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Nanostructured ferritic oxide dispersion strengthened (ODS) alloy is an ideal candidate for fission/fusion power plant materials, particularly in the use of a first-wall and blanket structure of a next generation reactor. These steels usually contain a high density of Y-Al-O nanoparticles, high dislocation densities and fine grains. The material contains nanoparticles with an average diameter of 21 nm. Irradiation of these alloys was performed with a dual beam irradiation of 2.5 MeV Fe+/31 dpa and 350 keV He+/18 appm/dpa. Irradiation causes atomic displacements resulting in vacancy and self-interstitial lattice defects and dislocation loops. Additionally to structural changes, the effect of the irradiation generated defects on the mechanical properties of the ODS is investigated by nanoindentation. A clear hardness increase in the irradiated area is observed, which reaches a maximum at a close surface region. This feature is attributed to synergistic effects between the displacement damage and He implantation resulting in He filled vacancies.
Das ProInno-Projekt „Feinschleifen von Saphir“ (www.tfhwildau.de/mmueck) beschäftigt sich mit der Weiterentwicklung eines Verbundwerkstoffes für den Feinschleifprozess. Bei diesem Verbundwerkstoff handelt es sich um Diamantkörner, die in einer Kupfer-Zinn-Matrix eingebettet sind. In dem Projekt werden die Wirkungsmechanismen des neuartigen Verbundmaterials genauer untersucht. Mit diesen Erkenntnissen erfolgt eine Optimierung der einzelnen Komponenten und des Mischungsverhältnisses auf praxisbezogene Eigenschaften des Werkstoffes. Es ist geplant, hieraus ein marktfähiges Produkt zur Oberfl ächenbearbeitung harter Materialien zu entwickeln.
Da Bauteile immer kleiner und Beschichtungen immer dünner werden, erlangt die direkte und genaue Bestimmung mechanischer Eigenschaften im Nanobereich immer größere Bedeutung. Versteht man die Effekte im Nanobereich, wird es einfacher, auch Effekte im Makrobereich vorherzusagen. Damit bekommen die entsprechenden Messmethoden eine entscheidende Bedeutung bei der Entwicklung der Materialien und Herstellungsmethoden im Hinblick auf optimierte Produkteigenschaften. Aus diesem Grund entwickelte sich jenseits der klassischen mechanischen Prüfverfahren, welche in der Makrodimension angesiedelt sind, in den letzten fünf Jahren ein neuer Zweig der Werkstoffprüfung, der sich mit den Materialeigenschaften im Nanobereich beschäftigt. Dies ist von grundlegender Bedeutung für die Nanotechnologie. In diesem Bericht sollen zwei Geräte in Bezug zueinander gesetzt werden, die die Messung verschiedener nanomechanischer Eigenschaften erlauben. Dabei handelt es sich um das TriboScope (Hysitron Inc.) als Aufsatz für ein Rasterkraftmikroskop (SFM) und das Nanoscan (Technological Institute for Superhard and Novel Carbon Materials; Troitsk/Russland), dargestellt in den Abbildungen 1 und 2. Diese ermöglichen die Messung von Härte und E-Modul einer Oberfläche.
Vacancy-type defects created by helium implantation in tungsten and their impact on the nano-hardness characteristics were investigated by correlating the results from the positron annihilation spectroscopy and the nano-indentation technique. Helium implantation was performed at room temperature (RT) and at an elevated temperate of 600 °C. Also, the effect of post-annealing of the RT implanted sample was studied. The S parameter characterizing the open volume in the material was found to increase after helium irradiation and is significantly enhanced for the samples thermally treated at 600 °C either by irradiation at high temperature or by post-annealing. Two types of helium-vacancy defects were detected after helium irradiation; small defects with high helium-to-vacancy ratio (low S parameter) for RT irradiation and large defects with low helium-to-vacancy ratio (high S parameter) for thermally treated tungsten. The hardness of the heat treated tungsten coincides with the S parameter, and hence is controlled by the large helium-vacancy defects. The hardness of tungsten irradiated at RT without thermal treatment is dominated by manufacturing related defects such as dislocation loops and impurity clusters and additionally by trapped He atoms from irradiation effects, which enhance hardness. He-stabilized dislocation loops mainly cause the very high hardness values in RT irradiated samples without post-annealing.
We report the synthesis of aggregated diamondnanorods (ADNRs) from fullerene C60C60 at 20(1) GPa and 2200 °C using a multianvil apparatus. Individual diamond nanoroads are of 5–20 nm in diameter and longer than 1μm1μm. The x-ray and measured density of ADNRs is ∼0.2%–0.4%∼0.2%–0.4% higher than that of usual diamond. The extremely high isothermal bulk modulusKT=491(3)GPaKT=491(3)GPa [compare to KT=442(4)GPaKT=442(4)GPa of diamond] was obtained by in situx-ray diffraction study. Thus, ADNRs is the densest among all carbonmaterials and it has the lowest so far experimentally determined compressibility.
