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Die bei der Photosynthese verwendete Lichtenergie wird zu einem großen Anteil von Lichtsammlersystemen bereitgestellt. In der pflanzlichen Photosynthese wird unterschieden zwischen Lichtsammlersytem I (light harvesting complex I, LHC-I), assoziiert mit Photosystem I (PS-I) und Lichtsammlersystem II (light harvesting complex II, LHC-II), assoziiert mit Photosystem II (PS-II). LHC-II ist der häufigste Protein-Pigment Komplex der Chloroplasten und bindet bis zu 50% aller Chlorophylle in der Thylakoidmembran. Der Protein-Pigment Komplex LHC-II hat vier, teils miteinander verwandte Funktionen in der Photosynthese. I) Die Sammlung und Weiterleitung von Lichtenergie, II) Stabilisierung der Granastapel, III) Ausgleich der Anregungsenergie von PS-I und PS-II, IV) Schutz der Photosynthese vor Überanregung mittels nichtphotochemischer Eliminierung von Anregungsenergie (NPQ). In der Pflanze bildet LHC-II Trimere in verschiedenen Kombinationen dreier Isoformen (Lhcb1, Lhcb2 und Lhcb3), wobei Lhcb1 mit 70-90% den Hauptteil des LHC-II stellt. Jedes Monomer bindet 8 verschiedene Co-Faktoren in unterschiedlichen Mengen, die ca. 30% seiner Masse ausmachen. Die drei Isoformen des LHC-II sind in allen Pflanzen stark konserviert. Die funktionelle Bedeutung der Isoformen ist jedoch weitestgehend unklar. Dies liegt vor allem an der schwierigen Isolierung reiner Isoformen aus Pflanzenmaterial. Im ersten Teil dieser Arbeit wurden deshalb alle drei Isoformen rekombinant hergestellt und mit getrennt isolierten Lipiden und photosynthetischen Pigmenten in ihre native Form gefaltet. Die anschließende biochemische und spektroskopische Charakterisierung zeigte einen hohen Grad an Homologie zwischen den drei Isoformen, wobei Lhcb3 die größten Unterschiede aufwies (Standfuss und Kühlbrandt 2004). Die wahrscheinlichsten Funktionen für Lhcb1 und Lhcb2 ist die Anpassung der Photosynthese an variierende Lichtbedingungen. LHC-II Heterotrimere mit Lhcb3 Anteil könnten an der Weiterleitung von Lichtenergie von der Haupt Lhcb1/Lhcb2 Antenne zum PS-II Reaktionszentrum beteiligt sein. Für die Erforschung des LHC-II war das mittels Cryo-Elektronenmikroskopie an 2D Kristallen erstellte atomare Modell des Komplexes von enormer Bedeutung. Ein tiefes Verständnis der Funktionen des LHC-II benötigt jedoch eine Struktur von höherer Auflösung, welche mit 2D Kristallen nur schwer zu erreichen ist. Im Verlauf der Arbeit wurden deshalb mehr als 100000 3D Kristallisationsexperimente durchgeführt, wodurch die Kristallisation von aus Erbsenblättern isoliertem und in vitro gefaltetem LHC-II gelang. Die 3D Kristalle aus nativem Material zeigten einen für die röntgenkristallographische Strukturaufklärung ausreichenden Ordnungsgrad und führten zu einer Struktur des LHC-II bei 2.5 Å Auflösung (Standfuss et al., eingereicht). Die Struktur zeigt 223 der 232 Aminosäuren und die Position und Orientierung von 4 Carotinoiden (2 Luteine, 1 Neoxanthin und 1 Violaxanthin), 14 Chlorophyllen (8 Chl a und 6 Chl b) und zwei Lipiden (PG und DGDG) pro Monomer. Diese Informationen sind essentiell für das Verständnis des Energietransfers innerhalb des LHC-II und zu den Photoreaktionszentren und sollten zusammen mit der großen Anzahl von spektroskopischen Untersuchungen eine zukünftige detaillierte Modellierung dieser ultraschnellen und extrem effizienten Energietransfer Prozesse ermöglichen. Auf Basis der Ladungsverteilung der stromalen Seite des Komplexes konnte ein Modell für die Beteiligung des LHC-II an der Stapelung von Grana in Chloroplasten erstellt werden. Dieses liefert außerdem eine plausible Erklärung für den mittels Phosphorylierung des N-Terminus gesteuerten Ausgleich von Anregungsenergie zwischen PS-I und PS-II. Die 2.5 Å Struktur des LHC-II zeigt schließlich einen einfachen aber effektiven Mechanismus zur Optimierung und Schutz des Photosyntheseapparates mittels NPQ. Dieser benötigt keine Strukturänderungen des LHC-II oder der restlichen Lichtsammelantenne und beruht auf der reversiblen Bindung der Xanthophylle Violaxanthin und Zeaxanthin an LHC-II. Diese Arbeit liefert damit Beiträge zu allen Funktionen des LHC-II Komplexes und hilft damit grundlegende Regulationsmechanismen und die Bereitstellung von solarer Energie für die pflanzliche Photosynthese zu verstehen.
