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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Kübel, Christian
in Cooperation with on an Cooperation-Score of 37%
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Publications (44/44 displayed)
- 2024Lifecycle of Pd Clusters:Following the Formation and Evolution of Active Pd Clusters on Ceria During CO Oxidation by In Situ/Operando Characterization Techniquescitations
- 2024Graphitizability of Polymer Thin Films: An In Situ TEM Study of Thickness Effects on Nanocrystalline Graphene/Glassy Carbon Formationcitations
- 2024Controlling shear band instability by nanoscale heterogeneities in metallic nanoglasses
- 2024Lifecycle of Pd Clusters: Following the Formation and Evolution of Active Pd Clusters on Ceria During CO Oxidation by In Situ/Operando Characterization Techniques
- 2024Dependence of the Structural and Magnetic Properties on the Growth Sequence in Heterostructures Designed by YbFeO$_3$ and BaFe$_{12}$O$_{19}$
- 2024The Impact of Microstructure on Filament Growth at the Sodium Metal Anode in All‐Solid‐State Sodium Batteries
- 2024Precipitate-mediated enhancement of mechanical and electrical properties in HPTE-processed Al–Mg–Si alloy
- 2024Deformation twins as a probe for tribologically induced stress statescitations
- 2023Graphitizability of Polymer Thin Films: An In Situ TEM Study of Thickness Effects on Nanocrystalline Graphene/Glassy Carbon Formationcitations
- 2023Poly(ethylene oxide)-block-poly(hexyl acrylate) Copolymers as Templates for Large Mesopore Sizes─A Detailed Porosity Analysiscitations
- 2023Kinetics and Pore Formation of the Sodium Metal Anode on NASICON‐Type Na$_{3.4}$ Zr$_2$Si$_{2.4}$P$_{0.6}$O$_{12}$ for Sodium Solid‐State Batteries
- 2023Novel thin film high entropy alloys with tunable microstructure and enhanced mechanical properties
- 2023The Impact of Microstructure on Filament Growth at the Sodium Metal Anode in All‐Solid‐State Sodium Batteriescitations
- 2023Direct Observation of Quadrupolar Strain Fields forming a Shear Band in Metallic Glassescitations
- 2023Deposition of Sodium Metal at the Copper‐NaSICON Interface for Reservoir‐Free Solid‐State Sodium Batteriescitations
- 2023Multi‐component PtFeCoNi core‐shell nanoparticles on MWCNTs as promising bifunctional catalyst for oxygen reduction and oxygen evolution reactionscitations
- 2023Deformation twins as a probe for tribologically induced stress states
- 2023Unraveling the Electrochemical Mechanism in Tin Oxide/MXene Nanocomposites as Highly Reversible Negative Electrodes for Lithium‐Ion Batteriescitations
- 2022Kinetics and Pore Formation of the Sodium Metal Anode on NASICON‐Type Na$_{3.4}$ Zr$_2$Si$_{2.4}$P$_{0.6}$O$_{12}$ for Sodium Solid‐State Batteriescitations
- 2022In Situ Generated Shear Bands in Metallic Glass Investigated by Atomic Force and Analytical Transmission Electron Microscopycitations
- 2022Effects of metal-based additives on dehydrogenation process of 2NaBH4 + MgH2 systemcitations
- 2022Direct observation of Eshelby inclusions in metallic glasses
- 2021Unveiling the Local Atomic Arrangements in the Shear Band Regions of Metallic Glasscitations
- 2021Generating digital twins of mesoporous silica by graph-based stochastic microstructure modelingcitations
- 2020Early deformation mechanisms in the shear affected region underneath a copper sliding contactcitations
- 2020Designing Structurally Ordered Pt/Sn Nanoparticles in Ionic Liquids and their Enhanced Catalytic Performancecitations
- 2020Microfluidic Crystallization of Surfactant-Free Doped Zinc Sulfide Nanoparticles for Optical Bioimaging Applicationscitations
- 2020First-time synthesis of a magnetoelectric core-shell composite via conventional solid-state reactioncitations
- 2019Ostwald-like Ripening in Highly Defective Graphene
- 2019Electron beam effects on oxide thin films - structure and electrical property correlationscitations
- 2018Evolution of Glassy Carbon Microstructure: In Situ Transmission Electron Microscopy of the Pyrolysis Process
- 2018Evolution of Glassy Carbon Microstructure: In Situ Transmission Electron Microscopy of the Pyrolysis Processcitations
- 2018(De)Lithiation Mechanism of Hierarchically Layered LiNi$_{1/3}$Co$_{1/3}$Mn$_{1/3}$O$_{2}$ Cathodes during High-Voltage Cyclingcitations
- 2018MOF-templated synthesis of 3D Bi2O3 supracrystals with bcc packingcitations
- 2018Structure and Properties of Nanoglassescitations
- 2016Influence of gas atmospheres and ceria on the stability of nanoporous gold studied by environmental electron microscopy and in situ ptychographycitations
- 2015Light emission, light detection and strain sensing with nanocrystalline graphenecitations
- 2015Fatigue Behavior of Ultrafine-Grained Medium Carbon Steel with Different Carbide Morphologies Processed by High Pressure Torsioncitations
