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Statements

Subject Item
n2:RIV%2F00216305%3A26210%2F13%3APU111467%21RIV15-MSM-26210___
rdf:type
skos:Concept n21:Vysledek
rdfs:seeAlso
http://www.epj-conferences.org/articles/epjconf/pdf/2014/04/epjconf_efm-13_02068.pdf
dcterms:description
Measurement of velocity upstream and downstream a special wire mesh was performed to ascertain the effect of the mesh on the flow. The mesh consisted of two components, a basic rectangular mesh with mesh width 1.22 mm and wire diameter 0.2 mm, and a top steel wool with random position of wires and wire diameter 0.05 mm. The velocity was measured by Constant Temperature Anemometry using single wire probe in a Plexiglas channel of rectangular cross-section. As a first step, measurement of one horizontal and one vertical measuring line was performed 10 mm upstream and 6 mm downstream the wire mesh. A spatial velocity profile upstream of the wire mesh was smooth, while the downstream velocity profile was highly disturbed. However, velocity fluctuations expressed in terms of turbulence intensity downstream of the wire mesh were attenuated down to 1%. Further measurements of the area downstream the wire mesh will be performed to describe the development of the flow. Measurement of velocity upstream and downstream a special wire mesh was performed to ascertain the effect of the mesh on the flow. The mesh consisted of two components, a basic rectangular mesh with mesh width 1.22 mm and wire diameter 0.2 mm, and a top steel wool with random position of wires and wire diameter 0.05 mm. The velocity was measured by Constant Temperature Anemometry using single wire probe in a Plexiglas channel of rectangular cross-section. As a first step, measurement of one horizontal and one vertical measuring line was performed 10 mm upstream and 6 mm downstream the wire mesh. A spatial velocity profile upstream of the wire mesh was smooth, while the downstream velocity profile was highly disturbed. However, velocity fluctuations expressed in terms of turbulence intensity downstream of the wire mesh were attenuated down to 1%. Further measurements of the area downstream the wire mesh will be performed to describe the development of the flow.
dcterms:title
Measurement of the airflow velocity upstream and downstream a wire mesh using constant temperature anemometry Measurement of the airflow velocity upstream and downstream a wire mesh using constant temperature anemometry
skos:prefLabel
Measurement of the airflow velocity upstream and downstream a wire mesh using constant temperature anemometry Measurement of the airflow velocity upstream and downstream a wire mesh using constant temperature anemometry
skos:notation
RIV/00216305:26210/13:PU111467!RIV15-MSM-26210___
n3:aktivita
n14:S n14:P
n3:aktivity
P(ED0002/01/01), P(EE2.3.30.0039), S
n3:dodaniDat
n6:2015
n3:domaciTvurceVysledku
n7:4040619 Tuhovčák, Ján n7:1060910
n3:druhVysledku
n18:D
n3:duvernostUdaju
n5:S
n3:entitaPredkladatele
n19:predkladatel
n3:idSjednocenehoVysledku
86762
n3:idVysledku
RIV/00216305:26210/13:PU111467
n3:jazykVysledku
n22:eng
n3:klicovaSlova
constant temperature anemometry, velocity, wire mesh, wire screen
n3:klicoveSlovo
n10:constant%20temperature%20anemometry n10:velocity n10:wire%20screen n10:wire%20mesh
n3:kontrolniKodProRIV
[F1278E9C348A]
n3:mistoKonaniAkce
Kutná Hora
n3:mistoVydani
TU Liberec, Kutna Hora, CZECH REPUBLIC
n3:nazevZdroje
International conference Experimental Fluid Mechanics 2013
n3:obor
n23:BK
n3:pocetDomacichTvurcuVysledku
3
n3:pocetTvurcuVysledku
3
n3:projekt
n15:ED0002%2F01%2F01 n15:EE2.3.30.0039
n3:rokUplatneniVysledku
n6:2013
n3:tvurceVysledku
Tuhovčák, Ján Lízal, František Jícha, Miroslav
n3:typAkce
n20:WRD
n3:wos
000343672100071
n3:zahajeniAkce
2013-11-19+01:00
s:numberOfPages
4
n4:doi
10.1051/epjconf/20146702068
n17:hasPublisher
E D P SCIENCES
n16:isbn
978-80-260-5375-0
n9:organizacniJednotka
26210