2005
DOI: 10.1016/j.fluiddyn.2004.08.003
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Micro-fluid dynamics via laser metal surface interactions: Wave-vortex interpretation of emerging multiscale coherent structures

Abstract: Lugomer and colleagues have discovered filamentary-like coherent structures in small (∼3 mm diameter) laserbeam-metal-surface interactions. Experimental photographs of a small part of the laser spot area shows frozen "fossil" filament-like structures. We present reasonable arguments and preliminary computer results that suggest that these are due to vorticity deposited by accelerated flows due to blast and shock waves.

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Cited by 12 publications
(6 citation statements)
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“…RMI is known to appear in many natural phenomena ranging from astrophysical to atomic scales as well as in technological applications. Examples include supernova explosion with the formation of circumstellar structures (Kane et al 1999, Peng et al 2003, laser-material interactions (Fukumoto and Lugomer 2003, Zabusky et al 2005, Lugomer 2007, Lugomer 2016, 2017, 2018, laser inertial confinement fusion (Alon et al 1996, Nishihara et al 1998, Shvarts et al 2001, Matsuoka et al 2003, explosive combustion (Yang et al 1993), and shock-tube phenomena (Palekar et al 2007, Balakumar et al 2008, Probyn and Thornber 2013, Ting et al 2014.…”
Section: Introductionmentioning
confidence: 99%
“…RMI is known to appear in many natural phenomena ranging from astrophysical to atomic scales as well as in technological applications. Examples include supernova explosion with the formation of circumstellar structures (Kane et al 1999, Peng et al 2003, laser-material interactions (Fukumoto and Lugomer 2003, Zabusky et al 2005, Lugomer 2007, Lugomer 2016, 2017, 2018, laser inertial confinement fusion (Alon et al 1996, Nishihara et al 1998, Shvarts et al 2001, Matsuoka et al 2003, explosive combustion (Yang et al 1993), and shock-tube phenomena (Palekar et al 2007, Balakumar et al 2008, Probyn and Thornber 2013, Ting et al 2014.…”
Section: Introductionmentioning
confidence: 99%
“…Characteristics of plasma evolution also depend on the laser pulse duration and the wavelength. Considering the ns-LMIs and the wavelengths ranging from the far infrared CO 2 laser (λ = 10.8 µm, τ = 100 ns), to the infrared Nd-YAG laser (λ = 1.06 µm, τ = 40 ns), to the visible Ruby laser (τ = 30 ns, λ = 600 nm),and to the ultraviolet XeCl laser (λ = 308 nm, τ = 16-20 ns), one finds that in all cases plasma expansion depends on the interaction with the surrounding background gas [11,12]. The expanding plasma becomes a mixture of atoms and ions of both, vaporized target material (In, Co, Fe, Ti, etc.…”
Section: Short Outlines Of Plasmas Generated By Intense and Ultrainte...mentioning
confidence: 97%
“…Dynamics of plasmas created by ultraintense lasers are intended to mimic plasma dynamics in cosmic explosions and planetary cores creating ultrahigh-pressure shocks [47] In this respect, irradiation of a small sphere by an ultraintense laser creates intense shock waves and ultrahigh pressures reaching ~10 12 atmospheres. Such gigantic shock fronts are similar to the thin shock regions at the boundary between a collapsed supernova and the surrounding material-creating a spheroid of super-hot plasma.…”
Section: Plasmas Created By Ultraintense Power Lasersmentioning
confidence: 99%
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“…Across this layer the continuum hypothesis fails and steep changes in temperature, pressure and density occurs. It has been reported by Zabusky et al [15] that homogeneous boiling of the skin layer of material starts to occur directly beneath the liquid-vapour interface when the interface temperature reaches around 80% of the critical point. This accompanies a significant drop in the surface tension and huge amount of melt liquid superheat.…”
Section: Heat Conduction Across Thermal Boundary Layermentioning
confidence: 99%