Ingenieurwissenschaften und zugeordnete Tätigkeiten
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- CFD simulation (1)
- Dünnschichte (1)
- Multilayer (1)
- PVD (1)
- Pool fires (1)
- Slip-rolling resistance (1)
- Wälzbeständigkeit (1)
- Zr(C, N) coating (1)
- multilayer (1)
- organic peroxides flame characteristics (1)
Experimental investigation and CFD simulation of organic peroxide pool fires (TBPB and TBPEH)
(2010)
Time averaged mass burning rate (m˙′′f ), flame length (H), temperature (T ), irradi- ance (E) and surface emissive power (SEP ) of TBPB (tert -butyl peroxybenzoate) and TBPEH (tert-butyl peroxy-2-ethylhexanoate) pool fires are measured for six pool di- ameters (d = 0.059 m, 0.107 m, 0.18 m, 0.5 m, 1 m and 3.4 m) at BAM in house and outside test facility. The measured heats of combustion (–Δhc) of TBPB and TBPEH are 30113 kJ/kg and 34455 kJ/kg and the specific heat capacities at constant pressure (cp) are 1.8 kJ/(kg K) and 2.1 kJ/(kg K) respectively. The measured m˙′′f of TBPB and TBPEH pool fires are in the range of 0.37 kg/(m2 s)≤ m˙ ′′ f ≤ 0.83 kg/(m2 s) and show little dependence on the pool diameter d, and are four to sixty times higher (for d = 1 m) than that of hydrocarbon pool fires. It is shown that the mass burning rates of the investigated organic peroxides can be represented as an exponential function of the self-accelerating decomposition temperature (SADT). Low SADT implies that the organic peroxide pool fires burn at a much higher m˙′′f than hydrocarbon pool fires. Fuel Froude numbers (Frf) of TBPB and TBPEH are 5 to 100 times (depending on d) higher than for hydrocarbon pool fires. Due to higher Frf the H of TBPB and TBPEH (measured with a S-VHS Videocamera) are found to be two times larger (d = 1 m) than corresponding pool fires of hydrocarbons. Heskestads flame length correlation predicts the Hd (d = 3.4 m) of TBPB and TBPEH pool fires much better than Thomas and Fay correlations. The measured time averaged flame temperatures T (d = 3.4 m) for TBPB and TBPEH pool fires are in the range of 1400 K ≤ T ≤ 1500 K and are 200 K to 300 K higher than for JP-4, kerosene and gasoline. The irradiances of the TBPB and TBPEH pool fires measured by radiometers are E (Δy/d = 0.3) = 45 kW/m2 and E = 98 kW/m2 which are two to ten times higher in comparison to the corresponding n-pentane, super gasoline and diesel pool fires. So the thermal safety distances for organic peroxide pool fires are larger by a factor four in comparison to the hydrocarbon pool fires. An infrared thermography system is used for the determination of SEP of TBPB and TBPEH pool fires. The values of surface emissive power for TBPB and TBPEH are SEP (d = 3.4 m) = 196 kW/m2 and SEP = 258 kW/m2 and thus the SEP are by a factor of approximately two higher than for hydrocarbon pool fires. A self-sustained pulsating Hd (’W’-Effect) is found in TBPB pool flames and is further analysed to explain the reason of occurance on the basis of chemical structure of the fuel and discontinuous heat flux back from flame to the liquid pool. CFD simulations of TBPB and TBPEH pool fires at d = 0.18 m, 0.5 m, 1 m, 3.4 m and 8 m are carried out using the Unsteady Reynolds Averaged Navier Stokes (URANS) equa- tions. The three-dimensional geometries have been discritized with unstructured hybrid grids, with the number of cells in the range of 1 million. Depending on the grid resolu- tion and the pool diameter time steps of 0.0001 s ≤ Δt ≤ 0.01 s for the CFD simulations are used. For solving the discritized equations a finite volume based implicit solver AN- SYS CFX has been used. For modelling the combustion, stoichiometric combustion for both peroxides are assumed. The temperature dependence of the reaction rate has been determined by the Arrhenius approach. For modelling the combustion eddy dissipation concept (EDC) model has been used. For turbulence buoyancy modified k- � and SAS (Scale Adaptive Simulation) turbulence models are used. For the thermal radiation and soot mass fraction discrete transfer radiation model and Magnusson soot model have been used. A new method is suggested for the prediction of mass burning rate (m˙′′f ) by CFD simula- tion. Both peroxide pool fires show approximately constant mass burning rate indepen- dent of d whereas m˙′′f of TBPEH are under predicted at the beginning but show relatively good agreement with measurements for large pool diameters (d = 1 m). In case of TBPB the CFD simulation over predicts the mass burning rate m˙′′f of small TBPB pool fires and shows a continuous decrease with d. CFD predicts the flame length H close to the measured data provided that the constants in Thomas equation are modified. The CFD predicted time averaged surface emission flame temperatures of TBPB and TBPEH pool fires (d = 3.4 m, 1437 K and 1542 K) are in good agreement with the measured time averaged flame temperatures. The CFD predicted SEP for TBPB and TBPEH pool fires (d = 3.4 m, 217 kW/m2 and 288 kW/m2) are also in agreement with the measured values. From the CFD predicted irradiance ECFD it is possible to determine the thermal safety distances from large pool fires of hydrocarbons and organic peroxides.
