Funktion der C 4-Dicarboxylat-Transporter DctA und DcuB als Co-Sensoren von DcuS in Escherichia coli

Escherichia coli kann C4-Dicarboxylate sowohl unter aeroben als auch unter anaeroben Bedingungen zur Energiekonservierung nutzen. Die Synthese der beteiligten Transporter und Enzyme wird auf der Transkriptionsebene durch das Zweikomponentensystem DcuSR reguliert. DcuS ist der Sensor für C4-Dicarboxylate. Der Antwortregulator DcuR wird von DcuS aktiviert und induziert die Expression des C4-Dicarboxylat-Transporters DctA unter aeroben Verhältnissen. Anaerob verstärkt DcuSR die Expression des Fumarat/Succinat-Antiporters DcuB, der Fumarase B und der Fumaratreduktase FrdABCD. DctA und DcuB agieren als Co-Sensoren von DcuS und üben einen negativen Effekt auf die Genexpression von dctA bzw. dcuB aus.rnIn dieser Arbeit wurde die Funktion von DctA und DcuB als Co-Sensoren von DcuS untersucht. Sowohl für DcuB als auch für DctA wurde eine direkte Protein-Protein-Interaktion mit DcuS über ein bakterielles Two-Hybrid System nachgewiesen. DcuS bildete ein Transporter-Sensor-Cluster mit DctA und DcuB. C-terminale Verkürzung und die Mutagenese einzelner Aminosäuren der C-terminalen Helix 8b von DctA führten zu einem Verlust der Interaktion mit DcuS. Mit dieser Interaktion gingen sowohl die regulatorische Funktion als auch die Transportfunktion der Punktmutante DctA-L414A verloren. Ein Verlust der Interaktion wurde ebenfalls zwischen einer konstitutiv aktiven DcuS-Mutante und wildtypischem DctA beobachtet. Ebenso zeigte sich eine partielle Reduktion der Interaktion von DcuS mit DctA, wenn DcuS nach der zweiten Transmembranhelix verkürzt wurde. Die Interaktion zwischen DcuS und DctA wurde durch den Effektor Fumarat modifiziert, ging aber nicht komplett verloren.rnDctA konnte in verschiedenen Plasmidsystemen überproduziert werden und bildete Homotrimere. Die Topologie von DctA wurde mit experimentellen und in silico Methoden aufgeklärt. DctA ähnelt der Struktur und Topologie des Aminosäuretransporters Glt aus Pyrococcus horikoshii. DctA besitzt acht Transmembranhelices mit einem cytosolischen N- und C-Terminus sowie zwei Haarnadelschleifen. Die Substratbindung findet höchstwahrscheinlich in den Haarnadelschleifen statt und der Transport erfolgt nach dem „alternating access“ Modell.rnAußerdem wurde die Funktion des Transporters YfcC untersucht. Das Gen yfcC wurde mit Schlüsselgenen des Acetatstoffwechsels co-transkribiert. In yfcC-Deletionsstämmen zeigte sich ein stammspezifischer Defekt bei Wachstum mit Acetat und Transport von Acetat.

Na +-coupled betaine symporters involved in osmotic stress response in prokaryotes and eukaryotes

