2022
DOI: 10.48550/arxiv.2202.06342
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The water entry surface seal behavior of spheres at intermediate speed regimes

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“…Normalizing the seal time, we find that t cs U/D is constant for the disk impacts in the above-surface seal regime (figure 9e). For sphere water entry in the same We D range (2 × 10 3 − 3 × 10 4 ), Gilbarg & Anderson (1948) and Kiyama et al (2022) also found that t cs U/D is constant. Eshraghi et al (2020) rationalized this behaviour for spheres with a scaling analysis that balanced the radial splash rim inertia with the Bernoulli-induced pressure difference across the splash curtain that drives it to seal.…”
Section: Cavity Sealmentioning
confidence: 79%
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“…Normalizing the seal time, we find that t cs U/D is constant for the disk impacts in the above-surface seal regime (figure 9e). For sphere water entry in the same We D range (2 × 10 3 − 3 × 10 4 ), Gilbarg & Anderson (1948) and Kiyama et al (2022) also found that t cs U/D is constant. Eshraghi et al (2020) rationalized this behaviour for spheres with a scaling analysis that balanced the radial splash rim inertia with the Bernoulli-induced pressure difference across the splash curtain that drives it to seal.…”
Section: Cavity Sealmentioning
confidence: 79%
“…where m c ≈ ρwA is the splash curtain mass, R c the radial position of the curtain, A the splash curtain surface area, w the curtain thickness, ρ g the gas density and U g (t) the mean gas flow velocity into the cavity. Equation (6.1) assumes that the air-flow-induced pressure difference across the splash curtain is the dominant force, which is a reasonable assumption for these impact speeds (Lee 2000; Eshraghi et al 2020;Kiyama et al 2022). Simplifying (6.1) gives…”
Section: Cavity Sealmentioning
confidence: 99%