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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.
Electron tomography was used to investigate membrane proteins in a variety of contexts. A high-angle tilt holder, suitable for electron tomography was designed, constructed and characterised. 2D crystals of membrane proteins, NhaA and YidC, were examined as a resolution test, and a method established for determining planarity of crystals. A model for specific gold binding to NhaA crystals was also presented. ATP synthase, a membrane protein complex in mitochondria, were imaged in a frozen hydrated state. They were found to form ribbons of dimers at highly curved regions of the membrane. Dimers from bovine heart and rat liver were excised from the tomographic volumes and averaged. Based on the location of the dimers in the mitochondrion, a model was established whereby ATP synthase, a molecular motor driven by the proton motive force, benefits from the high curvature that it induces in the membrane. Whole yeast mitochondria, imaged by electron cryo-tomography, also contained long ribbons of dimeric ATP synthase. Multiple copies of an unknown membrane protein complex were visualised by electron cryo-tomography, excised and averaged. A general method for the identification of unknown proteins was presented to deal with this inevitable issue, as native tissues and organelles are imaged, and the structures of complexes determined in situ.
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.
Electron microscopy (EM) demarcates itself from other structural biology techniques by its applicability to a large range of biological objects that spans from whole cells to individual macromolecules. In single-particle cryo-EM, frozen-hydrated samples, prepared by vitrification with liquid ethane, retain macromolecules in a medium that approximates their natural aqueous environment and that, in this way, preserves high-resolution structural information. Nonetheless, the sensitivity of biological specimens to the high-energy electron beam introduces restrictions on the total dose that can be used during imaging while avoiding significant radiation damage. Consequently, the signal-to-noise ratio attained in each individual image is very low, and structures with high-resolution detail must be recovered by averaging thousands of projections in random orientations. This is achieved through the use of image processing algorithms capable of aligning and classifying particle images through the evaluation of cross-correlation functions between each particle and a reference.
In recent years, several innovations took place in the field of single-particle cryo-EM, among which the development of direct electron detectors must be highlighted. Direct electron detectors have a better detective quantum efficiency (DQE) than both photographic film and CCD cameras, and offer a fast readout, compatible with the acquisition of movie stacks. Additionally, new image processing software has become available, with more sophisticated algorithms and designed to take advantage of the specific characteristics of the movies produced with direct electron detectors. These technological advances in both hardware and software catalyzed a revolution in single-particle cryo-EM, which is now routinely used for the determination of near-atomic structures. As a result, the range of macromolecules accessible to cryo-EM has increased drastically, as targets that were unsuitable before for imaging due to their small dimensions can now be adequately visualized and refined to high-resolution.
During my doctoral work, I have used single-particle cryo-EM to structurally characterize challenging membrane proteins, with a strong emphasis on protein complexes from aerobic respiratory chains. In chapter I of this thesis, I present my results on the bovine respirasome, a mitochondrial supercomplex composed of complexes I, III and IV. Chapter II is dedicated to the analysis of the structure of alternative complex III (ACIII) from Rhodothermus marinus, a bacterial quinol:cytochrome c/HiPIP oxidoreductase unrelated to the canonical cytochrome bc1 complex (complex III). In addition, in chapter III I describe the structure of KimA, a high-affinity potassium transporter that drives the transport of its substrate by using the energy stored in the form of a proton gradient. These three membrane proteins, with molecular weights ranging from 140 kDa to 1.7 MDa, illustrate the possibilities and limitations faced in single-particle cryo-EM.
The aerobic respiratory chain is responsible for the generation of a transmembrane difference of electrochemical potential that is then used by ATP synthase for the production of ATP or for driving solute transport over the membrane. They catalyze the transfer of electrons from a substrate, such as NADH or succinate, to molecular oxygen and use the chemical energy released in these redox reactions to drive the translocation of protons, or in some cases sodium ions, to the intermembrane space in mitochondria or the periplasm in bacteria.
