<?xml version="1.0"?>
<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/"><rdf:Description rdf:about="https://repozitorij.uni-lj.si/IzpisGradiva.php?id=178214"><dc:title>Emergence and dynamics of gas-accelerated liquid sheets</dc:title><dc:creator>Kovačič,	Krištof	(Avtor)
	</dc:creator><dc:creator>Zahoor,	Rizwan	(Avtor)
	</dc:creator><dc:creator>Kušar,	Jernej	(Avtor)
	</dc:creator><dc:creator>Bajt,	Saša	(Avtor)
	</dc:creator><dc:creator>Šarler,	Božidar	(Avtor)
	</dc:creator><dc:subject>ideal gas</dc:subject><dc:subject>physical quantities</dc:subject><dc:subject>computer simulation</dc:subject><dc:subject>finite volume methods</dc:subject><dc:subject>adaptive mesh refinement</dc:subject><dc:subject>gas liquid interfaces</dc:subject><dc:subject>fluid dynamics</dc:subject><dc:subject>fluid flows</dc:subject><dc:subject>fluid jets</dc:subject><dc:subject>multiphase flows</dc:subject><dc:description>This study examines the behavior of liquid chain, open rim, and transitional jet–liquid chain regimes in gas-accelerated liquid micro-sheets using experimentally validated numerical simulations. The simulations employ the finite volume method with a volume-of-fluid framework to resolve compressible ideal gas flow impinging on a Newtonian, laminar liquid jet under atmospheric conditions. Adaptive mesh refinement is used to resolve the gas–liquid interface. The validation of the model is performed based on a purpose-built experimental setup over the range of gas–liquid momentum flux ratios 0.03 &lt; MFR &lt; 2.6, and Weber numbers, evaluated at the liquid capillary inlet, 3.8 &lt; We &lt; 49, achieving an agreement of the simulated liquid-sheet shape below experimental uncertainty. Three typical flow regimes are explained by the interplay of gas momentum, liquid inertia, and surface tension, scaled by the liquid-sheet rim Weber number (We▫$_{rim}$▫), based on rim curvature and the rim transverse velocity. The transitional jet–liquid chain regime occurs at We▫$_{rim}$▫ &lt; 0.1; where the surface tension dominates, result- ing in only a slight change of the liquid jet cross section. In the liquid chain regime (0.1 &lt; We▫$_{rim}$▫ &lt; 1) gas inertia forms the sheet, then surface tension bends the rim inward, and transverse momentum transfer forms an orthogonal secondary link. In the open rim regime (We▫$_{rim}$▫ &gt; 2), dominant rim inertia prevents sheet closure. The Weber number (We), based on the nozzle inlet parameters, can predict the liquid chain regime in the range 1.5 ≤ MFR We▫$^{0.84}$▫ ≤ 4. This relation provides practical guidance for stable liquid chain operation.</dc:description><dc:date>2026</dc:date><dc:date>2026-01-21 13:06:20</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>178214</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
