![]() Terwagne, Denis ![]() ![]() ![]() Conference (2009, May) Detailed reference viewed: 13 (5 ULiège)![]() Terwagne, Denis ![]() ![]() Poster (2009, March) Detailed reference viewed: 17 (4 ULiège)![]() ![]() Ludewig, François ![]() ![]() ![]() in Powders and Grains 2009 (2009) Detailed reference viewed: 17 (6 ULiège)![]() Lumay, Geoffroy ![]() ![]() ![]() in Physical Review. E : Statistical, Nonlinear, and Soft Matter Physics (2009), 80 Detailed reference viewed: 43 (15 ULiège)![]() Gilet, Tristan ![]() ![]() ![]() in Physical Review. E : Statistical, Nonlinear, and Soft Matter Physics (2009) Detailed reference viewed: 134 (27 ULiège)![]() Vandewalle, Nicolas ![]() ![]() ![]() in Colloids and Surfaces A : Physicochemical and Engineering Aspects (2009), 344 Detailed reference viewed: 125 (20 ULiège)![]() Terwagne, Denis ![]() ![]() ![]() in Physics of Fluids (2009), 21 Detailed reference viewed: 66 (20 ULiège)![]() Terwagne, Denis ![]() ![]() in Chaos (2009) Detailed reference viewed: 60 (23 ULiège)![]() Dorbolo, Stéphane ![]() ![]() ![]() in New Journal of Physics (2009), 11 Detailed reference viewed: 61 (19 ULiège)![]() Caps, Hervé ![]() ![]() in Europhysics Letters (2009), 88 Detailed reference viewed: 58 (25 ULiège)![]() Terwagne, Denis ![]() ![]() ![]() in Chaos (2008), 18(4), Detailed reference viewed: 52 (20 ULiège)![]() Dorbolo, Stéphane ![]() ![]() ![]() in New Journal of Physics (2008), 10 When an oil droplet is placed on a quiescent oil bath, it eventually collapses into the bath due to gravity. The resulting coalescence may be eliminated when the bath is vertically vibrated. The droplet ... [more ▼] When an oil droplet is placed on a quiescent oil bath, it eventually collapses into the bath due to gravity. The resulting coalescence may be eliminated when the bath is vertically vibrated. The droplet bounces periodically on the bath, and the air layer between the droplet and the bath is replenished at each bounce. This sustained bouncing motion is achieved when the forcing acceleration is higher than a threshold value. When the droplet has a sufficiently low viscosity, it significantly deforms: spherical harmonic Y-1(m) modes are excited, resulting in resonant effects on the threshold acceleration curve. Indeed, a lower acceleration is needed when I modes with m = 0 are excited. Modes m not equal 0 are found to decrease the bouncing ability of the droplet. A break of degeneracy is observed for the m parameter. In particular, when the mode 1 = 2 and m = 1 is excited, the droplet rolls on the vibrated surface without touching it, leading to a new self-propulsion mode. [less ▲] Detailed reference viewed: 37 (15 ULiège)![]() Terwagne, Denis ![]() ![]() ![]() Poster (2008, November) When a low viscosity oil droplet is laid onto the surface of a high viscosity oil liquid, it stays at rest for a moment before coalescence. The coalescence can be delayed and sometimes inhibited by ... [more ▼] When a low viscosity oil droplet is laid onto the surface of a high viscosity oil liquid, it stays at rest for a moment before coalescence. The coalescence can be delayed and sometimes inhibited by injecting fresh air under the droplet. This can happen when the surface of the bath oscillates vertically. In this case the droplet basically bounces on the interface [1, 2]. We observe that the conditions for bouncing depends on the frequency, more precisely we observe resonance when the eigenfrequency of the droplet is excited. Lord Rayleigh expressed the droplet deformation modes in terms of spherical harmonics Y m. We present different l experimental mode of deformation with the corresponding spherical harmonic model. In some conditions, a droplet presents a non axi-symmetric mode of deformation. That leads to a rotation of the droplet and to a horizontal displacement. [less ▲] Detailed reference viewed: 20 (2 ULiège)![]() Terwagne, Denis ![]() ![]() ![]() Conference (2008, November) Droplet coalescence in a liquid bath can be delayed by oscillating the surface of the bath vertically (frequency from 20 Hz to 400 Hz), the droplet bounces on the interface [1,2]. A low viscous oil ... [more ▼] Droplet coalescence in a liquid bath can be delayed by oscillating the surface of the bath vertically (frequency from 20 Hz to 400 Hz), the droplet bounces on the interface [1,2]. A low viscous oil droplet is dropped on a high viscous oil bath. We observe that the conditions for bouncing depends on the frequency, more precisely we observe resonance when the eigenfrequency of the droplet is excited. In some conditions, droplet presents a non axi-symmetric mode of deformation. That leads to a rotation of the drop and to a horizontal displacement. [less ▲] Detailed reference viewed: 12 (2 ULiège)![]() Terwagne, Denis ![]() ![]() ![]() Poster (2008, May) Detailed reference viewed: 11 (6 ULiège)![]() Terwagne, Denis ![]() ![]() ![]() Poster (2008, May) Detailed reference viewed: 16 (6 ULiège)![]() Terwagne, Denis ![]() ![]() ![]() Poster (2008, March) Detailed reference viewed: 19 (7 ULiège)![]() Terwagne, Denis ![]() ![]() in Physicalia Magazine (2008), 30(3), 161-168 When a low viscosity oil droplet is laid onto the surface ofa high viscosity oil liquid, it stays at rest for a moment before coalescence. The coalescence can be delayed and sometimes inlibited by ... [more ▼] When a low viscosity oil droplet is laid onto the surface ofa high viscosity oil liquid, it stays at rest for a moment before coalescence. The coalescence can be delayed and sometimes inlibited by injecting fresh air under the droplet. This can happen when the surface ofthe bath oscillates vertically. In this case the droplet basically bounces on the interface. We obsewe that the conditions for bouncing depends on the frequency, more precisely we observe resonance when the eigenfrequency of the droplet is excited. In some conditions, a droplet presents a non axi- symmetric mode of deformation. That leads to a rotation of the droplet and to a horizontal displacement. [less ▲] Detailed reference viewed: 52 (7 ULiège)![]() Gilet, Tristan ![]() ![]() ![]() in Physical Review Letters (2008), 100(16), Low viscosity (< 100 cSt) silicon oil droplets are placed on a high viscosity (1000 cSt) oil bath that vibrates vertically. The viscosity difference ensures that the droplet is more deformed than the bath ... [more ▼] Low viscosity (< 100 cSt) silicon oil droplets are placed on a high viscosity (1000 cSt) oil bath that vibrates vertically. The viscosity difference ensures that the droplet is more deformed than the bath interface. Droplets bounce periodically on the bath when the acceleration of its sinusoidal motion is larger than a threshold value. The threshold is minimum for a particular frequency of excitation: droplet and bath motions are in resonance. The bouncing droplet has been modeled by considering the deformation of the droplet and the lubrication force exerted by the air layer between the droplet and the bath. Threshold values are predicted and found to be in good agreement with our measurements. [less ▲] Detailed reference viewed: 78 (18 ULiège)![]() Ludewig, François ![]() ![]() ![]() in Europhysics Letters [=EPL] (2008), 84(4), We report numerical investigations for the compaction dynamics of dense granular assemblies. The studies are based on the non-smooth contact dynamics model. Our work suggests that the dimensionless ... [more ▼] We report numerical investigations for the compaction dynamics of dense granular assemblies. The studies are based on the non-smooth contact dynamics model. Our work suggests that the dimensionless acceleration parameter Gamma, used by a large majortiy of authors, is not appropriate for rescaling the data. We prove that the dimensionless energy Xi, injected in the granular system at lift-off, is more appropriate and leads to robust interpretations of the compaction dynamics. Indeed, the injected energy allows to pass energy barriers that separate local equilibrium states. Using the Eyring picture of relaxation dynamic, we show that the consideration of Xi leads to a new law for compaction. [less ▲] Detailed reference viewed: 61 (30 ULiège) |
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