In mitochondria, the respiratory chain is composed of four complexes: complex I (NADH:ubiquinone oxidoreductase), complex II (succinate dehydrogenase), complex III (cytochrome bc1 complex) and complex IV (cytochrome c oxidase). While it was for a long time believed that these complexes existed as single entities in the membrane, the use of milder procedures for protein purification and analysis revealed that respiratory complexes associate into well-ordered structures, known as supercomplexes. These have been proposed to offer different structural and functional advantages that are still controversial, including substrate channeling, stabilization of individual complexes and reduction of reactive oxygen species (ROS) production. The most thoroughly studied respiratory supercomplex has been the respirasome, conserved in higher eukaryotes and composed of one copy of complex I, a complex III dimer and one complex IV. By single-particle cryo-EM analysis, I retrieved a 9 Å map of the respirasome from Bos taurus, which allowed the accurate docking of atomic models of the three component complexes. The structure shows that complex III associates to the concave side of the membrane arm of complex I, while complex IV is located between the end of the complex I hydrophobic arm and complex III. Several defined protein-protein contacts are observed between the component complexes, which are mediated predominantly by supernumerary subunits and close to the membrane surfaces. The interactions established between complex I and complex III are extensive and may support the argument that the association of complex I into supercomplexes is required for the stabilization or even the biogenesis of this complex.
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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.
Inorganic phosphate is one of the most abundant and essential nutrients in living organisms. It plays an indispensable role in energy metabolism and serves as a building block for major cellular components such as the backbones of DNA and RNA, headgroups of phospholipids and in posttranslational modifcations of many proteins. Disturbances in cellular phosphate homeostasis have a detrimental effect on the viability of cells. There- fore, both the import and export of phosphate is strictly regulated in eukaryotic cells. In the eukaryotic model organism Saccharomyces cerevisiae, the uptake of phosphate is carried out either by transporters with high affinity or by transporters with low affinity, depending on the cytosolic phosphate concentration. While structures are available for homologues of the high-affinity transporters, no structures of low-affinity transporters have been solved so far. Interestingly, only the low-affinity transporters have a regulatory SPX domain, which is found in various proteins involved in phosphate homeostasis.
In this work, structures of Pho90 from Saccharomyces cerevisiae, a low-affinity phosphate transporter, were solved by cryo-EM, providing insights into its transport mechanism. The dimeric structure resembles the structures of proteins of the divalent anion symporter superfamily (DASS) and of mammalian transporters of the solute carrier 13 (SLC13) family. The transmembrane domain of each protomer consists of 13 helical elements and can be subdivided into scaffold and transport domains. The structure of ScPho90 in the presence of phosphate shows the phosphate binding site within the transporter domain in an outward-open conformation with a bound phosphate ion and two sodium ions. In the absence of phosphate, an asymmetric dimer structure was determined, with one protomer adopting an inward-open conformation. While the dimer contact and the scaffold domain are identical in both conformations, the transport domain is rotated by about 30° and shifted by 11 Å towards the cytoplasmic side, leading to the accessibility of the binding pocket from the cytoplasm. Based on these findings and by comparison with known structures, a phosphate transport mechanism is proposed in the present work that involves substrate binding on the extracellular side, conformational change by a rigid-body motion of the transport domain, in an "elevator-like" motion, and substrate release into the cytoplasm. The regulatory SPX domain is not well resolved in the ScPho90 structures, so that no direct conclusions were drawn about its regulatory mechanism. The findings provide new insights into the function and mechanism of eukaryotic low-affinity phosphate transporters.
While eukaryotic cells express various phosphate import proteins, most eukaryotes have only a single highly conserved and essential phosphate exporter. These exporters show no sequence homology to other transporters of known structure, but also possess a regulatory SPX domain. In this work, the structural basis for eukaryotic phosphate export is investigated by elucidating the structures of the homologous phosphate exporters Syg1 from Saccharomyces cerevisiae and Xpr1 from Homo sapiens, using cryo-EM. The structures of ScSyg1 and HsXpr1 show a conserved homodimeric structure and the transmembrane part of each protomer consists of 10 TM helices. Helix TM1 establishes the dimer contact by means of a glycine zipper motif, which is a known oligomerization motif. Helices TM2-5 form a hydrophobic pocket that has density for a lipid molecule. Whether the lipid binding into the hydrophobic pocket has an allosteric effect on the phosphate export activity or only serves protein stabilization is not known. Helices TM5-10 form a six-helix bundle, which constitutes a putative phosphate translocation pathway in its center. This bundle is formed by the protein sequence annotated as EXS domain.