The betaine/GABA transporter BGT1 is one of the most important osmolyte transporters in the kidney. BGT1 is a member of the neurotransmitter sodium symporter (NSS) family, facilitates Na+/Cl--coupled betaine uptake to cope with hyperosmotic stress. Betaine transport in kidney cells is upregulated under hypertonic conditions by a yet unknown mechanism when increasing amounts of intracellular BGT1 are inserted into the plasma membrane. Re-establishing isotonicity results in ensuing depletion of BGT1 from the membrane. BGT1 phosphorylation on serines and threonines might be a regulation mechanism. In the present study, four potential PKC phosphorylation sites were mutated to alanines and the responses to PKC activators, phorbol 12-myristate acetate (PMA) and dioctanoyl-sn-glycerol (DOG) were determined. GABA-sensitive currents were diminished after 30 min preincubation with these PKC activators. Staurosporine blocked the response to DOG. Three mutants evoked normal GABA-sensitive currents but currents in oocytes expressing the mutant T40A were greatly diminished. [3H]GABA uptake was also determined in HEK-293 cells expressing EGFP-tagged BGT1 with the same mutations. Three mutants showed normal upregulation of GABA uptake after hypertonic stress, and downregulation by PMA was normal compared to EGFP-BGT1. In contrast, GABA uptake by the T40A mutant showed no response to hypertonicity or PMA. Confocal microscopy of the EGFP-BGT1 mutants expressed in MDCK cells, grown on glass or filters, revealed that T40A was present in the cytoplasm after 24 h hypertonic stress while the other mutants and EGFP-BGT1 were predominantely present in the plasma membrane. All four mutants co-migrated with EGFP-BGT1 on Western blots suggesting they are full-length proteins. In conclusion, T235, S428, and S564 are not involved in downregulation of BGT1 due to phosphorylation by PKC. However, T40 near the N-terminus may be part of a hot spot important for normal trafficking or insertion of BGT1 into the plasma membrane. Additionally, a link between substrate transport regulation, insertion of BGT1 into the plasma membrane and N-glycosylation in the extracellular loop 2 (EL2) could be revealed. The functional importance of two predicted N-glycosylation sites, which are conserved in EL2 within the NSS family were investigated for trafficking, transport and regulated plasma membrane insertion by immunogold-labelling, electron microscopy, mutagenesis, two-electrode voltage clamp measurements in Xenopus laevis oocytes and uptake of radioactive-labelled substrate into MDCK cells. Trafficking and plasma membrane insertion of BGT1 was clearly promoted by proper N-glycosylation in both, oocytes and MDCK cells. De-glycosylation with PNGase F or tunicamycin led to a decrease in substrate affinity and transport rate. Mutagenesis studies revealed that in BGT1 N183 is the major N-glycosylation site responsible for full protein activity. Replacement of N183 with aspartate resulted in a mutant, which was not able to bind N-glycans suggesting that N171 is a non-glycosylated site in BGT1. N183D exhibited close to WT transport properties in oocytes. Surprisingly, in MDCK cells plasma membrane insertion of the N183D mutant was no longer regulated by osmotic stress indicating unambiguously that association with N-glycans at this position is linked to osmotic stress-induced transport regulation in BGT1. The molecular transport mechanism of BGT1 remains largely unknown in the absence of a crystal structure. Therefore investigating the structure-function relationship of BGT1 by a combination of structural biology (2D and 3D crystallization) and membrane protein biochemistry (cell culture, substrate transport by radioactive labeled GABA uptake into cells and proteoliposomes) was the aim of this work. While the functional assays are well established, structure determination of eukaryotic membrane transporters is still a challenge. Therefore, a suitable heterologous expression system could be defined, starting with cloning and overexpression of an optimized gene. The achieved expression levels in P. pastoris were high enough to proceed with isolation of BGT1. Furthermore, purification protocols could be established and resulted in pure protein, which could even be reconstituted in an active form. The quality and homogeneity of the protein allowed already 2D and 3D crystallization, in which initial crystals could be obtained. Interestingly, the striking structural similarity of BGT1 to the bacterial betaine transporter BetP, which became a paradigm for osmoregulated betaine transport, provided information on substrate coordination in BGT1. The structure of a BetP mutant that showed activity for GABA was solved to 3.2Å in complex with GABA in an inward facing open state. This structure shed some light into the molecular transport mechanisms in BGT1 and might help in future to design conformationally locked BGT1 to enforce the on-going structure determination.

Electronic transport in the heavy fermion superconductors UPd 2 Al 3 and UNi 2 Al 3

