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Statements

Subject Item
n2:RIV%2F00216305%3A26210%2F11%3APU92526%21RIV12-GA0-26210___
rdf:type
skos:Concept n15:Vysledek
dcterms:description
Original numerical model was applied to the simulation of the temperature field of concast steel slab, when melt of steel of quality A finished and immediately the melt of quality B followed. In the secondary-cooling zone in the unbending point, the breakout of the steel can occur in points of increased local chemical and temperature heterogeneity of the steel. The temperature field of the slab was calculated for three variants of the chemical composition. The first variant is for the chemical composition of steel quality A, the second for the chemical composition of steel quality B and the third for the average chemical composition from quality A and quality B. The temperature model was provides the temperature history of every points of a cross-section during its movement through the whole caster from the level of the melt in the crystallizer to the cutting torch, the course of isoliquidus, isosolidus and next isotherms, further temperature isozones. Heat transfer coefficient beneath the Original numerical model was applied to the simulation of the temperature field of concast steel slab, when melt of steel of quality A finished and immediately the melt of quality B followed. In the secondary-cooling zone in the unbending point, the breakout of the steel can occur in points of increased local chemical and temperature heterogeneity of the steel. The temperature field of the slab was calculated for three variants of the chemical composition. The first variant is for the chemical composition of steel quality A, the second for the chemical composition of steel quality B and the third for the average chemical composition from quality A and quality B. The temperature model was provides the temperature history of every points of a cross-section during its movement through the whole caster from the level of the melt in the crystallizer to the cutting torch, the course of isoliquidus, isosolidus and next isotherms, further temperature isozones. Heat transfer coefficient beneath the
dcterms:title
THE CALCULATION OF THE TEMPERATURE FIELD OF A CONCAST STEEL SLAB TIGHTLY BEFORE THE BREAKOUT THE CALCULATION OF THE TEMPERATURE FIELD OF A CONCAST STEEL SLAB TIGHTLY BEFORE THE BREAKOUT
skos:prefLabel
THE CALCULATION OF THE TEMPERATURE FIELD OF A CONCAST STEEL SLAB TIGHTLY BEFORE THE BREAKOUT THE CALCULATION OF THE TEMPERATURE FIELD OF A CONCAST STEEL SLAB TIGHTLY BEFORE THE BREAKOUT
skos:notation
RIV/00216305:26210/11:PU92526!RIV12-GA0-26210___
n15:predkladatel
n16:orjk%3A26210
n4:aktivita
n11:P
n4:aktivity
P(GA106/08/0606), P(GA106/09/0940), P(GA106/09/0969), P(GAP107/11/1566)
n4:dodaniDat
n20:2012
n4:domaciTvurceVysledku
n7:9844740 n7:1917781 n7:8193312 n7:5419174 n7:2766108
n4:druhVysledku
n18:D
n4:duvernostUdaju
n22:S
n4:entitaPredkladatele
n14:predkladatel
n4:idSjednocenehoVysledku
189032
n4:idVysledku
RIV/00216305:26210/11:PU92526
n4:jazykVysledku
n13:eng
n4:klicovaSlova
concast slab, temperature field, chemical composition, breakout, criteria of similarity
n4:klicoveSlovo
n9:temperature%20field n9:chemical%20composition n9:concast%20slab n9:criteria%20of%20similarity n9:breakout
n4:kontrolniKodProRIV
[D57900563773]
n4:mistoKonaniAkce
Brno
n4:mistoVydani
Ostrava
n4:nazevZdroje
METAL 2011 Conference Proceedings, (CD ROM Paper 774)
n4:obor
n21:JG
n4:pocetDomacichTvurcuVysledku
5
n4:pocetTvurcuVysledku
6
n4:projekt
n8:GA106%2F08%2F0606 n8:GAP107%2F11%2F1566 n8:GA106%2F09%2F0969 n8:GA106%2F09%2F0940
n4:rokUplatneniVysledku
n20:2011
n4:tvurceVysledku
Sekanina, Bohumil Kavička, František Mauder, Tomáš Stránský, Karel Štětina, Josef
n4:typAkce
n19:WRD
n4:zahajeniAkce
2011-05-18+02:00
s:numberOfPages
6
n6:hasPublisher
Tanger s.r.o.
n12:isbn
978-80-87294-24-6
n17:organizacniJednotka
26210