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Die membranintegrierten, rotierenden F-Typ ATP-Synthasen zählen zu den essentiellen Komponenten der bakteriellen Energieversorgung. Ihre Rolle im zellulären Energiehaushalt bestehtin der Synthese von ATP unter Nutzung des transmembranen, elektrischen Ionengradienten (Mitchell 1961, Duncan et al. 1995, Noji et al. 1997, Kinosita et al. 1998). Die rotierenden ATP-Synthasen werden entsprechend der Kationenselektivität, die sie unter physiologischen Bedingungen zeigen, in zwei verschiedene Klassen eingeteilt, die H+-selektiven, sowiedie Na+-selektiven ATP-Synthasen. Hierbei bildet die Selektivität beider Klassen für einwertige Kationen (H+ oder Na+) eine essenzielle Grundlage für ihre Rolle im Energiehaushalt der bakteriellen Zellen. Jedoch gibt es nur eine begrenzte Anzahl von anaeroben Eubakterien und Archaeen, die noch einen auf Na+- Ionen basierenden Energiehaushalt besitzen. Gut charakterisierte Beispiele für Na+-selektive ATP-Synthasen bilden die F-Typ-Synthasen von I. tartaricus, P. modestum, sowie die V/A-Typ-Enzyme von E. hirae und A. woodii. Trotz der Unterschiede in der Kationenselektivitätder unterschiedlichen F-Typ ATP-Synthasen sind sie jedoch sowohl inihre Organisation, als auch hinsichtlich ihre Wirkungsweisen ähnlich. Das Ziel, der im Rahmen dieser Arbeit durchgeführten Forschung, bestand in der Identifizierung der Faktoren, die sowohl die hohen Selektivität, als auch die Affinität des in der Membran-eingebetteten Rotor-C-Rings der ATP-Synthasezu Protonen (H+) und Na+- Ionen beeinflussen. Die Untersuchungen wurden hierbei andem c11-Ring der F-Typ-ATP-Synthase aus dem anaeroben Bakterium Ilyobacter tartaricus durchgeführt, das hierbei als Modellsystem diente. Der untersuchte Ring zeigt unter physiologischen Bedingungen eine hohe Bindungsselektivität für Na+ Ionen, kann jedoch unter nicht-physiologischen Bedingungen auch Li+ und H+ Ionen binden und zur ATP-Synthese verwenden (Neumann et al. 1998).
Das Ziel, der im Rahmen dieser Arbeit durchgeführten Forschung, bestand in der Identifizierung der Faktoren, die sowohl die hohen Selektivität, als auch die Affinität des in der Membran-eingebetteten Rotor-C-Rings der ATP-Synthasezu Protonen (H+) und Na+- Ionen beeinflussen. Die Untersuchungen wurden hierbei andem c11-Ring der F-Typ-ATP-Synthase aus dem anaeroben Bakterium Ilyobacter tartaricus durchgeführt, das hierbei als Modellsystem diente. Der untersuchte Ring zeigt unter physiologischen Bedingungen eine hohe Bindungsselektivität für Na+ Ionen, kann jedoch unter nicht-physiologischen Bedingungen auch Li+ und H+ Ionen binden und zur ATP-Synthese verwenden (Neumann et al. 1998). Die Kd- und KM-Werte wurden verwendet, um die Na+ -Bindungsaffinität der C-Ringe bzw. ATP-Synthasen zu quantifizieren. Über die Selektivität wurdebeschrieben, welche Kationen an die C-Ringe und ATP-Synthasen binden können (z. B. H+/Na+/Li+, H+/Na+ - oder nur H+ Ionen).Das Verhältnis der absoluten Bindungsaffinitäten zwischen zwei Kationen (z. B. Kd (Na+)/Kd (H+)) wurde verwendet, um die Präferenz des Enzyms für eines der Ionen zu quantifizieren. Die Faktoren, dieder Kationenselektivität und der Affinität des I. tartaricus c-Rings zugrunde liegen, wurden mit Hilfe von Mutageneseexperimenten der Aminosäuren in der Ionenbindungsstelle untersucht. Im I. tartaricus-c-Ring erfolgt die Na+ Bindung an der Grenzfläche von zwei benachbarten c-Untereinheiten des c-Rings. An der Bindung der Na+-Ionen sind sowohl Aminosäuren aus Helix 1 (Gln32), sowie von Helix 2 (Val63, Ser66, Thr67 und Tyr70) beteiligt, die in der Nähe, des für den Mechanismusessentiellen Glu65 liegen. Insgesamt wurden 19 verschiedene, spezifische Einzel- und Doppelmutationen in die Sequenz des atpE-Gens eingeführt, die für die I. tarticus-ATP-Synthase-c-Untereinheit kodiert. Bei den Experimenten mit dem I. tartaricus c-Ring (Ser66, Thr67 und Tyr70) wurden drei polare Reste der Ionenbindungsstelle durch die polaren Reste (Ser67, Ile67 oder Leu67) oder hydrophobe Reste (Ala66, Gln67 und Phe70) ersetzt, während das geladene Glu65 durch die kürzere, aber immer noch geladene Seitenkette Asp65 ausgetauscht wurde. Zur Charakterisierung der monovalenten Kationenbindung durch die Wildtyp, sowie die mutierten C-Ringe von I.-tartaricus, wurde ein Ansatz verwendet, der biochemische (DCCD-Ionen-Kompetitionsassay) und biophysikalische (ITC) Methoden kombiniert.
