Tytuł artykułu
Autorzy
Wybrane pełne teksty z tego czasopisma
Identyfikatory
Warianty tytułu
Języki publikacji
Abstrakty
The methodology of obtaining a logarithmic velocity profile describing the velocity distribution in the cross section of the boundary layer, which is based on the well-known equation of L. Prandtl, based on its semi-empirical turbulence theory, is considered. It is shown that the logarithmic velocity profile obtained in this way does not satisfy any boundary condition arising from the classical definition of such concept as the boundary layer. The perfect coincidence of this velocity profile with the experimental data of Nikuradze demonstrated in the world scientific literature is a consequence of making these profiles not in a fixed, but in a floating coordinate system. When rebuilding the velocity profiles obtained at different Reynolds numbers, all the profiles lose their versatility and do not coincide with the actual velocity profiles in cylindrical pipes.
Czasopismo
Rocznik
Tom
Strony
637--647
Opis fizyczny
Bibliogr. 4 poz., wykr.
Twórcy
autor
- National Research University, "Moscow Power Engineering Institute", Moscow, Russian Federation
Bibliografia
- [1] Sedov, L. I.: Continuum mechanics, Science, 2, 1976.
- [2] Loitsyansky, L.G.: Fluid and gas mechanics, Science, 1970.
- [3] Schlichting, H.: Theory of boundary layer, Science, 1969.
- [4] Prandtl, L.: Fluid mechanics, Second ed. RHD, Moscow-Izhevsk, 2002.
Uwagi
Opracowanie rekordu w ramach umowy 509/P-DUN/2018 ze środków MNiSW przeznaczonych na działalność upowszechniającą naukę (2018).
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-844745c6-4e5a-4d2d-be31-99f17374572d