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Linke, H.; Alemán, B. J.; Melling, L. D.; Taormina, M. J.; Francis, M. J.; Dow-Hygelund, C. C.; Narayanan, V.; Taylor, R. P.; Stout, A. Self-Propelled Leidenfrost Droplets. Phys. Rev. Lett. 2006, 96 (15), 154502.
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Most real surfaces show contact angle hysteresis. In many cases, hysteresis is due to some sort of imperfection. On a smooth surface, this imperfection may come from heterogeneities or contaminants. The analysis presented here is still valid if inherent hysteresis is zero
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Most real surfaces show contact angle hysteresis. In many cases, hysteresis is due to some sort of imperfection. On a smooth surface, this imperfection may come from heterogeneities or contaminants. The analysis presented here is still valid if inherent hysteresis is zero.
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Equations 4 and 5 are true for surface features that have a constant profile around the entire diameter of the capillary tube. If the shape of the sawtooth features shows radial variation or periodicity, then a different form of eqs 4 and 5 must be used in the analysis.
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Equations 4 and 5 are true for surface features that have a constant profile around the entire diameter of the capillary tube. If the shape of the sawtooth features shows radial variation or periodicity, then a different form of eqs 4 and 5 must be used in the analysis.
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If the liquid slug is shorter than the length of a single feature, then the analysis presented here probably is not valid. Otherwise, it should be fine
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If the liquid slug is shorter than the length of a single feature, then the analysis presented here probably is not valid. Otherwise, it should be fine.
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