Die Daten der in dieser Arbeit durchgeführten Experimente, zeigen, dass c-Ringe selektiv für H+ sind, solange in der Ionenbindungsstelle des c-Rings ein ionisierbarer Glu/Asp-Rest vorhanden ist. Die H+-Bindungsaffinität des c-Rings hängt von der Hydrophobizität der Reste ab, aus der die Ionenbindungsstelle aufgebaut ist.Jedoch ist die Zahl der Faktoren, die die Na+-Selektivität des C-Rings bestimmen, weitaus größer. Von den in dieser Arbeit untersuchten Faktoren war die Zahl der polaren Reste, die Wasserstoffbrücken zu Na+ bilden, die Co-Koordination von Na+ durch strukturell vorhandene Wassermoleküle und die Anwesenheit von negativ geladenen Resten besonders wichtig für die Bindung der Na+-Ionen an den Ring. Die hohe Bindungsaffinität des c-Rings für Na+-Ionen, wird sowohl durch Wechselwirkungen begünstigt die das gebundene Na+-Ion stabilisieren, als auch den gesamten atomaren Aufbau der Ionenbindestelle, der die enthalpiegetriebene Na+-Bindungan den c-Ring begünstigen. Im Rahmen dieser eingehenden Studien konnten zum ersten Mal die thermodynamischen Eigenschaften aufgeklärt werden, die der hohen Na+-Bindungsaffinität des c-Rings zugrunde liegen, sowie der Einfluss von Mutationen auf diese Parameter ermittelt werden. Durch zahlreiche Experimente mit ATP-Synthasen, die mit mutierten c-Ringen zusammengesetzt wurden, sollte eine Verbindung zwischen Veränderungen der H+- und der Na+-Bindungsaffinitäten und Unterschiede im Betrieb der ATP-Synthase aufgeklärt werden. Die wichtigste Schlussfolgerung, die sich aus dieser Arbeit ableiten lässt, ist, besteht darin, dass sich Na+/H+-selektiven ATP-Synthasen durch den Austausch von 1-2 Aminosäureresten innerhalb der rotierenden c-Ring-Ionenbindungsstelle in ausschließlich H+-selektive, vollfunktionelle ATP-Synthasen umwandeln lassen.
Diese Arbeit ist ein detaillierter Bericht über die Forschungsaktivitäten, die ich während meiner Promotion am Max-Planck-Institut für Biophysik durchgeführt habe. Mit dem Aufkommen der direkten Elektronendetektoren erlebte die Transmissionselektronenmikroskopie von gefrorenen hydratisierten Proben (Kryo-EM) einen epochalen Wandel, die sogenannte “Auflösungsrevolution”. Ab den 2010er Jahren ermöglichte die Kommerzialisierung der ersten direkten Detektoren die Erforschung biologischer Phänomene in beispiellosem Detail und machte Kryo-EM zu einer der leistungsstärksten (und gefragtesten) Forschungsmethoden in den Biowissenschaften. Meine Forschung konzentrierte sich auf die Verwendung der Elektronen-Kryotomographie, um zwei herausfordernde Ziele zu erreichen. Das erste bestand darin, die Denaturierung von Proteinen an der Luft-Wasser-Grenzfläche zu untersuchen, und das zweite die molekulare Landschaft eines lichtempfindlichen Chloroplastenvorläufers, des Etioplasten, zu beschreiben. Um die Relevanz, Herausforderungen und Auswirkungen meiner Arbeit zu vermitteln, habe ich diese Arbeit in drei Kapitel unterteilt.