The universal biological energy currency adenosine triphosphate (ATP) is synthesized by the F1Fo-ATP synthase in most living organisms. The overall structure and function of F-type ATPases is conserved in the different organisms. The F1Fo-ATP synthase consist of two domains; the soluble F1 complex has the subunit stoichiometry α3β3γδε and the membrane embedded Fo complex consists of subunits ab2c10-15 in its simplest form found in bacteria. F1 and Fo both function as reversible rotary motors that are connected by a central stalk (γε) and a peripheral stalk (b2δ).
For ATP synthesis, the electrochemical energy formed by a proton or sodium ion gradient is required. The ion translocation across the Fo subcomplex induces torque in the motor part of the enzyme (cnγε), which causes conformational changes in the α3β3 domain leading to ATP synthesis from ADP and inorganic phosphate (Pi) catalyzed in the β-subunits. ATP hydrolysis causes a reverse torque in the Fo subcomplex triggering uphill ion translocation from cytoplasm to periplasm, and the enzyme functions as an ion pump.
The ATP synthesis mechanism is well understood, since several high-resolution structures of F1 are available. In contrast, the ion translocation mechanism across the membrane, mediated by the Fo subcomplex, is not understood in its structural detail.
Subunit a and the c-ring form an ion pathway, but subunit b is needed to form an active ion translocation pathway in both H+- and Na+-dependent systems. Several high-resolution structures of c-rings have provided insights in the ion translocation mechanism. The different ion translocation models based on biochemical, biophysical and structural analysis are in agreement in the fact that ions are translocated through a periplasmic ion access pathway in subunit a to the middle of the membrane and there to the binding site of a c-subunit. After almost a whole rotation of the c-ring the ion returns into the a-c interface, where it can be released to the cytoplasm. In the different models the cytoplasmic access pathway has been proposed to be located in subunit a, at the a-c interface or within the c-ring. The driving force of torque generation has been proposed to be the pH gradient or membrane potential. Several biochemical studies show that a conserved arginine in helix four of subunit a (R226 in Ilyobacter tartaricus or R210 in Escherichia coli)plays a critical role in the ion translocation. The arginine has been proposed to function as an electrostatic separator between the cytoplasmic and periplasmic pathways and as a mediator of the ion exchange into the c-ring ion-binding site.
Structural data of a related enzyme (V1Vo-ATPase from Thermus thermophilus) has provided insight into the helical arrangement of the ion translocating subunits I and Lring (related to subunit a and the c-ring). These structures indicated a small interface between subunit I and the L-ring, and two four-helix bundles in the N-terminal domain of subunit I were proposed to build the periplasmic and cytoplasmic ion pathways. To comprehend the ion-translocation and torque generation mechanism in F1Fo-ATP synthase, structural data of an intact a-c complex is needed.
