Ansatz zur Generierung einer konditionalen, reversiblen Wt1 k.o.-Maus

Ansatz zur Generierung einer konditionalen, reversiblen Wt1 k.o.-Maus Der Wilms-Tumor (WT, Nephroblastom) ist ein embryonaler Nierentumor, der durch die maligne Transformation von undifferenziertem Nierengewebe, sog. nephrogenen Resten, entsteht. WT treten mit einer Inzidenz von 1 in 10.000 Lebendgeburten auf. Das Hauptmanifestationsalter, der normalerweise einseitig und sporadisch auftretenden Tumore, liegt zwischen dem 3. und 4. Lebensjahr. Etwa 10 % der Patienten entwickeln jedoch bilaterale Tumore. In diesen Fällen ist eine Assoziation mit komplexen genetischen Krankheitsbildern (u. a. WAGR-, Denys-Drash-, Frasier- und Beckwith-Wiedemann-Syndrom) festzustellen. In 15 % der sporadischen WT sind Mutationen im WT1 (Wilms-Tumor 1)-Gen beschrieben. WT1 besteht aus zehn Exons und weist typische Merkmale von Transkriptionsfaktoren (z. B. vier Zinkfinger) auf. Zwei alternative Spleißereignisse betreffen Exon 5 (+/−Exon 5) und Exon 9 (Transkripte mit bzw. ohne die codierenden Sequenzen für die AS Lysin-Threonin-Serin; +/−KTS). Die Lage der drei alternativ vorhandenen AS zwischen den Zinkfingern 3 und 4 bestimmt die verschiedenen Funktionen der WT1-Proteine (4 Isoformen) als Transkriptionsfaktor (−KTS) bzw. als RNA-bindendes Protein (+KTS). Das zunächst im Zusammenhang mit WT als Tumorsuppressorgen identifizierte WT1 ist ein Entwicklungsgen mit einem sehr komplexen Expressionsmuster in der Embryonalentwicklung. Dabei ist v. a. die Bedeutung in der Urogenitalentwicklung entscheidend. Konstitutive, homozygote Wt1−/− k.o.-Mäuse sind embryonal (~ E12,5 dpc) letal und bilden u. a. keine Gonaden und keine Nieren. Aus diesem Grund existiert bisher kein Wilms-Tumormodell. Die Herstellung eines konditionalen murinen Tiermodells auf Basis des Tet on/off-Systems zur Untersuchung der Nierenentwicklung bzw. zur Analyse der Wilms-Tumorpathogenese war Ziel dieser Arbeit. Hierfür wurden drei Mauslinien generiert: Zwei transgene sog. Responder-Linien, die eine chimäre spleißbare Wt1-cDNA der Variante musWt1+Exon 5;+/−KTS unter der Kontrolle eines Tet-responsiven Promotors im Genom tragen. Dieses tTA/Dox-abhängig regulierbare Wt1-Transgen (tgWt1) sollte (exogen regulierbar) die Expression des endogenen Wt1-Lokus ausreichend nachahmen, um die kritischen Phasen der Embryogenese zu überwinden und lebensfähige Tiere zu erhalten. Parallel dazu wurde die Wt1-Effektor-Mauslinie (WE2) generiert. Diese trägt einen tetrazyklinabhängigen Transaktivator (tTA) zur Steuerung Tet-regulierbarer Transgene unter der Kontrolle des endogenen Wt1-Promotors. Die durch homologe Rekombination in ES-Zellen erreichte Integration des tTA direkt am Translationsstartpunkt des Wt1-Lokus hat in den Tieren einen heterozygoten Wt1 knock out/tTA knock in zur Folge. Die bisher vorgenommenen Verpaarungen doppelt transgener Wt1-tTA+/−/Resp-Mäuse ergaben keinen Rescue des letalen Wt1 k.o. und es konnten bislang keine Wilms-Tumore induziert werden. Alle im Verlauf der Arbeit generierten Mauslinien wurden umfassend charakterisiert. So konnte für die Tiere der Responder-Linien Wt1-Resp1 (mit zusätzlichen Isolator-Sequenzen zum Schutz des Transgens vor Positionseffekten) und Wt1-Resp2 (ohne Isolatoren) konnte die Tet-induzierbare Expression und die Spleißbarkeit des tgWt1 in MEF-Assays und mittels Effektor-Mäusen auf RNA-Ebene nachgewiesen werden. Die genomische Charakterisierung der WE2-Linie ergab eine ungeklärte etwa 120 kb große Inversion am Wt1-Lokus, die alle 5'-regulatorischen Sequenzen mitsamt des tTA vom Rest von Wt1 trennt. Tiere dieser Linie weisen aber dennoch einen funktionalen Wt1 k.o. auf: Unter den Nachkommen aus Intercross-Verpaarungen von Wt1-tTA+/−-Mäusen lassen sich auf Grund der Letalität keine Wt1−/−-Genotypen nachweisen. Die Charakterisierung der Effektor-Linie auf RNA-Ebene und mittels Reporter-Mäusen liefert ein Wt1-analoges tTA-Expressionsmuster: So findet man eine deutliche tTA-Expression u. a. in Niere (Glomeruli), Uterus, Ovar und Testis. Die hier vorgestellten Experimente ergeben darüber hinaus eindeutige Hinweise einer Beteiligung von Wt1 in der Entstehung der glatten Muskulatur bzw. in der Vaskulogenese.