Kapitel eins enthält eine Einführung in die Transmission-Elektronenmikroskopie.
Nach einer kurzen Zusammenfassung der historischen Meilensteine in der Disziplin beschreibe ich die wesentlichen Komponenten des TEM und deren Funktionsweise. Hier lege ich besonderen Wert auf die Struktur elektromagnetischer Linsensysteme, wie sie den Weg der Elektronen beim Durchlaufen der Säule beeinflussen und wie Bilder entstehen. Der hardwarebezogene Teil der Einführung wird durch eine vereinfachte Beschreibung der Elektronendetektoren abgeschlossen, in der ich die revolutionären Aspekte der direkten Elektronendetektoren, mit der Struktur und Funktion von CCD-Detektoren (Charge Coupled Device detector) vergleiche. Als nächstes konzentriere ich mich auf die theoretischen Prinzipien der Bilderzeugung. Um die Hauptphänomene im Zusammenhang mit der Bildqualität in TEM hervorzuheben, stelle ich grundlegende Konzepte wie den Einfluss von Elektronenenergie und optischen Aberrationen vor, gefolgt von einer ausführlicheren Beschreibung des Ursprungs von Kontrast und Rauschen. Der Unterabschnitt schließt mit einigen Überlegungen darüber, wie - und vor allem wie effizient - Detektoren kontinuierliche Elektronenwellen in diskrete Bereiche (Pixel) abtasten. Der folgende Unterabschnitt ist der Erfassung und Verarbeitung tomografischer Daten gewidmet. Hier gebe ich eine vereinfachte Beschreibung, wie Kippserien mit dem Mikroskop erfasst werden und wie die Rohdaten zu einer dreidimensionalen Darstellung der Probe verarbeitet werden. Der Einfluss der Neigungsgeometrie und der Dosisverteilung auf die Rekonstruktionsqualität wird ebenfalls diskutiert. Der zweite Teil des Unterabschnitts befasst sich mit der Strukturbestimmung durch Subtomogramm-Mittelung und der Errechnung der Auflösung von Kryo-EM-Rekonstruktion. Zuletzt schließe ich das Kapitel mit einer Beschreibung der Vorbereitung biologischer Proben für die Kryo-EM-Bildgebung mit einigen abschließenden Bemerkungen zur Dynamik und den Grenzen der Vitrifizierung ab.
Kapitel zwei folgt dem Thema der Kryo-Präparation biologischer Proben mit der Untersuchung der Denaturierung von Proteinen an der Luft-Wasser-Grenzfläche.
Im Einführungsabschnitt skizziere ich die wichtigsten Aspekte dieses Phänomens. Frühe Experimente zum Verhalten von Proteinen in Lösung zeigten ihre Neigung, aus der Lösung zu ihrer Grenzfläche mit der Atmosphäre zu diffundieren. Hier bilden sie meist unlösliche Schichten denaturierter Fibrillen Es wurde vorgeschlagen, dass die Korrelation zwischen Proteindenaturierung und Kontakt mit der Grenzfläche auf einen allmählichen Entfaltungsprozess zurückzuführen ist, bei dem Tausende von Wechselwirkungen pro Sekunde zu einer immer größeren strukturellen Schädigung führen würden. Ein direkter Beweis für diesen Mechanismus wurde jedoch nie dokumentiert. Um einen tieferen Einblick in die Dynamik an der Luft-Wasser-Grenzfläche zu erhalten, sammelte ich Kryotomogramme vitrifizierter Präparate der Fettsäuresynthase (FAS, Fatty Acid Synthase) aus Hefe. Im ersten Unterabschnitt der Ergebnisse beschreibe ich, wie die biochemische und Negativkontrastierung-TEM-Analyse von FAS-Fraktionen zeigte, dass der Komplex während des gesamten Reinigungsverfahrens intakt und katalytisch aktiv blieb. Nach der Vitrifizierung ergab die Einzelpartikelanalyse jedoch, dass 90% aller Komplexe stark beschädigt waren. Die tomographische Rekonstruktion derselben Proben zeigte, dass alle FAS-Komplexe an die Luft-Wasser-Grenzfläche gebunden waren. Die Seite des Moleküls, die der Grenzfläche ausgesetzt war, schien abgeflacht zu sein, während die Seite, in der wässrigen Phase, ihre native Struktur beibehielt. Die Mittelung der Subtomogramme bestätigte, dass eine Seite von fast 90% der Partikel stark beschädigt war. Durch den Vergleich der Ausrichtung dieser beschädigten Seite mit der Position eines Rechenmodells der Luft-Wasser-Grenzfläche konnte ich nachweisen, dass sie perfekt übereinstimmen, was den ersten direkten Beweis dafür liefert, dass die Wechselwirkung mit der Luft-Wasser-Grenzfläche die lokale Denaturierung großer Proteinkomplexe herbeiführt.