The respective phosphate translocation pathways of ScSyg1 and HsXpr1 show structural differences. While the translocation pathway in HsXpr1 is accessible from the cytoplasm, in ScSyg1 it is closed by a large loop of the SPX domain. Interestingly, this loop is not conserved in higher eukaryotes and is therefore not present in HsXpr1. Another difference are distinct conformations of helix TM9. In ScSyg1, TM9 adopts a kinked conformation, which results in the translocation pathway being open to the extracellular side. In contrast, TM9 adopts a straight conformation in HsXpr1, resulting in the placement of a highly conserved tryptophane residue in the middle of the translocation pathway. As a result, the translocation pathway in HsXpr1 is closed to the extracellular side.
Glutamat ist der häufigste Neurotransmitter im menschlichen Hirn. Die Konzentration des Glutamats in der extrazellulären Flüssigkeit wird durch Glutamat-Transporter (Sekundärtransporter) kontrolliert. Liegt es in zu hoher Konzentration im synaptischen Spalt vor, kommt es zur Schädigung von Nervenzellen, ein Prozess, der als Exzitotoxizität bezeichnet wird. Eine Fehlfunktion oder fehlerhafte Produktion der Glutamat-Transporter im zentralen Nervensystem wird bei verschiedenen Krankheiten, wie der amyotrophen Lateralsklerose, der Ischämie, der Epilepsie, der Schizophrenie und der Alzheimer-Krankheit vermutet. Ziel dieser Arbeit war die Funktions- und Strukturanalyse der Glutamat-Transporter GLT-1 aus Rattus norvegicus und GltP aus E. coli, um die Familie der Glutamat-Transporter und die Entstehung der mit diesen Transportern in Verbindung gebrachten Krankheiten besser zu verstehen. Um die für diese Analysen gebrauchten Mengen an Protein herzustellen, mussten die Proteine heterolog produziert werden, da sie in natürlichen Geweben nicht in ausreichender Menge vorkommen. In dieser Arbeit wurde Glutamat-Transporter GLT-1 aus Rattus norvegicus funktional mit dem Semliki Forest Virus Expressionssystem überproduziert. Dazu wurden verschiedene Vektorkonstrukte hergestellt. Die routinemäßige Überproduktion des Transporters wurde im 8 l - Maßstab durchgeführt. In Zellen, die für die Produktion von GLT-1 mit rekombinanten, aktiven SF-Viren infiziert wurden, konnte eine sehr hohe Aktivität des Glutamat-Transporters nachgewiesen werden. Die Menge des hergestellten GLT-1 wurde in Bindungsexperimenten mit (2S,4R)-4-Methylglutamat quantifiziert: jede Zelle enthielt 3,5 x 106 Transporter: 61,04 pmol GLT-1/mg Gesamtprotein. Das entspricht einer Ausbeute von etwa 2-3 mg/8 l Zellkultur. Die hier durchgeführte Überproduktion des GLT-1-Glutamat-Transporters ist die erste Überproduktion eines eukaryotischen Sekundärtransporters mit dem Semliki Forest Virus Expressionssystem, bei dem große Mengen an aktivem Protein hergestellt werden konnten. Zudem ist die Ausbeute an funktionalem GLT-1 mit 61 pmol/mg Gesamtprotein verglichen mit den in der Literatur vorliegenden Daten zur Überproduktion eukaryotischer sekundärer Transporter mit anderen Expressionssystemen die höchste, die bis dato erreicht werden konnte. Der größte Anteil des heterolog produzierten GLT-1 war glykosyliert. Die gelelektrophoretische Analyse des aufgereinigten Transporters ergab zwei Banden, die ein apparentes Molekulargewicht von etwa 70-75 kDa und etwa 53-58 kDa hatten. In einer Western-Blot-Analyse konnten beide Banden des GLT-1-Transporters mit einem anti-His-Antikörper und einem