2015
DOI: 10.1093/imamat/hxv016
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Liquid-bridge shape stability by energy bounding

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Cited by 9 publications
(2 citation statements)
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“…Stickiness, in particular, is characterized by three parameters: maximum stickiness value Lmax, maximum sticking moisture wmax and initial sticking moisture w0 [18]. Stickiness does not appear when the moisture is below w0, at which the water pressures are equal in the form of a "film" (pʹ) and a "cuff" (pʹʹ) [19,20]. Sticking occurs at moisture values w > w0 as a result of the pressure difference ∆p=pʹʹ-pʹ which taking into account ( 8), ( 9) and (10), is obtained in the form…”
Section: Methodsmentioning
confidence: 99%
“…Stickiness, in particular, is characterized by three parameters: maximum stickiness value Lmax, maximum sticking moisture wmax and initial sticking moisture w0 [18]. Stickiness does not appear when the moisture is below w0, at which the water pressures are equal in the form of a "film" (pʹ) and a "cuff" (pʹʹ) [19,20]. Sticking occurs at moisture values w > w0 as a result of the pressure difference ∆p=pʹʹ-pʹ which taking into account ( 8), ( 9) and (10), is obtained in the form…”
Section: Methodsmentioning
confidence: 99%
“…The interplay between temperature gradients and surface tension forces gives rise to intriguing fluid flow patterns and transport phenomena, making TCC an area of significant interest in both fundamental and applied research. A large number of theoretical and experimental papers have been published over time to study the behaviour of liquid bridges in microgravity environments, but most have only considered the behaviour of axially symmetric liquid bridges [1][2][3], with only a few studies of the behaviour of non-axially symmetric liquid bridges [4,5] and of special forms of liquid bridges [6][7][8]. Lowry and Steen [9] extended the application to capillary surfaces from axisymmetric liquid bridges to droplets and non-axisymmetric liquid bridges.…”
Section: Introductionmentioning
confidence: 99%