The goal of this work was to obtain structural data of subunit a, most preferably in a complex with the c-ring or additionally with subunit b. Therefore, a new purification procedure for the I. tartaricus Fo-subcomplex, heterologously expressed in E. coli cells, was established. The purified Fo was characterized biochemically and by Laserinduced liquid bead ion desorption mass spectrometry (LILBID-MS). These analyses showed that pure and completely assembled Fo containing all its subunits in the correct stoichiometry (ab2c11) was obtained. The purified Fo complex was stable at 4°C for several months and at room temperature in the presence of lipids for several weeks. A lipid analysis was performed by thin-layer chromatography (TLC) to investigate the qualitative lipid composition of I. tartaricus whole lipid extract and various I. tartaricus F1Fo isolates. The whole lipid extract contained PC, PG and PE lipids and probably cardiolipin. PC, PG and PE lipids were bound to wild type I. tartaricus F1Fo, whereas recombinant I. tartaricus F1Fo did not have any bound lipids, but was able to bind the synthetic lipids POPC and POPG if they were provided during the purification.
For subsequent structural studies the purified Fo was subjected to two-dimensional (2D) crystallization trials. Vesicles and sheets tightly packed with protein and crystals with a rare plane group for I. tartaricus c11 (p121) were obtained. The c-ring was visible in the CCD images, and immunogold-labeling revealed the presence of the His-tagged a-subunit in the reconstituted vesicles. Furthermore, atomic force microscopy (AFM) imaging showed protein densities next to the c-rings, which protruded less from the membrane (0.4±0.1 nm) than the c-ring (0.7±0.1 nm). These protein densities presumably belonged to subunit a.
Cryo-electronmicroscopy (cryo-EM) was used to collect data of the p121 crystals and a merged projection density map was calculated to 7.0 Å resolution. The unit cell of the crystals (81 × 252 Å) contained two asymmetric units with three c-rings in each and next to the c11-rings new prominent densities were visible. In each extra density up to 7 transmembrane helices were visible, belonging to the stator subunit a and/or subunit b. To elucidate whether there are conserved elements in the three extra densities non-crystallographic averaging was applied using a single-particle approach.
Six possible arrangements for the c-rings and the extra densities were identified and used for the averaging. The extra densities were enhanced only in one of the possible arrangements. The average showed a four-helix bundle and a fifth helix in close proximity to the c-ring. Two more helices were present in each position but their position was ambivalent. The data obtained in this work provides the first insight in the helical arrangement in the a-c interface of F1Fo-ATP synthase.
The light-harvesting complex of photosystem II (LHC-II) is the major antenna complex in plant photosynthesis. It accounts for roughly 30% of the total protein in plant chloroplasts, which makes it arguably the most abundant membrane protein on Earth, and binds about half of plant chlorophyll (Chl). The complex assembles as a trimer in the thylakoid membrane and binds a total of 54 pigment molecules, including 24 Chl a, 18 Chl b, 6 lutein (Lut), 3 neoxanthin (Neo) and 3 violaxanthin (Vio). LHC-II has five key roles in plant photosynthesis. It: (1) harvests sunlight and transmits excitation energy to the reaction centres of photosystems II and I, (2) regulates the amount of excitation energy reaching each of the two photosystems, (3) has a structural role in the architecture of the photosynthetic supercomplexes, (4) contributes to the tight appression of thylakoid membranes in chloroplast grana, and (5) protects the photosynthetic apparatus from photo damage by non photochemical quenching (NPQ). A major fraction of NPQ is accounted for its energy-dependent component qE. Despite being critical for plant survival and having been studied for decades, the exact details of how excess absorbed light energy is dissipated under qE conditions remain enigmatic. Today it is accepted that qE is regulated by the magnitude of the pH gradient (ΔpH) across the thylakoid membrane. It is also well documented that the drop in pH in the thylakoid lumen during high-light conditions activates the enzyme