Analysing the possible influence of transposon TCl4.7 insertion on the function of the genome of Cydia pomonella granulovirus

CpGV-MCp5 is a natural mutant of the Cydia pomonella Granulovirus (Mexican isolate) (CpGV-M) that harbors an insect host transposon termed TCl4.7 in its genome. TCl4.7 is located between the open reading frames Cp15 and Cp16 and separates two homologous regions hr3 and hr4, which have been recently shown to be origins of replication of CpGV-M. The MCp5 has a significant replication disadvantage in the presence of the wild-type CpGV-M. In this study, the possible effects of TCl4.7 transposon insertion on the genome function of its insertion site has been analysed. The role of Cp15 and Cp16 in the context of the virus infection cycle was examined by generating a CpGV-Bacmid (CpBAC) and Cp15 knock-out (CpBACCp15KO) and Cp16 knock-out (CpBACCp16KO) mutants. The mutant CpBACCp15KO was not able to replicate in CM larvae suggesting that Cp15 was essential for virus replication. In contrast, the mutant CpBACCp16KO infected CM larvae and produced viable occlusion bodies (OBs) demonstrating that Cp16 is a non-essential gene for virus in vivo infection of C. pomonella. The temporal transcription of Cp15 and Cp16, as well as of Cp31 (F protein) as a control, was analysed using RT-PCR and quantitative real-time PCR. It suggested a general delay or reduction of gene transcription of MCp5 compared to the parental CpGV-M. Western blot analyses using anti-Cp15 and anti-Cp16 polyclonal antibodies, however, did not show any immuno-reactive response. Thus, a direct influence of TCl4.7 on the expression of Cp15 and Cp16 could not be substantiated. To investigate whether the interruption of hr3 and hr4 palindromes affects the virus replication, two mutant bacmids with a deletion of hr3 and hr4 (CpBAChr3/hr4-KO) and another with an insertion of a Kanamycin resistance cassette between hr3 and hr4 (CpBAChr3-kan-hr4) were generated. Both mutant bacmids replicated and produced infectious virus OBs, which did not significantly differ in their median lethal concentration (LC50) and median survival time (ST50) compared to the parental CpBAC. Interestingly, the mutant CpBAChr3-kan-hr4 was very effectively out-competed by parental CpBAC, when CM larvae were co-infected with known ratios of OBs of CpBAC and the mutant CpBAChr3-kan-hr4. These observations suggested a functional co-operation between hr3 and hr4 which was interrupted by the KanR insertion in CpBAChr3-kan-hr4 and possibly by TCl4.7 transposon insertion in the mutant MCp5. This hypothesis may explain the observed replication disadvantage of the mutants MCp5 and CpBAChr3-kan-hr4 in the presence of the parental viruses CpGV-M and CpBAC, respectively.

