Secondary flow of second kind in a short channel observed by PIV

Kód výsledku v IS VaVaI

<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F61388998%3A_____%2F20%3A00517246" target="_blank" >RIV/61388998:_____/20:00517246 - isvavai.cz</a>

Nalezeny alternativní kódy

RIV/49777513:23210/20:43957446

Výsledek na webu

<a href="https://www.sciencedirect.com/science/article/pii/S0997754619304029" target="_blank" >https://www.sciencedirect.com/science/article/pii/S0997754619304029</a>

DOI - Digital Object Identifier

<a href="http://dx.doi.org/10.1016/j.euromechflu.2019.10.005" target="_blank" >10.1016/j.euromechflu.2019.10.005</a>

Jazyk výsledku

angličtina

Název v původním jazyce

Secondary flow of second kind in a short channel observed by PIV

Popis výsledku v původním jazyce

By using the Stereo Particle Image Velocimetry (PIV) technique we observe the secondary flow of second kind in a corner of a channel of square cross-section. The boundary layer thickness is much lower than the channel size. Therefore, the flow is still developing, not filling the entire channel cross-section, which is the case more widely reported in literature studied in a very long channel. The non-linear secondary effects of interacting boundary layers are observed as a single stream-wise vortex close to the channel corner in case of laminar boundary layers. In the case of turbulent boundary layers, the secondary flow takes shape of a symmetric pair of counter-rotating vortices. This pattern is observable only in the average velocity field, while the instantaneous ones display large amount of vortices, whose spatial distribution close to the corner in dependence on their orientation leads to statistically emergent net vorticity. At the same time, this pattern is reproduced by using a numerical simulation.

Název v anglickém jazyce

Secondary flow of second kind in a short channel observed by PIV

Popis výsledku anglicky

By using the Stereo Particle Image Velocimetry (PIV) technique we observe the secondary flow of second kind in a corner of a channel of square cross-section. The boundary layer thickness is much lower than the channel size. Therefore, the flow is still developing, not filling the entire channel cross-section, which is the case more widely reported in literature studied in a very long channel. The non-linear secondary effects of interacting boundary layers are observed as a single stream-wise vortex close to the channel corner in case of laminar boundary layers. In the case of turbulent boundary layers, the secondary flow takes shape of a symmetric pair of counter-rotating vortices. This pattern is observable only in the average velocity field, while the instantaneous ones display large amount of vortices, whose spatial distribution close to the corner in dependence on their orientation leads to statistically emergent net vorticity. At the same time, this pattern is reproduced by using a numerical simulation.

Druh

J_imp - Článek v periodiku v databázi Web of Science

CEP obor

—

OECD FORD obor

20302 - Applied mechanics

Projekt

—

Návaznosti

I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace

Rok uplatnění

2020

Kód důvěrnosti údajů

S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Název periodika

European Journal of Mechanics B-Fluids

ISSN

0997-7546

e-ISSN

1873-7390

Svazek periodika

79

Číslo periodika v rámci svazku

January

Stát vydavatele periodika

FR - Francouzská republika

Počet stran výsledku

10

Strana od-do

444-453

Kód UT WoS článku

000503315100038

EID výsledku v databázi Scopus

2-s2.0-85074360691