violaxanthin de-epoxidase (VDE), which converts the carotenoid Vio into zeaxanthin (Zea) as part of the xanthophyll cycle. Additionally, studies with Arabidopsis mutants revealed that the photosystem II subunit PsbS is necessary for qE. How these physiological responses switch LHC-II from the active, energy transmitting to the quenched, energy-dissipating state, in which the solar energy is not transmitted to the photosystems but instead dissipated as heat, remains unclear and is the subject of this thesis. From the results obtained during this doctoral work, five main conclusions can be drawn concerning the mechanism of qE: 1. Substitution of Vio by Zea in LHC-II is not sufficient for efficient dissipation of excess excitation energy. 2. Aggregation quenching of LHC-II does not require Vio, Neo nor a specific Chl pair. 3. With one exception, the pigment structure in LHC-II is rigid. 4. The two X-ray structures of LHC-II show the same energy transmitting state of the complex. 5. Crystalline LHC-II resembles the complex in the thylakoid membrane. Models of the aggregation quenching mechanism in vitro and the qE mechanism in vivo are presented as a corollary of this doctoral work. LHC-II aggregation quenching in vitro is attributed to the formation of energy sinks on the periphery of LHC-II through random interaction with other trimers, free pigments or impurities. A similar but unrelated process is proposed to occur in the thylakoid membrane, by which excess excitation energy is dissipated upon specific interaction between LHC-II and a PsbS monomer carrying Zea. At the end of this thesis, an innovative experimental model for the analysis of all key aspects of qE is proposed in order to finally solve the qE enigma, one of the last unresolved problems in photosynthesis research.
This thesis presents a 5.9 Å map of yeast FAS obtained by cryo-electron microscopy using single particle analysis (SPA). The EM-map has been analyzed both by quantitative and qualitative analysis to aid in understanding of the structure and dynamics of yeast FAS. This study approaches the factors limiting the resolution in EM (>20 Å) and further discusses the possibilities of achieving higher-resolutions (<10 Å) in cryo-EM by single particle analysis. Here, SPA is highlighted as a powerful tool for understanding the structure and dynamics of macro-molecular complexes at near native conditions. Though SPA has been used over the last four decades, the low-resolution range (20-30 Å) of the method has limited its use in structural biology. Over the last decade, sub nanometer resolution (<10 Å) structures solved by SPA have been reported --both in studies involving symmetric particles, such as GroEL (D7) and asymmetric particles, such as ribosomes (C1). Recently, near-atomic resolution in the range of 3.8-4.2 Å has been achieved in cases of highly symmetric icosahedral viral capsid structures as well. The yeast FAS structure (D3) presented here is one of two low symmetry structures submitted to the EM-database in a resolution range of 5-6 Å; the other being GroEL (D7). Fatty acid synthase (FAS) is the key enzyme for the biosynthesis of fatty acids in living organisms. There are two types of FAS, namely the type II FAS system in prokaryotes, consisting of a set of individual enzymes, and type I FAS found in eukaryotes as a multienzyme complex. Yeast fatty acid synthase (FAS) is a 2.6 MDa barrel-shaped multienzyme complex, which carries out cyclic synthesis of fatty acids. By electron cryomicroscopy of single particles we obtained a 3D map of yeast FAS at 5.9 Å resolution. Compared to the crystal structures of fungal FAS, the EM map reveals major differences and new features that indicate a considerably different arrangement of the complex in solution, as well as a high degree of variance inside the barrel. Distinct density regions in the reaction chambers next to each of the catalytic domains fit well with the substratebinding acyl carrier protein (ACP) domain. In each case, this resulted in the expected distance of ~18 Å from the ACP substrate binding site to the active site of the catalytic domains. The multiple, partially occupied positions of the ACP within the reaction chamber provide direct insight into the proposed substrate-shuttling mechanism of fatty acid synthesis in this large cellular machine.
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.
