1944
DOI: 10.1002/jcp.1030240102
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Bubble formation in animals. I. Physical factors

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Cited by 351 publications
(152 citation statements)
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“…4,7,13,14 Thus, e.g., in a 46 kHz acoustic field, Barger 14 measured tensile strengths ranging from 1.2 bar in water saturated with air at 760 torr to 12.1 bar when saturated at 10 torr. Likewise, in acoustic cavitation experiments at 15 kHz Sirotyuk 7 found that by reducing the content of surface-active substances in water until only traces of them were present, a tensile strength of 7.5 bar could be obtained.…”
Section: Literature Analysis and Synthesismentioning
confidence: 99%
See 1 more Smart Citation
“…4,7,13,14 Thus, e.g., in a 46 kHz acoustic field, Barger 14 measured tensile strengths ranging from 1.2 bar in water saturated with air at 760 torr to 12.1 bar when saturated at 10 torr. Likewise, in acoustic cavitation experiments at 15 kHz Sirotyuk 7 found that by reducing the content of surface-active substances in water until only traces of them were present, a tensile strength of 7.5 bar could be obtained.…”
Section: Literature Analysis and Synthesismentioning
confidence: 99%
“…The immediate candidate would be free gas bubbles, but they either disappear by buoyancy, or shrink and dissolve due to diffusion of gas into the liquid, driven by the excess pressure in the bubble that is set up by surface tension-they are inherently unstable. 3 Harvey et al 4 suggested cavitation nuclei to be gas pockets stabilized in crevices of solid surfaces, either bounding walls or particles present in the liquid. Many experimental results could be explained from their model, but not all, and other models of stabilization of free gas bubbles were developed.…”
Section: Introductionmentioning
confidence: 99%
“…This puts a first constraint on when an ice drop can explode: R i /R o has to be small enough to make the pressure fall below the cavitation threshold of the liquid, which for clean water, free of gas pockets, can easily be 100 MPa into the negative [32,33]. Of course, for millimetric droplets, the micron sized gap formed by the crack will be an effective nucleation site, lowering the nucleation threshold to ∆P ≈ 2γ/x e ≈ 0.1 MPa [34], where γ ≈ 75 mN/m is the surface tension of water at 0 • C. However, for a small cloud droplet of say R o ∼ 10 µm, equation (3) predicts a hundred fold thinner gap, and a corresponding higher threshold tension. For such droplets the cavitation threshold would form a serious barrier to explosion.…”
mentioning
confidence: 99%
“…This effect would be similar to the induction of gushing by carbon, where adsorbed gases act as the nuclei; the carbon is simply a carrier and is not itself responsible for nucleation. 18 It should be noted that a high surface viscosity is not the "cause" of gushing but only a reflection of the intense surface activity which may be necessary to stabilize nuclei. Hence it is possible for non-gushing beers to have high surface viscosities.…”
Section: Discussionmentioning
confidence: 99%