Impact of melt flow on the process of glass melting
Identifikátory výsledku
Kód výsledku v IS VaVaI
<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F67985891%3A_____%2F22%3A00562745" target="_blank" >RIV/67985891:_____/22:00562745 - isvavai.cz</a>
Nalezeny alternativní kódy
RIV/60461373:22310/22:43925518
Výsledek na webu
<a href="https://www.tandfonline.com/doi/full/10.1080/21870764.2022.2099102" target="_blank" >https://www.tandfonline.com/doi/full/10.1080/21870764.2022.2099102</a>
DOI - Digital Object Identifier
<a href="http://dx.doi.org/10.1080/21870764.2022.2099102" target="_blank" >10.1080/21870764.2022.2099102</a>
Alternativní jazyky
Jazyk výsledku
angličtina
Název v původním jazyce
Impact of melt flow on the process of glass melting
Popis výsledku v původním jazyce
The glass melting process was mathematically modeled in the designed space to establish the controlled melt flow and study its effect on the process character and melting performance. The conversion region of the space with combined heating was intended for batch conversion, and the homogenization region heated by the longitudinal energy barrier guaranteed bubble removal and sand dissolution. The theoretical background was formulated to define the melt flow conditions in a space with batch blanket. High batch conversion rates were acquired under conditions of structured heating, and the values increased almost linearly with the growing fraction of combustion heat delivered in the space conversion region. The increased fraction of total heat in the conversion region and cooling effect of the flue gases adjusted the effective helical flow in the space homogenization region, increased the space utilization and, consequently, the melting performance. The effects of energy distribution and position of the batch borderline on the sand dissolution and bubble removal kinetics were clarified, and the competence of modeling results for advanced melting was discussed.
Název v anglickém jazyce
Impact of melt flow on the process of glass melting
Popis výsledku anglicky
The glass melting process was mathematically modeled in the designed space to establish the controlled melt flow and study its effect on the process character and melting performance. The conversion region of the space with combined heating was intended for batch conversion, and the homogenization region heated by the longitudinal energy barrier guaranteed bubble removal and sand dissolution. The theoretical background was formulated to define the melt flow conditions in a space with batch blanket. High batch conversion rates were acquired under conditions of structured heating, and the values increased almost linearly with the growing fraction of combustion heat delivered in the space conversion region. The increased fraction of total heat in the conversion region and cooling effect of the flue gases adjusted the effective helical flow in the space homogenization region, increased the space utilization and, consequently, the melting performance. The effects of energy distribution and position of the batch borderline on the sand dissolution and bubble removal kinetics were clarified, and the competence of modeling results for advanced melting was discussed.
Klasifikace
Druh
J<sub>imp</sub> - Článek v periodiku v databázi Web of Science
CEP obor
—
OECD FORD obor
20504 - Ceramics
Návaznosti výsledku
Projekt
<a href="/cs/project/TH02020316" target="_blank" >TH02020316: Pokročilé technologie výroby skel</a><br>
Návaznosti
P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)
Ostatní
Rok uplatnění
2022
Kód důvěrnosti údajů
S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů
Údaje specifické pro druh výsledku
Název periodika
Journal of Asian Ceramic Societies
ISSN
2187-0764
e-ISSN
2187-0764
Svazek periodika
10
Číslo periodika v rámci svazku
3
Stát vydavatele periodika
GB - Spojené království Velké Británie a Severního Irska
Počet stran výsledku
17
Strana od-do
621-637
Kód UT WoS článku
000827017900001
EID výsledku v databázi Scopus
2-s2.0-85134368566