Rotary adenosine triphosphate (ATP)ases are ubiquitous, membrane-bound enzyme complexes involved in biological energy conversion. The first subtype, the so-called F1Fo ATP synthase, predominantly functions as an ATP synthesizing machinery in most bacteria, mitochondria and chloroplasts. The vacuolar subtype of enzyme, the V1Vo ATPase, operates as an ATP driven ion pump in eukaryotic membranes. The subtype found in archaea and some bacteria is called A1Ao ATP (synth)ase and is capable of working in both directions either to synthesize ATP or to generate an ion motive force by consuming the same.
All the three above-mentioned subtypes of rotary ATPases work as nanomolecular machines sharing a conserved mechanism to perform the energy conservation process. The simplest form of these enzymes is the bacterial F1Fo ATP synthase. Here, ions are channelled via the membrane stator subunit a to the rotor ring of the enzyme. After almost a complete rotation of the ring the ions are released again on the other side of the membrane. This rotation is further transmitted via the central stalk to the soluble part of the enzyme, the F1-complex, where conformational changes within the nucleotide binding sites result in the synthesis of ATP from ADP and Pi.
The rotor or c-ring of the enzyme is the key protein complex in mediating transmembrane ion translocation. Several structural and biochemical methods have been applied in the past years to study the rotor rings from many different organisms. The results revealed that the stoichiometry of a c-ring of a given species is constant while it can vary between different species within a range of 8 to 15 c subunits. The c-ring stoichiometry determines directly the number of ions transported through Fo per rotation whereby three molecules of ATP are concurrently synthesized in the water-soluble F1 headgroup. Hence the number of c subunits has an important influence on the bioenergetics of the corresponding enzyme and thus the entire organism.
The c-ring of a rotary ATPase is able to specifically bind either protons (H+) or sodium ions (Na+) as the coupling ion for the enzyme. Several structures are already available revealing the coordination network of both types of rotor rings. In each case ion binding includes a highly-conserved carboxylic acid residue (glutamate or aspartate), in addition to a more varying combination of amino acid residues, whereby Na+ coordination is structurally more demanding than H+ binding.
In the first part of my PhD thesis, I aimed to characterize the F1Fo ATP synthase rotor ring of the opportunistic pathogenic bacterium Fusobacterium nucleatum on a functional and structural level. F. nucleatum is an anaerobic bacterium which uses peptides and amino acids as a primary energy source. It is one of the most frequently occuring bacteria in human body infections and involved in human periodontal diseases.
The protein complex was heterologously expressed within a hybrid ATP synthase in Escherichia coli and purified without an affinity tag for further analysis. Two high resolution X-ray structures of the c-ring were solved at low (5.3) and high (8.7) pH to 2.2 and 2.64 Å, respectively. In both structures, the conserved glutamate is in an ion-locked conformation, revealing that the conformational state of the ion binding carboxylate is not depending on the pH of the crystallization condition, which is in good agreement with previous structural and biochemical studies of other c-rings.
A Na+ ion is present within the c-ring binding site and directly coordinated by four amino acid residues and a structural water molecule. Remarkably, the Na+ is bound by two glutamate residues instead of one as is the case in the I. tartaricus Na+ binding c-ring, of which the first high resolution X-ray structure of a c-ring has been solved in 2005. Thus, a new type of Na+ coordination in an ATP synthase rotor ring with a two-carboxylate ion binding motif is described here, which also occurs in other bacteria, including several pathogens. Na+ specificity of the investigated c-ring was further confirmed by a competitive biochemical labeling reaction performed with a fluorescent ATP synthase inhibitor molecule (N-cyclohexyl-N`-[4(dimethylamino)-α-naphtyl] carbodiimide, NCD-4).
We furthermore complemented our functional and structural data of the F. nucleatum c-ring by computational studies to explore the ion translocation mechanism of this enzyme in more details. We therefore analyzed the protonation state of the second, additional glutamate in the ion binding site. Molecular dynamics (MD) simulations and free-energy calculations indicated that this glutamate is constitutively protonated, in the ion-locked as well as in a simulated, more hydrated open-conformation of the ion binding glutamate as when it is travelling through the a/c-ring interface upon c-ring rotation.