Since in-depth sensing indentation load–depth data of the entire loading–unloading cycle are available, more information than a single hardness value and an elastic modulus can be extracted from the experimental data. The conventional hardness H (h) = F (h)/Ac(h) and the differential hardness Hd(h)=dF/dAc are calculated as continuous functions of depth h and compared to each other in this paper (F: load, Ac: contact area). It turns out that Hd describes the momentary material resistance to deformation, whereas H integrates over deformation states from first tip–sample contact to current penetration h. This difference is particularly important for materials not homogeneous in depth (e.g. layer systems), and for situations where time-dependent external factors influence the momentary deformation resistance. Photoplasticity is considered as an example for the latter.
Complementary large scale molecular-dynamics simulations and experiments have been carried out to determine the atomistic mechanisms of the nanoindentation process in single crystal Fe {110}, {100}, and {111}. The defect formation and motion causes the complex mechanisms of plastic and elastic deformation which is reflected in the pileup patterns. The experimental results show distinct patterns of pileup material which are dependent on the individual crystal faces and the superposition of the stress field of the indenter. The highest pileup around the indenter hole occurs on the {100} surface and the shallowest on {111}. The least symmetric surface is {110} which produces an experimental pileup pattern displaying only twofold symmetry with the axially symmetric indenter. The pyramidal indenter produces an asymmetric pattern which changes as the crystal is rotated with respect to the tip but repeats with threefold rotational symmetry. Material displacement occurs primarily in planes of the {110} family. Pileup is formed by cross slip between planes of the same family which intersect in ⟨111⟩ directions. For the {110} surface, dislocation loops propagate in the four in-plane ⟨111⟩ directions and the two inclined
⟨111⟩ directions. The loops that propagate in the in-plane directions are terminated by edge dislocations at the surface. These transport material away from the tip but cannot produce pileup. The loops that propagate in the inclined direction cross slip and cause the observed pileup. The {100} surface has fourfold rotational symmetry and all the ⟨111⟩ directions are inclined. The dislocation loops propagate in these directions and cross slip readily occurs, leading to a large pileup. The {111} face shows the least pileup which is more spread out over the surface. In this case the dislocation loops propagate in shallow slip planes and do not readily cross slip. Experimentally determined force-depth curves show distinct “pop-ins” which correspond to the formation of dislocations. The contact pressure (nanohardness) is not a constant and increases with decreasing indentation depth. It also changes with crystal face. Calculated force-depth curves match the experimental trend but give estimates of the nanohardness and Young’s modulus higher than those values experimentally determined.
"Computersimulation & Computergraphik" : Sommerschule vom 22.-26. September 1997 an der TFH Wildau
(1998)
Ziel der Sommerschule "Computersimulation & Computergraphik" war es, in einem Piloprojekt Kontakte, Wissensaustausch und Vernetzung zwischen verschiedenen Fachdisziplinen über gemeinsam genutzte moderne Medien und Computertechniken zu erreichen. Gleichzeitig wurden praktische Fertigkeiten für die Computersimulation und Computergraphik vermittelt und interessante Anwendungen in Technik und Wirtschaft demonstriert. Es wurde während dieser Woche auf anschauliche und praktische Weise anhand verschiedener Softwarepakete eine Einführung in die komplexe Thematik gegeben und gezeigt, wie Visualisierung auf PCs und im Internet realisiert werden kann.
A project was funded by the European Union to build foundations for a virtual laboratory where experimental and theoretical results could be combined into an audio-visual interactive presentation through the use of modern computers. The process of thin film growth and modification by energetic ion beams was chosen as the first topic for this new educational tool.
Different models for thin film growth are developed and compared to experimental results in the presentation. Particular examples include spiral formation, modelled using cellular automata, island growth using Monte-Carlo methods and the first few layers of growth using classical molecular dynamics. Most of the examples are related to the growth of C60 films for which a number of experimental results had been obtained and previously reported in this journal [1]. The principle property under investigation was the structure and morphology of the films. Nine separate computer movies of the dynamics of these processes were developed on a fast PC under Windows95 and incorporated into a computer presentation made using the Authorware package. Experimental images obtained from a scanning force microscope were also included and compared to the computer models along with music and verbal explanation. In addition to the interactive version of the multi-media presentation, a non-interactive version was also made which is suitable for lectures or conference presentation. This version lasts approximately 25 minutes. Approximately 100 CD's of this work were made and are being distributed to various laboratories. A copy of the CD is available on request.
Diamanten kommen in der Natur vor und werden technisch über die Hochdruck-Hochtemperatur-Synthese erzeugt oder als polykristalline Schicht durch chemische Gasphasenabscheidung aus einem Kohlenwasserstoffplasma abgeschieden. Mit der Verarbeitung von Diamantkörnern in Verbundwerkstoffen werden neue leistungsfähige Schneid- und Polierwerkzeuge entwiCkelt. Diamantbeschichtungen oder Diamantkeramiken ermöglichen die Herstellung von dünnen Schneidwerkzeugen und Anwendungen in Elektronik und Optik mit extremer Belastbarkeit. Fullerene, Nanoröhrchen und Zwiebelstrukturen aus Kohlenstoff haben sich seit ihrer Entdeckung im Jahre 1985 zu einem eigenständigen Forschungsgebiet entwickelt und besitzen außergewöhnliche mechanische, optische und elektronische Eigenschaften, die sie für unterschiedlichste Anwendungen prädestinieren.