This work addresses the electronical properties of the superconductors UPd2Al3 and UNi2Al3 on the basis of thin film experiments. These isotructural compounds are ideal candiates to study the interplay of magnetism and superconductivity due to the differences of their magnetically ordered states, as well as the experimental evidence for a magnetic pairing mechanism in UPd2Al3. Epitaxial thin film samples of UPd2Al3 and UNi2Al3 were prepared using UHV Molecular Beam Epitaxy (MBE). For UPd2Al3, the change of the growth direction from the intrinsic (001) to epitaxial (100) was predicted and sucessfully demonstrated using LaAlO3 substrates cut in (110) direction. With optimized deposition process parameters for UPd2Al3 (100) on LaAlO3 (110) superconducting samples with critical temperatures up to Tc = 1.75K were obtained. UPd2Al3-AlOx-Ag mesa junctions with superconducting base electrode were prepared and shown to be in the tunneling regime. However, no signatures of a superconducting density of states were observed in the tunneling spectra. The resistive superconducting transition was probed for a possible dependence on the current direction. In contrast to UNi2Al3, the existence of such feature was excluded in UPd2Al3 (100) thin films. The second focus of this work is the dependence of the resisitive transition in UNi2Al3 (100) thin films on the current direction. The experimental fact that the resisitive transition occurs at slightly higher temperatures for I║a than for I║c can be explained within a model of two weakly coupled superconducting bands. Evidence is presented for the key assumption of the two-band model, namely that transport in and out of the ab-plane is generated on different, weakly coupled parts of the Fermi surface. Main indications are the angle dependence of the superconducting transition and the dependence of the upper critical field Bc2 on current and field orientation. Additionally, several possible alternative explanations for the directional splitting of the transition are excluded in this work. An origin due to scattering on crystal defects or impurities is ruled out, likewise a relation to ohmic heating or vortex dynamics. The shift of the transition temperature as function of the current density was found to behave as predicted by the Ginzburg-Landau theory for critical current depairing, which plays a significant role in the two-band model. In conclusion, the directional splitting of the resisitive transition has to be regarded an intrinsic and unique property of UNi2Al3 up to now. Therefore, UNi2Al3 is proposed as a role model for weakly coupled multiband superconductivity. Magnetoresistance in the normalconducting state was measured for UPd2Al3 and UNi2Al3. For UNi2Al3, a negative contribution was observed close to the antiferromagnetic ordering temperature TN only for I║a, which can be associated to reduced spin-disorder scattering. In agreement with previous results it is concluded that the magnetic moments have to be attributed to the same part of the Fermi surface which generates transport in the ab-plane.

Transport properties of YBa 2 Cu 3 O 7, PrBa 2 Cu 3 O 7-superlattices

The understanding of the coupling between superconducting YBa2Cu3O7 (YBCO) layers decoupled by non superconducting PrBa2Cu3O7 (PBCO) layers in c-axis oriented superlattices was the aim of this thesis. For this purpose two conceptually different kind of transport experiments have been performed. rnrnIn the first type of transport experiments the current is flowing parallel to the layers. Here the coupling is probed indirectly using magnetic vortex lines, which are penetrating the superlattice. Movement of the vortex segments in neighbouring YBCO layers is more or less coherent depending on the thickness of both the superconducting and non superconducting layers. This in-plane transport was measured either by sending an external current through bridges patterned in the superlattice or by an induced internal current. rnThe vortex-creep activation energy U was determined by analysis of the in-plane resistive transition in an external magnetic field B oriented along the c-axis. The activation energies for two series of superlattices were investigated. In one series the thickness of the YBCO layers was constant (nY=4 unit cells) and the number of the PBCO unit cells was varied, while in the other the number of PBCO layers was constant (nP=4) and nY varied. The correlation length of the vortex system was determined to be 80 nm along the c-axis direction. It was found that even a single PBCO unit cell in a superlattice effectively cuts the flux lines into shorter weakly coupled segments, and the coupling of the vortex systems in neighbouring layers is negligible already for a thickness of four unit cells of the PBCO layers. A characteristic variation of the activation energy for the two series of superlattices was found, where U0 is proportional to the YBCO thickness. A change in the variation of U0 with the current I in the specimen was observed, which can be explained in terms of a crossover in the vortex creep process, generated by the transport current. At low I values the dislocations mediated (plastic) vortex creep leads to thermally assisted flux-flow behaviour, whereas at high current the dc transport measurements are dominated by elastic (collective) creep.rnThe analysis of standard dc magnetization relaxation data obtained for a series superlattices revealed the occurrence of a crossover from elastic (collective) vortex creep at low temperature to plastic vortex creep at high T. The crossover is generated by the T dependent macroscopic currents induced in the sample. The existence of this creep crossover suggests that, compared with the well known Maley technique, the use of the normalized vortex creep activation energy is a better solution for the determination of vortex creep parameters.rnrnThe second type of transport experiments was to measure directly a possible Josephson coupling between superconducting CuO2 double planes in the superlattices by investigation of the transport properties perpendicular to the superconducting planes. Here three different experiments have been performed. The first one was to pattern mesa structures photolithographically as in previous works. The second used three-dimensional nanostructures cut by a focused ion beam. For the these two experiments insufficient patterning capabilities prevented an observation of the Josephson effect in the current voltage curves. rnA third experiment used a-axis and (110) oriented YBCO films, where in-plane patterning can in principle be sufficient to measure transport perpendicular to the superconducting planes. Therefore the deposition of films with this unusual growth orientation was optimized and investigated. The structural and microstructural evolution of c-axis to a-axis orientation was monitored using x-ray diffraction, scanning electron microscopy and magnetization measurements. Films with full a-axis alignment parallel to the substrate normal could be achieved on (100)SrTiO3. Due to the symmetry of the substrate the c-axis direction in-plane is twofold. Transferring the deposition conditions to films grown on (110)SrTiO3 allowed the growth of (110) oriented YBCO films with a unique in-plane c-axis orientation. While these films were of high quality by crystallographic and macroscopic visual inspection, electron microscopy revealed a coherent crack pattern on a nanoscale. Therefore the actual current path in the sample was not determined by the macroscopic patterning which prohibited investigations of the in-plane anisotropy in this case.rn