Im Rahmen dieser Arbeit wurden zum Vergleich die Strukturen der ATP-Synthasen von Arabidopsis thaliana, Asparagus officinalis, Allium cepa, Helianthus annus, Solanum tuberosum, Bos taurus und Saccharomyces cerevisiae gelöst. Die ATP-Synthase von S. cerevisiae konnte mit einer Auflösung von 19 Å gelöst werden. Der Winkel zwischen den zwei ATP-Synthase-Monomeren in dem ATP-Synthase-Dimer hatte für jede Spezies einen bestimmten Wert. Dieser Winkel änderte sich innerhalb einer Spezies nur wenig im Gegensatz zu Untersuchungen mit Einzelpartikelanalyse.
Die ATP-Synthase-Dimere aus den untersuchten Spezies besitzen unterschiedliche Winkel zwischen 78˚ und 122˚. Der Winkel des ATP-Synthase-Dimers aus S. tuberosum (122˚) viel größer als der in anderen Pflanzen (~98˚), B. taurus (105˚) und S. cerevisiae (78˚). Die Proben von S. tuberosum und B. taurus waren jedoch dünner, was den Winkel eventuell beeinflussen könnte. Um dies auszuschließen müssen in Zukunft weitere Untersuchungen durchgeführt werden.
Des Weiteren wurde im peripheren Stiel der ATP-Synthasen von allen Pflanzenspezies eine Dichte entdeckt, die in B. taurus und S. cerevisiae nicht vorhanden ist. Die Dichte könnte durch eine zusätzliche Untereinheit oder veränderte Untereinheit im Vergleich zu B. taurus und S. cerevisiae kommen.
Weiterhin wurde die Bildung von Reihen aus ATP-Synthase-Dimeren untersucht. Es wurden ATP-Synthase-Dimere von Polytomella sp. gereinigt und in Lipid rekonstituiert. Es wurde das ATP-Synthase-Dimer von Polytomella sp. verwendet, da dieses besonders stabil ist und während der Reinigung nicht zum ATP-Synthase-Monomer zerfällt. Zur Rekonstitution wurde die milde GRecon-Methode verwendet. Hierbei werden Membranproteine in einem Zuckergradienten gleichzeitig in Lipid rekonstituiert und nach ihrer Dichte getrennt. Abhängig von der Dichte der Proteoliposomen ist die Konzentration an Membranproteinen unterschiedlich. In Proteoliposomen mit einer hohen Konzentration bilden sich dünne Schichten in denen die ATP-Synthase-Dimeren Zickzack-Muster formen. Dies deutet darauf hin, dass das ATP-Synthase-Dimer die Membran verformt. In Proteoliposomen mit einer niedrigeren Konzentration an ATP-Synthase-Dimeren wurden runde Vesikel detektiert, in denen die ATP-Synthase-Dimere lange Reihen bilden und die Membran innerhalb jedes ATP-Synthase-Dimer ebenfalls verformt ist. Molekulare Simulationen bestätigen dieses Ergebnis.
Zudem wurde das ATP-Synthase-Dimer in zwei verschiedene Lipide ohne Cardiolipin rekonstituiert, da Cardiolipin ein Lipid ist welches in der bakteriellen und mitochondrialen Membran gefunden wurde und in hohen Konzentrationen in Membrankrümmungen lokalisiert ist (Huang et al., 2006), wie auch die ATP-Synthase-Dimere. Ohne Cardiolipin ist die Rekonstitution nicht geglückt beziehungsweise sind die ATP-Synthase-Dimere weniger gut zueinander angeordnet. Das deutet auf die Wichtigkeit von Cardiolipin in der Stabilisierung der Reihen von ATP-Synthase-Dimeren hin. Weitere Experimente mit verschiedenen ATP-Synthase-Dimeren in verschiedenen Lipiden sind nötig um dies zu untermauern.
