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Osborne Reynolds (* 23. August 1842 in Belfast, Nordirland; † 21. Februar 1912 in Watchet in Somerset, England) war ein britischer Physiker. Nach ihm ist die Reynolds-Zahl, eine Kennzahl zur Beurteilung reibungsbehafteter Strömungs vorgänge und den Übergang zur Turbulenz, und die Reynolds-Gleichungen für turbulente Strömungen ...
Osborne Reynolds FRS (23 August 1842 – 21 February 1912) was an Irish-born British innovator in the understanding of fluid dynamics. Separately, his studies of heat transfer between solids and fluids brought improvements in boiler and condenser design. He spent his entire career at what is now the University of Manchester.
4. Apr. 2024 · Osborne Reynolds (born Aug. 23, 1842, Belfast, Ire.—died Feb. 21, 1912, Watchet, Somerset, Eng.) was a British engineer, physicist, and educator best known for his work in hydraulics and hydrodynamics. Reynolds was born into a family of Anglican clerics.
- The Editors of Encyclopaedia Britannica
Quick Info. Born. 23 August 1842. Belfast, Ireland. Died. 21 February 1912. Watchet, Somerset, England. Summary. Osborne Reynolds was an Irish mathematician and physicist best known for introducing the Reynolds number classifying fluid flow. View three larger pictures. Biography.
9. Okt. 1995 · Abstract. The paper seeks to place the landmark paper ‘On the dynamical theory of incompressible viscous fluids and the determination of the criterion’, published by the Royal Society in 1895, within the broader context of the complete scientific works of its author, Osborne Reynolds.
9. Dez. 2020 · Reynolds und die Turbulenz. Die Reihe namhafter Physiker und Mathematiker mit Bezug zur Meteorologie setzen wir im heutigen Tagesthema fort mit Osborne Reynolds, einem der Pioniere auf dem Gebiet der Strömungsmechanik. Osborne Reynolds wurde am 23. August 1842 in Belfast, Irland geboren.
In 1883 Osborne Reynolds, a British engineer and physicist, demonstrated that the transition from laminar to turbulent flow in a pipe depends upon the value of a mathematical quantity equal to the average velocity of flow times the diameter of the tube times the mass density of the fluid divided by its absolute viscosity.