Lysosomaler Transport kationischer Aminosäuren durch Mitglieder der SLC7-Familie

Lysosomaler Transport kationischer Aminosäuren (KAS) stellt einen Rettungsweg in der Cystinose-Therapie dar. Ein solches Transportsystem wurde in humanen Hautfibroblasten beschrieben und mit System c benannt. Des Weiteren stellt lysosomales Arginin eine Substratquelle für die endotheliale NO-Synthase (eNOS) dar. Das von der eNOS gebildete NO ist ein wichtiges vasoprotektiv wirkendes Signalmolekül. Ziel war es daher, herauszufinden, ob Mitglieder der SLC7-Unterfamilie hCAT möglicherweise System c repräsentieren.rnIn dieser Arbeit konnte ich die lysosomale Lokalisation verschiedener endogener, sowie als EGFP-Fusionsproteine überexprimierter CAT-Isoformen nachweisen. Mittels Fluoreszenz-mikroskopie wurde festgestellt, dass die in U373MG-Zellen überexprimierten Fusionsproteine hCAT-1.EGFP sowie SLC7A14.EGFP mit dem lysosomalen Fluoreszenz-Farbstoff LysoTracker co-lokalisieren. Eine Lokalisation in Mitochondrien oder dem endoplasmatischem Retikulum konnte mit entsprechenden Fluoreszenz-Farbstoffen ausgeschlossen werden. Zusätzlich reicherten sich die überexprimierten Proteine hCAT-1.EGFP, hCAT-2B.EGFP und SLC7A14.EGFP in der lysosomalen Fraktion C aus U373MG-Zellen zusammen mit den lysosomalen Markern LAMP-1 und Cathepsin D an. Gleiches galt für den endogenen hCAT-1 in der lysosomalen Fraktion C aus EA.hy926- und U373MG-Zellen sowie für den SLC7A14 in den humanen Hautfibroblasten FCys5. Mit dem im Rahmen dieser Arbeit generierte Antikörper gegen natives SLC7A14 konnte erstmals die endogene Expression und Lokalisation von SLC7A14 in verschiedenen Zelltypen analysiert werden.rnObwohl eine Herunterregulation des hCAT-1 in EA.hy926-Endothelzellen nicht zu einer Reduktion der Versorgung der eNOS mit lysosomalem Arginin führte, ist eine Funktion von hCAT-1 im Lysosom wahrscheinlich. Sowohl die [3H]Arginin- als auch die [3H]Lysin-Aufnahme der Fraktion C aus U373MG-hCAT-1.EGFP war signifikant höher als in die Fraktion C aus EGFP-Kontrollzellen. Dies konnte ebenfalls für den hCAT-2B.EGFP gezeigt werden. Zusätzlich zeigten lysosomale Proben aus U373MG-hCAT-2B.EGFP-Zellen in der SSM-basierten Elektrophysiologie eine elektrogene Transportaktivität für Arginin. Das Protein SLC7A14.EGFP zeigte in keiner der beiden durchgeführten Transportstudien eine Aktivität. Dies war unerwartet, da die aus der Diplomarbeit stammende und im Rahmen dieser Dissertation erweiterte Charakterisierung der hCAT-2/A14_BK-Chimäre, die die „funktionelle Domäne“ des SLC7A14 im Rückgrat des hCAT-2 trug, zuvor den Verdacht erhärtet hatte, dass SLC7A14 ein lysosomal lokalisierter Transporter für KAS sein könnte. Diese Studien zeigten allerding erstmals, dass die „funktionelle Domäne“ der hCATs die pH-Abhängigkeit vermittelt und eine Rolle in der Substraterkennung spielt.rnZukünftig soll weiter versucht werden auch endogen eine Transportaktivität der hCATs für KAS im Lysosom nachzuweisen und das Substrat für das intrazellulär lokalisierte Waisen-Protein SLC7A14 zu finden. Eine mögliche Rolle könnte SLC7A14 als Transporter für Neurotransmitter spielen, da eine sehr prominente Expression im ZNS festgestellt wurde.rn