Ein weiteres Ziel dieser Arbeit war es ein klonierbares Label zu etablieren, um ein bestimmtes Protein in Kryo-Elektronentomogramme zu identifizieren. Das Label sollte klein sein, um das zu identifizierbare Protein nicht zu beeinflussen und groß genug um in Kryo-Elektronentomogramme identifizierbar zu sein. In Einzelbildern wurde das 6 kDa große Metallothionein gebunden mit Gold identifiziert, wenn zwei Metallothioneine an dem gewünschten Protein kloniert wurden. Metallothionein besteht zu 33 % aus Cysteinen, welche Schwermetalle binden.
In meinen Studien habe ich bewiesen, dass drei Metallothioneine, gebunden mit Gold, in Kryo-Elektronentomogramme detektiert werden können. Jedoch tritt bei der Verwendung von Metallothionein durch die hohe Anzahl an Cysteinen vermehrt Aggregation auf. Bei meinen Untersuchungen fand ich heraus, dass auch das Maltose-Binde-Protein (MBP) ein Signal gleicher Intensität erzeugt. Durch Verwendung von MBP tritt aber keine Aggregation auf und man kann MBP auch zum Reinigen des Proteins verwenden.
During my thesis, I worked on two different membrane proteins. One is a bacterial secondary transporter and the second is a human mitochondrial calcium channel.
The first part of my thesis involves the structural and biochemical characterization of an L-carnitine/ γ-butyrobetaine antiporter from bacteria called CaiT. The aim of the project was to understand the Na+ independence of CaiT and to determine the crystal structures of CaiT in different conformations to expand the mechanistic understanding of substrate/ product antiport in CaiT.
The study revealed how a positively charged amino acid side chain (arginine 262) in CaiT could structurally and functionally mimic a sodium ion. Additionally, various crystal structures of CaiT obtained in this study demonstrate that the central substrate-binding site is highly dynamic and can accommodate the substrate in various orientations.
In the second part of my thesis, I was able to optimize the expression and purification conditions for the human mitochondrial calcium uniporter or the MCU. Understanding how this channel functions can help us unravel the mechanism of calcium uptake by mitochondria. Secondary structure prediction analysis in combination with mass spectrometry of degraded MCU products obtained during the purification of the full-length protein led to the identification of a stable MCU construct. This study resulted in the successful purification of milligram quantities of stable MCU protein for the first time. Further optimization may be required to obtain more homogenous protein that is amenable for crystallization.
Die Atmungskette in der inneren Membran der Mitochondrien besteht aus fünf großen Enzymkomplexen. Die NADH-Dehydrogenase (I), Succinat-Dehydrogenase (II, indirekt), Cytochrom c-Reduktase (III) und Cytochrom c-Oxidase (IV) nutzen die Energie aus Elektronentransfers zum Aufbau eines Protonengradienten über die innere Mitochondrienmembran. Dieser wird anschließend von der FOF1-ATP-Synthase (V) als Energiequelle zur Phospho-rylierung von ADP verwendet. Für lange Zeit bestand eine Kontroverse, wie diese Proteine in der Membran organisiert sind. Nach dem „random collision“-Modell diffundieren sie frei als Einzelmoleküle und treffen sich nur zufällig, während sie nach dem „solid state“-Modell größere funktionelle Einheiten bilden. In den letzten Jahren gab es vermehrt Hinweise darauf, dass das letztere Modell das zutreffendere ist, da tatsächlich sogenannte Superkomplexe der Atmungskette in aktiver Form isoliert werden konnten. Schließlich konnte 2007 die erste drei-dimensionale Rekonstruktion eines Superkomplexes, bestehend aus Komplex I, dimerem Komplex III