- 2015Nanoporous-gold-based composites : toward tensile ductility
- 2014Laser ablation mechanism for modification of composite electrodes with improved electrolyte wetting behaviour
- 2014Density changes in shear bands of a metallic glass determined by correlative analytical transmission electron microscopycitations
- 2013Influence of particle size and fluorination ratio of CFₓ precursor compounds on the electrochemical performance of C-FeF₂ nanocomposites for reversible lithium storagecitations
- 2011Microstructure of sol-gel derived nanoscaled La0.6Sr0.4CoO 3-delta cathodes for intermediate-temperature SOFCs
- 2010Tungsten materials for structural divertor applications
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document
Tungsten materials for structural divertor applications
Abstract
Michael Rieth1, Andreas Hoffmann2, Edeltraud Materna-Morris1, Magnus Rohde1 1 Karlsruhe Institute of Technology, Institute for Materials Research I, Karlsruhe, Germany; 2 PLANSEE Metall GmbH, Development Refractory Alloys, Reutte, Austria Introduction Present design studies for extremely high loaded plasma facing cooling components make use of the high temperature strength and good heat conductivity of tungsten [e.g. 1, 2]. The most critical issue of tungsten materials in connection with structural applications is their brittleness. It is known that fracture behaviour as well as thermal conductivity depends on textures. Therefore, the microstructure, the chemical composition and their influence on thermal conductivity as well as on impact bending properties were investigated, using commercial tungsten and other refractory alloys. Results and Discussion Heat conductivity was measured by the laser-flash method for a tungsten plate (4 mm thick), for a W-1wt.%La2O3 (WL10) rod and plate, for a DENSIMET (W3.5wt.%Ni-1.5wt.%Fe) plate, and for a Ta-10wt.%W (TaW10) rod and plate. DENSIMET and WL10 are binary phase materials while TaW10 is an alloy (solid solution). The measurements were performed perpendicular to the plate surfaces and parallel to the rod axis. The results are given in Fig. 1. Fig. 1: Thermal conductivity of various refractory materials. With rising temperatures, the tungsten plate and WL10 materials show a continuous decrease of conductivity whereas TaW10 and DENSIMET show an increase. With values higher than 90 W/mK at 1300°C, pure tungsten and WL exhibit the best results. However, a clear reduction of the conductivity can be observed in the case of the pure tungsten and WL10 plates. On the one hand, this behaviour is a consequence of the lanthanum-oxide content, and of the microstructure (compared to the WL10 rod), on the other. Fabrication and testing of Charpy specimens has been performed according to the EU standards DIN EN ISO 148-1 and 14556:2006-10. That is, small size specimens (27 mm x 3 mm x 4 mm, 1 mm notch depth, 22 mm span) have been used. To avoid oxidation the whole Charpy testing machine was placed inside a vacuum vessel which was operated at typical pressures of about 10-3 mBar. The Charpy tests were performed on specimens fabricated from rods as well as from standard and with highest possible level of deformation (WL10opt), potassium (0.005 wt.%) doped tungsten (WVM), and WL10 with 1 wt.% Re (W1Re1-La2O3). Plates of pure W, WL10, WVM, and molybdenum-Ti-Zr (TZM) were also used for the investigation. More detailed information about material fabrication, microstructure examinations, and Charpy test results can be found in [3, 4]. Typically, bcc metals show a transition from brittle (transcrystalline) to ductile fracture. But the tungsten based rod materials don’t show this single transition. Moreover, only specimens of pure tungsten and WVM show fully ductile fractures, starting at 900 °C and 1000 °C, respectively. Fig. 3: Side view of delamination fractures in Charpy specimens of various tungsten rod materials. However, all materials tend to exhibit brittle fracture temperatures below 600 °C. Above that temperature, the specimens show fractures which propagate along the rod axis, that is, parallel to the specimen’s long side and perpendicular to the notch (see Fig. 3). There are obviously similarities to the fracturing of fiber reinforced materials and, therefore, this type of fracture is usually called delamination. In summary, there are three types of fracture (brittle, delamination, and ductile) which are linked by a brittle-to-delamination transition and a delamination-to-ductile transition. Compared to the rod materials, the Charpy energies of specimens of the plate materials are lower by more than 50 %. Moreover, all plate material specimens don’t show fully ductile fractures, even at test temperatures up to 1100 °C. Below 500 °C the