...
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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TeaABC from the halophilic bacterium Halomonas elongata belongs to the family of tripartite ATP-independent periplasmic (TRAP) transporters. It facilitates the uptake of the compatible solutes ectoine and hydroxyectoine which protect the cell from dehydration by accumulating in the cytoplasm during hyperosmotic stress. It is the only known TRAP transporter activated by osmotic stress. Ectoine and hydroxyectoine accumulation in H. elongata is regulated by the cytoplasmic universal stress protein TeaD. The gene encoding TeaD is located in the same operon as the TeaABC gene. TeaD regulates the cellular homeostasis of ectoine possibly by interacting directly or indirectly with TeaABC. All subunits of TeaABC and TeaD were expressed in E. coli and purified. With TeaD and the solute binding protein (SBP) TeaA high levels of expression suitable for crystallization could be obtained and their 3D structures solved. The small transmembrane protein TeaB and the transporter TeaC showed only moderate and low levels of expression respectively. Functional analysis on TeaA was performed using Isothermal Titration Calorimetry. The measurements demonstrate that TeaA is a high affinity ectoine-binding protein (Kd = 0.19 _M) that also has a significant affinity for hydroxyectoine (Kd = 3.8 _M). The structure of TeaA was solved using ab initio phase determination by MAD (multiple anomalous dispersion). TeaA structures were determined in three conformations: TeaA alone, TeaA in complex with ectoine and TeaA in complex with hydroxyectoine. The resolutions of the structures were 2.2, 1.55 and 1.80 Å, respectively. These represent the first structures of an osmolyte SBP associated to a TRAP transporter. The structures reveal similar ligand binding compared to osmolyte SBPs of ABC transporter pointing to coevolution of the ligand binding modes. Moreover, unique features such as the solvent-mediated specific binding of the ligands ectoine and hydroxyectoine could be observed for TeaA. The structure of TeaD in complex with its cofactor ATP was solved by molecular replacement at a resolution of 1.9 Å. Comparison with other structures of universal stress proteins shows striking oligomerization and ATP binding in TeaD. In conclusion, this work presents the first detailed analysis of the molecular mechanisms underlying ligand recognition of an osmoregulated transporter from the TRAP-transporter family.
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.
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.
Channelrhodopsin-2 (ChR2) is a light-gated cation selective channel from the unicellular alga Chlamydomonas reinhardtii, which is involved in phototaxis and photophobic responses. As other rhodopsins, ChR2 comprises a seven-transmembrane helix (TMH) motif and a retinal as the light-sensitive chromophore. The chromophore is covalently attached via a protonated Schiff base to the conserved lysine residue Lys257 located in TMH7. Based on its primary sequence and the all-trans configuration of the retinal in the ground state, ChR2 is assigned to the type I rhodopsins, also referred to as microbial-type rhodopsins. Upon light activation, the retinal isomerizes from the all-trans to the 13-cis form. This photoisomerization, which is accompanied by conformational changes of the protein, eventually leads to the opening of the channel and cation translocation. Cation flux during the conductive state leads to depolarization of the cell membrane and subsequent triggering of action potentials when expressed in neurons. Therefore, ChR2 has become the most versatile optogenetic tool, enabling a non-invasive investigation of neural circuits at high spatial and temporal resolution. With the rapidly increasing importance of ChR2 as a tool in neurobiology and cell biology, structural information is the prerequisite to an unambiguous understanding of the molecular mechanisms of this unique light-activated ion channel. The coupling between isomerization and structural alterations is well understood for other microbial-type rhodopsins, like bacteriorhodopsin (bR), halorhodopsin (HR) and sensory rhodopsin II (SRII). In case of ChR2, the first data on light-induced conformational changes came from spectroscopic studies and structural information is still missing. However, in order to fully understand the mechanism of light transduction by ChR2, it is necessary to determine the changes in the protein structure at specific steps in the photocycle.