und Komplex IV publiziert werden. Aufgrund der Einschränkungen der verwendeten Negativkontrasttechnik hatte dieses Modell allerdings nur eine niedrige Auflösung und repräsentierte durch die Dehydrierung keinen nativen Zustand. Dadurch ließen sich die Strukturen der einzelnen Komplexe nur ungenau einpassen. Um diese Probleme zu umgehen, sollte eine Struktur unter Kryo-Bedingungen rekonstruiert werden. Um die für Kryo-EM benötigte größere Ausbeute und höhere Konzentration zu erzielen, wurde ein neues Reinigungsprotokoll für die Superkomplexe etabliert. Die wesentlichen Punkte darin sind der Austausch des für die Solubilisierung verwendeten Digitonins durch Amphipol A8-35 mittels ?-Cyclodextrin und eine anschließende Dichtegradienten-Ultrazentrifugation. Im BN-PAGE zeigten die auf diese Art gereinigten Superkomplexe das gleiche Banden- und Aktivitätsmuster wie Proben in Digitonin. Auch bei einer Einzelpartikelanalyse nach Negativ-kontrastfärbung konnten keine Unterschiede festgestellt werden und die Partikel zeigten ähnliche Orientierungen wie in der vorherigen Studie. Einige neue Ansichten ließen sich jedoch nicht zuordnen und stellten eventuell eine Verunreinigung mit größeren Superkomplexen dar. Da auch bei der Reinigung mit Amphipol die Proteinkonzentration letztlich nicht wesentlich erhöht werden konnte und sich die Superkomplexe nicht wie für Kryo-EM erforderlich in einen löchrigen Kohlefilm einlagerten, wurden die Proteine auf einem durchgehenden Kohlefilm in einer dünnen Pufferschicht vitrifiziert. Die dabei zu beobachtenden bevorzugten Orientierungen, sollten auch die Unterscheidung von verschiedenen Populationen von Superkomplexen erleichtern. Eine erste 3D-Rekonstruktion wurde mit Hilfe der „random conical tilt“-Methode errechnet. Dieses Modell wurde durch „projection matching“ bis zu einer Auflösung von 19 Å verfeinert, womit die Auflösung fast doppelt so hoch ist, wie bei der Rekonstruktion aus Negativ-kontrastfärbung (36 Å). Die Struktur repräsentiert einen natürlichen Zustand des Proteins und zeigt Details wie einzelne Domänen, Spalten zwischen Domänen und eine starke Krümmung des Membranarms von Komplex I, die zuvor nicht erkenn-bar waren. Die Amphipole bilden einen Gürtel um den Transmembranbereich. Die Röntgenstrukturen von Komplex I, III2 und IV konnten mit großer Präzision in die Dichtekarte eingepasst werden. Die wenigen kleinen Unterschiede zwischen Röntgenstrukturen und EM-Dichtekarte sind auf leichte Konformations-änderungen zurückzuführen. Die Kryo-EM-Rekonstruktion ist erheblich größer als die Rekonstruktion aus Negativfärbung, wodurch die enthaltenen Komplexe nur noch wenige punktuelle Kontakte haben. In den Zwischenräumen könnte eine spezielle Lipidumgebung die kleinen Elektronenüberträger Ubichinon und Cytochrom c in den Superkomplex integrieren. Ihre Bindestellen sind jeweils zueinander orientiert und die geringen Abstände, die zum ersten Mal bestimmt werden konnten, stützen die Hypothese eines gerichteten Substrattransfers über kurze Entfernungen. Von den möglichen Übertragungswegen scheint der kürzere mit weniger Transferreaktionen bevorzugt zu werden. Während der Entwicklung des neuen Reinigungsprotokolls für die Superkomplexe konnte zusätzlich eine neue Methode zur Rekonstitution von Membranproteinen entwickelt werden. Die solubilisierten Proteine werden dabei in Dichtegradienten mit steigenden Konzentrationen von ansolubilisierten Liposomen und Cyclodextrin zentrifugiert, wodurch ihnen langsam das Detergens entzogen und durch Lipid ersetzt wird. Proteoliposomen werden gleichzeitig von überschüssigem Lipid und Cyclodextrin-Detergens-Komplexen getrennt.
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.