Soil biogenic emissions of nitric oxide from arid and semi-arid ecosystems

The biogenic production of NO in the soil accounts for between 10% and 40% of the global total. A large degree of the uncertainty in the estimation of the biogenic emissions stems from a shortage of measurements in arid regions, which comprise 40% of the earth’s land surface area. This study examined the emission of NO from three ecosystems in southern Africa which cover an aridity gradient from semi-arid savannas in South Africa to the hyper-arid Namib Desert in Namibia. A laboratory method was used to determine the release of NO as a function of the soil moisture and the soil temperature. Various methods were used to up-scale the net potential NO emissions determined in the laboratory to the vegetation patch, landscape or regional level. The importance of landscape, vegetation and climatic characteristics is emphasized. The first study occurred in a semi-arid savanna region in South Africa, where soils were sampled from 4 landscape positions in the Kruger National Park. The maximum NO emission occurred at soil moisture contents of 10%-20% water filled pore space (WFPS). The highest net potential NO emissions came from the low lying landscape positions, which have the largest nitrogen (N) stocks and the largest input of N. Net potential NO fluxes obtained in the laboratory were converted in field fluxes for the period 2003-2005, for the four landscape positions, using soil moisture and temperature data obtained in situ at the Kruger National Park Flux Tower Site. The NO emissions ranged from 1.5-8.5 kg ha-1 a-1. The field fluxes were up-scaled to a regional basis using geographic information system (GIS) based techniques, this indicated that the highest NO emissions occurred from the Midslope positions due to their large geographical extent in the research area. Total emissions ranged from 20x103 kg in 2004 to 34x103 kg in 2003 for the 56000 ha Skukuza land type. The second study occurred in an arid savanna ecosystem in the Kalahari, Botswana. In this study I collected soils from four differing vegetation patch types including: Pan, Annual Grassland, Perennial Grassland and Bush Encroached patches. The maximum net potential NO fluxes ranged from 0.27 ng m-2 s-1 in the Pan patches to 2.95 ng m-2 s-1 in the Perennial Grassland patches. The net potential NO emissions were up-scaled for the year December 2005-November 2006. This was done using 1) the net potential NO emissions determined in the laboratory, 2) the vegetation patch distribution obtained from LANDSAT NDVI measurements 3) estimated soil moisture contents obtained from ENVISAT ASAR measurements and 4) soil surface temperature measurements using MODIS 8 day land surface temperature measurements. This up-scaling procedure gave NO fluxes which ranged from 1.8 g ha-1 month-1 in the winter months (June and July) to 323 g ha-1 month-1 in the summer months (January-March). Differences occurred between the vegetation patches where the highest NO fluxes occurred in the Perennial Grassland patches and the lowest in the Pan patches. Over the course of the year the mean up-scaled NO emission for the studied region was 0.54 kg ha-1 a-1 and accounts for a loss of approximately 7.4% of the estimated N input to the region. The third study occurred in the hyper-arid Namib Desert in Namibia. Soils were sampled from three ecosystems; Dunes, Gravel Plains and the Riparian zone of the Kuiseb River. The net potential NO flux measured in the laboratory was used to estimate the NO flux for the Namib Desert for 2006 using modelled soil moisture and temperature data from the European Centre for Medium Range Weather Forecasts (ECMWF) operational model on a 36km x 35km spatial resolution. The maximum net potential NO production occurred at low soil moisture contents (<10%WFPS) and the optimal temperature was 25°C in the Dune and Riparian ecosystems and 35°C in the Gravel Plain Ecosystems. The maximum net potential NO fluxes ranged from 3.0 ng m-2 s-1 in the Riparian ecosystem to 6.2 ng m-2 s-1 in the Gravel Plains ecosystem. Up-scaling the net potential NO flux gave NO fluxes of up to 0.062 kg ha-1 a-1 in the Dune ecosystem and 0.544 kg h-1 a-1 in the Gravel Plain ecosystem. From these studies it is shown that NO is emitted ubiquitously from terrestrial ecosystems, as such the NO emission potential from deserts and scrublands should be taken into account in the global NO models. The emission of NO is influenced by various factors such as landscape, vegetation and climate. This study looks at the potential emissions from certain arid and semi-arid environments in southern Africa and other parts of the world and discusses some of the important factors controlling the emission of NO from the soil.