Slip-rolling resistance of novel Zr(C,N) thin film coatings under high Hertzian contact pressures
(2010)
The present work was carried out within the framework of my four years activities as a scientific co-worker in the Working Group Tribological Optimization; Failure Analysis; Extreme Exposure in the division Tribology and Wear protection (VI.2) of the BAM Federal Institute for Materials Research and testing in Berlin, Germany and generously funded by the German Research Foundation (DFG WO521/6-1). First of all, I would like to express my sincere thanks to my supervisor Dr.-Ing. Mathias Woydt, head of the aforementioned working group, who gave me the opportunity to start my professional development, initiated and intensively supported this PhD work as well as accepted to take part in thesis committee. Prof. Dr. rer. nat. Walter Reimers, Chairman of the Institute for Materials Science and Technology of the Technical University of Berlin (TU Berlin), is also gratefully thanked for his interest in the thesis subject, for helpful comments and suggestions as well as for agreeing to participate in the referee of this work. I would like to thank also Prof. Dr.-Ing. Claudia Fleck, Chairman of the Material Engineering Department (Fachgebiet Werkstofftechnik) of the Technical University Berlin (TU Berlin), for assuming the chairmanship of the thesis committee. All the staff of the tribology division is also greatly acknowledged for bringing a pleasant working environment. Dr. Dirk Spaltmann is particularly thanked for the helpful discussions as well as for his assistance in English formulation. Dipl.-Ing. Manuel Reichelt and my bureau colleague Dr.-Ing. Géraldine Theiler will find here my many thanks for promoting constantly a good working atmosphere. Sigrid Binkowski and Dipl.-Ing. Norbert Kelling are also gratefully acknowledged for their constant and helpful technical support. André Otto is also thanked for his substantial administrative support. My sincere thanks go to Dr. rer. nat. (and “by the way” world and olympic champion in eights rowing) Ilona Dörfel (BAM V.1, Composition and Microstructure of Engineering Materials) for performing the highly relevant TEM investigations as also Heidemarie Rooch, and Ing. Wolfgang Gesatzke for the specific preparation of the samples. Furthermore, I greatly appreciate the contributions of Dr.-Ing. Vasile-Dan Hodoroaba, Birgid Strauß, Sigrid Benemann and Dipl.-Phys. Thomas Wirth (BAM VI.4) for their valuable contributions in microscopy analysis and to Dr.-Ing. Eric Wild (TU Berlin) for the substantial residual stress analysis of the coatings. Acknowledgement is also due to Dr. Thomas Chudoba from ASMEC GmbH for performing hardness measurements with his QCSM module. Thanks are surely extended to Fundación Tekniker, specifically Josu Goikoetxea and Dr. Javier Barriga for the manufacturing of the coatings in industrial deposition chambers and to the machining shop BAM Z.5 for the specimens preparation. Last, but by no means the least, I would like to thank all my friends for their support and to all the people who helped me directly or indirectly in my doctoral work and/or for my pleasant German adaptation. My very special thanks (du fond du coeur) go to my beloved parents Marie-Hélène (What is Tribology?) and Gérard (I miss you so much) and “of course” to my bright (and sometimes nerve-racking) sister Sophie, for everlasting encouragement and plenty of good advices in a wide range of domains. Ania, especially for your contribution in the decision of pursuing my “German experiment”.