2008
DOI: 10.1007/s12217-008-9040-5
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Velocity Distribution of Vibration-driven Granular Gas in Knudsen Regime in Microgravity

Abstract: Dynamics of quasi-2D dissipative granular gas is studied in micro-gravity condition (of the order of 10 −4 g) in the limit of Knudsen regime. The gas, made of 4 spheres, is confined in a square cell enforced to follow linear sinusoidal vibration in ten different vibration modes. The trajectory of one of the particles is followed for 2 hours, and is reconstructed from video data by particle tracking. From statistical analysis, we find that (i) loss due to wall friction is small, (ii) trajectory looks ergodic in… Show more

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Cited by 47 publications
(39 citation statements)
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“…Experimental systems of driven granular gases typically consists of collections of granular particles, such as steel, glass beads, etc., that may be spherical, ellipsoidal, dumbbell-shaped, etc., that undergo inelastic collisions and is driven either through collision of the particles with vibrating walls [24,25,26,27,28,29,30,31,32,33,34,35,22,36,37] or as bilayers where the vibrated bottom layer drives the top layer [38,39,40], or by using electric [41,42] or magnetic fields [43,44]. In some experiments, the effects of gravity are minimised by performing them in microgravity [45,46,47]. Several experiments observe a universal stretched exponential form P(v) ∼ exp(−a|v| β ) with β ≈ 1.5 for wide range of system parameters [29,31,41,34,35,45,22,36], while other experiments find that β differs from 1.5 and lies between 1 and 2 or is a gaussian, and may depend on the driving parameters [28,30,32,39,43,46,37,44,40,47].…”
mentioning
confidence: 99%
“…Experimental systems of driven granular gases typically consists of collections of granular particles, such as steel, glass beads, etc., that may be spherical, ellipsoidal, dumbbell-shaped, etc., that undergo inelastic collisions and is driven either through collision of the particles with vibrating walls [24,25,26,27,28,29,30,31,32,33,34,35,22,36,37] or as bilayers where the vibrated bottom layer drives the top layer [38,39,40], or by using electric [41,42] or magnetic fields [43,44]. In some experiments, the effects of gravity are minimised by performing them in microgravity [45,46,47]. Several experiments observe a universal stretched exponential form P(v) ∼ exp(−a|v| β ) with β ≈ 1.5 for wide range of system parameters [29,31,41,34,35,45,22,36], while other experiments find that β differs from 1.5 and lies between 1 and 2 or is a gaussian, and may depend on the driving parameters [28,30,32,39,43,46,37,44,40,47].…”
mentioning
confidence: 99%
“…Therefore, experimental systems must be very large to have invariant conditions at least in the center region of the system, far from the confinement; (c) gravitation impedes force-free conditions. While (c) can be overcome by performing experiments in microgravity [28][29][30], arguments (a) and (b) persist.…”
mentioning
confidence: 99%
“…We shall particularly focus on the ratio between rotational and translational temperatures. Several other groups have already presented experimental results on granular flow under such conditions [27][28][29][30], but to our knowledge, this is the first experimental study giving access to rotational and translational velocities and so the corresponding temperatures.…”
Section: Translational and Rotational Temperaturesmentioning
confidence: 90%