Simulations of charge transport in organic compounds

To aid the design of organic semiconductors, we study the charge transport properties of organic liquid crystals, i.e. hexabenzocoronene and carbazole macrocycle, and single crystals, i.e. rubrene, indolocarbazole and benzothiophene derivatives (BTBT, BBBT). The aim is to find structure-property relationships linking the chemical structure as well as the morphology with the bulk charge carrier mobility of the compounds. To this end, molecular dynamics (MD) simulations are performed yielding realistic equilibrated morphologies. Partial charges and molecular orbitals are calculated based on single molecules in vacuum using quantum chemical methods. The molecular orbitals are then mapped onto the molecular positions and orientations, which allows calculation of the transfer integrals between nearest neighbors using the molecular orbital overlap method. Thus we obtain realistic transfer integral distributions and their autocorrelations. In case of organic crystals the differences between two descriptions of charge transport, namely semi-classical dynamics (SCD) in the small polaron limit and kinetic Monte Carlo (KMC) based on Marcus rates, are studied. The liquid crystals are investigated solely in the hopping limit. To simulate the charge dynamics using KMC, the centers of mass of the molecules are mapped onto lattice sites and the transfer integrals are used to compute the hopping rates. In the small polaron limit, where the electronic wave function is spread over a limited number of neighboring molecules, the Schroedinger equation is solved numerically using a semi-classical approach. The results are compared for the different compounds and methods and, where available, with experimental data. The carbazole macrocycles form columnar structures arranged on a hexagonal lattice with side chains facing inwards, so columns can closely approach each other allowing inter-columnar and thus three-dimensional transport. When taking only intra-columnar transport into account, the mobility is orders of magnitude lower than in the three-dimensional case. BTBT is a promising material for solution-processed organic field-effect transistors. We are able to show that, on the time-scales of charge transport, static disorder due to slow side chain motions is the main factor determining the mobility. The resulting broad transfer integral distributions modify the connectivity of the system but sufficiently many fast percolation paths remain for the charges. Rubrene, indolocarbazole and BBBT are examples of crystals without significant static disorder. The high mobility of rubrene is explained by two main features: first, the shifted cofacial alignment of its molecules, and second, the high center of mass vibrational frequency. In comparsion to SCD, only KMC based on Marcus rates is capable of describing neighbors with low coupling and of taking static disorder into account three-dimensionally. Thus it is the method of choice for crystalline systems dominated by static disorder. However, it is inappropriate for the case of strong coupling and underestimates the mobility of well-ordered crystals. SCD, despite its one-dimensionality, is valuable for crystals with strong coupling and little disorder. It also allows correct treatment of dynamical effects, such as intermolecular vibrations of the molecules. Rate equations are incapable of this, because simulations are performed on static snapshots. We have thus shown strengths and weaknesses of two state of the art models used to study charge transport in organic compounds, partially developed a program to compute and visualize transfer integral distributions and other charge transport properties, and found structure-mobility relations for several promising organic semiconductors.