296 research outputs found

    Crossover of the weighted mean fragment mass scaling in 2D brittle fragmentation

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    We performed vertical and horizontal sandwich 2D brittle fragmentation experiments. The weighted mean fragment mass was scaled using the multiplicity μ\mu. The scaling exponent crossed over at logμc1.4\log \mu_c \simeq -1.4. In the small μ(μc)\mu (\ll\mu_c) regime, the binomial multiplicative (BM) model was suitable and the fragment mass distribution obeyed log-normal form. However, in the large μ(μc)\mu (\gg\mu_c) regime, in which a clear power-law cumulative fragment mass distribution was observed, it was impossible to describe the scaling exponent using the BM model. We also found that the scaling exponent of the cumulative fragment mass distribution depended on the manner of impact (loading conditions): it was 0.5 in the vertical sandwich experiment, and approximately 1.0 in the horizontal sandwich experiment.Comment: 5 pages, 3 figure

    Fingering induced by a solid sphere impact to viscous fluid

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    The number of splashed fingers generated by a solid projectile's impact onto a viscous liquid layer is experimentally studied. A steel sphere is dropped onto a viscous liquid pool. Then, a fingering instability occurs around the crater's rim, depending on the experimental conditions such as projectile's inertia and the viscosity of the target liquid. When the impact inertia is not sufficient, any fingering structure cannot be observed. Contrastively, if the impact inertia is too much, the random splashing is induced and the counting of fingers becomes difficult. The clear fingering instability is observable in between these two regimes. The number of fingers NN is counted by using high-speed video data. The scaling of NN is discussed on the basis of dimensionless numbers. By assuming Rayleigh-Taylor instability, scaling laws for NN can be derived using Reynolds number ReRe, Weber number WeWe, and Froude number FrFr. Particularly, the scaling N=(ρrFr)1/4We1/2/33/4N=(\rho_r Fr)^{1/4}We^{1/2}/3^{3/4} is obtained for the gravity-dominant cratering regime, where ρr\rho_r is the density ratio between a projectile and a target. Although the experimental data considerably scatters, the scaling law is consistent with the global trend of the data behavior. Using one of the scaling laws, planetary nano crater's rim structure is also evaluated.Comment: 5 pages, 3 figure

    Dendritic side-branching with anisotropic viscous fingering

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    We studied dendritic side-branching mechanism in the experiment of anisotropic viscous fingering. We measured the time dependence of growth speed of side-branch and the envelop of side-branches. We found that the speed of side-branch gets to be faster than one of the stem and the growth exponent of the speed changes at a certain time. The envelope of side-branches is represented as Y ~ X^1.47.Comment: 8 pages, 8 figures, to submited in J. Crystal Growt
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