anti-GLT-1-Antikörper nachgewiesen werden. Durch Deglykosylierung mit PNGase F und einer Trennung beider Banden durch Lektin-Affinitätschromatographie konnte gezeigt werden, dass es sich bei der 70-75 kDa-Bande um die glykosylierte Form und bei der 53-58 kDa-Bande um die nicht glykosylierte Form des Glutamat-Transporters handelte. Es wurde gezeigt, dass zwischen der Aktivität des GLT-1 und dessen Glykosylierung kein Zusammenhang besteht. Denn beide Formen lagen als vollständige, funktionale Transporter vor und transportierten nach Rekonstitution in Liposomen Glutamat. Der prokaryotische Glutamat-Transporter GltP aus E. coli wurde in dem E. coli-Stamm C43 (DE3) überproduziert. Die Ausbeute war etwa 2 mg pro Liter Kultur. Die Funktionalität des Transporters nach Rekonstitution in Lipidvesikel wurde durch spezifische Aufnahme von Glutamat gezeigt. Für die Solubilisierung beider Transporter aus den Zellmembranen wurden verschiedene Detergentien getestet. GltP ließ sich am besten mit DM oder DDM aus der Membran extrahieren, für die Solubilisierung des GLT-1 wurde mit großer Effizienz DDM oder CYMAL-7 eingesetzt. GltP und GLT-1 wurden mit einer Ni2+-NTA-Affinitätschromatographie in großer Menge und hoher Reinheit angereichert werden. Die Aufreinigungsprozedur beeinträchtigte nicht die Funktionalität des prokaryotischen GltP. Bei dem eukaryotischen Transporter GLT-1 war nach der Ni2+-NTA-Säule keine Transportaktivität mehr messbar. Durch Zusatz von Asolectin in den Wasch- und Elutionspuffern während der Aufreinigung konnte die Funktionalität des Transporters jedoch erhalten werden. Aufreinigungen mit anderen Lipiden unter anderem in Kombination mit Cholesterin lieferten einen Glutamat-Transporter, der in seiner Konformation stabilisiert, jedoch nach Rekonstitution nicht aktiv war. Eine weitere Steigerung der Ausbeute an aktivem GLT-1 konnte durch den Einsatz von Reduktionsmitteln, wie DTT oder b-Mercaptoethanol, die die Aggregation des Transporters verhinderten, erreicht werden. GltP katalysiert den elektrogenen Transport von Glutamat bzw. Aspartat unter Symport von mindestens zwei Protonen. GLT-1 transportiert ein Molekül Glutamat zusammen mit drei Na+-Ionen und einem Proton im Austausch gegen ein K+-Ion. Durch Transportmessungen konnte der hochspezifische Glutamat-Transport der aufgereinigten Transporter belegt werden. Der Glutamat-Transport des in Liposomen rekonstituierten GltP zeigte eine klare Abhängigkeit von einem anliegenden Protonengradienten. Aufgereinigtes und rekonstituiertes GLT-1 transportierte nur Aspartat bzw. Glutamat, wenn ein Na+ und ein K+-Gradient vorhanden waren. Die Aspartat- bzw. Glutamat-Aufnahme konnte bei beiden Transportern durch den kompetitiven nichttransportablen Inhibitor (2S,4R)-4-Methylglutamat blockiert werden. Der Assoziationsgrad der Glutamat-Transporter GltP und GLT-1 und das Gleichwicht zwischen den verschiedenen oligomeren Zuständen wurde in dieser Arbeit eingehend mit biochemischen Methoden untersucht: 1. „Cross-linking“-Studien, 2. Blaue Nativgelelektrophorese, 3. Analytische Ultrazentrifugation, 4. Laserlichtstreuung, 5. Gelfiltrationschromatographie. Die dabei erhaltenen Ergebnisse bewiesen eine tetramere Assoziierung beider Proteine. Die Gelfiltrationsexperimente zeigten, dass die Transporter in Detergenzlösung in unterschiedlichen Assoziationsgraden vorliegen. Das Gleichgewicht zwischen den oligomeren Formen war reversibel und abhängig von