By the time I started my PhD thesis, there was no structural information of ChR2 available. Therefore, the objective of this thesis was to obtain structural information of the transmembrane domain containing the first 315 amino acids of ChR2 by cryo electron crystallography. Besides revealing the structure of membrane proteins, cryo-EM of two-dimensional (2D) crystals is ideal for investigating conformational changes in membrane proteins induced by different stimuli. Therefore, the second objective of my thesis was the investigation of light-induced conformational changes in the slow C128T ChR2 mutant. The ~1,000 times longer lifetime of the open state of the C128T mutant compared to the wild-type allowed to trap different intermediates that accumulate during the photocycle.
In 2012, the X-ray structure of a channelrhodopsin-1/channelrhodopsin-2 chimaera (C1C2) at 2.3 Å resolution in the closed dark-adapted state was published (Kato et al., 2012). The structure revealed the essential molecular architecture of C1C2, including the retinal-binding pocket and the putative cation conduction pathway. Together with biochemical, spectroscopic, mutagenesis experiments, and the high-resolution model, some functionally important residues of ChR2 have been identified. However, unambiguous explanation of the molecular determinants that contribute to activation (gating) and transport were still mostly unknown.
RESULTS AND CONCLUSIONS
The first half of my theses dealt with 2D crystallization of ChR2. I succeeded in obtaining 2D crystals of ChR2 of four different types, which differed in size, crystal packing, crystal contacts and resolution, yielding structure factors up to 6 Å resolution. The crystals were grown by reconstituting the protein with different lipids at various lipid-to-protein ratios. The best crystals formed with the synthetic lipid DMPC and EPL upon detergent removal by dialysis. The projection maps calculated from these crystals revealed the overall structure of C128T ChR2 at 6 Å resolution and were published in 2011 (Müller et al., 2011). Surprisingly, ChR2 was found to be a dimer in all crystal types. The ChR2 dimer was stable both in detergent solution and in the presence of lipids for 2D crystallization. The monomers clearly showed the expected densities for the seven TMHs.
The arrangement of the ChR2 dimers on the four 2D lattices was different. However, comparison of the individual rojection maps revealed no significant differences within the ChR2 interface in the four crystal forms. The observation that the structure of the dimer was the same in all four crystal forms and in different lipids suggested strong specific contacts between the two protomers and implied that the protein was also dimeric in the native membrane. These findings were in agreement with Western blot analysis of plasma membranes from oocytes expressing ChR2 and laser-induced liquid bead ion desorption mass spectrometry, which both showed ChR2 as a dimer. The unusual stability of the ChR2 dimer contrasts with other microbial rhodopsins, which exist in different oligomeric states, i.e. monomers, trimers or dimers. These observations raised the question whether the functional unit is the monomer or the dimer.
The comparison of the projection map of the light-driven proton pump bR at the same resolution showed similar overall dimensions. Based on this comparison, the densities which became evident in the ChR2 projection maps could be assigned to the corresponding seven densities in bR. The shape of the densities near the dimer interface suggested that TMHs 2, 3, and 4 are oriented more or less perpendicular to the membrane plane, while the other four helices appear to be more tilted, as in bR.
Based on the high-resolution bR structure and the projection structures obtained, I have built a homology model. On the basis of this homology model, several residues found in the dimer interface were selected for mutational studies in order to disrupt the dimer interface.
The investigation of light-induced conformational changes in C128T ChR2 was the second part of my thesis. I designed an experimental setup for trapping light-induced conformational changes in C128T ChR2. In addition, I optimized the sample preparation in a way that the different illumination conditions did not alter the quality of the crystals. I have trapped two different functional states, namely the conductive open state and the non-conductive closed dark-adapted state.
In order to visualize the location and the extent of conformational changes, projection difference maps were calculated between the open and the closed state. Visual inspection of the difference maps between the open and the two closed states revealed three difference peaks that map to the TMHs 2, 6, and 7, indicating significant and specific rearrangements of these helices. The strong pair of positive/negative peaks at TMH6 suggests an outward tilt movement of approximately 2 Å. Close comparison of similar work on bR revealed that this movement is likely to occur at the cytoplasmic end of TMH6. A second highly significant negative peak is observed at TMH7, indicating a less pronounced tilt compared to TMH6. The third negative peak at TMH2 indicates a loss of density in this region. No significant differences were recorded at the TMH1, 5 and at the dimer interface formed by TMH3 and 4.
