High energy physics. Proc. ICHEP'06, vol.2 by Alexey Sissakian, Gennady Kozlov, Elena Kolganova

By Alexey Sissakian, Gennady Kozlov, Elena Kolganova

Belonging to the celebrated "Rochester convention Series", ICHEP 2006 is an important foreign convention in 2006 on excessive power physics. those lawsuits offer a entire overview of modern advancements in experimental and theoretical physics of debris at excessive energies. This quantity good points articles at the most up-to-date ends up in all of the crucial parts: particle astrophysics and cosmology, neutrino physics, lattice calculations and computational quantum box concept, heavy ion collisions and quark subject, difficult and gentle interactions in quantum chromodynamics, electroweak physics, additional dimensions and additional gauge bosons, CP violation and infrequent decays, most sensible and Higgs seek, hadron spectroscopy and exotics, heavy quark physics, GRID disbursed research, R&D for destiny accelerators, detectors and new amenities, and mathematical points of quantum box thought and string concept.

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4: Temperaturabhangigkeit dynamischen Zahigkeit /i der Druckabhangigkeit der Zahigkeit /i. 4 zeigt den qualitativen Verlauf der Temper aturabhangigkeit fiir Fliissigkeiten und Gase bei konstantem Druck. In Fliissigkeiten nimmt die kinematische Zahigkeit /i mit steigender Temperatur ab, wahrend sie in Gasen zunimmt. Die Zahigkeit von Fliissigkeiten und Gasen nimmt mit wachsendem Druck zu. An diesen kurzen Exkurs in die Molekiilphysik schhefit sich die Begriindung fiir die bereits eingefiihrte Randbedingung an festen Wanden an.

Bei einem Wassertropfen auf einer Wachsoberflache tritt dagegen keine Benetzung auf und der Kontaktwinkel ist damit grower als 90°. 01 auf Glas benetzt nahezu vollstandig mit ce ^ 0. Die Oberflachenspannung des 01s ist verschwindend klein gegeniiber der Adhasionskraft zwischen 01 und Glas. 16) , sofern die einzelnen Oberflachenspannungen bekannt sind. Aufgrund der Oberflachenspannung ist die Fliissigkeit bestrebt, Minimalflachen zu bilden. 9 nachweisen. In eine Seifenlaugenhaut wird ein Faden mit Schlaufe eingebracht.

B. die Zahigkeit (Reibung), Warmeleitung (Energietransport), Diffusion (Massentransport). Fiir die unterschiedlichen Bereiche des stromenden Fluids gelten die entsprechenden 11 — /// j \ 1 \ \ \ — ^^ 1 Staupunkt Abb. £) ( ^ Abb. 34: Stofi zweier Kugeln (Punktmechanik) Grundgleichungen der Kontinuumsmechanik: Masse-, Impuls- und Energieerhaltung, die sowohl fiir die reibungsbehaftete Grenzschichtstromung also auch fiir die reibungsfreie Aufienstromung gelten und in Kapitel 3 behandelt werden. Eine ganz andere Einteilung der Stromungsgebiete erlauben die Stromungsgrofien Geschwindigkeit v und Dichte p.

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