der Art und Konzentration des Detergenz, der Proteinkonzentration und der Temperatur. Zur Untersuchung der Struktur der Glutamat-Transporter wurden vor allem mit GltP zahlreiche 2D-Kristallisationsexperimente durchgeführt. Trotz Variation aller denkbar möglichen Parameter konnten keine Kristalle erhalten werden. Das beste Ergebnis war ein guter Einbau des Proteins in Lipidvesikel (etwa 80%). Da keine Kristalle erhalten wurden, wurde für beide Proteine eine Einzelpartikelanalyse durchgeführt. Dabei wurde nach zweidimensionaler Alignierung und Klassifizierung die „random conical tilt“-Methode angewendet. Die daraus resultierenden dreidimensionalen Dichtekarten des GltP und GLT-1 waren sehr ähnlich und wiesen vier nicht exakt symmetrische Massen in annähernd quadratischer Anordnung auf. Die Auflösung war 26 Å bzw. 36 Å. Die Größe der Einzelpartikel (für GltP: Höhe 37 Å, Breite 75 Å bzw. 86 Å, Länge 100 Å). ihre annähernd quadratische Anordnung und ihre Symmetrie lassen vermuten, dass es sich dabei um Tetramere der Glutamat-Transporter handelt, die aus zwei nicht symmetrischen Dimeren zusammengesetzt sind. Die hier präsentierten Daten sind die ersten zur dreidimensionalen Struktur von Glutamat-Transportern. Schließlich wurde nachgewiesen, dass der in BHK-Zellen heterolog exprimierte Glutamat-Transporter GLT-1 vorwiegend in „lipid rafts“ lokalisiert ist. Die Größe der „rafts“, die anhand der Größe der „Proteininseln“ in Gefrierbrüchen bestimmt wurde, war etwa 200 nm im Durchmesser. Die „GLT-1-Inseln“ bzw. „lipid rafts“ konnten durch das teilweise Entfernen von Cholesterin aus der Membran zerstört werden. Damit ging eine Reduktion der Glutamat-Transporter-Aktivität von etwa 20% einher. Es ist das erste Mal, dass „lipid rafts“ durch die natürliche Assemblierung von Proteinen mit Hilfe von Gefrierbruchanalysen und Elektronenmikroskopie beobachtet wurden.
This thesis investigates the structure of the translocase of the outer membrane (TOM) complex in mitochondria, focusing on the TOM holo complex through single-particle electron cryo-microscopy (cryoEM) complemented by mass spectrometry and computational structure prediction. Mitochondria, crucial for energy production in eukaryotic cells, import most of their proteins from the cytoplasm. These proteins enter through the TOM complex, which in its core form consists of a membrane-embedded homodimer of Tom40 pores, two Tom22 cytoplasmic receptors, and six small TOM stabilizing subunits (Tom7, Tom6, and Tom5). The holo complex includes two additional subunits, Tom70 and Tom20, whose stoichiometry and positioning are less understood due to their easy dissociation during isolation of the complex. CryoEM analysis revealed the high-resolution structure of the Neurospora crassa TOM core complex at 3.3 Å, containing all core subunits, and the presence of a central phospholipid causing the Tom40 dimer to tilt to 20°. Furthermore, a 4 Å resolution map indicated the binding of a precursor protein as it transitions through the translocation barrel. Finally, at 6-7 Å resolution, the structure of the TOM holo complex highlighted Tom20's flexibility as it interacts with the core complex, emphasizing its role in protein translocation. This work provides significant insights into the architecture and functioning of the TOM complex, contributing to the understanding of mitochondrial protein import mechanisms.
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.