I succeeded in trapping and characterizing the open and closed state in the photocycle of ChR2 and could demonstrate that the transition from the closed to the open state is linked to significant light-induced tilt movements of TMH6 and 7, plus a loss of order in TMH2. These conformational changes are likely to create a large water-filled conducting pore, which seems to be required for the conductance of up to 2,000 ions per photocycle. The previously mentioned spectroscopic studies support the difference structures I obtained. This approach sets the stage for studying structural changes accompanying the formation and decay of other photocycle intermediates in ChR2. Future studies will aim at three-dimensional maps of the open and closed state at higher resolution.
ATP synthases are multi-subunit membrane enzymes, which utilize the energy stored in a transmembrane electrochemical ion gradient to produce adenosine-5´-triphosphate (ATP), the universal energy carrier in biological systems. Research on these important enzymes goes back more than 50 years and has produced innumerable studies. The F-type ATP synthase consists of two functionally distinct, but tightly coupled subcomplexes, the water-soluble F1 and the membrane-embedded Fo complex. In its simplest form, F1 consists of five different subunits with a stoichiometry of α 3β3γδε, and harbors three catalytic centers in the α 3β3-headpiece, while Fo consists of three different subunits in a stoichiometry of ab2cn, where n varies between 8 to 15 depending on the species. From a mechanistic standpoint, the complex can also be divided into two different units, namely a stator, α3β3δ-ab2, and a rotor, γε-cn. The enzyme utilizes the energy stored in a transmembrane electrochemical gradient of protons, or in some cases Na+, to drive ATP synthesis. In particular, the downhill translocation of these ions across the Fo complex drives rotation of the γε-cn unit, which is then transduced to the active centers, catalyzing the phosphorylation of adenosine-5`-diphosphate (ADP) with inorganic phosphate (Pi), and the release of ATP....
Transport of proteins into or across cellular membranes is mediated by the conserved and ubiquitous Sec-machinery. The Sec-homologue in the inner membrane of Escherichia coli is SecYEG. Sec-mediated insertion of numerous membrane proteins is aided by YidC, another protein integral to the inner membrane of Escherichia coli. YidC fulfils in addition the integration of a variety of membrane proteins Sec-independently. It belongs to a conserved but structurally uncharacterised family of proteins important for membrane protein biogenesis and comprises homologues in mitochondria and chloroplasts. By modification of a former crystallisation protocol two-dimensional crystals of SecYEG were grown in presence of the signal sequence peptide of LamB. Recording of structural data by electron cryo-microscopy and calculation of a difference structure comparing a former SecYEG projection structure with the one of SecYEG crystallised in presence of the substrate revealed several new and vacant densities. These hint to signal peptide binding close to the translocation pore and to significant rearrangements in proximity to the lateral exit site for transmembrane domains in SecYEG. The difference structure suggests that dimeric SecYEG is an asymmetric molecule consisting of one active and one inactive SecYEG monomer. Detergent removal from a mixture of purified YidC and lipids produced two-dimensional crystals that were highly dependent on the ionic strength and lipid composition for their growth. Electron cryo-microscopy on the frozen-hydrated crystals and image processing visualised structural details at about 10 Å resolution. Averaging two alternative projection structures in p2 and p121_a symmetry, respectively, yielded essentially the same features. Four YidC monomers form one unit cell (dimensions 82 x 71 Å, included angle 85 ° and 90 °, respectively) and seem to be arranged as two sets of dimers integrated in an anti-parallel fashion into the membrane. An area of low density in the centre of each YidC monomer resembles possibly a constriction of the membrane, which could have particular relevance for the integration of substrate proteins into the lipid bilayer.
