. I succeeded in obtaining 2D crystals of ChR2 of four different types, which differed in size, crystal packing, crystal contacts and resolution, yielding structure factors up to 6 Å resolution. The crystals were grown by reconstituting the protein with different lipids at various lipid-to-protein ratios. The best crystals formed with the synthetic lipid DMPC and EPL upon detergent removal by dialysis. The projection maps calculated from these crystals revealed the overall structure of C128T ChR2 at 6 Å resolution and were published in 2011 (Müller et al., 2011). Surprisingly, ChR2 was found to be a dimer in all crystal types. The ChR2 dimer was stable both in detergent solution and in the presence of lipids for 2D crystallization. The monomers clearly showed the expected densities for the seven TMHs.
The arrangement of the ChR2 dimers on the four 2D lattices was different. However, comparison of the individual rojection maps revealed no significant differences within the ChR2 interface in the four crystal forms. The observation that the structure of the dimer was the same in all four crystal forms and in different lipids suggested strong specific contacts between the two protomers and implied that the protein was also dimeric in the native membrane. These findings were in agreement with Western blot analysis of plasma membranes from oocytes expressing ChR2 and laser-induced liquid bead ion desorption mass spectrometry, which both showed ChR2 as a dimer. The unusual stability of the ChR2 dimer contrasts with other microbial rhodopsins, which exist in different oligomeric states, i.e. monomers, trimers or dimers. These observations raised the question whether the functional unit is the monomer or the dimer.
The comparison of the projection map of the light-driven proton pump bR at the same resolution showed similar overall dimensions. Based on this comparison, the densities which became evident in the ChR2 projection maps could be assigned to the corresponding seven densities in bR. The shape of the densities near the dimer interface suggested that TMHs 2, 3, and 4 are oriented more or less perpendicular to the membrane plane, while the other four helices appear to be more tilted, as in bR.
Based on the high-resolution bR structure and the projection structures obtained, I have built a homology model. On the basis of this homology model, several residues found in the dimer interface were selected for mutational studies in order to disrupt the dimer interface.
The investigation of light-induced conformational changes in C128T ChR2 was the second part of my thesis. I designed an experimental setup for trapping light-induced conformational changes in C128T ChR2. In addition, I optimized the sample preparation in a way that the different illumination conditions did not alter the quality of the crystals. I have trapped two different functional states, namely the conductive open state and the non-conductive closed dark-adapted state.
In order to visualize the location and the extent of conformational changes, projection difference maps were calculated between the open and the closed state. Visual inspection of the difference maps between the open and the two closed states revealed three difference peaks that map to the TMHs 2, 6, and 7, indicating significant and specific rearrangements of these helices. The strong pair of positive/negative peaks at TMH6 suggests an outward tilt movement of approximately 2 Å. Close comparison of similar work on bR revealed that this movement is likely to occur at the cytoplasmic end of TMH6. A second highly significant negative peak is observed at TMH7, indicating a less pronounced tilt compared to TMH6. The third negative peak at TMH2 indicates a loss of density in this region. No significant differences were recorded at the TMH1, 5 and at the dimer interface formed by TMH3 and 4.
I succeeded in trapping and characterizing the open and closed state in the photocycle of ChR2 and could demonstrate that the transition from the closed to the open state is linked to significant light-induced tilt movements of TMH6 and 7, plus a loss of order in TMH2. These conformational changes are likely to create a large water-filled conducting pore, which seems to be required for the conductance of up to 2,000 ions per photocycle. The previously mentioned spectroscopic studies support the difference structures I obtained. This approach sets the stage for studying structural changes accompanying the formation and decay of other photocycle intermediates in ChR2. Future studies will aim at three-dimensional maps of the open and closed state at higher resolution.
ATP synthases are multi-subunit membrane enzymes, which utilize the energy stored in a transmembrane electrochemical ion gradient to produce adenosine-5´-triphosphate (ATP), the universal energy carrier in biological systems. Research on these important enzymes goes back more than 50 years and has produced innumerable studies. The F-type ATP synthase consists of two functionally distinct, but tightly coupled subcomplexes, the water-soluble F1 and the membrane-embedded Fo complex. In its simplest form, F1 consists of five different subunits with a stoichiometry of α 3β3γδε, and harbors three catalytic centers in the α 3β3-headpiece, while Fo consists of three different subunits in a stoichiometry of ab2cn, where n varies between 8 to 15 depending on the species. From a mechanistic standpoint, the complex can also be divided into two different units, namely a stator, α3β3δ-ab2, and a rotor, γε-cn. The enzyme utilizes the energy stored in a transmembrane electrochemical gradient of protons, or in some cases Na+, to drive ATP synthesis. In particular, the downhill translocation of these ions across the Fo complex drives rotation of the γε-cn unit, which is then transduced to the active centers, catalyzing the phosphorylation of adenosine-5`-diphosphate (ADP) with inorganic phosphate (Pi), and the release of ATP....