Life-threatening fungal infections are becoming increasingly common for immunocompromised patients such as those with AIDS, or those undergoing organ transplantation or chemotheraphy, as well as for other health-vulnerable patients. Excellent targets for antifungal drugs are chitin synthases, which are essential for survival of the fungus and lacking in humans. To design new antifungal drugs, knowledge of the three-dimensional structure and mechanism of action of chitin synthases are crucial. Chitin synthases are members of an important family of enzymes that synthesize structural polysaccharides, such as cellulose, β(1,3)-glucan, β(1,4)-mannan and hyaluronan. Therefore, chitin synthases could be used as a model system to understand these more complex enzymes, which are also of major medical and commercial importance. Chitin synthase 2 from Saccharomyces cerevisiae (ScChS2), the protein under study, is an integral membrane protein that synthesizes the primary septum between mother and daughter cells in budding yeast. It is essential for proper cell separation and expected to be highly regulated. An important aspect is that ScChS2 shows 55% sequence identity and is functionally analogous to chitin synthase 1 from the human opportunistic pathogen Candida albicans, this enzyme is also essential for cell survival (Munro, Winter et al. 2001). ...
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.
Membrane proteins are a diverse group of proteins that serve a multitude of purposes with one of the most important ones being transport. All kinds of substrates are shuffled over biological membranes with the help of dedicated proteins enabling the transport along and against a concentration gradient. Within the group of actively transporting proteins a diverse set of proteins that rely on an electrochemical gradient to facilitate transport of a substrate against its concentration gradient can be found. Those so-called secondary active
transporters are a group on integral membrane proteins ubiquitous to all cells. They allow the transport of all kinds of substrates like nutrients, ions, other metabolites and drugs over the hydrophobic barrier created by the cellular and organellar membrane. The gradients that provide the main driving force for most of the transporters are either sodium ions or protons, although transporters utilizing other ions or organic compounds are found as well. In case of exchangers two very similar substrates are transported in opposing direction over the membrane, one against its electrochemical gradient driven by the other.
Along with a structural diversity of the transporters concerning overall shape, oligomerization and number of transmembrane elements comes a mechanistic variety though still following the principle of alternating access. In humans the malfunction of secondary active transporters can lead to a physiological disorders such as epilepsy, depression or obesity.
The focus of this thesis was the structural and functional characterization of the secondary active transporter SeCitS from Salmonella enterica, a symporter of the 2-hydroxycarboxylate family. The transport of citrate as a bivalent ion is facilitated by the flux of sodium ions that have an inward-facing gradient over the inner membrane of Salmonella enterica. Transport experiments showed that the transport ratio is two sodium ions per citrate molecule, netting in an electroneutral transport. Compared to other members of the family the specificity of the transporter towards its main substrate is very high.
Structural information on the protein was initially obtained through 2D electron crystallography, which allowed the identification of the oval shaped dimer and a first hint towards a significant conformational change that the protein undergoes during its transport cycle. Using 3D crystallography, the X-ray structure of the transporter was solved. The protein crystalizes as a stable, but conformationally asymmetric dimer. As bound citrate can be readily identified in both protomers they can be assigned into an outward- and an inward-facing conformation, with the main citrate binding site in the outward-facing conformation.
One interesting feature of the crystal structure was the large surface available for multimerization, providing a platform for tight dimerization of the two protomers. On the other hand, SeCitS did not show a true cooperativity of transport. With those two aspects taken into account the question arose if any potential crosstalk between the monomers within the dimer takes place and influences transport (negative cooperativity) or the conformational distribution within the dimer (stabilization of the protein within the membrane).
The functional approach in answering this question was the use of mutated variants of the protein for cross-linking within one monomer. Two residues were chosen respectively to lock one of either conformation to be able to test for transport activity in the remaining protomer. The suitability of the residues was derived from the crystal structure (D112 – R205 to lock the inward-facing conformation and L337 – S412 for the outward-facing conformation). After initial promising results the final variants were not stable enough to be analyzed in transport assays.
To analyze the distribution of relative conformations within the dimer the protein was reconstituted into native-like lipid environment such as nanodiscs or saposin nanoparticles to be analyzed by cryo-electron microscopy. The first images were recorded and did yield promising 2D classes where the general features of the transporter were identified. Yet, an improved preparation is required to obtain a high resolution structure.
The key functional aspects of a transporter are its ability to bind and transport its substrates. In a set of experiments those features were investigated by a radioligand transport assay and by isothermal titration calorimetry (ITC). The transport properties of the protein were assessed in a filter assay using a radioactively labeled citrate as a read-out. The protein was reconstituted into proteoliposomes and subjected to different substrate conditions. Different ions were tested in its ability to drive or inhibit transport, but only sodium ions were able to drive transport and also not hindered by the presence of other ions...
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.